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    <title>Open access article in Journal of Synchrotron Radiation</title>
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    <description>Synchrotron radiation research is rapidly expanding with many new sources of radiation being created globally. Synchrotron radiation plays a leading role in pure science and in emerging technologies.  The Journal of Synchrotron Radiation provides comprehensive coverage of the entire field of synchrotron radiation and free-electron laser research including instrumentation, theory, computing and scientific applications in areas such as biology, nanoscience and materials science. Rapid publication ensures an up-to-date information resource for scientists and engineers in the field.</description>
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    <dc:rights>Copyright (c) 2013 International Union of Crystallography</dc:rights>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:creator>International Union of Crystallography</dc:creator>
    <dc:source>http://journals.iucr.org</dc:source>
    <dc:identifier>urn:issn:0909-0495</dc:identifier>
    <dc:description>Synchrotron radiation research is rapidly expanding with many new sources of radiation being created globally. Synchrotron radiation plays a leading role in pure science and in emerging technologies.  The Journal of Synchrotron Radiation provides comprehensive coverage of the entire field of synchrotron radiation and free-electron laser research including instrumentation, theory, computing and scientific applications in areas such as biology, nanoscience and materials science. Rapid publication ensures an up-to-date information resource for scientists and engineers in the field.</dc:description>
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    <dc:title>Open access article in Journal of Synchrotron Radiation</dc:title>
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    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>Copyright (c) 2013 International Union of Crystallography</prism:copyright>
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    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0506</link>
    <dc:rights>Copyright (c) 2013 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2013-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049513008960</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2013 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-05-01</prism:publicationDate>
    <prism:startingPage>515</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
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  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5054">
    <title>Efficient focusing of 8 keV X-rays with multilayer Fresnel zone plates fabricated by atomic layer deposition and focused ion beam milling</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5054</link>
    <description>Fresnel zone plates (FZPs) recently showed significant improvement by focusing soft X-rays down to ∼10 nm. In contrast to soft X-rays, generally a very high aspect ratio FZP is needed for efficient focusing of hard X-rays. Therefore, FZPs had limited success in the hard X-ray range owing to difficulties of manufacturing high-aspect-ratio zone plates using conventional techniques. Here, employing a method of fabrication based on atomic layer deposition (ALD) and focused ion beam (FIB) milling, FZPs with very high aspect ratios were prepared. Such multilayer FZPs with outermost zone widths of 10 and 35 nm and aspect ratios of up to 243 were tested for their focusing properties at 8 keV and shown to focus hard X-rays efficiently. This success was enabled by the outstanding layer quality thanks to ALD. Via the use of FIB for slicing the multilayer structures, desired aspect ratios could be obtained by precisely controlling the thickness. Experimental diffraction efficiencies of multilayer FZPs fabricated via this combination reached up to 15.58% at 8 keV. In addition, scanning transmission X-ray microscopy experiments at 1.5 keV were carried out using one of the multilayer FZPs and resolved a 60 nm feature size. Finally, the prospective of different material combinations with various outermost zone widths at 8 and 17 keV is discussed in the light of the coupled wave theory and the thin-grating approximation. Al2O3/Ir is outlined as a promising future material candidate for extremely high resolution with a theoretical efficiency of more than 20% for as small an outermost zone width as 10 nm at 17 keV.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Mayer, M.</dc:creator>
    <dc:creator>Keskinbora, K.</dc:creator>
    <dc:creator>Grévent, C.</dc:creator>
    <dc:creator>Szeghalmi, A.</dc:creator>
    <dc:creator>Knez, M.</dc:creator>
    <dc:creator>Weigand, M.</dc:creator>
    <dc:creator>Snigirev, A.</dc:creator>
    <dc:creator>Snigireva, I.</dc:creator>
    <dc:creator>Schütz, G.</dc:creator>
    <dc:date>2013-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049513006602</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The fabrication and performance of multilayer Al2O3/Ta2O5 Fresnel zone plates in the hard X-ray range and a discussion of possible future developments considering available materials are reported.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SPUTTERED-SLICED; MULTILAYER; FRESNEL ZONE PLATE; HARD X-RAY; ALD; FIB</dc:subject>
    <dc:description>Fresnel zone plates (FZPs) recently showed significant improvement by focusing soft X-rays down to ∼10 nm. In contrast to soft X-rays, generally a very high aspect ratio FZP is needed for efficient focusing of hard X-rays. Therefore, FZPs had limited success in the hard X-ray range owing to difficulties of manufacturing high-aspect-ratio zone plates using conventional techniques. Here, employing a method of fabrication based on atomic layer deposition (ALD) and focused ion beam (FIB) milling, FZPs with very high aspect ratios were prepared. Such multilayer FZPs with outermost zone widths of 10 and 35 nm and aspect ratios of up to 243 were tested for their focusing properties at 8 keV and shown to focus hard X-rays efficiently. This success was enabled by the outstanding layer quality thanks to ALD. Via the use of FIB for slicing the multilayer structures, desired aspect ratios could be obtained by precisely controlling the thickness. Experimental diffraction efficiencies of multilayer FZPs fabricated via this combination reached up to 15.58% at 8 keV. In addition, scanning transmission X-ray microscopy experiments at 1.5 keV were carried out using one of the multilayer FZPs and resolved a 60 nm feature size. Finally, the prospective of different material combinations with various outermost zone widths at 8 and 17 keV is discussed in the light of the coupled wave theory and the thin-grating approximation. Al2O3/Ir is outlined as a promising future material candidate for extremely high resolution with a theoretical efficiency of more than 20% for as small an outermost zone width as 10 nm at 17 keV.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Efficient focusing of 8 keV X-rays with multilayer Fresnel zone plates fabricated by atomic layer deposition and focused ion beam milling</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-05-01</prism:publicationDate>
    <prism:startingPage>433</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
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  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0502">
    <title>Free-electron lasers and JSR</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0502</link>
    <dc:rights>Copyright (c) 2013 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schlichting, I.</dc:creator>
    <dc:date>2013-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049513004147</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Editorial.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Free-electron lasers and JSR</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2013 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-03-01</prism:publicationDate>
    <prism:startingPage>209</prism:startingPage>
    <prism:section>editorial</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>210</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
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  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0495">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0495</link>
    <dc:rights>Copyright (c) 2013 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2013-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049513003798</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2013 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-03-01</prism:publicationDate>
    <prism:startingPage>393</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>394</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5039">
    <title>Radiation damage to biological macromolecules: some answers and more questions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5039</link>
    <description>Research into radiation damage in macromolecular crystallography has matured over the last few years, resulting in a better understanding of both the processes and timescales involved. In turn this is now allowing practical recommendations for the optimization of crystal dose lifetime to be suggested. Some long-standing questions have been answered by recent investigations, and from these answers new challenges arise and areas of investigation can be proposed. Six papers published in this volume give an indication of some of the current directions of this field and also that of single-particle cryo-microscopy, and the brief summary below places them into the overall framework of ongoing research into macromolecular crystallography radiation damage.</description>
    <dc:rights>Copyright (c) 2013 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:creator>Weik, M.</dc:creator>
    <dc:date>2013-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512050418</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Introductory overview to the special issue papers on radiation damage to biological macromolecules.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY AND ELECTRON RADIATION DAMAGE; MACROMOLECULAR CRYSTALLOGRAPHY; RADICAL SCAVENGER; TEMPERATURE DEPENDENCE; XFEL</dc:subject>
    <dc:description>Research into radiation damage in macromolecular crystallography has matured over the last few years, resulting in a better understanding of both the processes and timescales involved. In turn this is now allowing practical recommendations for the optimization of crystal dose lifetime to be suggested. Some long-standing questions have been answered by recent investigations, and from these answers new challenges arise and areas of investigation can be proposed. Six papers published in this volume give an indication of some of the current directions of this field and also that of single-particle cryo-microscopy, and the brief summary below places them into the overall framework of ongoing research into macromolecular crystallography radiation damage.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Radiation damage to biological macromolecules: some answers and more questions</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2013 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-01-01</prism:publicationDate>
    <prism:startingPage>1</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>6</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5215">
    <title>Enhancement in statistical and image analysis for in situ µSXRF studies of elemental distribution and co-localization, using Dioscorea balcanica</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5215</link>
    <description>Synchrotron-based X-ray microfluorescence (µSXRF) is an analytical method suitable for in situ investigation of the distribution of micronutrient and macronutrient elements in several-micrometres-thick unstained biological samples, e.g. single cells and tissues. Elements are mapped and quantified at sub-p.p.m. concentrations. In this study the quantity, distribution and grouping/co-localization of various elements have been identified in straight and twisted internodes of the stems of the monocotyledonous climber D. balcanica Košanin. Three different statistical methods were employed to analyse the macro­nutrient and micronutrient distributions and co-localization. Macronutrient elements (K, P, Ca, Cl) are distributed homogeneously in both straight and twisted internodes. Micronutrient elements are mostly grouped in the vasculature and in the sclerenchyma cell layer. In addition, co-localization of micronutrient elements is much more prominent in twisted than in straight internodes. These image analyses and statistical methods provided very similar outcomes and could be applied to various types of biological samples imaged by µSXRF.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Dučić, T.</dc:creator>
    <dc:creator>Borchert, M.</dc:creator>
    <dc:creator>Savić, A.</dc:creator>
    <dc:creator>Kalauzi, A.</dc:creator>
    <dc:creator>Mitrović, A.</dc:creator>
    <dc:creator>Radotić, K.</dc:creator>
    <dc:date>2013-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512050170</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Synchrotron-radiation-based X-ray microfluorescence has been used for in situ investigation of the distribution of micronutrient and macronutrient elements in an unstained cross section of a stem of monocotyledonous liana plant Dioscorea balcanica Košanin. The elemental allocation has been quantified and the grouping/co-localization in straight and twisted stem internodes has been analysed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY FLUORESCENCE MICROSCOPY; IMAGE ANALYSIS; STATISTICAL ANALYSIS; DIOSCOREABALCANICA KOSANIN</dc:subject>
    <dc:description>Synchrotron-based X-ray microfluorescence (µSXRF) is an analytical method suitable for in situ investigation of the distribution of micronutrient and macronutrient elements in several-micrometres-thick unstained biological samples, e.g. single cells and tissues. Elements are mapped and quantified at sub-p.p.m. concentrations. In this study the quantity, distribution and grouping/co-localization of various elements have been identified in straight and twisted internodes of the stems of the monocotyledonous climber D. balcanica Košanin. Three different statistical methods were employed to analyse the macro­nutrient and micronutrient distributions and co-localization. Macronutrient elements (K, P, Ca, Cl) are distributed homogeneously in both straight and twisted internodes. Micronutrient elements are mostly grouped in the vasculature and in the sclerenchyma cell layer. In addition, co-localization of micronutrient elements is much more prominent in twisted than in straight internodes. These image analyses and statistical methods provided very similar outcomes and could be applied to various types of biological samples imaged by µSXRF.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Enhancement in statistical and image analysis for in situ µSXRF studies of elemental distribution and co-localization, using Dioscorea balcanica</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-03-01</prism:publicationDate>
    <prism:startingPage>339</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>346</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ve5014">
    <title>Mo/Si multilayer-coated amplitude-division beam splitters for XUV radiation sources</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ve5014</link>
    <description>Amplitude-division beam splitters for XUV radiation sources have been developed and extensively characterized. Mo/Si multilayer coatings were deposited on 50 nm-thick SiN membranes. By changing the multilayer structure (periodicity, number of bilayers, etc.) the intensity of the reflected and transmitted beams were optimized for selected incident radiation parameters (wavelength, incident angle). The developed optical elements were characterized by means of XUV reflectometry and transmission measurements, atomic force microscopy and optical interferometry. Special attention was paid to the spatial homogeneity of the optical response and reflected beam wavefront distortions. Here the results of the characterization are presented and improvements required for advanced applications at XUV free-electron lasers are identified. A flatness as low as 4 nm r.m.s. on 3 × 3 mm beam splitters and 22 nm r.m.s. on 10 × 10 mm beam splitters has been obtained. The high-spatial-frequency surface roughness was about 0.7–1 nm r.m.s. The middle-spatial-frequency roughness was in the range 0.2–0.8 nm r.m.s. The reflection and transmission of the beam splitters were found to be very homogeneous, with a deviation of less than 2% across the full optical element.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sobierajski, R.</dc:creator>
    <dc:creator>Loch, R.A.</dc:creator>
    <dc:creator>van de Kruijs, R.W.E.</dc:creator>
    <dc:creator>Louis, E.</dc:creator>
    <dc:creator>von Blanckenhagen, G.</dc:creator>
    <dc:creator>Gullikson, E.M.</dc:creator>
    <dc:creator>Siewert, F.</dc:creator>
    <dc:creator>Wawro, A.</dc:creator>
    <dc:creator>Bijkerk, F.</dc:creator>
    <dc:date>2013-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512049990</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Short-wavelength XUV beam splitters consisting of multilayer reflective and transmissive coatings on 3 × 3 mm and 10 × 10 mm SiN membranes have been developed and fully characterized.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MO/SI; MULTILAYER; XUV; BEAM SPLITTER; FREE-ELECTRON LASER; AMPLITUDE DIVISION</dc:subject>
    <dc:description>Amplitude-division beam splitters for XUV radiation sources have been developed and extensively characterized. Mo/Si multilayer coatings were deposited on 50 nm-thick SiN membranes. By changing the multilayer structure (periodicity, number of bilayers, etc.) the intensity of the reflected and transmitted beams were optimized for selected incident radiation parameters (wavelength, incident angle). The developed optical elements were characterized by means of XUV reflectometry and transmission measurements, atomic force microscopy and optical interferometry. Special attention was paid to the spatial homogeneity of the optical response and reflected beam wavefront distortions. Here the results of the characterization are presented and improvements required for advanced applications at XUV free-electron lasers are identified. A flatness as low as 4 nm r.m.s. on 3 × 3 mm beam splitters and 22 nm r.m.s. on 10 × 10 mm beam splitters has been obtained. The high-spatial-frequency surface roughness was about 0.7–1 nm r.m.s. The middle-spatial-frequency roughness was in the range 0.2–0.8 nm r.m.s. The reflection and transmission of the beam splitters were found to be very homogeneous, with a deviation of less than 2% across the full optical element.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Mo/Si multilayer-coated amplitude-division beam splitters for XUV radiation sources</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-03-01</prism:publicationDate>
    <prism:startingPage>249</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>257</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wa5030">
    <title>Sagittal focusing of synchrotron radiation X-rays using a winged crystal</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wa5030</link>
    <description>A Si(111) winged crystal has been designed to minimize anticlastic bending and improve sagittal focusing efficiency. The crystal was thin with wide stiffening wings. The length-to-width ratio of the crystal was optimized by finite element analysis, and the optimal value was larger than the `golden value'. The analysis showed that the slope error owing to anticlastic bending is less than the Darwin width. The X-rays were focused two-dimensionally using the crystal and a tangentially bent mirror. The observed profiles of the focal spot agreed well with the results of a ray-tracing calculation in the energy range from 8 to 17.5 keV. X-ray diffraction measurements with a high signal-to-noise ratio using this focusing system were demonstrated for a small protein crystal.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Nisawa, A.</dc:creator>
    <dc:creator>Yoneda, Y.</dc:creator>
    <dc:creator>Ueno, G.</dc:creator>
    <dc:creator>Murakami, H.</dc:creator>
    <dc:creator>Okajima, Y.</dc:creator>
    <dc:creator>Yamamoto, K.</dc:creator>
    <dc:creator>Senba, Y.</dc:creator>
    <dc:creator>Uesugi, K.</dc:creator>
    <dc:creator>Tanaka, Y.</dc:creator>
    <dc:creator>Yamamoto, M.</dc:creator>
    <dc:creator>Goto, S.</dc:creator>
    <dc:creator>Ishikawa, T.</dc:creator>
    <dc:date>2013-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512049813</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A Si(111) winged crystal has been designed for sagittal focusing of synchrotron radiation X-rays. The results of performance tests at beamlines are reported.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAGITTAL FOCUSING; DOUBLE-CRYSTAL MONOCHROMATOR; WINGED CRYSTAL; TWO-DIMENSIONAL FOCUSING; CRYSTAL BENDER; SPRING-8</dc:subject>
    <dc:description>A Si(111) winged crystal has been designed to minimize anticlastic bending and improve sagittal focusing efficiency. The crystal was thin with wide stiffening wings. The length-to-width ratio of the crystal was optimized by finite element analysis, and the optimal value was larger than the `golden value'. The analysis showed that the slope error owing to anticlastic bending is less than the Darwin width. The X-rays were focused two-dimensionally using the crystal and a tangentially bent mirror. The observed profiles of the focal spot agreed well with the results of a ray-tracing calculation in the energy range from 8 to 17.5 keV. X-ray diffraction measurements with a high signal-to-noise ratio using this focusing system were demonstrated for a small protein crystal.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Sagittal focusing of synchrotron radiation X-rays using a winged crystal</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-03-01</prism:publicationDate>
    <prism:startingPage>219</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>225</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5038">
    <title>To scavenge or not to scavenge, that is STILL the question</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5038</link>
    <description>An extensive radiation chemistry literature would suggest that the addition of certain radical scavengers might mitigate the effects of radiation damage during protein crystallography diffraction data collection. However, attempts to demonstrate and quantify such an amelioration and its dose dependence have not yielded consistent results, either at room temperature (RT) or 100 K. Here the information thus far available is summarized and reasons for this lack of quantitative success are identified. Firstly, several different metrics have been used to monitor and quantify the rate of damage, and, as shown here, these can give results which are in conflict regarding scavenger efficacy. In addition, significant variation in results from data collected from crystals treated in nominally the same way has been observed. Secondly, typical crystallization conditions contain substantial concentrations of chemical species which already interact strongly with some of the X-ray-induced radicals that the added scavengers are intended to intercept. These interactions are probed here by the complementary technique of on-line microspectrophotometry carried out on solutions and crystals held both at 100 K and RT, the latter enabled by the use of a beamline-mounted humidifying device. With the help of computational chemistry, attempts are made to assign some of the characteristic spectral features observed experimentally. A further source of uncertainty undoubtedly lies in the challenge of reliably measuring the parameters necessary for the accurate calculation of the absorbed dose (e.g. crystal size and shape, beam profile) and its distribution within the volume of the crystal (an issue addressed in detail in another article in this issue). While microspectrophotometry reveals that the production of various species can be quenched by the addition of scavengers, it is less clear that this observation can be translated into a significant gain in crystal dose tolerance for macromolecular crystallographers.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Allan, E.G.</dc:creator>
    <dc:creator>Kander, M.C.</dc:creator>
    <dc:creator>Carmichael, I.</dc:creator>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:date>2013-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512046237</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The reasons for the conflicting results on the efficacy of scavengers in macromolecular crystallography are examined in the light of some new results.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; CRYSTALLIZATION BUFFERS; RADICALS; SCAVENGERS; LITHIUM NITRATE</dc:subject>
    <dc:description>An extensive radiation chemistry literature would suggest that the addition of certain radical scavengers might mitigate the effects of radiation damage during protein crystallography diffraction data collection. However, attempts to demonstrate and quantify such an amelioration and its dose dependence have not yielded consistent results, either at room temperature (RT) or 100 K. Here the information thus far available is summarized and reasons for this lack of quantitative success are identified. Firstly, several different metrics have been used to monitor and quantify the rate of damage, and, as shown here, these can give results which are in conflict regarding scavenger efficacy. In addition, significant variation in results from data collected from crystals treated in nominally the same way has been observed. Secondly, typical crystallization conditions contain substantial concentrations of chemical species which already interact strongly with some of the X-ray-induced radicals that the added scavengers are intended to intercept. These interactions are probed here by the complementary technique of on-line microspectrophotometry carried out on solutions and crystals held both at 100 K and RT, the latter enabled by the use of a beamline-mounted humidifying device. With the help of computational chemistry, attempts are made to assign some of the characteristic spectral features observed experimentally. A further source of uncertainty undoubtedly lies in the challenge of reliably measuring the parameters necessary for the accurate calculation of the absorbed dose (e.g. crystal size and shape, beam profile) and its distribution within the volume of the crystal (an issue addressed in detail in another article in this issue). While microspectrophotometry reveals that the production of various species can be quenched by the addition of scavengers, it is less clear that this observation can be translated into a significant gain in crystal dose tolerance for macromolecular crystallographers.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>To scavenge or not to scavenge, that is STILL the question</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-01-01</prism:publicationDate>
    <prism:startingPage>23</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>36</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5048">
    <title>ANKAphase: software for single-distance phase retrieval from inline X-ray phase-contrast radiographs. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5048</link>
    <description>An equation in the paper by Weitkamp et al. [(2011), J. Synchrotron Rad. 18, 617–629] is corrected.</description>
    <dc:rights>Copyright (c) 2013 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Weitkamp, T.</dc:creator>
    <dc:creator>Haas, D.</dc:creator>
    <dc:creator>Wegrzynek, D.</dc:creator>
    <dc:creator>Rack, A.</dc:creator>
    <dc:date>2013-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512044871</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Erratum to Weitkamp et al. [(2011), J. Synchrotron Rad. 18, 617–629].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>An equation in the paper by Weitkamp et al. [(2011), J. Synchrotron Rad. 18, 617–629] is corrected.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>ANKAphase: software for single-distance phase retrieval from inline X-ray phase-contrast radiographs. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2013 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-01-01</prism:publicationDate>
    <prism:startingPage>205</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>205</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5032">
    <title>Non-rigid image registration to reduce beam-induced blurring of cryo-electron microscopy images</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5032</link>
    <description>The typical dose used to record cryo-electron microscopy images from vitrified biological specimens is so high that radiation-induced structural alterations are bound to occur during data acquisition. Integration of all scattered electrons into one image can lead to significant blurring, particularly if the data are collected from an unsupported thin layer of ice suspended over the holes of a support film. Here, the dose has been fractioned and exposure series have been acquired in order to study beam-induced specimen movements under low dose conditions, prior to bubbling. Gold particles were added to the protein sample as fiducial markers. These were automatically localized and tracked throughout the exposure series and showed correlated motions within small patches, with larger amplitudes of motion vectors at the start of a series compared with the end of each series. A non-rigid scheme was used to register all images within each exposure series, using natural neighbor interpolation with the gold particles as anchor points. The procedure increases the contrast and resolution of the examined macromolecules.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Karimi Nejadasl, F.</dc:creator>
    <dc:creator>Karuppasamy, M.</dc:creator>
    <dc:creator>Newman, E.R.</dc:creator>
    <dc:creator>McGeehan, J.E.</dc:creator>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:date>2013-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512044408</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Cryo-electron microscopy images of vitrified large macromolecular complexes can become blurred due to beam-induced specimen alterations. Exposure series are examined, and rigid and non-rigid image registration schemes are applied to reduce such blurring.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CRYO-ELECTRON MICROSCOPY; SINGLE PARTICLE; BEAM-INDUCED MOVEMENTS; EXPOSURESERIES; RADIATION DAMAGE</dc:subject>
    <dc:description>The typical dose used to record cryo-electron microscopy images from vitrified biological specimens is so high that radiation-induced structural alterations are bound to occur during data acquisition. Integration of all scattered electrons into one image can lead to significant blurring, particularly if the data are collected from an unsupported thin layer of ice suspended over the holes of a support film. Here, the dose has been fractioned and exposure series have been acquired in order to study beam-induced specimen movements under low dose conditions, prior to bubbling. Gold particles were added to the protein sample as fiducial markers. These were automatically localized and tracked throughout the exposure series and showed correlated motions within small patches, with larger amplitudes of motion vectors at the start of a series compared with the end of each series. A non-rigid scheme was used to register all images within each exposure series, using natural neighbor interpolation with the gold particles as anchor points. The procedure increases the contrast and resolution of the examined macromolecules.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Non-rigid image registration to reduce beam-induced blurring of cryo-electron microscopy images</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-01-01</prism:publicationDate>
    <prism:startingPage>58</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>66</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xa5012">
    <title>International Workshop on Improving Data Quality and Quantity for XAFS Experiments (Q2XAFS 2011)</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xa5012</link>
    <description>An introductory overview to the special issue papers from the Q2XAFS Workshop in this issue of the journal.</description>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ascone, I.</dc:creator>
    <dc:creator>Asakura, K.</dc:creator>
    <dc:creator>George, G.N.</dc:creator>
    <dc:creator>Wakatsuki, S.</dc:creator>
    <dc:date>2012-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512043506</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An introductory overview to the special issue papers from the Q2XAFS Workshop in this issue of the journal.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>An introductory overview to the special issue papers from the Q2XAFS Workshop in this issue of the journal.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>International Workshop on Improving Data Quality and Quantity for XAFS Experiments (Q2XAFS 2011)</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-11-01</prism:publicationDate>
    <prism:startingPage>849</prism:startingPage>
    <prism:section>editorial</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>850</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cn5041">
    <title>A simultaneous multiple angle-wavelength dispersive X-ray reflectometer using a bent-twisted polychromator crystal</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cn5041</link>
    <description>An X-ray reflectometer has been developed, which can simultaneously measure the whole specular X-ray reflectivity curve with no need for rotation of the sample, detector or monochromator crystal during the measurement. A bent-twisted crystal polychromator is used to realise a convergent X-ray beam which has continuously varying energy E (wavelength λ) and glancing angle α to the sample surface as a function of horizontal direction. This convergent beam is reflected in the vertical direction by the sample placed horizontally at the focus and then diverges horizontally and vertically. The normalized intensity distribution of the reflected beam measured downstream of the specimen with a two-dimensional pixel array detector (PILATUS 100K) represents the reflectivity curve. Specular X-ray reflectivity curves were measured from a commercially available silicon (100) wafer, a thin gold film coated on a silicon single-crystal substrate and the surface of liquid ethylene glycol with data collection times of 0.01 to 1000 s using synchrotron radiation from a bending-magnet source of a 6.5 GeV electron storage ring. A typical value of the simultaneously covered range of the momentum transfer was 0.01–0.45 Å−1 for the silicon wafer sample. The potential of this reflectometer for time-resolved X-ray studies of irreversible structural changes is discussed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Matsushita, T.</dc:creator>
    <dc:creator>Arakawa, E.</dc:creator>
    <dc:creator>Voegeli, W.</dc:creator>
    <dc:creator>Yano, Y.F.</dc:creator>
    <dc:date>2013-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512043415</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Using a convergent X-ray beam having continuously varying energy and glancing angle as a function of direction, the whole profile of a specular X-ray reflectivity curve is measured with no need for any mechanical motion during the measurement.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY REFLECTIVITY CURVE; TIME-RESOLVED MEASUREMENT; BENT-TWISTED POLYCHROMATOR CRYSTAL; SIMULTANEOUS MEASUREMENT</dc:subject>
    <dc:description>An X-ray reflectometer has been developed, which can simultaneously measure the whole specular X-ray reflectivity curve with no need for rotation of the sample, detector or monochromator crystal during the measurement. A bent-twisted crystal polychromator is used to realise a convergent X-ray beam which has continuously varying energy E (wavelength λ) and glancing angle α to the sample surface as a function of horizontal direction. This convergent beam is reflected in the vertical direction by the sample placed horizontally at the focus and then diverges horizontally and vertically. The normalized intensity distribution of the reflected beam measured downstream of the specimen with a two-dimensional pixel array detector (PILATUS 100K) represents the reflectivity curve. Specular X-ray reflectivity curves were measured from a commercially available silicon (100) wafer, a thin gold film coated on a silicon single-crystal substrate and the surface of liquid ethylene glycol with data collection times of 0.01 to 1000 s using synchrotron radiation from a bending-magnet source of a 6.5 GeV electron storage ring. A typical value of the simultaneously covered range of the momentum transfer was 0.01–0.45 Å−1 for the silicon wafer sample. The potential of this reflectometer for time-resolved X-ray studies of irreversible structural changes is discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A simultaneous multiple angle-wavelength dispersive X-ray reflectometer using a bent-twisted polychromator crystal</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-01-01</prism:publicationDate>
    <prism:startingPage>80</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>88</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0481">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0481</link>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2012-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512042987</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-11-01</prism:publicationDate>
    <prism:startingPage>1064</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1065</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0487">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0487</link>
    <dc:rights>Copyright (c) 2013 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2013-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512050285</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>20</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2013 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2013-01-01</prism:publicationDate>
    <prism:startingPage>206</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>207</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?gb5004">
    <title>X-ray photon correlation spectroscopy using a fast pixel array detector with a grid mask resolution enhancer</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?gb5004</link>
    <description>The performance of a fast pixel array detector with a grid mask resolution enhancer has been demonstrated for X-ray photon correlation spectroscopy (XPCS) measurements to investigate fast dynamics on a microscopic scale. A detecting system, in which each pixel of a single-photon-counting pixel array detector, PILATUS, is covered by grid mask apertures, was constructed for XPCS measurements of silica nanoparticles in polymer melts. The experimental results are confirmed to be consistent by comparison with other independent experiments. By applying this method, XPCS measurements can be carried out by customizing the hole size of the grid mask to suit the experimental conditions, such as beam size, detector size and sample-to-detector distance.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hoshino, T.</dc:creator>
    <dc:creator>Kikuchi, M.</dc:creator>
    <dc:creator>Murakami, D.</dc:creator>
    <dc:creator>Harada, Y.</dc:creator>
    <dc:creator>Mitamura, K.</dc:creator>
    <dc:creator>Ito, K.</dc:creator>
    <dc:creator>Tanaka, Y.</dc:creator>
    <dc:creator>Sasaki, S.</dc:creator>
    <dc:creator>Takata, M.</dc:creator>
    <dc:creator>Jinnai, H.</dc:creator>
    <dc:creator>Takahara, A.</dc:creator>
    <dc:date>2012-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512038769</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The performance of a fast pixel array detector with a grid mask resolution enhancer has been demonstrated for X-ray photon correlation spectroscopy experiments.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY PHOTON CORRELATION SPECTROSCOPY; GRID MASK RESOLUTION ENHANCER</dc:subject>
    <dc:description>The performance of a fast pixel array detector with a grid mask resolution enhancer has been demonstrated for X-ray photon correlation spectroscopy (XPCS) measurements to investigate fast dynamics on a microscopic scale. A detecting system, in which each pixel of a single-photon-counting pixel array detector, PILATUS, is covered by grid mask apertures, was constructed for XPCS measurements of silica nanoparticles in polymer melts. The experimental results are confirmed to be consistent by comparison with other independent experiments. By applying this method, XPCS measurements can be carried out by customizing the hole size of the grid mask to suit the experimental conditions, such as beam size, detector size and sample-to-detector distance.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray photon correlation spectroscopy using a fast pixel array detector with a grid mask resolution enhancer</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-11-01</prism:publicationDate>
    <prism:startingPage>988</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>993</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xa5006">
    <title>Towards data format standardization for X-ray absorption spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xa5006</link>
    <description>A working group on data format standardization for X-ray absorption spectroscopy (XAS) has recently formed under the auspices of the International X-ray Absorption Society and the XAFS Commission of the International Union of Crystallography. This group of beamline scientists and XAS practitioners has been tasked to propose data format standards to meet the needs of the world-wide XAS community. In this report, concepts for addressing three XAS data storage needs are presented: a single spectrum interchange format, a hierarchical format for multispectral X-ray experiment, and a relational database format for XAS data libraries.</description>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ravel, B.</dc:creator>
    <dc:creator>Hester, J.R.</dc:creator>
    <dc:creator>Solé, V.A.</dc:creator>
    <dc:creator>Newville, M.</dc:creator>
    <dc:date>2012-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512036886</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>In this first report from an ad hoc working group on XAS data format standardization, concepts for addressing three XAS data storage needs are presented: a single spectrum interchange format, a hierarchical format for multispectral X-ray experiment, and a relational database format for XAS data libraries.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>XAFS; STANDARDIZATION; DATA FORMATS</dc:subject>
    <dc:description>A working group on data format standardization for X-ray absorption spectroscopy (XAS) has recently formed under the auspices of the International X-ray Absorption Society and the XAFS Commission of the International Union of Crystallography. This group of beamline scientists and XAS practitioners has been tasked to propose data format standards to meet the needs of the world-wide XAS community. In this report, concepts for addressing three XAS data storage needs are presented: a single spectrum interchange format, a hierarchical format for multispectral X-ray experiment, and a relational database format for XAS data libraries.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Towards data format standardization for X-ray absorption spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-11-01</prism:publicationDate>
    <prism:startingPage>869</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>874</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5086">
    <title>A hard X-ray nanoprobe beamline for nanoscale microscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5086</link>
    <description>The Hard X-ray Nanoprobe Beamline (or Nanoprobe Beamline) is an X-ray microscopy facility incorporating diffraction, fluorescence and full-field imaging capabilities designed and operated by the Center for Nanoscale Materials and the Advanced Photon Source at Sector 26 of the Advanced Photon Source at Argonne National Laboratory. This facility was constructed to probe the nanoscale structure of biological, environmental and material sciences samples. The beamline provides intense focused X-rays to the Hard X-ray Nanoprobe (or Nanoprobe) which incorporates Fresnel zone plate optics and a precision laser sensing and control system. The beamline operates over X-ray energies from 3 to 30 keV, enabling studies of most elements in the periodic table, with a particular emphasis on imaging transition metals.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Winarski, R.P.</dc:creator>
    <dc:creator>Holt, M.V.</dc:creator>
    <dc:creator>Rose, V.</dc:creator>
    <dc:creator>Fuesz, P.</dc:creator>
    <dc:creator>Carbaugh, D.</dc:creator>
    <dc:creator>Benson, C.</dc:creator>
    <dc:creator>Shu, D.</dc:creator>
    <dc:creator>Kline, D.</dc:creator>
    <dc:creator>Stephenson, G.B.</dc:creator>
    <dc:creator>McNulty, I.</dc:creator>
    <dc:creator>Maser, J.</dc:creator>
    <dc:date>2012-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512036783</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The Hard X-ray Nanoprobe Beamline is a precision platform for scanning probe and full-field microscopy with 3–30 keV X-rays. A combination of high-stability X-ray optics and precision motion sensing and control enables detailed studies of the internal features of samples with resolutions approaching 30 nm.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY NANOPROBE; X-RAY MICROSCOPY; ZONE PLATE; X-RAY FLUORESCENCE; NANODIFFRACTION; NANOTOMOGRAPHY</dc:subject>
    <dc:description>The Hard X-ray Nanoprobe Beamline (or Nanoprobe Beamline) is an X-ray microscopy facility incorporating diffraction, fluorescence and full-field imaging capabilities designed and operated by the Center for Nanoscale Materials and the Advanced Photon Source at Sector 26 of the Advanced Photon Source at Argonne National Laboratory. This facility was constructed to probe the nanoscale structure of biological, environmental and material sciences samples. The beamline provides intense focused X-rays to the Hard X-ray Nanoprobe (or Nanoprobe) which incorporates Fresnel zone plate optics and a precision laser sensing and control system. The beamline operates over X-ray energies from 3 to 30 keV, enabling studies of most elements in the periodic table, with a particular emphasis on imaging transition metals.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A hard X-ray nanoprobe beamline for nanoscale microscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-11-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>beamlines</prism:section>
    <prism:startingPage>1056</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1060</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?gb5007">
    <title>Capturing dynamics with Eiger, a fast-framing X-ray detector</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?gb5007</link>
    <description>Eiger is the next-generation single-photon-counting pixel detector following the widely used Pilatus detector. Its smaller pixel size of 75 µm × 75 µm, higher frame rate of up to 22 kHz, and practically zero dead-time (∼4 µs) between exposures will further various measurement methods at synchrotron sources. In this article Eiger's suitability for X-ray photon correlation spectroscopy (XPCS) is demonstrated. By exploiting its high frame rate, complementary small-angle X-ray scattering (SAXS) and XPCS data are collected in parallel to determine both the structure factor and collective diffusion coefficient of a nano-colloid suspension. For the first time, correlation times on the submillisecond time scale are accessible with a large-area pixel detector.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Johnson, I.</dc:creator>
    <dc:creator>Bergamaschi, A.</dc:creator>
    <dc:creator>Buitenhuis, J.</dc:creator>
    <dc:creator>Dinapoli, R.</dc:creator>
    <dc:creator>Greiffenberg, D.</dc:creator>
    <dc:creator>Henrich, B.</dc:creator>
    <dc:creator>Ikonen, T.</dc:creator>
    <dc:creator>Meier, G.</dc:creator>
    <dc:creator>Menzel, A.</dc:creator>
    <dc:creator>Mozzanica, A.</dc:creator>
    <dc:creator>Radicci, V.</dc:creator>
    <dc:creator>Satapathy, D.K.</dc:creator>
    <dc:creator>Schmitt, B.</dc:creator>
    <dc:creator>Shi, X.</dc:creator>
    <dc:date>2012-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512035972</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A high-frame-rate single-photon-counting pixel detector named Eiger and its suitability for X-ray photon correlation spectroscopy are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DETECTOR; SINGLE PHOTON COUNTING; X-RAY DIFFRACTION; X-RAY PHOTON CORRELATION SPECTROSCOPY</dc:subject>
    <dc:description>Eiger is the next-generation single-photon-counting pixel detector following the widely used Pilatus detector. Its smaller pixel size of 75 µm × 75 µm, higher frame rate of up to 22 kHz, and practically zero dead-time (∼4 µs) between exposures will further various measurement methods at synchrotron sources. In this article Eiger's suitability for X-ray photon correlation spectroscopy (XPCS) is demonstrated. By exploiting its high frame rate, complementary small-angle X-ray scattering (SAXS) and XPCS data are collected in parallel to determine both the structure factor and collective diffusion coefficient of a nano-colloid suspension. For the first time, correlation times on the submillisecond time scale are accessible with a large-area pixel detector.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Capturing dynamics with Eiger, a fast-framing X-ray detector</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-11-01</prism:publicationDate>
    <prism:startingPage>1001</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1005</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wa5044">
    <title>The point-spread function of fiber-coupled area detectors</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wa5044</link>
    <description>The point-spread function (PSF) of a fiber-optic taper-coupled CCD area detector was measured over five decades of intensity using a 20 µm X-ray beam and ∼2000-fold averaging. The `tails' of the PSF clearly revealed that it is neither Gaussian nor Lorentzian, but instead resembles the solid angle subtended by a pixel at a point source of light held a small distance (∼27 µm) above the pixel plane. This converges to an inverse cube law far from the beam impact point. Further analysis revealed that the tails are dominated by the fiber-optic taper, with negligible contribution from the phosphor, suggesting that the PSF of all fiber-coupled CCD-type detectors is best described as a Moffat function.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Holton, J.M.</dc:creator>
    <dc:creator>Nielsen, C.</dc:creator>
    <dc:creator>Frankel, K.A.</dc:creator>
    <dc:date>2012-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512035571</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The point-spread function (PSF) of a powdered-phosphor fiber-optic taper-coupled CCD area detector was measured, and an analytic expression for its functional form proposed. The `tails' of this PSF were shown to be due almost entirely to the fiber-optic taper, with no contribution from the phosphor itself.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROTEIN CRYSTALLOGRAPHY X-RAY DETECTOR; CCD; PHOSPHOR; FIBER OPTIC</dc:subject>
    <dc:description>The point-spread function (PSF) of a fiber-optic taper-coupled CCD area detector was measured over five decades of intensity using a 20 µm X-ray beam and ∼2000-fold averaging. The `tails' of the PSF clearly revealed that it is neither Gaussian nor Lorentzian, but instead resembles the solid angle subtended by a pixel at a point source of light held a small distance (∼27 µm) above the pixel plane. This converges to an inverse cube law far from the beam impact point. Further analysis revealed that the tails are dominated by the fiber-optic taper, with negligible contribution from the phosphor, suggesting that the PSF of all fiber-coupled CCD-type detectors is best described as a Moffat function.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The point-spread function of fiber-coupled area detectors</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-11-01</prism:publicationDate>
    <prism:startingPage>1006</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1011</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0477">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0477</link>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2012-09-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951203508X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:number>5</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-09-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>current events</prism:section>
    <prism:startingPage>846</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>847</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pp5022">
    <title>Regridding reconstruction algorithm for real-time tomographic imaging</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pp5022</link>
    <description>Sub-second temporal-resolution tomographic microscopy is becoming a reality at third-generation synchrotron sources. Efficient data handling and post-processing is, however, difficult when the data rates are close to 10 GB s−1. This bottleneck still hinders exploitation of the full potential inherent in the ultrafast acquisition speed. In this paper the fast reconstruction algorithm gridrec, highly optimized for conventional CPU technology, is presented. It is shown that gridrec is a valuable alternative to standard filtered back-projection routines, despite being based on the Fourier transform method. In fact, the regridding procedure used for resampling the Fourier space from polar to Cartesian coordinates couples excellent performance with negligible accuracy degradation. The stronger dependence of the observed signal-to-noise ratio for gridrec reconstructions on the number of angular views makes the presented algorithm even superior to filtered back-projection when the tomographic problem is well sampled. Gridrec not only guarantees high-quality results but it provides up to 20-fold performance increase, making real-time monitoring of the sub-second acquisition process a reality.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Marone, F.</dc:creator>
    <dc:creator>Stampanoni, M.</dc:creator>
    <dc:date>2012-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512032864</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A fast algorithm for tomographic reconstruction based on the Fourier method is presented. On CPU, it provides an up to 20-fold performance increase compared with filtered back-projection routines with negligible accuracy degradation.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TOMOGRAPHIC RECONSTRUCTION; FAST ALGORITHM; FOURIER METHOD; REGRIDDING; PSWF</dc:subject>
    <dc:description>Sub-second temporal-resolution tomographic microscopy is becoming a reality at third-generation synchrotron sources. Efficient data handling and post-processing is, however, difficult when the data rates are close to 10 GB s−1. This bottleneck still hinders exploitation of the full potential inherent in the ultrafast acquisition speed. In this paper the fast reconstruction algorithm gridrec, highly optimized for conventional CPU technology, is presented. It is shown that gridrec is a valuable alternative to standard filtered back-projection routines, despite being based on the Fourier transform method. In fact, the regridding procedure used for resampling the Fourier space from polar to Cartesian coordinates couples excellent performance with negligible accuracy degradation. The stronger dependence of the observed signal-to-noise ratio for gridrec reconstructions on the number of angular views makes the presented algorithm even superior to filtered back-projection when the tomographic problem is well sampled. Gridrec not only guarantees high-quality results but it provides up to 20-fold performance increase, making real-time monitoring of the sub-second acquisition process a reality.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Regridding reconstruction algorithm for real-time tomographic imaging</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-11-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5083">
    <title>The new ambient-pressure X-ray photoelectron spectroscopy instrument at MAX-lab</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5083</link>
    <description>The new instrument for near-ambient-pressure X-ray photoelectron spectroscopy which has been installed at the MAX II ring of the Swedish synchrotron radiation facility MAX IV Laboratory in Lund is presented. The new instrument, which is based on a SPECS PHOIBOS 150 NAP analyser, is the first to feature the use of retractable and exchangeable high-pressure cells. This implies that clean vacuum conditions are retained in the instrument's analysis chamber and that it is possible to swiftly change between near-ambient and ultrahigh-vacuum conditions. In this way the instrument implements a direct link between ultrahigh-vacuum and in situ studies, and the entire pressure range from ultrahigh-vacuum to near-ambient conditions is available to the user. Measurements at pressures up to 10−5 mbar are carried out in the ultrahigh-vacuum analysis chamber, while measurements at higher pressures are performed in the high-pressure cell. The installation of a mass spectrometer on the exhaust line of the reaction cell offers the users the additional dimension of simultaneous reaction data monitoring. Moreover, the chosen design approach allows the use of dedicated cells for different sample environments, rendering the Swedish ambient-pressure X-ray photoelectron spectroscopy instrument a highly versatile and flexible tool.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schnadt, J.</dc:creator>
    <dc:creator>Knudsen, J.</dc:creator>
    <dc:creator>Andersen, J.N.</dc:creator>
    <dc:creator>Siegbahn, H.</dc:creator>
    <dc:creator>Pietzsch, A.</dc:creator>
    <dc:creator>Hennies, F.</dc:creator>
    <dc:creator>Johansson, N.</dc:creator>
    <dc:creator>Mårtensson, N.</dc:creator>
    <dc:creator>Öhrwall, G.</dc:creator>
    <dc:creator>Bahr, S.</dc:creator>
    <dc:creator>Mähl, S.</dc:creator>
    <dc:creator>Schaff, O.</dc:creator>
    <dc:date>2012-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512032700</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The new instrument for ambient-pressure X-ray photoelectron spectroscopy at the Swedish synchrotron radiation facility MAX IV Laboratory is presented. The instrument is based on the use of a retractable and exchangeable high-pressure cell, which implies that ultrahigh-vacuum conditions are retained in the analysis chamber and that dual ambient pressure and ultrahigh-vacuum use is possible.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AMBIENT-PRESSURE X-RAY PHOTOELECTRON SPECTROSCOPY; HIGH-PRESSURE X-RAY PHOTOELECTRON SPECTROSCOPY; X-RAY PHOTOELECTRON SPECTROSCOPY; IN SITU; OPERANDO; CATALYSIS</dc:subject>
    <dc:description>The new instrument for near-ambient-pressure X-ray photoelectron spectroscopy which has been installed at the MAX II ring of the Swedish synchrotron radiation facility MAX IV Laboratory in Lund is presented. The new instrument, which is based on a SPECS PHOIBOS 150 NAP analyser, is the first to feature the use of retractable and exchangeable high-pressure cells. This implies that clean vacuum conditions are retained in the instrument's analysis chamber and that it is possible to swiftly change between near-ambient and ultrahigh-vacuum conditions. In this way the instrument implements a direct link between ultrahigh-vacuum and in situ studies, and the entire pressure range from ultrahigh-vacuum to near-ambient conditions is available to the user. Measurements at pressures up to 10−5 mbar are carried out in the ultrahigh-vacuum analysis chamber, while measurements at higher pressures are performed in the high-pressure cell. The installation of a mass spectrometer on the exhaust line of the reaction cell offers the users the additional dimension of simultaneous reaction data monitoring. Moreover, the chosen design approach allows the use of dedicated cells for different sample environments, rendering the Swedish ambient-pressure X-ray photoelectron spectroscopy instrument a highly versatile and flexible tool.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The new ambient-pressure X-ray photoelectron spectroscopy instrument at MAX-lab</dc:title>
    <dc:type>text</dc:type>
    <prism:number>5</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-09-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>701</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>704</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5209">
    <title>Exploration of synchrotron Mössbauer microscopy with micrometer resolution: forward and a new backscattering modality on natural samples</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5209</link>
    <description>New aspects of synchrotron Mössbauer microscopy are presented. A 5 µm spatial resolution is achieved, and sub-micrometer resolution is envisioned. Two distinct and unique methods, synchrotron Mössbauer imaging and nuclear resonant incoherent X-ray imaging, are used to resolve spatial distribution of species that are chemically and magnetically distinct from one another. Proof-of-principle experiments were performed on enriched 57Fe phantoms, and on samples with natural isotopic abundance, such as meteorites.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yan, L.</dc:creator>
    <dc:creator>Zhao, J.</dc:creator>
    <dc:creator>Toellner, T.S.</dc:creator>
    <dc:creator>Divan, R.</dc:creator>
    <dc:creator>Xu, S.</dc:creator>
    <dc:creator>Cai, Z.</dc:creator>
    <dc:creator>Boesenberg, J.S.</dc:creator>
    <dc:creator>Friedrich, J.M.</dc:creator>
    <dc:creator>Cramer, S.P.</dc:creator>
    <dc:creator>Alp, E.E.</dc:creator>
    <dc:date>2012-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512032414</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>New aspects of synchrotron Mössbauer microscopy have been reported, including micrometer spatial resolution, forward as well as backscattering geometry, and the ability to measure samples with natural isotopic abundance, such as meteorites.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SYNCHROTRON MOSSBAUER MICROSCOPY; NUCLEAR RESONANT INCOHERENT X-RAY IMAGING; METEORITE; 57FE PHANTOM; 5MICROM RESOLUTION</dc:subject>
    <dc:description>New aspects of synchrotron Mössbauer microscopy are presented. A 5 µm spatial resolution is achieved, and sub-micrometer resolution is envisioned. Two distinct and unique methods, synchrotron Mössbauer imaging and nuclear resonant incoherent X-ray imaging, are used to resolve spatial distribution of species that are chemically and magnetically distinct from one another. Proof-of-principle experiments were performed on enriched 57Fe phantoms, and on samples with natural isotopic abundance, such as meteorites.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Exploration of synchrotron Mössbauer microscopy with micrometer resolution: forward and a new backscattering modality on natural samples</dc:title>
    <dc:type>text</dc:type>
    <prism:number>5</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-09-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>814</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>820</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pp5026">
    <title>Zone-doubled Fresnel zone plates for high-resolution hard X-ray full-field transmission microscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pp5026</link>
    <description>Full-field transmission X-ray microscopy is a unique non-destructive technique for three-dimensional imaging of specimens at the nanometer scale. Here, the use of zone-doubled Fresnel zone plates to achieve a spatial resolution better than 20 nm in the hard X-ray regime (8–10 keV) is reported. By obtaining a tomographic reconstruction of a Ni/YSZ solid-oxide fuel cell, the feasibility of performing three-dimensional imaging of scientifically relevant samples using such high-spatial-resolution Fresnel zone plates is demonstrated.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Vila-Comamala, J.</dc:creator>
    <dc:creator>Pan, Y.</dc:creator>
    <dc:creator>Lombardo, J.</dc:creator>
    <dc:creator>Harris, W.M.</dc:creator>
    <dc:creator>Chiu, W.K. .</dc:creator>
    <dc:creator>David, C.</dc:creator>
    <dc:creator>Wang, Y.</dc:creator>
    <dc:date>2012-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512029640</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The use of zone-doubled Fresnel zone plates for sub-20 nm spatial resolution in full-field transmission X-ray microscopy and tomography at the hard X-ray regime (8–10 keV) is demonstrated.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FRESNEL ZONE PLATE; HARD X-RAYS; FULL-FIELD TRANSMISSION X-RAY MICROSCOPY; SOLID-OXIDE FUEL CELL</dc:subject>
    <dc:description>Full-field transmission X-ray microscopy is a unique non-destructive technique for three-dimensional imaging of specimens at the nanometer scale. Here, the use of zone-doubled Fresnel zone plates to achieve a spatial resolution better than 20 nm in the hard X-ray regime (8–10 keV) is reported. By obtaining a tomographic reconstruction of a Ni/YSZ solid-oxide fuel cell, the feasibility of performing three-dimensional imaging of scientifically relevant samples using such high-spatial-resolution Fresnel zone plates is demonstrated.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Zone-doubled Fresnel zone plates for high-resolution hard X-ray full-field transmission microscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:number>5</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-09-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>705</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>709</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0476">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0476</link>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2012-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512027021</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-07-01</prism:publicationDate>
    <prism:startingPage>658</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>659</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5206">
    <title>Glitch-free X-ray absorption spectrum under high pressure obtained using nano-polycrystalline diamond anvils</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5206</link>
    <description>Nano-polycrystalline diamond (NPD) [Irifune et al. (2003), Nature (London), 421, 599] has been used to obtain a glitch-free X-ray absorption spectrum under high pressure. In the case of conventional single-crystal diamond (SCD) anvils, glitches owing to Bragg diffraction from the anvils are superimposed on X-ray absorption spectra. The glitch has long been a serious problem for high-pressure research activities using X-ray spectroscopy because of the difficulties of its complete removal. It is demonstrated that NPD is one of the best candidate materials to overcome this problem. Here a glitch-free absorption spectrum using the NPD anvils over a wide energy range is shown. The advantage and capability of NPD anvils is discussed by a comparison of the glitch map with that of SCD anvils.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ishimatsu, N.</dc:creator>
    <dc:creator>Matsumoto, K.</dc:creator>
    <dc:creator>Maruyama, H.</dc:creator>
    <dc:creator>Kawamura, N.</dc:creator>
    <dc:creator>Mizumaki, M.</dc:creator>
    <dc:creator>Sumiya, H.</dc:creator>
    <dc:creator>Irifune, T.</dc:creator>
    <dc:date>2012-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512026088</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Nano-polycrystalline diamond has been used to obtain a glitch-free X-ray absorption spectrum under high pressure. The advantage and capability of nano-polycrystalline diamond anvils is discussed by a comparison of the glitch map with that of single-crystal diamond anvils.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY SPECTROSCOPY; HIGH PRESSURE; GLITCH; NANO-POLYCRYSTALLINE DIAMOND; DIAMOND ANVIL CELL</dc:subject>
    <dc:description>Nano-polycrystalline diamond (NPD) [Irifune et al. (2003), Nature (London), 421, 599] has been used to obtain a glitch-free X-ray absorption spectrum under high pressure. In the case of conventional single-crystal diamond (SCD) anvils, glitches owing to Bragg diffraction from the anvils are superimposed on X-ray absorption spectra. The glitch has long been a serious problem for high-pressure research activities using X-ray spectroscopy because of the difficulties of its complete removal. It is demonstrated that NPD is one of the best candidate materials to overcome this problem. Here a glitch-free absorption spectrum using the NPD anvils over a wide energy range is shown. The advantage and capability of NPD anvils is discussed by a comparison of the glitch map with that of SCD anvils.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Glitch-free X-ray absorption spectrum under high pressure obtained using nano-polycrystalline diamond anvils</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-09-01</prism:publicationDate>
    <prism:startingPage>768</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>772</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?co5015">
    <title>High-energy-resolution X-ray monochromator calibration using the detailed-balance principle</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?co5015</link>
    <description>A new method is presented to calibrate an X-ray energy scale with sub-meV relative accuracy by using the detailed-balance principle of the phonon creation and annihilation. This method is conveniently used to define or verify the energy scale of high-energy-resolution monochromators that are used in inelastic X-ray scattering and nuclear resonant inelastic X-ray scattering instruments at synchrotron radiation facilities. This method does not rely on sample properties and its precision only depends on the statistical data quality. Well calibrated instruments are essential for reliable comparison of data sets obtained at different synchrotron radiation beamlines, of data with theoretical predictions, and of data from other techniques such as neutron or light scattering. The principle of the detailed-balance method is described in this paper and demonstrated experimentally.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Zhao, J.Y.</dc:creator>
    <dc:creator>Sturhahn, W.</dc:creator>
    <dc:date>2012-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512022339</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A sample-independent method is presented to calibrate an X-ray energy scale of a high-energy-resolution monochromator with sub-meV relative accuracy by using the detailed-balance principle.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY; MONOCHROMATOR; ENERGY CALIBRATION; NUCLEAR RESONANT SCATTERING</dc:subject>
    <dc:description>A new method is presented to calibrate an X-ray energy scale with sub-meV relative accuracy by using the detailed-balance principle of the phonon creation and annihilation. This method is conveniently used to define or verify the energy scale of high-energy-resolution monochromators that are used in inelastic X-ray scattering and nuclear resonant inelastic X-ray scattering instruments at synchrotron radiation facilities. This method does not rely on sample properties and its precision only depends on the statistical data quality. Well calibrated instruments are essential for reliable comparison of data sets obtained at different synchrotron radiation beamlines, of data with theoretical predictions, and of data from other techniques such as neutron or light scattering. The principle of the detailed-balance method is described in this paper and demonstrated experimentally.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>High-energy-resolution X-ray monochromator calibration using the detailed-balance principle</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-07-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>602</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>608</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi5632">
    <title>An X-ray diffraction study on a single rod outer segment from frog retina</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi5632</link>
    <description>X-ray diffraction patterns were recorded from isolated single rod outer segments of frog. The outer segments in Ringer's solution were exposed to a 6 µm microbeam (15 keV) at the BL40XU beamline, SPring-8. The diffraction pattern demonstrated a remarkable regularity in the stacking and flatness of the disk membranes. The electron density profile calculated from the intensity of up to tenth-order reflections showed a pair of bilayers that comprise a disk membrane. The structure of the disk membrane and the changes in the profile on swelling generally agreed with previous reports. Radiation damage was significant with an irradiation of 5 × 105 Gy which is much lower than the known damaging dose on proteins at the liquid-nitrogen temperature.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:creator>Matsuo, T.</dc:creator>
    <dc:creator>Ohta, N.</dc:creator>
    <dc:date>2012-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512018535</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>X-ray diffraction was recorded from retinal rod outer segments of frog using a microbeam.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RETINA; MICROBEAM; LAMELLAR DIFFRACTION</dc:subject>
    <dc:description>X-ray diffraction patterns were recorded from isolated single rod outer segments of frog. The outer segments in Ringer's solution were exposed to a 6 µm microbeam (15 keV) at the BL40XU beamline, SPring-8. The diffraction pattern demonstrated a remarkable regularity in the stacking and flatness of the disk membranes. The electron density profile calculated from the intensity of up to tenth-order reflections showed a pair of bilayers that comprise a disk membrane. The structure of the disk membrane and the changes in the profile on swelling generally agreed with previous reports. Radiation damage was significant with an irradiation of 5 × 105 Gy which is much lower than the known damaging dose on proteins at the liquid-nitrogen temperature.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>An X-ray diffraction study on a single rod outer segment from frog retina</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-07-01</prism:publicationDate>
    <prism:startingPage>574</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>578</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5202">
    <title>Local structural studies of the cubic Cd1–xCaxO system through Cd K-edge extended X-ray absorption spectroscopic studies</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5202</link>
    <description>Cd K-edge extended X-ray absorption fine-structure spectroscopic studies were carried out on Cd1–xCaxO (0 ≤ x ≤0.9) solid solutions and the first and second nearest neighbour (NN) distances and their mean square relative displacement σ2 were estimated. The first NN distance, dCd–O(x), was found to be smaller than its expected value, a(x)/2, obtained from the X-ray diffraction measurements. It increases monotonically and non-linearly with a negative curvature, comparable with that of the a(x) value variation. The variation σ2 of the 1NN with x is consistent with a disordered solid solution model. The 2NN distances dCd–Cd(x) and dCd–Ca(x) are found to follow the average values obtained by X-ray diffraction with dCd–Ca(x) &gt; dCd–Cd(x). From detailed analysis it is argued that the solid solution exhibits a bimodal distribution of the 1NN distances, dCd–O(x) and dCa–O(x), and that the system belongs to a persistent type.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Srihari, V.</dc:creator>
    <dc:creator>Sridharan, V.</dc:creator>
    <dc:creator>Nomura, M.</dc:creator>
    <dc:creator>Sastry, V.S.</dc:creator>
    <dc:creator>Sundar, C.S.</dc:creator>
    <dc:date>2012-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512018419</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Local structure studies about Cd in the Cd1–xCaxO solid solution through Cd K-edge EXAFS studies are described, indicating a bimodal distribution of the first nearest neighbour distance for Cd and that the optical properties should belong to a persistence type.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>EXAFS; CDO; CAO; TERNARY SOLID SOLUTION; OXIDE SEMICONDUCTORS</dc:subject>
    <dc:description>Cd K-edge extended X-ray absorption fine-structure spectroscopic studies were carried out on Cd1–xCaxO (0 ≤ x ≤0.9) solid solutions and the first and second nearest neighbour (NN) distances and their mean square relative displacement σ2 were estimated. The first NN distance, dCd–O(x), was found to be smaller than its expected value, a(x)/2, obtained from the X-ray diffraction measurements. It increases monotonically and non-linearly with a negative curvature, comparable with that of the a(x) value variation. The variation σ2 of the 1NN with x is consistent with a disordered solid solution model. The 2NN distances dCd–Cd(x) and dCd–Ca(x) are found to follow the average values obtained by X-ray diffraction with dCd–Ca(x) &gt; dCd–Cd(x). From detailed analysis it is argued that the solid solution exhibits a bimodal distribution of the 1NN distances, dCd–O(x) and dCa–O(x), and that the system belongs to a persistent type.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Local structural studies of the cubic Cd1–xCaxO system through Cd K-edge extended X-ray absorption spectroscopic studies</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-07-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>541</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>546</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5078">
    <title>P03, the microfocus and nanofocus X-ray scattering (MiNaXS) beamline of the PETRA III storage ring: the microfocus endstation</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5078</link>
    <description>The P03 beamline, also called the microfocus and nanofocus X-ray scattering (MiNaXS) beamline, exploits the excellent photon beam properties of the low-emittance source PETRA III to provide a microfocused/nanofocused beam with ultra-high intensity for time-resolved X-ray scattering experiments. The beamline has been designed to perform X-ray scattering in both transmission and reflection geometries. The microfocus endstation started user operation in May 2011. An overview of the beamline status and of some representative results highlighting the performance of the microfocus endstation at MiNaXS are given.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Buffet, A.</dc:creator>
    <dc:creator>Rothkirch, A.</dc:creator>
    <dc:creator>Döhrmann, R.</dc:creator>
    <dc:creator>Körstgens, V.</dc:creator>
    <dc:creator>Abul Kashem, M.M.</dc:creator>
    <dc:creator>Perlich, J.</dc:creator>
    <dc:creator>Herzog, G.</dc:creator>
    <dc:creator>Schwartzkopf, M.</dc:creator>
    <dc:creator>Gehrke, R.</dc:creator>
    <dc:creator>Müller-Buschbaum, P.</dc:creator>
    <dc:creator>Roth, S.V.</dc:creator>
    <dc:date>2012-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512016895</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The MiNaXS (P03) beamline of the new third-generation synchrotron radiation source PETRA III (DESY, Germany) has been designed to perform small-, ultra-small- and wide-angle X-ray scattering in both transmission and grazing-incidence geometries. The high photon flux available at the beamline enables time-resolved investigations of kinetic phenomena with a time resolution below 100 ms. The microfocus endstation started user operation in May 2011.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY SCATTERING; MICROFOCUS; KINETIC STUDIES; NANOCOMPOSITES</dc:subject>
    <dc:description>The P03 beamline, also called the microfocus and nanofocus X-ray scattering (MiNaXS) beamline, exploits the excellent photon beam properties of the low-emittance source PETRA III to provide a microfocused/nanofocused beam with ultra-high intensity for time-resolved X-ray scattering experiments. The beamline has been designed to perform X-ray scattering in both transmission and reflection geometries. The microfocus endstation started user operation in May 2011. An overview of the beamline status and of some representative results highlighting the performance of the microfocus endstation at MiNaXS are given.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>P03, the microfocus and nanofocus X-ray scattering (MiNaXS) beamline of the PETRA III storage ring: the microfocus endstation</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-07-01</prism:publicationDate>
    <prism:startingPage>647</prism:startingPage>
    <prism:section>beamlines</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>653</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5076">
    <title>The 7BM beamline at the APS: a facility for time-resolved fluid dynamics measurements</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5076</link>
    <description>In recent years, X-ray radiography has been used to probe the internal structure of dense sprays with microsecond time resolution and a spatial resolution of 15 µm even in high-pressure environments. Recently, the 7BM beamline at the Advanced Photon Source (APS) has been commissioned to focus on the needs of X-ray spray radiography measurements. The spatial resolution and X-ray intensity at this beamline represent a significant improvement over previous time-resolved X-ray radiography measurements at the APS.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Kastengren, A.</dc:creator>
    <dc:creator>Powell, C.F.</dc:creator>
    <dc:creator>Arms, D.</dc:creator>
    <dc:creator>Dufresne, E.M.</dc:creator>
    <dc:creator>Gibson, H.</dc:creator>
    <dc:creator>Wang, J.</dc:creator>
    <dc:date>2012-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512016883</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The 7BM beamline, a facility for time-resolved fluid dynamics measurements at the Advanced Photon Source, is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TIME-RESOLVED; RADIOGRAPHY; MULTILAYER MONOCHROMATOR; KIRKPATRICK-BAEZ MIRRORS</dc:subject>
    <dc:description>In recent years, X-ray radiography has been used to probe the internal structure of dense sprays with microsecond time resolution and a spatial resolution of 15 µm even in high-pressure environments. Recently, the 7BM beamline at the Advanced Photon Source (APS) has been commissioned to focus on the needs of X-ray spray radiography measurements. The spatial resolution and X-ray intensity at this beamline represent a significant improvement over previous time-resolved X-ray radiography measurements at the APS.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The 7BM beamline at the APS: a facility for time-resolved fluid dynamics measurements</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-07-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>beamlines</prism:section>
    <prism:startingPage>654</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>657</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0474">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0474</link>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2012-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512015713</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-05-01</prism:publicationDate>
    <prism:startingPage>468</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>469</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5073">
    <title>Adapting federated cyberinfrastructure for shared data collection facilities in structural biology</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5073</link>
    <description>Early stage experimental data in structural biology is generally unmaintained and inaccessible to the public. It is increasingly believed that this data, which forms the basis for each macromolecular structure discovered by this field, must be archived and, in due course, published. Furthermore, the widespread use of shared scientific facilities such as synchrotron beamlines complicates the issue of data storage, access and movement, as does the increase of remote users. This work describes a prototype system that adapts existing federated cyberinfra­structure technology and techniques to significantly improve the operational environment for users and administrators of synchrotron data collection facilities used in structural biology. This is achieved through software from the Virtual Data Toolkit and Globus, bringing together federated users and facilities from the Stanford Synchrotron Radiation Lightsource, the Advanced Photon Source, the Open Science Grid, the SBGrid Consortium and Harvard Medical School. The performance and experience with the prototype provide a model for data management at shared scientific facilities.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Stokes-Rees, I.</dc:creator>
    <dc:creator>Levesque, I.</dc:creator>
    <dc:creator>Murphy IV, F.V.</dc:creator>
    <dc:creator>Yang, W.</dc:creator>
    <dc:creator>Deacon, A.</dc:creator>
    <dc:creator>Sliz, P.</dc:creator>
    <dc:date>2012-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512009776</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>It has been difficult, historically, to manage and maintain early-stage experimental data collected by structural biologists in synchrotron facilities. This work describes a prototype system that adapts existing federated cyberinfrastructure technology and techniques to manage collected data at synchrotrons and to facilitate the efficient and secure transfer of data to the owner's home institution.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>GRID COMPUTING; DATA HANDLING AND SECURITY; DIFFRACTION IMAGES; COLLABORATIVE TOOLS; STRUCTURAL BIOLOGY</dc:subject>
    <dc:description>Early stage experimental data in structural biology is generally unmaintained and inaccessible to the public. It is increasingly believed that this data, which forms the basis for each macromolecular structure discovered by this field, must be archived and, in due course, published. Furthermore, the widespread use of shared scientific facilities such as synchrotron beamlines complicates the issue of data storage, access and movement, as does the increase of remote users. This work describes a prototype system that adapts existing federated cyberinfra­structure technology and techniques to significantly improve the operational environment for users and administrators of synchrotron data collection facilities used in structural biology. This is achieved through software from the Virtual Data Toolkit and Globus, bringing together federated users and facilities from the Stanford Synchrotron Radiation Lightsource, the Advanced Photon Source, the Open Science Grid, the SBGrid Consortium and Harvard Medical School. The performance and experience with the prototype provide a model for data management at shared scientific facilities.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Adapting federated cyberinfrastructure for shared data collection facilities in structural biology</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-05-01</prism:publicationDate>
    <prism:startingPage>462</prism:startingPage>
    <prism:section>computer programs</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>467</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ve5009">
    <title>Performance upgrade in the JAEA actinide science beamline BL23SU at SPring-8 with a new twin-helical undulator</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ve5009</link>
    <description>The soft X-ray beamline BL23SU at SPring-8 has undergone an upgrade with a twin-helical undulator of in-vacuum type to enhance the experimental capabilities of the endstations. The new light source with a fast helicity-switching operation allows not only the data throughput but also the sensitivity in X-ray magnetic circular dichroism (XMCD) to be improved. The operational performance and potential are described by presenting XMCD results of paramagnetic β-US2 measured with a 10 T superconducting magnet.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Saitoh, Y.</dc:creator>
    <dc:creator>Fukuda, Y.</dc:creator>
    <dc:creator>Takeda, Y.</dc:creator>
    <dc:creator>Yamagami, H.</dc:creator>
    <dc:creator>Takahashi, S.</dc:creator>
    <dc:creator>Asano, Y.</dc:creator>
    <dc:creator>Hara, T.</dc:creator>
    <dc:creator>Shirasawa, K.</dc:creator>
    <dc:creator>Takeuchi, M.</dc:creator>
    <dc:creator>Tanaka, T.</dc:creator>
    <dc:creator>Kitamura, H.</dc:creator>
    <dc:date>2012-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512006772</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The commissioning studies and an application to a uranium compound with the helicity-switching mode of a new twin-helical undulator installed in soft X-ray beamline BL23SU at SPring-8 are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TWIN-HELICAL UNDULATOR; HELICITY SWITCHING; SOFT X-RAY BEAMLINE; X-RAY MAGNETIC CIRCULAR DICHROISM; URANIUM COMPOUNDS</dc:subject>
    <dc:description>The soft X-ray beamline BL23SU at SPring-8 has undergone an upgrade with a twin-helical undulator of in-vacuum type to enhance the experimental capabilities of the endstations. The new light source with a fast helicity-switching operation allows not only the data throughput but also the sensitivity in X-ray magnetic circular dichroism (XMCD) to be improved. The operational performance and potential are described by presenting XMCD results of paramagnetic β-US2 measured with a 10 T superconducting magnet.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Performance upgrade in the JAEA actinide science beamline BL23SU at SPring-8 with a new twin-helical undulator</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-05-01</prism:publicationDate>
    <prism:startingPage>388</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>393</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5071">
    <title>Facilities for macromolecular crystallography at the Helmholtz-Zentrum Berlin</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5071</link>
    <description>Three macromolecular crystallography (MX) beamlines at the Helmholtz-Zentrum Berlin (HZB) are available for the regional, national and international structural biology user community. The state-of-the-art synchrotron beamlines for MX BL14.1, BL14.2 and BL14.3 are located within the low-β section of the BESSY II electron storage ring. All beamlines are fed from a superconducting 7 T wavelength-shifter insertion device. BL14.1 and BL14.2 are energy tunable in the range 5–16 keV, while BL14.3 is a fixed-energy side station operated at 13.8 keV. All three beamlines are equipped with CCD detectors. BL14.1 and BL14.2 are in regular user operation providing about 200 beam days per year and about 600 user shifts to approximately 50 research groups across Europe. BL14.3 has initially been used as a test facility and was brought into regular user mode operation during the year 2010. BL14.1 has recently been upgraded with a microdiffractometer including a mini-κ goniometer and an automated sample changer. Additional user facilities include office space adjacent to the beamlines, a sample preparation laboratory, a biology laboratory (safety level 1) and high-end computing resources. In this article the instrumentation of the beamlines is described, and a summary of the experimental possibilities of the beamlines and the provided ancillary equipment for the user community is given.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Mueller, U.</dc:creator>
    <dc:creator>Darowski, N.</dc:creator>
    <dc:creator>Fuchs, M.R.</dc:creator>
    <dc:creator>Förster, R.</dc:creator>
    <dc:creator>Hellmig, M.</dc:creator>
    <dc:creator>Paithankar, K.S.</dc:creator>
    <dc:creator>Pühringer, S.</dc:creator>
    <dc:creator>Steffien, M.</dc:creator>
    <dc:creator>Zocher, G.</dc:creator>
    <dc:creator>Weiss, M.S.</dc:creator>
    <dc:date>2012-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512006395</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The three macromolecular crystallography beamlines BL14.1, BL14.2 and BL14.3 at the BESSY II storage ring at the Helmholtz-Zentrum Berlin are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY BEAMLINES; HIGH-THROUGHPUT METHODS; CRYSTAL DEHYDRATION; UV RADIATION-DAMAGE-INDUCED PHASING; LONG-WAVELENGTH PHASING</dc:subject>
    <dc:description>Three macromolecular crystallography (MX) beamlines at the Helmholtz-Zentrum Berlin (HZB) are available for the regional, national and international structural biology user community. The state-of-the-art synchrotron beamlines for MX BL14.1, BL14.2 and BL14.3 are located within the low-β section of the BESSY II electron storage ring. All beamlines are fed from a superconducting 7 T wavelength-shifter insertion device. BL14.1 and BL14.2 are energy tunable in the range 5–16 keV, while BL14.3 is a fixed-energy side station operated at 13.8 keV. All three beamlines are equipped with CCD detectors. BL14.1 and BL14.2 are in regular user operation providing about 200 beam days per year and about 600 user shifts to approximately 50 research groups across Europe. BL14.3 has initially been used as a test facility and was brought into regular user mode operation during the year 2010. BL14.1 has recently been upgraded with a microdiffractometer including a mini-κ goniometer and an automated sample changer. Additional user facilities include office space adjacent to the beamlines, a sample preparation laboratory, a biology laboratory (safety level 1) and high-end computing resources. In this article the instrumentation of the beamlines is described, and a summary of the experimental possibilities of the beamlines and the provided ancillary equipment for the user community is given.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Facilities for macromolecular crystallography at the Helmholtz-Zentrum Berlin</dc:title>
    <dc:type>text</dc:type>
    <prism:number>3</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-05-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>beamlines</prism:section>
    <prism:startingPage>442</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>449</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5061">
    <title>Evaluating the peak-to-valley dose ratio of synchrotron microbeams using PRESAGE fluorescence</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5061</link>
    <description>Synchrotron-generated microbeam radiotherapy holds great promise for future treatment, but the high dose gradients present conventional dosimetry with a challenge. Measuring the important peak-to-valley dose ratio (PVDR) of a microbeam-collimated synchrotron source requires both a dosimeter and an analysis method capable of exceptional spatial resolution. The PVDR is of great interest since it is the limiting factor for potential application of the microbeam radiation therapy technique clinically for its tissue-sparing properties (i.e. the valley dose should be below the tolerance of normal tissue). In this work a new method of measuring the dose response of PRESAGE dosimeters is introduced using the fluorescence from a 638 nm laser on a confocal laser-scanning microscope. This fluorescent microscopy method produces dosimetry data at a pixel size as low as 78 nm, giving a much better spatial resolution than optical computed tomography, which is normally used for scanning PRESAGE dosimeters. Using this technique the PVDR of the BL28B2 microbeam at the SPring-8 synchrotron in Japan is estimated to be approximately 52:1 at a depth of 2.5 mm. The PVDR was also estimated with EBT2 GAFchromic films as 30.5:1 at the surface in order to compare the PRESAGE fluorescent results with a more established dosimetry system. This estimation is in good agreement with previously measured ratios using other dosimeters and Monte Carlo simulations. This means that it is possible to use PRESAGE dosimeters with confocal microscopy for the determination of PVDR.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Annabell, N.</dc:creator>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:creator>Umetani, K.</dc:creator>
    <dc:creator>Wong, C.</dc:creator>
    <dc:creator>Geso, M.</dc:creator>
    <dc:date>2012-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512005237</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The peak-to-valley dose ratio of a microbeam array can be measured by fluorescence of PRESAGE dosimeters. Peak-to-valley dose ratios are calculated using this new technique and also by EBT2 film.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PRESAGE FLUORESCENT DOSIMETRY</dc:subject>
    <dc:description>Synchrotron-generated microbeam radiotherapy holds great promise for future treatment, but the high dose gradients present conventional dosimetry with a challenge. Measuring the important peak-to-valley dose ratio (PVDR) of a microbeam-collimated synchrotron source requires both a dosimeter and an analysis method capable of exceptional spatial resolution. The PVDR is of great interest since it is the limiting factor for potential application of the microbeam radiation therapy technique clinically for its tissue-sparing properties (i.e. the valley dose should be below the tolerance of normal tissue). In this work a new method of measuring the dose response of PRESAGE dosimeters is introduced using the fluorescence from a 638 nm laser on a confocal laser-scanning microscope. This fluorescent microscopy method produces dosimetry data at a pixel size as low as 78 nm, giving a much better spatial resolution than optical computed tomography, which is normally used for scanning PRESAGE dosimeters. Using this technique the PVDR of the BL28B2 microbeam at the SPring-8 synchrotron in Japan is estimated to be approximately 52:1 at a depth of 2.5 mm. The PVDR was also estimated with EBT2 GAFchromic films as 30.5:1 at the surface in order to compare the PRESAGE fluorescent results with a more established dosimetry system. This estimation is in good agreement with previously measured ratios using other dosimeters and Monte Carlo simulations. This means that it is possible to use PRESAGE dosimeters with confocal microscopy for the determination of PVDR.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Evaluating the peak-to-valley dose ratio of synchrotron microbeams using PRESAGE fluorescence</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-05-01</prism:publicationDate>
    <prism:startingPage>332</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>339</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?vv5033">
    <title>Improved count rate corrections for highest data quality with PILATUS detectors</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?vv5033</link>
    <description>The PILATUS detector system is widely used for X-ray experiments at third-generation synchrotrons. It is based on a hybrid technology combining a pixelated silicon sensor with a CMOS readout chip. Its single-photon-counting capability ensures precise and noise-free measurements. The counting mechanism introduces a short dead-time after each hit, which becomes significant for rates above 106 photons s−1 pixel−1. The resulting loss in the number of counted photons is corrected for by applying corresponding rate correction factors. This article presents the results of a Monte Carlo simulation which computes the correction factors taking into account the detector settings as well as the time structure of the X-ray beam at the synchrotron. The results of the simulation show good agreement with experimentally determined correction factors for various detector settings at different synchrotrons. The application of accurate rate correction factors improves the X-ray data quality acquired at high photon fluxes. Furthermore, it is shown that the use of fast detector settings in combination with an optimized time structure of the X-ray beam allows for measurements up to rates of 107 photons s−1 pixel−1.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Trueb, P.</dc:creator>
    <dc:creator>Sobott, B.A.</dc:creator>
    <dc:creator>Schnyder, R.</dc:creator>
    <dc:creator>Loeliger, T.</dc:creator>
    <dc:creator>Schneebeli, M.</dc:creator>
    <dc:creator>Kobas, M.</dc:creator>
    <dc:creator>Rassool, R.P.</dc:creator>
    <dc:creator>Peake, D.J.</dc:creator>
    <dc:creator>Broennimann, C.</dc:creator>
    <dc:date>2012-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512003950</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A Monte Carlo simulation is presented, which computes the rate correction factors taking into account the detector settings and the time structure of the X-ray beam. The results show good agreement with experimentally determined correction factors.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PILATUS DETECTORS; PHOTON COUNTING; COUNT RATE CORRECTION; BUNCH PATTERN; MONTE CARLO SIMULATION</dc:subject>
    <dc:description>The PILATUS detector system is widely used for X-ray experiments at third-generation synchrotrons. It is based on a hybrid technology combining a pixelated silicon sensor with a CMOS readout chip. Its single-photon-counting capability ensures precise and noise-free measurements. The counting mechanism introduces a short dead-time after each hit, which becomes significant for rates above 106 photons s−1 pixel−1. The resulting loss in the number of counted photons is corrected for by applying corresponding rate correction factors. This article presents the results of a Monte Carlo simulation which computes the correction factors taking into account the detector settings as well as the time structure of the X-ray beam at the synchrotron. The results of the simulation show good agreement with experimentally determined correction factors for various detector settings at different synchrotrons. The application of accurate rate correction factors improves the X-ray data quality acquired at high photon fluxes. Furthermore, it is shown that the use of fast detector settings in combination with an optimized time structure of the X-ray beam allows for measurements up to rates of 107 photons s−1 pixel−1.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Improved count rate corrections for highest data quality with PILATUS detectors</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-05-01</prism:publicationDate>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pp5014">
    <title>Development of a laser-based heating system for in situ synchrotron-based X-ray tomographic microscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pp5014</link>
    <description>Understanding the formation of materials at elevated temperatures is critical for determining their final properties. Synchrotron-based X-ray tomographic microscopy is an ideal technique for studying such processes because high spatial and temporal resolutions are easily achieved and the technique is non-destructive, meaning additional analyses can take place after data collection. To exploit the state-of-the-art capabilities at the tomographic microscopy and coherent radiology experiments (TOMCAT) beamline of the Swiss Light Source, a general-use moderate-to-high-temperature furnace has been developed. Powered by two diode lasers, it provides controlled localized heating, from 673 to 1973 K, to examine many materials systems and their dynamics in real time. The system can also be operated in various thermal modalities. For example, near-isothermal conditions at a given sample location can be achieved with a prescribed time-dependent temperature. This mode is typically used to study isothermal phase transformations; for example, the formation of equiaxed grains in metallic systems or to nucleate and grow bubble foams in silicate melts under conditions that simulate volcanic processes. In another mode, the power of the laser can be fixed and the specimen moved at a constant speed in a user-defined thermal gradient. This is similar to Bridgman solidification, where the thermal gradient and cooling rate control the microstructure formation. This paper details the experimental set-up and provides multiple proofs-of-concept that illustrate the versatility of using this laser-based heating system to explore, in situ, many elevated-temperature phenomena in a variety of materials.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Fife, J.L.</dc:creator>
    <dc:creator>Rappaz, M.</dc:creator>
    <dc:creator>Pistone, M.</dc:creator>
    <dc:creator>Celcer, T.</dc:creator>
    <dc:creator>Mikuljan, G.</dc:creator>
    <dc:creator>Stampanoni, M.</dc:creator>
    <dc:date>2012-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512003287</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A laser-based heating system has been developed at the TOMCAT beamline of the Swiss Light Source for in situ observations of moderate-to-high-temperature applications of materials.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>IN SITU X-RAY TOMOGRAPHIC MICROSCOPY; ULTRA-FAST IMAGING; DIODE LASERS; METALS SOLIDIFICATION; VOLCANIC PROCESSES</dc:subject>
    <dc:description>Understanding the formation of materials at elevated temperatures is critical for determining their final properties. Synchrotron-based X-ray tomographic microscopy is an ideal technique for studying such processes because high spatial and temporal resolutions are easily achieved and the technique is non-destructive, meaning additional analyses can take place after data collection. To exploit the state-of-the-art capabilities at the tomographic microscopy and coherent radiology experiments (TOMCAT) beamline of the Swiss Light Source, a general-use moderate-to-high-temperature furnace has been developed. Powered by two diode lasers, it provides controlled localized heating, from 673 to 1973 K, to examine many materials systems and their dynamics in real time. The system can also be operated in various thermal modalities. For example, near-isothermal conditions at a given sample location can be achieved with a prescribed time-dependent temperature. This mode is typically used to study isothermal phase transformations; for example, the formation of equiaxed grains in metallic systems or to nucleate and grow bubble foams in silicate melts under conditions that simulate volcanic processes. In another mode, the power of the laser can be fixed and the specimen moved at a constant speed in a user-defined thermal gradient. This is similar to Bridgman solidification, where the thermal gradient and cooling rate control the microstructure formation. This paper details the experimental set-up and provides multiple proofs-of-concept that illustrate the versatility of using this laser-based heating system to explore, in situ, many elevated-temperature phenomena in a variety of materials.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Development of a laser-based heating system for in situ synchrotron-based X-ray tomographic microscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-05-01</prism:publicationDate>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pp5013">
    <title>Micrometre resolution of a charge integrating microstrip detector with single photon sensitivity</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pp5013</link>
    <description>A synchrotron beam has been used to test the spatial resolution of a single-photon-resolving integrating readout-chip coupled to a 320 µm-thick silicon strip sensor with a dedicated readout system. Charge interpolation methods have yielded a spatial resolution of σx ≃ 1.8 µm for a 20 µm-pitch strip.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schubert, A.</dc:creator>
    <dc:creator>Bergamaschi, A.</dc:creator>
    <dc:creator>David, C.</dc:creator>
    <dc:creator>Dinapoli, R.</dc:creator>
    <dc:creator>Elbracht-Leong, S.</dc:creator>
    <dc:creator>Gorelick, S.</dc:creator>
    <dc:creator>Graafsma, H.</dc:creator>
    <dc:creator>Henrich, B.</dc:creator>
    <dc:creator>Johnson, I.</dc:creator>
    <dc:creator>Lohmann, M.</dc:creator>
    <dc:creator>Mozzanica, A.</dc:creator>
    <dc:creator>Radicci, V.</dc:creator>
    <dc:creator>Rassool, R.</dc:creator>
    <dc:creator>Schädler, L.</dc:creator>
    <dc:creator>Schmitt, B.</dc:creator>
    <dc:creator>Shi, X.</dc:creator>
    <dc:creator>Sobott, B.</dc:creator>
    <dc:date>2012-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951200235X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The spatial resolution of a single-photon-resolving integrating system has been improved using a non-linear charge interpolation approach. The resolution limit for a 20 µm-pitch sensor is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SYNCHROTRON RADIATION INSTRUMENTATION; CHARGE INTEGRATING; STRIP DETECTORS</dc:subject>
    <dc:description>A synchrotron beam has been used to test the spatial resolution of a single-photon-resolving integrating readout-chip coupled to a 320 µm-thick silicon strip sensor with a dedicated readout system. Charge interpolation methods have yielded a spatial resolution of σx ≃ 1.8 µm for a 20 µm-pitch strip.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Micrometre resolution of a charge integrating microstrip detector with single photon sensitivity</dc:title>
    <dc:type>text</dc:type>
    <prism:number>3</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-05-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>359</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>365</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kt5030">
    <title>Real sample temperature: a critical issue in the experiments of nuclear resonant vibrational spectroscopy on biological samples</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kt5030</link>
    <description>There are several practical and intertangled issues which make the experiments of nuclear resonant vibrational spectroscopy (NRVS) on biological samples difficult to perform. The sample temperature is one of the most important issues. In NRVS the real sample temperatures can be very different from the readings on the temperature sensors. In this study the following have been performed: (i) citing and analyzing various existing NRVS data to assess the real sample temperatures during the NRVS measurements and to understand their trends with the samples' loading conditions; (ii) designing several NRVS measurements with (Et4N)[FeCl4] to verify these trends; and (iii) proposing a new sample-loading procedure to achieve significantly lower real sample temperatures and to balance among the intertangled experimental issues in biological NRVS measurements.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Wang, H.</dc:creator>
    <dc:creator>Yoda, Y.</dc:creator>
    <dc:creator>Kamali, S.</dc:creator>
    <dc:creator>Zhou, Z.-H.</dc:creator>
    <dc:creator>Cramer, S.P.</dc:creator>
    <dc:date>2012-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512001380</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The real sample temperatures during the nuclear resonant vibrational spectroscopy on biological samples have been assessed and significantly reduced (116 → 52 K) by improving the sample-loading procedures.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>NUCLEAR RESONANT VIBRATIONAL SPECTROSCOPY; REAL SAMPLE TEMPERATURE(S); CRYOGENIC ADHESIVE; HEAT TRANSFER; X-RAY RADIATION DAMAGE</dc:subject>
    <dc:description>There are several practical and intertangled issues which make the experiments of nuclear resonant vibrational spectroscopy (NRVS) on biological samples difficult to perform. The sample temperature is one of the most important issues. In NRVS the real sample temperatures can be very different from the readings on the temperature sensors. In this study the following have been performed: (i) citing and analyzing various existing NRVS data to assess the real sample temperatures during the NRVS measurements and to understand their trends with the samples' loading conditions; (ii) designing several NRVS measurements with (Et4N)[FeCl4] to verify these trends; and (iii) proposing a new sample-loading procedure to achieve significantly lower real sample temperatures and to balance among the intertangled experimental issues in biological NRVS measurements.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Real sample temperature: a critical issue in the experiments of nuclear resonant vibrational spectroscopy on biological samples</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-03-01</prism:publicationDate>
    <prism:startingPage>257</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>263</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?rx5003">
    <title>The kinetic dose limit in room-temperature time-resolved macromolecular crystallography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?rx5003</link>
    <description>Protein X-ray structures are determined with ionizing radiation that damages the protein at high X-ray doses. As a result, diffraction patterns deteriorate with the increased absorbed dose. Several strategies such as sample freezing or scavenging of X-ray-generated free radicals are currently employed to minimize this damage. However, little is known about how the absorbed X-ray dose affects time-resolved Laue data collected at physiological temperatures where the protein is fully functional in the crystal, and how the kinetic analysis of such data depends on the absorbed dose. Here, direct evidence for the impact of radiation damage on the function of a protein is presented using time-resolved macromolecular crystallography. The effect of radiation damage on the kinetic analysis of time-resolved X-ray data is also explored.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schmidt, M.</dc:creator>
    <dc:creator>Šrajer, V.</dc:creator>
    <dc:creator>Purwar, N.</dc:creator>
    <dc:creator>Tripathi, S.</dc:creator>
    <dc:date>2012-03-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951105549X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The effect of the X-ray dose on room-temperature time-resolved Laue data is discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; X-RAY DOSE; ROOM TEMPERATURE; TIME-RESOLVED CRYSTALLOGRAPHY; LAUE CRYSTALLOGRAPHY</dc:subject>
    <dc:description>Protein X-ray structures are determined with ionizing radiation that damages the protein at high X-ray doses. As a result, diffraction patterns deteriorate with the increased absorbed dose. Several strategies such as sample freezing or scavenging of X-ray-generated free radicals are currently employed to minimize this damage. However, little is known about how the absorbed X-ray dose affects time-resolved Laue data collected at physiological temperatures where the protein is fully functional in the crystal, and how the kinetic analysis of such data depends on the absorbed dose. Here, direct evidence for the impact of radiation damage on the function of a protein is presented using time-resolved macromolecular crystallography. The effect of radiation damage on the kinetic analysis of time-resolved X-ray data is also explored.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The kinetic dose limit in room-temperature time-resolved macromolecular crystallography</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-03-01</prism:publicationDate>
    <prism:startingPage>264</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>273</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5648">
    <title>MFM and PEEM observation of micrometre-sized magnetic dot arrays fabricated by ion-microbeam irradiation in FeRh thin films</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5648</link>
    <description>FeRh thin films were irradiated with a 10 MeV iodine ion microbeam to produce micrometre-scale ferromagnetic microstructures by modifying the local magnetic character from antiferromagnetism to ferromagnetism using ion-microbeam irradiation. Two-dimensional magnetic dot arrays of dimensions ∼2 µm × 4 µm as well as 10 µm × 10 µm were successfully produced on the FeRh surface, which was confirmed by magnetic force microscopy (MFM). The results of photoemission electron microscopy (PEEM) combined with X-ray magnetic circular dichroism reveal that the easy axis of the magnetization of the ion-beam-irradiated ferromagnetism in the FeRh thin films lies in the film planes along the 〈001〉 direction of the MgO substrates.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Aikoh, K.</dc:creator>
    <dc:creator>Tohki, A.</dc:creator>
    <dc:creator>Matsui, T.</dc:creator>
    <dc:creator>Iwase, A.</dc:creator>
    <dc:creator>Satoh, T.</dc:creator>
    <dc:creator>Takano, K.</dc:creator>
    <dc:creator>Kohka, M.</dc:creator>
    <dc:creator>Saitoh, Y.</dc:creator>
    <dc:creator>Kamiya, T.</dc:creator>
    <dc:creator>Ohkochi, T.</dc:creator>
    <dc:creator>Kotsugi, M.</dc:creator>
    <dc:creator>Nakamura, T.</dc:creator>
    <dc:creator>Kinoshita, T.</dc:creator>
    <dc:date>2012-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511054057</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Micrometre-size lateral magnetic modulations were fabricated in FeRh thin films by ion-microbeam irradiation. Their magnetic domain structures were characterized by XMCD–PEEM.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ENERGETIC ION-BEAM IRRADIATION; FIRST-ORDER MAGNETIC PHASE TRANSITION; MAGNETIC PATTERNING; MFM; XMCD-PEEM</dc:subject>
    <dc:description>FeRh thin films were irradiated with a 10 MeV iodine ion microbeam to produce micrometre-scale ferromagnetic microstructures by modifying the local magnetic character from antiferromagnetism to ferromagnetism using ion-microbeam irradiation. Two-dimensional magnetic dot arrays of dimensions ∼2 µm × 4 µm as well as 10 µm × 10 µm were successfully produced on the FeRh surface, which was confirmed by magnetic force microscopy (MFM). The results of photoemission electron microscopy (PEEM) combined with X-ray magnetic circular dichroism reveal that the easy axis of the magnetization of the ion-beam-irradiated ferromagnetism in the FeRh thin films lies in the film planes along the 〈001〉 direction of the MgO substrates.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>MFM and PEEM observation of micrometre-sized magnetic dot arrays fabricated by ion-microbeam irradiation in FeRh thin films</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-03-01</prism:publicationDate>
    <prism:startingPage>223</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>226</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?vv9019">
    <title>On the calculation of the gauge volume size for energy-dispersive X-ray diffraction. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?vv9019</link>
    <description>An equation in the paper by Rowles [(2011), J. Synchrotron Rad. 18, 938–941] is corrected.</description>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Rowles, M.R.</dc:creator>
    <dc:date>2012-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511053878</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Erratum to Rowles [(2011), J. Synchrotron Rad. 18, 938–941].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>An equation in the paper by Rowles [(2011), J. Synchrotron Rad. 18, 938–941] is corrected.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>On the calculation of the gauge volume size for energy-dispersive X-ray diffraction. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-01-01</prism:publicationDate>
    <prism:startingPage>136</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>136</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0470">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0470</link>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2012-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049512006784</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-03-01</prism:publicationDate>
    <prism:startingPage>290</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>291</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0466">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0466</link>
    <dc:rights>Copyright (c) 2012 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2012-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511052770</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2012 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-01-01</prism:publicationDate>
    <prism:startingPage>137</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>138</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5024">
    <title>Sub-10 nm beam confinement by X-ray waveguides: design, fabrication and characterization of optical properties</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5024</link>
    <description>The propagation of hard X-ray synchrotron beams in waveguides with guiding layer diameters in the 9–35 nm thickness range has been studied. The planar waveguide structures consist of an optimized two-component cladding. The presented fabrication method is suitable for short and leak-proof waveguide slices with lengths (along the optical axis) in the sub-500 µm range, adapted for optimized transmission at photon energies of 11.5–18 keV. A detailed comparison between finite-difference simulations of waveguide optics and the experimental results is presented, concerning transmission, divergence of the waveguide exit beam, as well as the angular acceptance. In a second step, two crossed waveguides have been used to create a quasi-point source for propagation-based X-ray imaging at the new nano-focus endstation of the P10 coherence beamline at Petra III. By inverting the measured Fraunhofer diffraction pattern by an iterative error-reduction algorithm, a two-dimensional focus of 10 nm × 10 nm is obtained. Finally, holographic imaging of a lithographic test structure based on this optical system is demonstrated.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Krüger, S.P.</dc:creator>
    <dc:creator>Neubauer, H.</dc:creator>
    <dc:creator>Bartels, M.</dc:creator>
    <dc:creator>Kalbfleisch, S.</dc:creator>
    <dc:creator>Giewekemeyer, K.</dc:creator>
    <dc:creator>Wilbrandt, P.J.</dc:creator>
    <dc:creator>Sprung, M.</dc:creator>
    <dc:creator>Salditt, T.</dc:creator>
    <dc:date>2012-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511051983</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Optimized X-ray waveguides have been fabricated and characterized in terms of transmission, angular acceptance, farfield pattern and imaging applications. Beam confinement down to sub-10 nm in two orthogonal directions has been demonstrated, at the nano-focus endstation at P10 of PETRA III at HASYLAB/DESY.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY WAVEGUIDES; X-RAY IMAGING</dc:subject>
    <dc:description>The propagation of hard X-ray synchrotron beams in waveguides with guiding layer diameters in the 9–35 nm thickness range has been studied. The planar waveguide structures consist of an optimized two-component cladding. The presented fabrication method is suitable for short and leak-proof waveguide slices with lengths (along the optical axis) in the sub-500 µm range, adapted for optimized transmission at photon energies of 11.5–18 keV. A detailed comparison between finite-difference simulations of waveguide optics and the experimental results is presented, concerning transmission, divergence of the waveguide exit beam, as well as the angular acceptance. In a second step, two crossed waveguides have been used to create a quasi-point source for propagation-based X-ray imaging at the new nano-focus endstation of the P10 coherence beamline at Petra III. By inverting the measured Fraunhofer diffraction pattern by an iterative error-reduction algorithm, a two-dimensional focus of 10 nm × 10 nm is obtained. Finally, holographic imaging of a lithographic test structure based on this optical system is demonstrated.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Sub-10 nm beam confinement by X-ray waveguides: design, fabrication and characterization of optical properties</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-03-01</prism:publicationDate>
    <prism:startingPage>227</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>236</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5192">
    <title>TXM-Wizard: a program for advanced data collection and evaluation in full-field transmission X-ray microscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5192</link>
    <description>Transmission X-ray microscopy (TXM) has been well recognized as a powerful tool for non-destructive investigation of the three-dimensional inner structure of a sample with spatial resolution down to a few tens of nanometers, especially when combined with synchrotron radiation sources. Recent developments of this technique have presented a need for new tools for both system control and data analysis. Here a software package developed in MATLAB for script command generation and analysis of TXM data is presented. The first toolkit, the script generator, allows automating complex experimental tasks which involve up to several thousand motor movements. The second package was designed to accomplish computationally intense tasks such as data processing of mosaic and mosaic tomography datasets; dual-energy contrast imaging, where data are recorded above and below a specific X-ray absorption edge; and TXM X-ray absorption near-edge structure imaging datasets. Furthermore, analytical and iterative tomography reconstruction algorithms were implemented. The compiled software package is freely available.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Liu, Y.</dc:creator>
    <dc:creator>Meirer, F.</dc:creator>
    <dc:creator>Williams, P.A.</dc:creator>
    <dc:creator>Wang, J.</dc:creator>
    <dc:creator>Andrews, J.C.</dc:creator>
    <dc:creator>Pianetta, P.</dc:creator>
    <dc:date>2012-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511049144</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A suite of GUI programs written in MATLAB for advanced data collection and analysis of full-field transmission X-ray microscopy data including mosaic imaging, tomography and XANES imaging is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY MICROSCOPY; FULL-FIELD; TOMOGRAPHY; XANES IMAGING</dc:subject>
    <dc:description>Transmission X-ray microscopy (TXM) has been well recognized as a powerful tool for non-destructive investigation of the three-dimensional inner structure of a sample with spatial resolution down to a few tens of nanometers, especially when combined with synchrotron radiation sources. Recent developments of this technique have presented a need for new tools for both system control and data analysis. Here a software package developed in MATLAB for script command generation and analysis of TXM data is presented. The first toolkit, the script generator, allows automating complex experimental tasks which involve up to several thousand motor movements. The second package was designed to accomplish computationally intense tasks such as data processing of mosaic and mosaic tomography datasets; dual-energy contrast imaging, where data are recorded above and below a specific X-ray absorption edge; and TXM X-ray absorption near-edge structure imaging datasets. Furthermore, analytical and iterative tomography reconstruction algorithms were implemented. The compiled software package is freely available.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>TXM-Wizard: a program for advanced data collection and evaluation in full-field transmission X-ray microscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:number>2</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-03-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>computer programs</prism:section>
    <prism:startingPage>281</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>287</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?vv5023">
    <title>Moiré pattern from a multiple Bragg–Laue interferometer</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?vv5023</link>
    <description>In X-ray section topography of Si 220 diffraction in a multiple Bragg–Laue mode, a moiré pattern is observed when the incident beam is divided into two parts by inserting a platinum wire in the middle of the beam. The moiré pattern can be explained by the summation of two interference fringes corresponding to the two incident beams. The coherency of the X-rays from the bending-magnet beamline is estimated using the moiré pattern.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hirano, K.</dc:creator>
    <dc:creator>Fukamachi, T.</dc:creator>
    <dc:creator>Kanematsu, Y.</dc:creator>
    <dc:creator>Jongsukswat, S.</dc:creator>
    <dc:creator>Negishi, R.</dc:creator>
    <dc:creator>Ju, D.</dc:creator>
    <dc:creator>Hirano, K.</dc:creator>
    <dc:creator>Kawamura, T.</dc:creator>
    <dc:date>2012-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511047078</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A moiré pattern is observed by dividing the incident beam into two and formed by multiple Bragg–Laue interference fringes corresponding to the two incident beams. The coherency of X-rays from a bending-magnet beamline is evaluated using the moiré pattern.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MOIRE; INTERFEROMETER; INTERFERENCE FRINGE; BRAGG-LAUE DIFFRACTION; DYNAMICAL THEORY; COHERENCY</dc:subject>
    <dc:description>In X-ray section topography of Si 220 diffraction in a multiple Bragg–Laue mode, a moiré pattern is observed when the incident beam is divided into two parts by inserting a platinum wire in the middle of the beam. The moiré pattern can be explained by the summation of two interference fringes corresponding to the two incident beams. The coherency of the X-rays from the bending-magnet beamline is estimated using the moiré pattern.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Moiré pattern from a multiple Bragg–Laue interferometer</dc:title>
    <dc:type>text</dc:type>
    <prism:number>1</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-01-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>101</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>105</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5187">
    <title>Automatic XAFS measurement system developed at BL14B2 in SPring-8</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5187</link>
    <description>A novel XAFS measurement system has been developed in which XAFS measurements can be performed including sample-loading and detector adjustments. With this system, XAFS measurements of up to 80 samples in both transmission and fluorescence modes can be carried out. The adjustment of the optical components has also been automated. It not only saves manpower and measurement time, but also improves the accuracy and reliability of sample alignments.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Oji, H.</dc:creator>
    <dc:creator>Taniguchi, Y.</dc:creator>
    <dc:creator>Hirayama, S.</dc:creator>
    <dc:creator>Ofuchi, H.</dc:creator>
    <dc:creator>Takagaki, M.</dc:creator>
    <dc:creator>Honma, T.</dc:creator>
    <dc:date>2012-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511042518</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A novel automatic measurement system has been developed, in which the XAFS measurement of up to 80 samples in transmission and fluorescence modes can be carried out.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>XAFS; AUTOMATION</dc:subject>
    <dc:description>A novel XAFS measurement system has been developed in which XAFS measurements can be performed including sample-loading and detector adjustments. With this system, XAFS measurements of up to 80 samples in both transmission and fluorescence modes can be carried out. The adjustment of the optical components has also been automated. It not only saves manpower and measurement time, but also improves the accuracy and reliability of sample alignments.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Automatic XAFS measurement system developed at BL14B2 in SPring-8</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>19</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2012-01-01</prism:publicationDate>
    <prism:startingPage>54</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>59</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5066">
    <title>Two-dimensional approach to fluorescence yield XANES measurement using a silicon drift detector. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5066</link>
    <description>An error in the paper by Tamenori et al. [(2011), J. Synchrotron Rad. 18, 747–752] is corrected.</description>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Tamenori, Y.</dc:creator>
    <dc:creator>Morita, M.</dc:creator>
    <dc:creator>Nakamura, T.</dc:creator>
    <dc:date>2011-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511041951</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An error in the paper by Tamenori et al. [(2011), J. Synchrotron Rad. 18, 747–752] is corrected.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>An error in the paper by Tamenori et al. [(2011), J. Synchrotron Rad. 18, 747–752] is corrected.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Two-dimensional approach to fluorescence yield XANES measurement using a silicon drift detector. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>18</prism:volume>
    <prism:publicationDate>2011-11-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>addenda and errata</prism:section>
    <prism:startingPage>944</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>944</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0462">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0462</link>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2011-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511041227</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>18</prism:volume>
    <prism:publicationDate>2011-11-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>current events</prism:section>
    <prism:startingPage>945</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>947</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kt5031">
    <title>Assessing noise sources at synchrotron infrared ports</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kt5031</link>
    <description>Today, the vast majority of electron storage rings delivering synchrotron radiation for general user operation offer a dedicated infrared port. There is growing interest expressed by various scientific communities to exploit the mid-IR emission in microspectroscopy, as well as the far infrared (also called THz) range for spectroscopy. Compared with a thermal (laboratory-based source), IR synchrotron radiation sources offer enhanced brilliance of about two to three orders of magnitude in the mid-IR energy range, and enhanced flux and brilliance in the far-IR energy range. Synchrotron radiation also has a unique combination of a broad wavelength band together with a well defined time structure. Thermal sources (globar, mercury filament) have excellent stability. Because the sampling rate of a typical IR Fourier-transform spectroscopy experiment is in the kHz range (depending on the bandwidth of the detector), instabilities of various origins present in synchrotron radiation sources play a crucial role. Noise recordings at two different IR ports located at the Swiss Light Source and SOLEIL (France), under conditions relevant to real experiments, are discussed. The lowest electron beam fluctuations detectable in IR spectra have been quantified and are shown to be much smaller than what is routinely recorded by beam-position monitors.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Lerch, P.</dc:creator>
    <dc:creator>Dumas, P.</dc:creator>
    <dc:creator>Schilcher, T.</dc:creator>
    <dc:creator>Nadji, A.</dc:creator>
    <dc:creator>Luedeke, A.</dc:creator>
    <dc:creator>Hubert, N.</dc:creator>
    <dc:creator>Cassinari, L.</dc:creator>
    <dc:creator>Boege, M.</dc:creator>
    <dc:creator>Denard, J.-C.</dc:creator>
    <dc:creator>Stingelin, L.</dc:creator>
    <dc:creator>Nadolski, L.</dc:creator>
    <dc:creator>Garvey, T.</dc:creator>
    <dc:creator>Albert, S.</dc:creator>
    <dc:creator>Gough, Ch.</dc:creator>
    <dc:creator>Quack, M.</dc:creator>
    <dc:creator>Wambach, J.</dc:creator>
    <dc:creator>Dehler, M.</dc:creator>
    <dc:creator>Filhol, J.-M.</dc:creator>
    <dc:date>2012-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511041884</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Low-frequency noise present in the electron and photon beams of two comparable storage rings, SOLEIL and SLS, are carefully compared in the context of IR spectroscopy using the Fourier transform technique.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>NOISE; FTIR; SPECTROSCOPY</dc:subject>
    <dc:description>Today, the vast majority of electron storage rings delivering synchrotron radiation for general user operation offer a dedicated infrared port. There is growing interest expressed by various scientific communities to exploit the mid-IR emission in microspectroscopy, as well as the far infrared (also called THz) range for spectroscopy. Compared with a thermal (laboratory-based source), IR synchrotron radiation sources offer enhanced brilliance of about two to three orders of magnitude in the mid-IR energy range, and enhanced flux and brilliance in the far-IR energy range. Synchrotron radiation also has a unique combination of a broad wavelength band together with a well defined time structure. Thermal sources (globar, mercury filament) have excellent stability. Because the sampling rate of a typical IR Fourier-transform spectroscopy experiment is in the kHz range (depending on the bandwidth of the detector), instabilities of various origins present in synchrotron radiation sources play a crucial role. Noise recordings at two different IR ports located at the Swiss Light Source and SOLEIL (France), under conditions relevant to real experiments, are discussed. The lowest electron beam fluctuations detectable in IR spectra have been quantified and are shown to be much smaller than what is routinely recorded by beam-position monitors.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Assessing noise sources at synchrotron infrared ports</dc:title>
    <dc:type>text</dc:type>
    <prism:number>1</prism:number>
    <prism:volume>19</prism:volume>
    <prism:publicationDate>2012-01-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>1</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>9</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5013">
    <title>X-ray near-field speckle: implementation and critical analysis</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5013</link>
    <description>The newly introduced coherence-based technique of X-ray near-field speckle (XNFS) has been implemented at 8-ID-I at the Advanced Photon Source. In the near-field regime of high-brilliance synchrotron X-rays scattered from a sample of interest, it turns out that, when the scattered radiation and the main beam both impinge upon an X-ray area detector, the measured intensity shows low-contrast speckles, resulting from interference between the incident and scattered beams. A micrometer-resolution XNFS detector with a high numerical aperture microscope objective has been built and its capability for studying static structures and dynamics at longer length scales than traditional far-field X-ray scattering techniques is demonstrated. Specifically, the dynamics of dilute silica and polystyrene colloidal samples are characterized. This study reveals certain limitations of the XNFS technique, especially in the characterization of static structures, which is discussed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Lu, X.</dc:creator>
    <dc:creator>Mochrie, S.G.J.</dc:creator>
    <dc:creator>Narayanan, S.</dc:creator>
    <dc:creator>Sandy, A.R.</dc:creator>
    <dc:creator>Sprung, M.</dc:creator>
    <dc:date>2011-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511037149</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A coherence-based X-ray near-field speckle detector has been implemented and characterized for its capability of studying static structure and dynamics.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY; NEAR FIELD; SPECKLE; SPECTROSCOPY; SCATTERING</dc:subject>
    <dc:description>The newly introduced coherence-based technique of X-ray near-field speckle (XNFS) has been implemented at 8-ID-I at the Advanced Photon Source. In the near-field regime of high-brilliance synchrotron X-rays scattered from a sample of interest, it turns out that, when the scattered radiation and the main beam both impinge upon an X-ray area detector, the measured intensity shows low-contrast speckles, resulting from interference between the incident and scattered beams. A micrometer-resolution XNFS detector with a high numerical aperture microscope objective has been built and its capability for studying static structures and dynamics at longer length scales than traditional far-field X-ray scattering techniques is demonstrated. Specifically, the dynamics of dilute silica and polystyrene colloidal samples are characterized. This study reveals certain limitations of the XNFS technique, especially in the characterization of static structures, which is discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray near-field speckle: implementation and critical analysis</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-11-01</prism:publicationDate>
    <prism:startingPage>823</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>834</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?tc5018">
    <title>Development of a soft X-ray angle-resolved photoemission system applicable to 100 µm crystals</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?tc5018</link>
    <description>A system for angle-resolved photoemission spectroscopy (ARPES) of small single crystals with sizes down to 100 µm has been developed. Soft X-ray synchrotron radiation with a spot size of ∼40 µm × 65 µm at the sample position is used for the excitation. Using this system an ARPES measurement has been performed on a Si crystal of size 120 µm × 100 µm × 80 µm. The crystal was properly oriented on a sample stage by measuring the Laue spots. The crystal was cleaved in situ with a microcleaver at 100 K. The cleaved surface was adjusted to the beam spot using an optical microscope. Consequently, clear band dispersions along the Γ–X direction reflecting the bulk electronic states were observed with a photon energy of 879 eV.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Muro, T.</dc:creator>
    <dc:creator>Kato, Y.</dc:creator>
    <dc:creator>Matsushita, T.</dc:creator>
    <dc:creator>Kinoshita, T.</dc:creator>
    <dc:creator>Watanabe, Y.</dc:creator>
    <dc:creator>Okazaki, H.</dc:creator>
    <dc:creator>Yokoya, T.</dc:creator>
    <dc:creator>Sekiyama, A.</dc:creator>
    <dc:creator>Suga, S.</dc:creator>
    <dc:date>2011-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511034418</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A soft X-ray angle-resolved photoemission system applicable to 100 µm crystals has been developed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ANGLE-RESOLVED PHOTOEMISSION SPECTROSCOPY (ARPES); SOFT X-RAY; SMALL CRYSTAL; MICROCLEAVING; MICROPOSITIONING</dc:subject>
    <dc:description>A system for angle-resolved photoemission spectroscopy (ARPES) of small single crystals with sizes down to 100 µm has been developed. Soft X-ray synchrotron radiation with a spot size of ∼40 µm × 65 µm at the sample position is used for the excitation. Using this system an ARPES measurement has been performed on a Si crystal of size 120 µm × 100 µm × 80 µm. The crystal was properly oriented on a sample stage by measuring the Laue spots. The crystal was cleaved in situ with a microcleaver at 100 K. The cleaved surface was adjusted to the beam spot using an optical microscope. Consequently, clear band dispersions along the Γ–X direction reflecting the bulk electronic states were observed with a photon energy of 879 eV.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Development of a soft X-ray angle-resolved photoemission system applicable to 100 µm crystals</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-11-01</prism:publicationDate>
    <prism:startingPage>879</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>884</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?gf5038">
    <title>Time-over-threshold readout to enhance the high flux capabilities of single-photon-counting detectors</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?gf5038</link>
    <description>The MYTHEN single-photon-counting (SPC) detector has been characterized using the time-over-threshold (ToT) readout method, i.e. measuring the time that the signal produced by the detected X-rays remains above the comparator threshold. In the following it is shown that the ToT readout preserves the sensitivity, dynamic range and capability of background suppression of the SPC mode, while enhancing the count-rate capability, which is the main limitation of state-of-the-art SPC systems.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Bergamaschi, A.</dc:creator>
    <dc:creator>Dinapoli, R.</dc:creator>
    <dc:creator>Greiffenberg, D.</dc:creator>
    <dc:creator>Henrich, B.</dc:creator>
    <dc:creator>Johnson, I.</dc:creator>
    <dc:creator>Mozzanica, A.</dc:creator>
    <dc:creator>Radicci, V.</dc:creator>
    <dc:creator>Schmitt, B.</dc:creator>
    <dc:creator>Shi, X.</dc:creator>
    <dc:creator>Stoppani, L.</dc:creator>
    <dc:date>2011-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511034480</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The MYTHEN photon-counting ASIC operated in time-over-threshold mode shows an innovative approach towards the development of a detector operating with very high photon intensities while maintaining the single-photon sensitivity for synchrotron radiation experiments.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DETECTORS; SINGLE-PHOTON COUNTING; TIME OVER THRESHOLD</dc:subject>
    <dc:description>The MYTHEN single-photon-counting (SPC) detector has been characterized using the time-over-threshold (ToT) readout method, i.e. measuring the time that the signal produced by the detected X-rays remains above the comparator threshold. In the following it is shown that the ToT readout preserves the sensitivity, dynamic range and capability of background suppression of the SPC mode, while enhancing the count-rate capability, which is the main limitation of state-of-the-art SPC systems.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Time-over-threshold readout to enhance the high flux capabilities of single-photon-counting detectors</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>18</prism:volume>
    <prism:publicationDate>2011-11-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>923</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>929</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0449">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0449</link>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2011-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511030949</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-09-01</prism:publicationDate>
    <prism:startingPage>819</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>821</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5188">
    <title>In situ two-dimensional imaging quick-scanning XAFS with pixel array detector</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5188</link>
    <description>Quick-scanning X-ray absorption fine structure (XAFS) measurements were performed in transmission mode using a PILATUS 100K pixel array detector (PAD). The method can display a two-dimensional image for a large area of the order of a centimetre with a spatial resolution of 0.2 mm at each energy point in the XAFS spectrum. The time resolution of the quick-scanning method ranged from 10 s to 1 min per spectrum depending on the energy range. The PAD has a wide dynamic range and low noise, so the obtained spectra have a good signal-to-noise ratio.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Tanida, H.</dc:creator>
    <dc:creator>Yamashige, H.</dc:creator>
    <dc:creator>Orikasa, Y.</dc:creator>
    <dc:creator>Oishi, M.</dc:creator>
    <dc:creator>Takanashi, Y.</dc:creator>
    <dc:creator>Fujimoto, T.</dc:creator>
    <dc:creator>Sato, K.</dc:creator>
    <dc:creator>Takamatsu, D.</dc:creator>
    <dc:creator>Murayama, H.</dc:creator>
    <dc:creator>Arai, H.</dc:creator>
    <dc:creator>Matsubara, E.</dc:creator>
    <dc:creator>Uchimoto, Y.</dc:creator>
    <dc:creator>Ogumi, Z.</dc:creator>
    <dc:date>2011-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511031232</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Two-dimensional imaging quick-scanning XAFS measurements were performed using a pixel array detector.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>XAFS; TWO-DIMENSIONAL IMAGING; IN SITU; QUICK SCANNING; PIXEL ARRAY DETECTOR</dc:subject>
    <dc:description>Quick-scanning X-ray absorption fine structure (XAFS) measurements were performed in transmission mode using a PILATUS 100K pixel array detector (PAD). The method can display a two-dimensional image for a large area of the order of a centimetre with a spatial resolution of 0.2 mm at each energy point in the XAFS spectrum. The time resolution of the quick-scanning method ranged from 10 s to 1 min per spectrum depending on the energy range. The PAD has a wide dynamic range and low noise, so the obtained spectra have a good signal-to-noise ratio.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>In situ two-dimensional imaging quick-scanning XAFS with pixel array detector</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>18</prism:volume>
    <prism:publicationDate>2011-11-01</prism:publicationDate>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:issn>0909-0495</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>919</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>922</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?vv5017">
    <title>Fluorescence detection of white-beam X-ray absorption anisotropy: towards element-sensitive projections of local atomic structure</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?vv5017</link>
    <description>Projections of the atomic structure around Nb atoms in a LiNbO3 single crystal were obtained from a white-beam X-ray absorption anisotropy (XAA) pattern detected using Nb K fluorescence. This kind of anisotropy results from the interference of X-rays inside a sample and, owing to the short coherence length of a white beam, is visible only at small angles around interatomic directions. Consequently, the main features of the recorded XAA corresponded to distorted real-space projections of dense-packed atomic planes and atomic rows. A quantitative analysis of XAA was carried out using a wavelet transform and allowed well resolved projections of Nb atoms to be obtained up to distances of 10 Å. The signal of nearest O atoms was detected indirectly by a comparison with model calculations. The measurement of white-beam XAA using characteristic radiation indicates the possibility of obtaining element-sensitive projections of the local atomic structure in more complex samples.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Korecki, P.</dc:creator>
    <dc:creator>Tolkiehn, M.</dc:creator>
    <dc:creator>Dąbrowski, K.M.</dc:creator>
    <dc:creator>Novikov, D.V.</dc:creator>
    <dc:date>2011-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511030688</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A method for a direct measurement of X-ray projections of the atomic structure is described. Projections of the atomic structure around Nb atoms in a LiNbO3 single crystal were obtained from a white-beam X-ray absorption anisotropy pattern detected using Nb K fluorescence.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY DIFFRACTION AND ABSORPTION; ATOMIC STRUCTURE DETERMINATION; POLYCHROMATIC RADIATION; WAVELET TRANSFORM</dc:subject>
    <dc:description>Projections of the atomic structure around Nb atoms in a LiNbO3 single crystal were obtained from a white-beam X-ray absorption anisotropy (XAA) pattern detected using Nb K fluorescence. This kind of anisotropy results from the interference of X-rays inside a sample and, owing to the short coherence length of a white beam, is visible only at small angles around interatomic directions. Consequently, the main features of the recorded XAA corresponded to distorted real-space projections of dense-packed atomic planes and atomic rows. A quantitative analysis of XAA was carried out using a wavelet transform and allowed well resolved projections of Nb atoms to be obtained up to distances of 10 Å. The signal of nearest O atoms was detected indirectly by a comparison with model calculations. The measurement of white-beam XAA using characteristic radiation indicates the possibility of obtaining element-sensitive projections of the local atomic structure in more complex samples.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Fluorescence detection of white-beam X-ray absorption anisotropy: towards element-sensitive projections of local atomic structure</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-11-01</prism:publicationDate>
    <prism:startingPage>851</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>861</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5646">
    <title>Two-dimensional approach to fluorescence yield XANES measurement using a silicon drift detector</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5646</link>
    <description>The objective of this article is to describe the capability of a two-dimensional (2D) approach to X-ray absorption near-edge structure (XANES) measurement by means of a partial fluorescence yield (PFY) method. 2D-XANES measurements were achieved by using a silicon drift detector as an energy-dispersive fluorescence detector. The advantage of this technique is that it allows full surveys of X-ray fluorescence data that are lost in conventional PFY measurements. The availability of a map approach was demonstrated by applying it to XANES measurements in both a diluted (Mn-doped nano-diamond) and a concentrated (MnO crystal) manganese sample. The 2D approach clearly distinguished between the PFY spectra of Mn and O atoms, where absorption edges of both elements are close to each other. Further, the 2D approach extracted an unambiguous PFY spectrum of phosphorus in the XANES measurement of SS304 (P &lt; 0.045 wt%).</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Tamenori, Y.</dc:creator>
    <dc:creator>Morita, M.</dc:creator>
    <dc:creator>Nakamura, T.</dc:creator>
    <dc:date>2011-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511027531</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Partial fluorescence yield XANES measurements were performed using a silicon drift detector in the soft X-ray region. This technique provides unambiguous XANES data in the soft X-ray region, where absorption edges of different elements are close to each other, or where fluorescence lines overlap.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>XANES; SOFT X-RAYS; SILICON DRIFT DETECTOR; PARTIAL FLUORESCENCE YIELD; MAPAPPROACH</dc:subject>
    <dc:description>The objective of this article is to describe the capability of a two-dimensional (2D) approach to X-ray absorption near-edge structure (XANES) measurement by means of a partial fluorescence yield (PFY) method. 2D-XANES measurements were achieved by using a silicon drift detector as an energy-dispersive fluorescence detector. The advantage of this technique is that it allows full surveys of X-ray fluorescence data that are lost in conventional PFY measurements. The availability of a map approach was demonstrated by applying it to XANES measurements in both a diluted (Mn-doped nano-diamond) and a concentrated (MnO crystal) manganese sample. The 2D approach clearly distinguished between the PFY spectra of Mn and O atoms, where absorption edges of both elements are close to each other. Further, the 2D approach extracted an unambiguous PFY spectrum of phosphorus in the XANES measurement of SS304 (P &lt; 0.045 wt%).</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Two-dimensional approach to fluorescence yield XANES measurement using a silicon drift detector</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-09-01</prism:publicationDate>
    <prism:startingPage>747</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>752</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?bf5038">
    <title>SHADOW3: a new version of the synchrotron X-ray optics modelling package</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?bf5038</link>
    <description>A new version of the popular X-ray tracing code SHADOW is presented. An important step has been made in restructuring the code following new computer engineering standards, ending with a modular Fortran 2003 structure and an application programming interface (API). The new code has been designed to be compatible with the original file-oriented SHADOW philosophy, but simplifying the compilation, installation and use. In addition, users can now become programmers using the newly designed SHADOW3 API for creating scripts, macros and programs; being able to deal with optical system optimization, image simulation, and also low transmission calculations requiring a large number of rays (&gt;106). Plans for future development and questions on how to accomplish them are also discussed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sanchez del Rio, M.</dc:creator>
    <dc:creator>Canestrari, N.</dc:creator>
    <dc:creator>Jiang, F.</dc:creator>
    <dc:creator>Cerrina, F.</dc:creator>
    <dc:date>2011-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511026306</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>SHADOW3, a new version of the X-ray tracing code SHADOW, is introduced.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SHADOW; RAY-TRACING; X-RAY OPTICS</dc:subject>
    <dc:description>A new version of the popular X-ray tracing code SHADOW is presented. An important step has been made in restructuring the code following new computer engineering standards, ending with a modular Fortran 2003 structure and an application programming interface (API). The new code has been designed to be compatible with the original file-oriented SHADOW philosophy, but simplifying the compilation, installation and use. In addition, users can now become programmers using the newly designed SHADOW3 API for creating scripts, macros and programs; being able to deal with optical system optimization, image simulation, and also low transmission calculations requiring a large number of rays (&gt;106). Plans for future development and questions on how to accomplish them are also discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>SHADOW3: a new version of the synchrotron X-ray optics modelling package</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-09-01</prism:publicationDate>
    <prism:startingPage>708</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>716</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5049">
    <title>Milli-electronvolt monochromatization of hard X-rays with a sapphire backscattering monochromator</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5049</link>
    <description>A sapphire backscattering monochromator with 1.1 (1) meV bandwidth for hard X-rays (20–40 keV) is reported. The optical quality of several sapphire crystals has been studied and the best crystal was chosen to work as the monochromator. The small energy bandwidth has been obtained by decreasing the crystal volume impinged upon by the beam and by choosing the crystal part with the best quality. The monochromator was tested at the energies of the nuclear resonances of 121Sb at 37.13 keV, 125Te at 35.49 keV, 119Sn at 23.88 keV, 149Sm at 22.50 keV and 151Eu at 21.54 keV. For each energy, specific reflections with sapphire temperatures in the 150–300 K region were chosen. Applications to nuclear inelastic scattering with these isotopes are demonstrated.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sergueev, I.</dc:creator>
    <dc:creator>Wille, H.-C.</dc:creator>
    <dc:creator>Hermann, R.P.</dc:creator>
    <dc:creator>Bessas, D.</dc:creator>
    <dc:creator>Shvyd'ko, Y.V.</dc:creator>
    <dc:creator>Zając, M.</dc:creator>
    <dc:creator>Rüffer, R.</dc:creator>
    <dc:date>2011-09-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951102485X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Monochromatization of hard X-rays in the 20–40 keV energy range to ∼1 meV bandwidth using a sapphire backscattering monochromator is demonstrated.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY OPTICS; MONOCHROMATOR; ENERGY RESOLUTION; SAPPHIRE; BACKSCATTERING; INELASTIC SCATTERING</dc:subject>
    <dc:description>A sapphire backscattering monochromator with 1.1 (1) meV bandwidth for hard X-rays (20–40 keV) is reported. The optical quality of several sapphire crystals has been studied and the best crystal was chosen to work as the monochromator. The small energy bandwidth has been obtained by decreasing the crystal volume impinged upon by the beam and by choosing the crystal part with the best quality. The monochromator was tested at the energies of the nuclear resonances of 121Sb at 37.13 keV, 125Te at 35.49 keV, 119Sn at 23.88 keV, 149Sm at 22.50 keV and 151Eu at 21.54 keV. For each energy, specific reflections with sapphire temperatures in the 150–300 K region were chosen. Applications to nuclear inelastic scattering with these isotopes are demonstrated.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Milli-electronvolt monochromatization of hard X-rays with a sapphire backscattering monochromator</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-09-01</prism:publicationDate>
    <prism:startingPage>802</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>810</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pf0086">
    <title>Introduction to XAFS. A Practical Guide to X-ray Absorption Fine Structure Spectroscopy. By Grant Bunker. Pp. viii + 260. Cambridge University Press, 2010. Price (hardback) GBP 40. ISBN-13: 978-0-521-76775-0.</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pf0086</link>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Paufler, P.</dc:creator>
    <dc:date>2011-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511023703</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Introduction to XAFS. A Practical Guide to X-ray Absorption Fine Structure Spectroscopy. By Grant Bunker. Pp. viii + 260. Cambridge University Press, 2010. Price (hardback) GBP 40. ISBN-13: 978-0-521-76775-0.</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-09-01</prism:publicationDate>
    <prism:startingPage>818</prism:startingPage>
    <prism:section>books received</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>818</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0447">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0447</link>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511022898</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>686</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>687</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5010">
    <title>Six-reflection meV-monochromator for synchrotron radiation</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5010</link>
    <description>An in-line monochromatization scheme suitable for 10–40 keV synchrotron radiation is presented based on the use of six crystal reflections that achieves meV and sub-meV bandwidths with high efficiency. The theoretical spectral efficiency surpasses all previous multicrystal designs and approaches that of single room-temperature back-reflecting crystals. This article presents the designs of two such devices along with their theoretical and measured performances.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Toellner, T.S.</dc:creator>
    <dc:creator>Alatas, A.</dc:creator>
    <dc:creator>Said, A.H.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511017535</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A design is presented for a cryogenically stabilized monochromator for 10–40 keV synchrotron radiation that uses six crystal reflections to achieve a meV-bandpass with high efficiency.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HIGH RESOLUTION; MONOCHROMATOR; X-RAY</dc:subject>
    <dc:description>An in-line monochromatization scheme suitable for 10–40 keV synchrotron radiation is presented based on the use of six crystal reflections that achieves meV and sub-meV bandwidths with high efficiency. The theoretical spectral efficiency surpasses all previous multicrystal designs and approaches that of single room-temperature back-reflecting crystals. This article presents the designs of two such devices along with their theoretical and measured performances.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Six-reflection meV-monochromator for synchrotron radiation</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>605</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>611</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5011">
    <title>Development of an X-ray real-time stereo imaging technique using synchrotron radiation</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5011</link>
    <description>An X-ray stereo imaging system with synchrotron radiation was developed at BL20B2, SPring-8. A portion of a wide X-ray beam was Bragg-reflected by a silicon crystal to produce an X-ray beam which intersects with the direct X-ray beam. Samples were placed at the intersection point of the two beam paths. X-ray stereo images were recorded simultaneously by a detector with a large field of view placed close to the sample. A three-dimensional wire-frame model of a sample was created from the depth information that was obtained from the lateral positions in the stereo image. X-ray stereo angiography of a mouse femoral region was performed as a demonstration of real-time stereo imaging. Three-dimensional arrangements of the femur and blood vessels were obtained.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hoshino, M.</dc:creator>
    <dc:creator>Uesugi, K.</dc:creator>
    <dc:creator>Pearson, J.</dc:creator>
    <dc:creator>Sonobe, T.</dc:creator>
    <dc:creator>Shirai, M.</dc:creator>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511017547</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An X-ray stereo imaging system with synchrotron radiation was developed to perform real-time stereo imaging and stereo angiography.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY STEREO IMAGING; REAL-TIME IMAGING; ANGIOGRAPHY</dc:subject>
    <dc:description>An X-ray stereo imaging system with synchrotron radiation was developed at BL20B2, SPring-8. A portion of a wide X-ray beam was Bragg-reflected by a silicon crystal to produce an X-ray beam which intersects with the direct X-ray beam. Samples were placed at the intersection point of the two beam paths. X-ray stereo images were recorded simultaneously by a detector with a large field of view placed close to the sample. A three-dimensional wire-frame model of a sample was created from the depth information that was obtained from the lateral positions in the stereo image. X-ray stereo angiography of a mouse femoral region was performed as a demonstration of real-time stereo imaging. Three-dimensional arrangements of the femur and blood vessels were obtained.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Development of an X-ray real-time stereo imaging technique using synchrotron radiation</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>569</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>574</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi9618">
    <title>Calcifications in human osteoarthritic articular cartilage: ex vivo assessment of calcium compounds using XANES spectroscopy. Addendum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi9618</link>
    <description>An acknowledgment is published for the paper by Nguyen et al. [(2011), J. Synchrotron Rad. 18, 475–480].</description>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Nguyen, C.</dc:creator>
    <dc:creator>Ea, H.K.</dc:creator>
    <dc:creator>Thiaudiere, D.</dc:creator>
    <dc:creator>Reguer, S.</dc:creator>
    <dc:creator>Hannouche, D.</dc:creator>
    <dc:creator>Daudon, M.</dc:creator>
    <dc:creator>lioté, F.</dc:creator>
    <dc:creator>Bazin, D.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951101689X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An acknowledgment is published for the paper by Nguyen et al. [(2011), J. Synchrotron Rad. 18, 475–480].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>An acknowledgment is published for the paper by Nguyen et al. [(2011), J. Synchrotron Rad. 18, 475–480].</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Calcifications in human osteoarthritic articular cartilage: ex vivo assessment of calcium compounds using XANES spectroscopy. Addendum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>685</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>685</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?vv5014">
    <title>Radiation-induced melting in coherent X-ray diffractive imaging at the nanoscale</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?vv5014</link>
    <description>Coherent X-ray diffraction techniques play an increasingly significant role in the imaging of nanoscale structures, ranging from metallic and semiconductor to biological objects. In material science, X-rays are usually considered to be of a low-destructive nature, but under certain conditions they can cause significant radiation damage and heat loading on the samples. The qualitative literature data concerning the tolerance of nanostructured samples to synchrotron radiation in coherent diffraction imaging experiments are scarce. In this work the experimental evidence of a complete destruction of polymer and gold nanosamples by the synchrotron beam is reported in the case of imaging at 1–10 nm spatial resolution. Numerical simulations based on a heat-transfer model demonstrate the high sensitivity of temperature distribution in samples to macroscopic experimental parameters such as the conduction properties of materials, radiation heat transfer and convection. However, for realistic experimental conditions the calculated rates of temperature rise alone cannot explain the melting transitions observed in the nanosamples. Comparison of these results with the literature data allows a specific scenario of the sample destruction in each particular case to be presented, and a strategy for damage reduction to be proposed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ponomarenko, O.</dc:creator>
    <dc:creator>Nikulin, A.Y.</dc:creator>
    <dc:creator>Moser, H.O.</dc:creator>
    <dc:creator>Yang, P.</dc:creator>
    <dc:creator>Sakata, O.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511016335</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Coherent X-ray diffraction techniques play an increasingly significant role in imaging nanoscale structures which range from metallic and semiconductor samples to biological objects. The conventional knowledge about radiation damage effects caused by ever higher brilliance X-ray sources has to be critically revised while studying nanostructured materials.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COHERENT X-RAY DIFFRACTION IMAGING; HIGH-RESOLUTION SYNCHROTRON RADIATION; HEATLOAD; NANOSIZE EFFECTS</dc:subject>
    <dc:description>Coherent X-ray diffraction techniques play an increasingly significant role in the imaging of nanoscale structures, ranging from metallic and semiconductor to biological objects. In material science, X-rays are usually considered to be of a low-destructive nature, but under certain conditions they can cause significant radiation damage and heat loading on the samples. The qualitative literature data concerning the tolerance of nanostructured samples to synchrotron radiation in coherent diffraction imaging experiments are scarce. In this work the experimental evidence of a complete destruction of polymer and gold nanosamples by the synchrotron beam is reported in the case of imaging at 1–10 nm spatial resolution. Numerical simulations based on a heat-transfer model demonstrate the high sensitivity of temperature distribution in samples to macroscopic experimental parameters such as the conduction properties of materials, radiation heat transfer and convection. However, for realistic experimental conditions the calculated rates of temperature rise alone cannot explain the melting transitions observed in the nanosamples. Comparison of these results with the literature data allows a specific scenario of the sample destruction in each particular case to be presented, and a strategy for damage reduction to be proposed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Radiation-induced melting in coherent X-ray diffractive imaging at the nanoscale</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>580</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>594</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5028">
    <title>Macromolecular crystallography radiation damage research: what's new?</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5028</link>
    <description>Radiation damage in macromolecular crystallography has become a mainstream concern over the last ten years. The current status of research into this area is briefly assessed, and the ten new papers published in this issue are set into the context of previous work in the field. Some novel and exciting developments emerging over the last two years are also summarized.</description>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:creator>Weik, M.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511013859</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An introductory overview of the special issue papers on radiation damage in this issue..</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>Radiation damage in macromolecular crystallography has become a mainstream concern over the last ten years. The current status of research into this area is briefly assessed, and the ten new papers published in this issue are set into the context of previous work in the field. Some novel and exciting developments emerging over the last two years are also summarized.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Macromolecular crystallography radiation damage research: what's new?</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>313</prism:startingPage>
    <prism:section>editorial</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>317</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0446">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0446</link>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511012805</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>534</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>536</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ms5033">
    <title>Automatic loop centring with a high-precision goniometer head at the SLS macromolecular crystallography beamlines</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ms5033</link>
    <description>Automatic loop centring has been developed as part of the automation process in crystallographic data collection at the Swiss Light Source. The procedure described here consists of an optional set-up part, in which the background images are taken, and the actual centring part. The algorithm uses boundary and centre-of-mass detection at two different microscope image magnifications. Micromounts can be handled as well. Centring of the loops can be achieved in 15–26 s, depending on their initial position, and as fast as manual centring. The alignment of the sample is carried out by means of a new flexural-hinge-based compact goniometer head. The device features an electromagnet for robotic wet mounting of samples. The circle of confusion was measured to be smaller than 1 µm (r.m.s.); its bidirectional backlash is below 2 µm.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Pauluhn, A.</dc:creator>
    <dc:creator>Pradervand, C.</dc:creator>
    <dc:creator>Rossetti, D.</dc:creator>
    <dc:creator>Salathe, M.</dc:creator>
    <dc:creator>Schulze-Briese, C.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511011848</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An automated loop-centring program and a high-precision goniometer head used at the Swiss Light Source are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>BEAMLINE AUTOMATION; SAMPLE CENTRING; GONIOMETER HEAD</dc:subject>
    <dc:description>Automatic loop centring has been developed as part of the automation process in crystallographic data collection at the Swiss Light Source. The procedure described here consists of an optional set-up part, in which the background images are taken, and the actual centring part. The algorithm uses boundary and centre-of-mass detection at two different microscope image magnifications. Micromounts can be handled as well. Centring of the loops can be achieved in 15–26 s, depending on their initial position, and as fast as manual centring. The alignment of the sample is carried out by means of a new flexural-hinge-based compact goniometer head. The device features an electromagnet for robotic wet mounting of samples. The circle of confusion was measured to be smaller than 1 µm (r.m.s.); its bidirectional backlash is below 2 µm.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Automatic loop centring with a high-precision goniometer head at the SLS macromolecular crystallography beamlines</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>595</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>600</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ms5030">
    <title>DNA damage and repair kinetics after microbeam radiation therapy emulation in living cells using monoenergetic synchrotron X-ray microbeams</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ms5030</link>
    <description>A novel synchrotron-based approach, known as microbeam radiation therapy (MRT), currently shows considerable promise in increased tumour control and reduced normal tissue damage compared with conventional radiotherapy. Different microbeam widths and separations were investigated using a controlled cell culture system and monoenergetic (5.35 keV) synchrotron X-rays in order to gain further insight into the underlying cellular response to MRT. DNA damage and repair was measured using fluorescent antibodies against phosphorylated histone H2AX, which also allowed us to verify the exact location of the microbeam path. Beam dimensions that reproduced promising MRT strategies were used to identify useful methods to study the underpinnings of MRT. These studies include the investigation of different spatial configurations on bystander effects. γH2AX foci number were robustly induced in directly hit cells and considerable DNA double-strand break repair occurred by 12 h post-10 Gy irradiation; however, many cells had some γH2AX foci at the 12 h time point. γH2AX foci at later time points did not directly correspond with the targeted regions suggesting cell movement or bystander effects as a potential mechanism for MRT effectiveness. Partial irradiation of single nuclei was also investigated and in most cases γH2AX foci were not observed outside the field of irradiation within 1 h after irradiation indicating very little chromatin movement in this time frame. These studies contribute to the understanding of the fundamental radiation biology relating to the MRT response, a potential new therapy for cancer patients.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sprung, C.N.</dc:creator>
    <dc:creator>Cholewa, M.</dc:creator>
    <dc:creator>Usami, N.</dc:creator>
    <dc:creator>Kobayashi, K.</dc:creator>
    <dc:creator>Crosbie, J.C.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511011836</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The molecular response of mammalian cells to a monoenergetic synchrotron X-ray microbeam which emulated microbeam radiation configurations has been investigated. Very few γH2AX foci were found outside the irradiated zone within 1 h of irradiation, even within a single nucleus. Furthermore, 12 h after radiation there was a large decrease in foci number but many cells still contained γH2AX foci, of which many were outside the directly irradiated regions.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DOUBLE-STRAND BREAKS; IONIZING RADIATION; X-RAYS; [GAMMA]H2AX</dc:subject>
    <dc:description>A novel synchrotron-based approach, known as microbeam radiation therapy (MRT), currently shows considerable promise in increased tumour control and reduced normal tissue damage compared with conventional radiotherapy. Different microbeam widths and separations were investigated using a controlled cell culture system and monoenergetic (5.35 keV) synchrotron X-rays in order to gain further insight into the underlying cellular response to MRT. DNA damage and repair was measured using fluorescent antibodies against phosphorylated histone H2AX, which also allowed us to verify the exact location of the microbeam path. Beam dimensions that reproduced promising MRT strategies were used to identify useful methods to study the underpinnings of MRT. These studies include the investigation of different spatial configurations on bystander effects. γH2AX foci number were robustly induced in directly hit cells and considerable DNA double-strand break repair occurred by 12 h post-10 Gy irradiation; however, many cells had some γH2AX foci at the 12 h time point. γH2AX foci at later time points did not directly correspond with the targeted regions suggesting cell movement or bystander effects as a potential mechanism for MRT effectiveness. Partial irradiation of single nuclei was also investigated and in most cases γH2AX foci were not observed outside the field of irradiation within 1 h after irradiation indicating very little chromatin movement in this time frame. These studies contribute to the understanding of the fundamental radiation biology relating to the MRT response, a potential new therapy for cancer patients.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>DNA damage and repair kinetics after microbeam radiation therapy emulation in living cells using monoenergetic synchrotron X-ray microbeams</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>630</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>636</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ms5034">
    <title>A narrow microbeam is more effective for tumor growth suppression than a wide microbeam: an in vivo study using implanted human glioma cells</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ms5034</link>
    <description>The tumoricidal mechanisms of microbeam radiation therapy, and the more recently proposed minibeam radiation therapy, for the treatment of brain tumors are as yet unclear. Moreover, from among the various parameters of beam geometry the impact of changing the beam width is unknown. In this study, suppression of tumor growth in human glioma cells implanted in mice was evaluated experimentally using microbeams of two different widths: a conventional narrow beam (20 µm width, 100 µm center-to-center distance) and a wide beam (100 µm width, 500 µm center-to-center distance). The tumor growth ratio was compared and acute cell death was studied histologically. With cross-planar irradiation, tumor growth was significantly suppressed between days 4 and 28 after 20 µm microbeam irradiation, whereas tumor growth was suppressed, and not significantly so, only between days 4 and 18 after 100 µm microbeam irradiation. Immunohistochemistry using TUNEL staining showed no increase in TUNEL-positive cells with either microbeam at 24 and 72 h post-irradiation. The 20 µm microbeam was found to be more tumoricidal than the 100 µm microbeam, and the effect was not related to apoptotic cell death. The underlying mechanism may be functional tissue deterioration rather than direct cellular damage in the beam path.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Uyama, A.</dc:creator>
    <dc:creator>Kondoh, T.</dc:creator>
    <dc:creator>Nariyama, N.</dc:creator>
    <dc:creator>Umetani, K.</dc:creator>
    <dc:creator>Fukumoto, M.</dc:creator>
    <dc:creator>Shinohara, K.</dc:creator>
    <dc:creator>Kohmura, E.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951101185X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A narrow microbeam is shown to be more effective than a wide microbeam for microbeam radiation therapy.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MICROBEAM RADIATION THERAPY; NARROW MICROBEAM; WIDE MICROBEAM; CO-PLANAR MICROBEAM; CROSS-PLANAR MICROBEAM</dc:subject>
    <dc:description>The tumoricidal mechanisms of microbeam radiation therapy, and the more recently proposed minibeam radiation therapy, for the treatment of brain tumors are as yet unclear. Moreover, from among the various parameters of beam geometry the impact of changing the beam width is unknown. In this study, suppression of tumor growth in human glioma cells implanted in mice was evaluated experimentally using microbeams of two different widths: a conventional narrow beam (20 µm width, 100 µm center-to-center distance) and a wide beam (100 µm width, 500 µm center-to-center distance). The tumor growth ratio was compared and acute cell death was studied histologically. With cross-planar irradiation, tumor growth was significantly suppressed between days 4 and 28 after 20 µm microbeam irradiation, whereas tumor growth was suppressed, and not significantly so, only between days 4 and 18 after 100 µm microbeam irradiation. Immunohistochemistry using TUNEL staining showed no increase in TUNEL-positive cells with either microbeam at 24 and 72 h post-irradiation. The 20 µm microbeam was found to be more tumoricidal than the 100 µm microbeam, and the effect was not related to apoptotic cell death. The underlying mechanism may be functional tissue deterioration rather than direct cellular damage in the beam path.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A narrow microbeam is more effective for tumor growth suppression than a wide microbeam: an in vivo study using implanted human glioma cells</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>671</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>678</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?bf5035">
    <title>Achromatic nested Kirkpatrick–Baez mirror optics for hard X-ray nanofocusing</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?bf5035</link>
    <description>The first test of nanoscale-focusing Kirkpatrick–Baez (KB) mirrors in the nested (or Montel) configuration used at a hard X-ray synchrotron beamline is reported. The two mirrors are both 40 mm long and coated with Pt to produce a focal length of 60 mm at 3 mrad incident angle, and collect up to a 120 µm by 120 µm incident X-ray beam with maximum angular acceptance of 2 mrad and a broad bandwidth of energies up to 30 keV. In an initial test a focal spot of about 150 nm in both horizontal and vertical directions was achieved with either polychromatic or monochromatic beam. The nested mirror geometry, with two mirrors mounted side-by-side and perpendicular to each other, is significantly more compact and provides higher demagnification than the traditional sequential KB mirror arrangement. Ultimately, nested mirrors can focus larger divergence to improve the diffraction limit of achromatic optics. A major challenge with the fabrication of the required mirrors is the need for near-perfect mirror surfaces near the edge of at least one of the mirrors. Special polishing procedures and surface profile coating were used to preserve the mirror surface quality at the reflecting edge. Further developments aimed at achieving diffraction-limited focusing below 50 nm are underway.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Liu, W.</dc:creator>
    <dc:creator>Ice, G.E.</dc:creator>
    <dc:creator>Assoufid, L.</dc:creator>
    <dc:creator>Liu, C.</dc:creator>
    <dc:creator>Shi, B.</dc:creator>
    <dc:creator>Khachatryan, R.</dc:creator>
    <dc:creator>Qian, J.</dc:creator>
    <dc:creator>Zschack, P.</dc:creator>
    <dc:creator>Tischler, J.Z.</dc:creator>
    <dc:creator>Choi, J.-Y.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511010995</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A nested Kirkpatrick–Baez mirror pair has been designed, fabricated and tested for achromatic nanofocusing synchrotron hard X-rays. The prototype system achieved a FWHM focal spot of about 150 nm in both horizontal and vertical directions.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HARD X-RAY NANOFOCUSING; ACHROMATIC; NESTED KIRKPATRICK-BAEZ; MONTEL</dc:subject>
    <dc:description>The first test of nanoscale-focusing Kirkpatrick–Baez (KB) mirrors in the nested (or Montel) configuration used at a hard X-ray synchrotron beamline is reported. The two mirrors are both 40 mm long and coated with Pt to produce a focal length of 60 mm at 3 mrad incident angle, and collect up to a 120 µm by 120 µm incident X-ray beam with maximum angular acceptance of 2 mrad and a broad bandwidth of energies up to 30 keV. In an initial test a focal spot of about 150 nm in both horizontal and vertical directions was achieved with either polychromatic or monochromatic beam. The nested mirror geometry, with two mirrors mounted side-by-side and perpendicular to each other, is significantly more compact and provides higher demagnification than the traditional sequential KB mirror arrangement. Ultimately, nested mirrors can focus larger divergence to improve the diffraction limit of achromatic optics. A major challenge with the fabrication of the required mirrors is the need for near-perfect mirror surfaces near the edge of at least one of the mirrors. Special polishing procedures and surface profile coating were used to preserve the mirror surface quality at the reflecting edge. Further developments aimed at achieving diffraction-limited focusing below 50 nm are underway.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Achromatic nested Kirkpatrick–Baez mirror optics for hard X-ray nanofocusing</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>575</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>579</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ve5004">
    <title>Measurement of persistence in YAG:Ce3+ scintillator with pulsed synchrotron X-rays</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ve5004</link>
    <description>The decay time of YAG:Ce3+ phosphor was studied using a CMOS camera with a frame rate of 1302000 s−1 and pulsed X-rays from SPring-8. A high-resolution X-ray detector with YAG:Ce3+ was used with the camera to view the focused beam from the helical undulator. Mismatch between the ring circulation time and the frame time gave rise to a periodic variation of beam intensity in successive frames. Analysis of data obtained with two bunch modes showed that the decay time of YAG:Ce3+ was 60 ns. The variation of the beam positions in isolated bunches was small enough to be neglected in experiments using the focused beam. The results also show the possibility of an X-ray diffraction study at high time and space resolution.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Matsuo, T.</dc:creator>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511010843</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The decay time of YAG:Ce3+ scintillator was estimated to be 60 ns by using a fast CMOS camera and synchrotron bunches.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HIGH-SPEED CAMERA; SCINTILLATOR; SYNCHROTRON BUNCHES</dc:subject>
    <dc:description>The decay time of YAG:Ce3+ phosphor was studied using a CMOS camera with a frame rate of 1302000 s−1 and pulsed X-rays from SPring-8. A high-resolution X-ray detector with YAG:Ce3+ was used with the camera to view the focused beam from the helical undulator. Mismatch between the ring circulation time and the frame time gave rise to a periodic variation of beam intensity in successive frames. Analysis of data obtained with two bunch modes showed that the decay time of YAG:Ce3+ was 60 ns. The variation of the beam positions in isolated bunches was small enough to be neglected in experiments using the focused beam. The results also show the possibility of an X-ray diffraction study at high time and space resolution.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Measurement of persistence in YAG:Ce3+ scintillator with pulsed synchrotron X-rays</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>601</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>604</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi5615">
    <title>Hard X-ray Fourier transform holography from an array of oriented referenced objects</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi5615</link>
    <description>Hard X-ray Fourier transform holography (HXFTH) is a promising method for imaging nanoscale objects, including biological molecules, with a spatial resolution of a nanometer or better. However, it suffers from low scattering intensities being available for imaging owing to smaller object size and the low scattering cross section inherent in hard X-rays. One technique to overcome the problem would be to use an array of oriented objects, each with its own reference. Here the feasibility of this approach was experimentally tested by recording diffraction patterns from nanofabricated test patterns arranged in a 5 × 5 matrix. At an X-ray energy of 8 keV (λ = 1.55 Å), the image of the original test pattern was clearly restored with 60 s exposure on an imaging plate; the image was still recognizable with a 500 ms exposure on a CCD detector at the BL40XU beamline at SPring-8. The results demonstrate that the use of an array of referenced oriented objects for HXFTH is workable, and that it can be considered as a practical candidate for imaging biological molecules, identical particles of which are available but diffract even more weakly than artificially fabricated test patterns.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Iwamoto, H.</dc:creator>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:date>2011-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511009836</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The use of multiple, oriented and singly referenced objects was evaluated as a means to overcome the low scattering cross section inherent in hard X-ray Fourier transform holography. It is shown that the image of each object can be restored as in the conventional single-object case.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FOURIER TRANSFORM HOLOGRAPHY; HARD X-RAYS; X-RAY BANDWIDTH; X-RAY MICROBEAM</dc:subject>
    <dc:description>Hard X-ray Fourier transform holography (HXFTH) is a promising method for imaging nanoscale objects, including biological molecules, with a spatial resolution of a nanometer or better. However, it suffers from low scattering intensities being available for imaging owing to smaller object size and the low scattering cross section inherent in hard X-rays. One technique to overcome the problem would be to use an array of oriented objects, each with its own reference. Here the feasibility of this approach was experimentally tested by recording diffraction patterns from nanofabricated test patterns arranged in a 5 × 5 matrix. At an X-ray energy of 8 keV (λ = 1.55 Å), the image of the original test pattern was clearly restored with 60 s exposure on an imaging plate; the image was still recognizable with a 500 ms exposure on a CCD detector at the BL40XU beamline at SPring-8. The results demonstrate that the use of an array of referenced oriented objects for HXFTH is workable, and that it can be considered as a practical candidate for imaging biological molecules, identical particles of which are available but diffract even more weakly than artificially fabricated test patterns.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Hard X-ray Fourier transform holography from an array of oriented referenced objects</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-07-01</prism:publicationDate>
    <prism:startingPage>564</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>568</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5025">
    <title>Radiation damage in room-temperature data acquisition with the PILATUS 6M pixel detector</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5025</link>
    <description>The first study of room-temperature macromolecular crystallography data acquisition with a silicon pixel detector is presented, where the data are collected in continuous sample rotation mode, with millisecond read-out time and no read-out noise. Several successive datasets were collected sequentially from single test crystals of thaumatin and insulin. The dose rate ranged between ∼1320 Gy s−1 and ∼8420 Gy s−1 with corresponding frame rates between 1.565 Hz and 12.5 Hz. The data were analysed for global radiation damage. A previously unreported negative dose-rate effect is observed in the indicators of global radiation damage, which showed an approximately 75% decrease in D1/2 at sixfold higher dose rate. The integrated intensity decreases in an exponential manner. Sample heating that could give rise to the enhanced radiation sensitivity at higher dose rate is investigated by collecting data between crystal temperatures of 298 K and 353 K. UV-Vis spectroscopy is used to demonstrate that disulfide radicals and trapped electrons do not accumulate at high dose rates in continuous data collection.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Rajendran, C.</dc:creator>
    <dc:creator>Dworkowski, F.S.N.</dc:creator>
    <dc:creator>Wang, M.</dc:creator>
    <dc:creator>Schulze-Briese, C.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951100968X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Observations of the dose-rate effect in continuous X-ray diffraction data acquisition at room temperature are presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ROOM-TEMPERATURE DATA COLLECTION; PILATUS 6M; DOSE RATE; RADIATION DAMAGE</dc:subject>
    <dc:description>The first study of room-temperature macromolecular crystallography data acquisition with a silicon pixel detector is presented, where the data are collected in continuous sample rotation mode, with millisecond read-out time and no read-out noise. Several successive datasets were collected sequentially from single test crystals of thaumatin and insulin. The dose rate ranged between ∼1320 Gy s−1 and ∼8420 Gy s−1 with corresponding frame rates between 1.565 Hz and 12.5 Hz. The data were analysed for global radiation damage. A previously unreported negative dose-rate effect is observed in the indicators of global radiation damage, which showed an approximately 75% decrease in D1/2 at sixfold higher dose rate. The integrated intensity decreases in an exponential manner. Sample heating that could give rise to the enhanced radiation sensitivity at higher dose rate is investigated by collecting data between crystal temperatures of 298 K and 353 K. UV-Vis spectroscopy is used to demonstrate that disulfide radicals and trapped electrons do not accumulate at high dose rates in continuous data collection.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Radiation damage in room-temperature data acquisition with the PILATUS 6M pixel detector</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>318</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>328</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5022">
    <title>Radiation damage in single-particle cryo-electron microscopy: effects of dose and dose rate</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5022</link>
    <description>Radiation damage is an important resolution limiting factor both in macromolecular X-ray crystallography and cryo-electron microscopy. Systematic studies in macromolecular X-ray crystallography greatly benefited from the use of dose, expressed as energy deposited per mass unit, which is derived from parameters including incident flux, beam energy, beam size, sample composition and sample size. In here, the use of dose is reintroduced for electron microscopy, accounting for the electron energy, incident flux and measured sample thickness and composition. Knowledge of the amount of energy deposited allowed us to compare doses with experimental limits in macromolecular X-ray crystallography, to obtain an upper estimate of radical concentrations that build up in the vitreous sample, and to translate heat-transfer simulations carried out for macromolecular X-ray crystallography to cryo-electron microscopy. Stroboscopic exposure series of 50–250 images were collected for different incident flux densities and integration times from Lumbricus terrestris extracellular hemoglobin. The images within each series were computationally aligned and analyzed with similarity metrics such as Fourier ring correlation, Fourier ring phase residual and figure of merit. Prior to gas bubble formation, the images become linearly brighter with dose, at a rate of approximately 0.1% per 10 MGy. The gradual decomposition of a vitrified hemoglobin sample could be visualized at a series of doses up to 5500 MGy, by which dose the sample was sublimed. Comparison of equal-dose series collected with different incident flux densities showed a dose-rate effect favoring lower flux densities. Heat simulations predict that sample heating will only become an issue for very large dose rates (50 e−Å−2 s−1 or higher) combined with poor thermal contact between the grid and cryo-holder. Secondary radiolytic effects are likely to play a role in dose-rate effects. Stroboscopic data collection combined with an improved understanding of the effects of dose and dose rate will aid single-particle cryo-electron microscopists to have better control of the outcome of their experiments.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Karuppasamy, M.</dc:creator>
    <dc:creator>Karimi Nejadasl, F.</dc:creator>
    <dc:creator>Vulovic, M.</dc:creator>
    <dc:creator>Koster, A.J.</dc:creator>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951100820X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The effects of dose and dose-rate were investigated for single-particle cryo-electron microscopy using stroboscopic data collection. A dose-rate effect was observed favoring lower flux densities.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SINGLE-PARTICLE CRYO-ELECTRON MICROSCOPY; RADIATION DAMAGE; DOSE; DOSE-RATE EFFECT; MACROMOLECULAR X-RAY CRYSTALLOGRAPHY</dc:subject>
    <dc:description>Radiation damage is an important resolution limiting factor both in macromolecular X-ray crystallography and cryo-electron microscopy. Systematic studies in macromolecular X-ray crystallography greatly benefited from the use of dose, expressed as energy deposited per mass unit, which is derived from parameters including incident flux, beam energy, beam size, sample composition and sample size. In here, the use of dose is reintroduced for electron microscopy, accounting for the electron energy, incident flux and measured sample thickness and composition. Knowledge of the amount of energy deposited allowed us to compare doses with experimental limits in macromolecular X-ray crystallography, to obtain an upper estimate of radical concentrations that build up in the vitreous sample, and to translate heat-transfer simulations carried out for macromolecular X-ray crystallography to cryo-electron microscopy. Stroboscopic exposure series of 50–250 images were collected for different incident flux densities and integration times from Lumbricus terrestris extracellular hemoglobin. The images within each series were computationally aligned and analyzed with similarity metrics such as Fourier ring correlation, Fourier ring phase residual and figure of merit. Prior to gas bubble formation, the images become linearly brighter with dose, at a rate of approximately 0.1% per 10 MGy. The gradual decomposition of a vitrified hemoglobin sample could be visualized at a series of doses up to 5500 MGy, by which dose the sample was sublimed. Comparison of equal-dose series collected with different incident flux densities showed a dose-rate effect favoring lower flux densities. Heat simulations predict that sample heating will only become an issue for very large dose rates (50 e−Å−2 s−1 or higher) combined with poor thermal contact between the grid and cryo-holder. Secondary radiolytic effects are likely to play a role in dose-rate effects. Stroboscopic data collection combined with an improved understanding of the effects of dose and dose rate will aid single-particle cryo-electron microscopists to have better control of the outcome of their experiments.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Radiation damage in single-particle cryo-electron microscopy: effects of dose and dose rate</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>398</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>412</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5026">
    <title>Assessment of radiation damage behaviour in a large collection of empirically optimized datasets highlights the importance of unmeasured complicating effects</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5026</link>
    <description>The radiation damage behaviour in 43 datasets of 34 different proteins collected over a year was examined, in order to gauge the reliability of decay metrics in practical situations, and to assess how these datasets, optimized only empirically for decay, would have benefited from the precise and automatic prediction of decay now possible with the programs RADDOSE [Murray, Garman &amp; Ravelli (2004). J. Appl. Cryst. 37, 513–522] and BEST [Bourenkov &amp; Popov (2010). Acta Cryst. D66, 409–419]. The results indicate that in routine practice the diffraction experiment is not yet characterized well enough to support such precise predictions, as these depend fundamentally on three interrelated variables which cannot yet be determined robustly and practically: the flux density distribution of the beam; the exact crystal volume; the sensitivity of the crystal to dose. The former two are not satisfactorily approximated from typical beamline information such as nominal beam size and transmission, or two-dimensional images of the beam and crystal; the discrepancies are particularly marked when using microfocus beams (&lt;20 µm). Empirically monitoring decay with the dataset scaling B factor (Bourenkov &amp; Popov, 2010) appears more robust but is complicated by anisotropic and/or low-resolution diffraction. These observations serve to delineate the challenges, scientific and logistic, that remain to be addressed if tools for managing radiation damage in practical data collection are to be conveniently robust enough to be useful in real time.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Krojer, T.</dc:creator>
    <dc:creator>von Delft, F.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511008235</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A retrospective analysis of radiation damage behaviour in a statistically significant number of real-life datasets is presented, in order to gauge the importance of the complications not yet measured or rigorously evaluated in current experiments, and the challenges that remain before radiation damage can be considered a problem solved in practice.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; DATA COLLECTION; STRATEGY; BEAMLINE SOFTWARE; DATASETS</dc:subject>
    <dc:description>The radiation damage behaviour in 43 datasets of 34 different proteins collected over a year was examined, in order to gauge the reliability of decay metrics in practical situations, and to assess how these datasets, optimized only empirically for decay, would have benefited from the precise and automatic prediction of decay now possible with the programs RADDOSE [Murray, Garman &amp; Ravelli (2004). J. Appl. Cryst. 37, 513–522] and BEST [Bourenkov &amp; Popov (2010). Acta Cryst. D66, 409–419]. The results indicate that in routine practice the diffraction experiment is not yet characterized well enough to support such precise predictions, as these depend fundamentally on three interrelated variables which cannot yet be determined robustly and practically: the flux density distribution of the beam; the exact crystal volume; the sensitivity of the crystal to dose. The former two are not satisfactorily approximated from typical beamline information such as nominal beam size and transmission, or two-dimensional images of the beam and crystal; the discrepancies are particularly marked when using microfocus beams (&lt;20 µm). Empirically monitoring decay with the dataset scaling B factor (Bourenkov &amp; Popov, 2010) appears more robust but is complicated by anisotropic and/or low-resolution diffraction. These observations serve to delineate the challenges, scientific and logistic, that remain to be addressed if tools for managing radiation damage in practical data collection are to be conveniently robust enough to be useful in real time.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Assessment of radiation damage behaviour in a large collection of empirically optimized datasets highlights the importance of unmeasured complicating effects</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>387</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>397</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5024">
    <title>Correlated single-crystal electronic absorption spectroscopy and X-ray crystallography at NSLS beamline X26-C</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5024</link>
    <description>The research philosophy and new capabilities installed at NSLS beamline X26-C to support electronic absorption and Raman spectroscopies coupled with X-ray diffraction are reviewed. This beamline is dedicated full time to multidisciplinary studies with goals that include revealing the relationship between the electronic and atomic structures in macromolecules. The beamline instrumentation has been fully integrated such that optical absorption spectra and X-ray diffraction images are interlaced. Therefore, optical changes induced by X-ray exposure can be correlated with X-ray diffraction data collection. The installation of Raman spectroscopy into the beamline is also briefly reviewed. Data are now routinely generated almost simultaneously from three complementary types of experiments from the same sample. The beamline is available now to the NSLS general user population.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Orville, A.M.</dc:creator>
    <dc:creator>Buono, R.</dc:creator>
    <dc:creator>Cowan, M.</dc:creator>
    <dc:creator>Héroux, A.</dc:creator>
    <dc:creator>Shea-McCarthy, G.</dc:creator>
    <dc:creator>Schneider, D.K.</dc:creator>
    <dc:creator>Skinner, J.M.</dc:creator>
    <dc:creator>Skinner, M.J.</dc:creator>
    <dc:creator>Stoner-Ma, D.</dc:creator>
    <dc:creator>Sweet, R.M.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511006315</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The instrumentation and methods available for collecting almost simultaneous single-crystal electronic absorption correlated with X-ray diffraction data at NSLS beamline X26-C are reviewed, as well as a very brief outline of its Raman spectroscopy capability.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>METALLOENZYMES; COFACTORS; ELECTRONIC ABSORPTION SPECTROSCOPY; RAMAN SPECTROSCOPY</dc:subject>
    <dc:description>The research philosophy and new capabilities installed at NSLS beamline X26-C to support electronic absorption and Raman spectroscopies coupled with X-ray diffraction are reviewed. This beamline is dedicated full time to multidisciplinary studies with goals that include revealing the relationship between the electronic and atomic structures in macromolecules. The beamline instrumentation has been fully integrated such that optical absorption spectra and X-ray diffraction images are interlaced. Therefore, optical changes induced by X-ray exposure can be correlated with X-ray diffraction data collection. The installation of Raman spectroscopy into the beamline is also briefly reviewed. Data are now routinely generated almost simultaneously from three complementary types of experiments from the same sample. The beamline is available now to the NSLS general user population.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Correlated single-crystal electronic absorption spectroscopy and X-ray crystallography at NSLS beamline X26-C</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>358</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>366</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0444">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0444</link>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511005188</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>308</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>310</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?bf5034">
    <title>Development of a hard X-ray delay line for X-ray photon correlation spectroscopy and jitter-free pump–probe experiments at X-ray free-electron laser sources</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?bf5034</link>
    <description>A hard X-ray delay line capable of splitting and delaying single X-ray pulses has been developed with the aim of performing X-ray photon correlation spectroscopy (XPCS) and X-ray pump–probe experiments at hard X-ray free-electron laser sources. The performance of the device was tested with 8.39 keV synchrotron radiation. Time delays up to 2.95 ns have been demonstrated. The feasibility of the device for performing XPCS studies was tested by recording static speckle patterns. The achieved speckle contrast of 56% indicates the possibility of performing ultra-fast XPCS studies with the delay line.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Roseker, W.</dc:creator>
    <dc:creator>Franz, H.</dc:creator>
    <dc:creator>Schulte-Schrepping, H.</dc:creator>
    <dc:creator>Ehnes, A.</dc:creator>
    <dc:creator>Leupold, O.</dc:creator>
    <dc:creator>Zontone, F.</dc:creator>
    <dc:creator>Lee, S.</dc:creator>
    <dc:creator>Robert, A.</dc:creator>
    <dc:creator>Grübel, G.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511004511</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A prototype device capable of splitting an X-ray pulse into two adjustable fractions, delaying one of them with the aim of performing split pulse X-ray photon correlation spectroscopy and pump–probe type studies was designed and manufactured. Time delays up to 2.95 ns have been demonstrated. The achieved contrast values of 56% indicate a feasibility of performing coherence-based experiments with the delay line.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DELAY LINE; XPCS; PUMP-PROBE; X-RAY OPTICS</dc:subject>
    <dc:description>A hard X-ray delay line capable of splitting and delaying single X-ray pulses has been developed with the aim of performing X-ray photon correlation spectroscopy (XPCS) and X-ray pump–probe experiments at hard X-ray free-electron laser sources. The performance of the device was tested with 8.39 keV synchrotron radiation. Time delays up to 2.95 ns have been demonstrated. The feasibility of the device for performing XPCS studies was tested by recording static speckle patterns. The achieved speckle contrast of 56% indicates the possibility of performing ultra-fast XPCS studies with the delay line.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Development of a hard X-ray delay line for X-ray photon correlation spectroscopy and jitter-free pump–probe experiments at X-ray free-electron laser sources</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>481</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>491</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5019">
    <title>Revealing low-dose radiation damage using single-crystal spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5019</link>
    <description>The structural information and functional insight obtained from X-ray crystallography can be enhanced by the use of complementary spectroscopies. Here the information that can be obtained from spectroscopic methods commonly used in conjunction with X-ray crystallography and best-practice single-crystal UV-Vis absorption data collection are briefly reviewed. Using data collected with the in situ system at the Swiss Light Source, the time and dose scales of low-dose X-ray-induced radiation damage and solvated electron generation in metalloproteins at 100 K are investigated. The effect of dose rate on these scales is also discussed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Owen, R.L.</dc:creator>
    <dc:creator>Yorke, B.A.</dc:creator>
    <dc:creator>Gowdy, J.A.</dc:creator>
    <dc:creator>Pearson, A.R.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511004250</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Data on the rapid reduction of haem proteins in the X-ray beam at synchrotron sources are presented. The use of single-crystal spectroscopy to detect these changes and their implication for diffraction data collection from oxidized species is also discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; SINGLE-CRYSTAL MICROSPECTROPHOTOMETRY; RADIATION DAMAGE; MYOGLOBIN; CYTOCHROME C</dc:subject>
    <dc:description>The structural information and functional insight obtained from X-ray crystallography can be enhanced by the use of complementary spectroscopies. Here the information that can be obtained from spectroscopic methods commonly used in conjunction with X-ray crystallography and best-practice single-crystal UV-Vis absorption data collection are briefly reviewed. Using data collected with the in situ system at the Swiss Light Source, the time and dose scales of low-dose X-ray-induced radiation damage and solvated electron generation in metalloproteins at 100 K are investigated. The effect of dose rate on these scales is also discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Revealing low-dose radiation damage using single-crystal spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>367</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>373</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5018">
    <title>Additional phase information from UV damage of selenomethionine labelled proteins</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5018</link>
    <description>Currently, selenium is the most widely used phasing vehicle for experimental phasing, either by single anomalous scattering or multiple-wavelength anomalous dispersion (MAD) procedures. The use of the single isomorphous replacement anomalous scattering (SIRAS) phasing procedure with selenomethionine containing proteins is not so commonly used, as it requires isomorphous native data. Here it is demonstrated that isomorphous differences can be measured from intensity changes measured from a selenium labelled protein crystal before and after UV exposure. These can be coupled with the anomalous signal from the dataset collected at the selenium absorption edge to obtain SIRAS phases in a UV-RIPAS phasing experiment. The phasing procedure for two selenomethionine proteins, the feruloyl esterase module of xylanase 10B from Clostridium thermocellum and the Mycobacterium tuberculosis chorismate synthase, have been investigated using datasets collected near the absorption edge of selenium before and after UV radiation. The utility of UV radiation in measuring radiation damage data for isomorphous differences is highlighted and it is shown that, after such measurements, the UV-RIPAS procedure yields comparable phase sets with those obtained from the conventional MAD procedure. The results presented are encouraging for the development of alternative phasing approaches for selenomethionine proteins in difficult cases.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sanctis, D. de</dc:creator>
    <dc:creator>Tucker, P.A.</dc:creator>
    <dc:creator>Panjikar, S.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511004092</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Successful examples of ultraviolet radiation-damage-induced phasing with anomalous scattering from selenomethionine protein crystals have been demonstrated.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>UV-RIPAS; SEMET; EXPERIMENTAL PHASING; RADIATION DAMAGE</dc:subject>
    <dc:description>Currently, selenium is the most widely used phasing vehicle for experimental phasing, either by single anomalous scattering or multiple-wavelength anomalous dispersion (MAD) procedures. The use of the single isomorphous replacement anomalous scattering (SIRAS) phasing procedure with selenomethionine containing proteins is not so commonly used, as it requires isomorphous native data. Here it is demonstrated that isomorphous differences can be measured from intensity changes measured from a selenium labelled protein crystal before and after UV exposure. These can be coupled with the anomalous signal from the dataset collected at the selenium absorption edge to obtain SIRAS phases in a UV-RIPAS phasing experiment. The phasing procedure for two selenomethionine proteins, the feruloyl esterase module of xylanase 10B from Clostridium thermocellum and the Mycobacterium tuberculosis chorismate synthase, have been investigated using datasets collected near the absorption edge of selenium before and after UV radiation. The utility of UV radiation in measuring radiation damage data for isomorphous differences is highlighted and it is shown that, after such measurements, the UV-RIPAS procedure yields comparable phase sets with those obtained from the conventional MAD procedure. The results presented are encouraging for the development of alternative phasing approaches for selenomethionine proteins in difficult cases.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Additional phase information from UV damage of selenomethionine labelled proteins</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>374</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>380</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?vv5013">
    <title>Three-dimensional diffraction mapping by tuning the X-ray energy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?vv5013</link>
    <description>Three-dimensional reciprocal-space maps of a single SiGe island around the Si(004) Bragg peak are recorded using an energy-tuning technique with a microfocused X-ray beam with compound refractive lenses as focusing optics. The map is in agreement with simulated data as well as with a map recorded by an ordinary rocking-curve scan. The energy-tuning approach circumvents both the comparatively large sphere of confusion of diffractometers compared with nanostructures and vibrations induced by motors. Thus, this method offers new possibilities for novel combinations of three-dimensional micro- and nano-focused X-ray diffraction with complex in situ sample environments such as scanning probe microscopes.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Cornelius, T.W.</dc:creator>
    <dc:creator>Carbone, D.</dc:creator>
    <dc:creator>Jacques, V.L.R.</dc:creator>
    <dc:creator>Schülli, T.U.</dc:creator>
    <dc:creator>Metzger, T.H.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511003190</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Three-dimensional reciprocal-space maps of a single SiGe island around the Si(004) Bragg peak are recorded using an energy-tuning technique with a microfocused X-ray beam with compound refractive lenses as focusing optics.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY DIFFRACTION; NANOFOCUSED AND MICROFOCUSED XRD; ENERGY SCAN; THREE-DIMENSIONAL RECIPROCAL-SPACE MAPPING</dc:subject>
    <dc:description>Three-dimensional reciprocal-space maps of a single SiGe island around the Si(004) Bragg peak are recorded using an energy-tuning technique with a microfocused X-ray beam with compound refractive lenses as focusing optics. The map is in agreement with simulated data as well as with a map recorded by an ordinary rocking-curve scan. The energy-tuning approach circumvents both the comparatively large sphere of confusion of diffractometers compared with nanostructures and vibrations induced by motors. Thus, this method offers new possibilities for novel combinations of three-dimensional micro- and nano-focused X-ray diffraction with complex in situ sample environments such as scanning probe microscopes.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Three-dimensional diffraction mapping by tuning the X-ray energy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>413</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>417</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5088">
    <title>Fast X-ray microdiffraction techniques for studying irreversible transformations in materials</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5088</link>
    <description>A pair of techniques have been developed for performing time-resolved X-ray microdiffraction on irreversible phase transformations. In one technique capillary optics are used to focus a high-flux broad-spectrum X-ray beam to a 60 µm spot size and a fast pixel array detector is used to achieve temporal resolution of 55 µs. In the second technique the X-rays are focused with Kirkpatrick–Baez mirrors to achieve a spatial resolution better than 10 µm and a fast shutter is used to provide temporal resolution better than 20 µs while recording the diffraction pattern on a (relatively slow) X-ray CCD camera. Example data from experiments are presented where these techniques are used to study self-propagating high-temperature synthesis reactions in metal laminate foils.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Kelly, S.T.</dc:creator>
    <dc:creator>Trenkle, J.C.</dc:creator>
    <dc:creator>Koerner, L.J.</dc:creator>
    <dc:creator>Barron, S.C.</dc:creator>
    <dc:creator>Walker, N.</dc:creator>
    <dc:creator>Pouliquen, P.O.</dc:creator>
    <dc:creator>Tate, M.W.</dc:creator>
    <dc:creator>Gruner, S.M.</dc:creator>
    <dc:creator>Dufresne, E.M.</dc:creator>
    <dc:creator>Weihs, T.P.</dc:creator>
    <dc:creator>Hufnagel, T.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511002640</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Techniques are described for X-ray diffraction combining micrometer-scale spatial resolution with microsecond-scale temporal resolution for studying rapid localized irreversible transformations in materials.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY DIFFRACTION; PHASE TRANSFORMATIONS</dc:subject>
    <dc:description>A pair of techniques have been developed for performing time-resolved X-ray microdiffraction on irreversible phase transformations. In one technique capillary optics are used to focus a high-flux broad-spectrum X-ray beam to a 60 µm spot size and a fast pixel array detector is used to achieve temporal resolution of 55 µs. In the second technique the X-rays are focused with Kirkpatrick–Baez mirrors to achieve a spatial resolution better than 10 µm and a fast shutter is used to provide temporal resolution better than 20 µs while recording the diffraction pattern on a (relatively slow) X-ray CCD camera. Example data from experiments are presented where these techniques are used to study self-propagating high-temperature synthesis reactions in metal laminate foils.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Fast X-ray microdiffraction techniques for studying irreversible transformations in materials</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>464</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>474</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ve5005">
    <title>High-efficiency Fresnel zone plates for hard X-rays by 100 keV e-beam lithography and electroplating</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ve5005</link>
    <description>The fabrication and characterization of Fresnel zone plates (FZPs) for hard X-ray microscopy applications are reported. High-quality 500 nm- and 1 µm-thick Au FZPs with outermost zone widths down to 50 nm and 70 nm, respectively, and with diameters up to 600 µm were fabricated. The diffraction efficiencies of the fabricated FZPs were measured for a wide range of X-ray energies (2.8–13.2 keV) showing excellent values up to 65–75% of the theoretical values, reflecting the good quality of the FZPs. Spatially resolved diffraction efficiency measurements indicate the uniformity of the FZPs and a defect-free structure.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Gorelick, S.</dc:creator>
    <dc:creator>Vila-Comamala, J.</dc:creator>
    <dc:creator>Guzenko, V.A.</dc:creator>
    <dc:creator>Barrett, R.</dc:creator>
    <dc:creator>Salomé, M.</dc:creator>
    <dc:creator>David, C.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511002366</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The efficiencies of several Fresnel zone plates, that were fabricated using a direct-write method with high-energy electrons, were measured over a wide range of photon energies.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FRESNEL ZONE PLATE; HARD X-RAYS; X-RAY OPTICS; ELECTRON-BEAM LITHOGRAPHY; AU ELECTROPLATING; PMMA</dc:subject>
    <dc:description>The fabrication and characterization of Fresnel zone plates (FZPs) for hard X-ray microscopy applications are reported. High-quality 500 nm- and 1 µm-thick Au FZPs with outermost zone widths down to 50 nm and 70 nm, respectively, and with diameters up to 600 µm were fabricated. The diffraction efficiencies of the fabricated FZPs were measured for a wide range of X-ray energies (2.8–13.2 keV) showing excellent values up to 65–75% of the theoretical values, reflecting the good quality of the FZPs. Spatially resolved diffraction efficiency measurements indicate the uniformity of the FZPs and a defect-free structure.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>High-efficiency Fresnel zone plates for hard X-rays by 100 keV e-beam lithography and electroplating</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>442</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>446</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5020">
    <title>Experimental procedure for the characterization of radiation damage in macromolecular crystals</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5020</link>
    <description>A reliable and reproducible method to automatically characterize the radiation sensitivity of macromolecular crystals at the ESRF beamlines has been developed. This new approach uses the slope of the linear dependence of the overall isotropic B-factor with absorbed dose as the damage metric. The method has been implemented through an automated procedure using the EDNA on-line data analysis framework and the MxCuBE data collection control interface. The outcome of the procedure can be directly used to design an optimal data collection strategy. The results of tests carried out on a number of model and real-life crystal systems are presented.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Leal, R.M.F.</dc:creator>
    <dc:creator>Bourenkov, G.P.</dc:creator>
    <dc:creator>Svensson, O.</dc:creator>
    <dc:creator>Spruce, D.</dc:creator>
    <dc:creator>Guijarro, M.</dc:creator>
    <dc:creator>Popov, A.N.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511002251</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A novel automatic procedure to determine the sensitivity of macromolecular crystals to radiation damage is presented. The information extracted from this procedure can be directly used for optimal planning of data collection or/and beamline calibration.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>BEST; EDNA; RADIATION DAMAGE</dc:subject>
    <dc:description>A reliable and reproducible method to automatically characterize the radiation sensitivity of macromolecular crystals at the ESRF beamlines has been developed. This new approach uses the slope of the linear dependence of the overall isotropic B-factor with absorbed dose as the damage metric. The method has been implemented through an automated procedure using the EDNA on-line data analysis framework and the MxCuBE data collection control interface. The outcome of the procedure can be directly used to design an optimal data collection strategy. The results of tests carried out on a number of model and real-life crystal systems are presented.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Experimental procedure for the characterization of radiation damage in macromolecular crystals</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>381</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>386</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?co5010">
    <title>New developments in fabrication of high-energy-resolution analyzers for inelastic X-ray spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?co5010</link>
    <description>In this work new improvements related to the fabrication of spherical bent analyzers for 1 meV energy-resolution inelastic X-ray scattering spectroscopy are presented. The new method includes the use of a two-dimensional bender to achieve the required radius of curvature for X-ray analyzers. The advantage of this method is the ability to monitor the focus during bending, which leads to higher-efficiency analyzers.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Said, A.H.</dc:creator>
    <dc:creator>Sinn, H.</dc:creator>
    <dc:creator>Divan, R.</dc:creator>
    <dc:date>2011-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049511001828</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>New improvements related to the fabrication of spherical bent analyzers for 1 meV energy-resolution inelastic X-ray scattering spectroscopy are presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HIGH-ENERGY-RESOLUTION ANALYZERS; INELASTIC X-RAY SCATTERING SPECTROSCOPY</dc:subject>
    <dc:description>In this work new improvements related to the fabrication of spherical bent analyzers for 1 meV energy-resolution inelastic X-ray scattering spectroscopy are presented. The new method includes the use of a two-dimensional bender to achieve the required radius of curvature for X-ray analyzers. The advantage of this method is the ability to monitor the focus during bending, which leads to higher-efficiency analyzers.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>New developments in fabrication of high-energy-resolution analyzers for inelastic X-ray spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-05-01</prism:publicationDate>
    <prism:startingPage>492</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>496</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5634">
    <title>Multi-frame acquisition scheme for efficient energy-dispersive X-ray magnetic circular dichroism in pulsed high magnetic fields at the Fe K-edge</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5634</link>
    <description>Using a fast silicon strip detector, a multi-frame acquisition scheme was implemented to perform energy-dispersive X-ray magnetic circular dichroism at the iron K-edge in pulsed high magnetic fields. The acquisition scheme makes use of the entire field pulse. The quality of the signal obtained from samples of ferrimagnetic erbium iron garnet allows for quantitative evaluation of the signal amplitude. Below the compensation point, two successive field-induced phase transitions and the reversal of the net magnetization of the iron sublattices in the intermediate phase were observed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Strohm, C.</dc:creator>
    <dc:creator>Perrin, F.</dc:creator>
    <dc:creator>Dominguez, M.-C.</dc:creator>
    <dc:creator>Headspith, J.</dc:creator>
    <dc:creator>Linden, P. van der</dc:creator>
    <dc:creator>Mathon, O.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951100080X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A multi-frame acquisition scheme for efficient energy-dispersive X-ray magnetic circular dichroism at the Fe K-edge is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ENERGY-DISPERSIVE XMCD; HIGH MAGNETIC FIELD; DETECTION</dc:subject>
    <dc:description>Using a fast silicon strip detector, a multi-frame acquisition scheme was implemented to perform energy-dispersive X-ray magnetic circular dichroism at the iron K-edge in pulsed high magnetic fields. The acquisition scheme makes use of the entire field pulse. The quality of the signal obtained from samples of ferrimagnetic erbium iron garnet allows for quantitative evaluation of the signal amplitude. Below the compensation point, two successive field-induced phase transitions and the reversal of the net magnetization of the iron sublattices in the intermediate phase were observed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Multi-frame acquisition scheme for efficient energy-dispersive X-ray magnetic circular dichroism in pulsed high magnetic fields at the Fe K-edge</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>224</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>228</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ve5006">
    <title>Numerical optimization of spherical variable-line-spacing grating X-ray spectrometers</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ve5006</link>
    <description>Operation of an X-ray spectrometer based on a spherical variable-line-spacing (VLS) grating is analyzed using dedicated ray-tracing software allowing fast optimization of the grating parameters and spectrometer geometry. The analysis is illustrated with optical design of a model spectrometer to deliver a resolving power above 20400 at a photon energy of 930 eV (Cu L-edge). With this energy taken as reference, the VLS coefficients are optimized to cancel the lineshape asymmetry (mostly from the coma aberrations) as well as minimize the symmetric aberration broadening at large grating illuminations, dramatically increasing the aberration-limited vertical acceptance of the spectrometer. For any energy away from the reference, corrections to the entrance arm and light incidence angle on the grating are evaluated to maintain the exactly symmetric lineshape. Furthermore, operational modes when these corrections are coordinated are evaluated to maintain either energy-independent focal curve inclination or maximal aberration-limited spectrometer acceptance. The results are supported by analytical evaluation of the coma term of the optical path function. This analysis thus gives a recipe for designing a high-resolution spherical VLS grating spectrometer operating with negligible aberrations at large acceptance and over an extended energy range.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Strocov, V.N.</dc:creator>
    <dc:creator>Schmitt, T.</dc:creator>
    <dc:creator>Flechsig, U.</dc:creator>
    <dc:creator>Patthey, L.</dc:creator>
    <dc:creator>Chiuzbăian, G.S.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510054452</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Operation of an X-ray spectrometer based on a spherical variable-line-spacing grating is analyzed using dedicated ray-tracing software allowing fast optimization of the grating parameters and spectrometer geometry.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RESONANT INELASTIC X-RAY SCATTERING; X-RAY OPTICS; X-RAY SPECTROMETERS; SPHERICAL VLS GRATINGS</dc:subject>
    <dc:description>Operation of an X-ray spectrometer based on a spherical variable-line-spacing (VLS) grating is analyzed using dedicated ray-tracing software allowing fast optimization of the grating parameters and spectrometer geometry. The analysis is illustrated with optical design of a model spectrometer to deliver a resolving power above 20400 at a photon energy of 930 eV (Cu L-edge). With this energy taken as reference, the VLS coefficients are optimized to cancel the lineshape asymmetry (mostly from the coma aberrations) as well as minimize the symmetric aberration broadening at large grating illuminations, dramatically increasing the aberration-limited vertical acceptance of the spectrometer. For any energy away from the reference, corrections to the entrance arm and light incidence angle on the grating are evaluated to maintain the exactly symmetric lineshape. Furthermore, operational modes when these corrections are coordinated are evaluated to maintain either energy-independent focal curve inclination or maximal aberration-limited spectrometer acceptance. The results are supported by analytical evaluation of the coma term of the optical path function. This analysis thus gives a recipe for designing a high-resolution spherical VLS grating spectrometer operating with negligible aberrations at large acceptance and over an extended energy range.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Numerical optimization of spherical variable-line-spacing grating X-ray spectrometers</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>134</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>142</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5181">
    <title>Assessment of chemical species of lead accumulated in tidemarks of human articular cartilage by X-ray absorption near-edge structure analysis</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5181</link>
    <description>A highly specific accumulation of the toxic element lead was recently measured in the transition zone between non-calcified and calcified normal human articular cartilage. This transition zone, the so-called `tidemark', is considered to be an active calcification front of great clinical importance. However, little is known about the mechanisms of accumulation and the chemical form of Pb in calcified cartilage and bone. Using spatially resolved X-ray absorption near-edge structure analysis (µ-XANES) at the Pb L3-edge, the chemical state of Pb in the osteochondral region was investigated. The feasibility of the µ-XANES set-up at the SUL-X beamline (ANKA synchrotron light source) was tested and confirmed by comparing XANES spectra of bulk Pb-reference compounds recorded at both the XAS and the SUL-X beamline at ANKA. The µ-XANES set-up was then used to investigate the tidemark region of human bone (two patella samples and one femoral head sample). The spectra recorded at the tidemark and at the trabecular bone were found to be highly correlated with the spectra of synthetic Pb-doped carbonated hydroxyapatite, suggesting that in both of these very different tissues Pb is incorporated into the hydroxyapatite structure.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Meirer, F.</dc:creator>
    <dc:creator>Pemmer, B.</dc:creator>
    <dc:creator>Pepponi, G.</dc:creator>
    <dc:creator>Zoeger, N.</dc:creator>
    <dc:creator>Wobrauschek, P.</dc:creator>
    <dc:creator>Sprio, S.</dc:creator>
    <dc:creator>Tampieri, A.</dc:creator>
    <dc:creator>Goettlicher, J.</dc:creator>
    <dc:creator>Steininger, R.</dc:creator>
    <dc:creator>Mangold, S.</dc:creator>
    <dc:creator>Roschger, P.</dc:creator>
    <dc:creator>Berzlanovich, A.</dc:creator>
    <dc:creator>Hofstaetter, J.G.</dc:creator>
    <dc:creator>Streli, C.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510052040</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Lead is a toxic trace element that shows a highly specific accumulation in the transition zone between calcified and non-calcified articular cartilage, the so-called `tidemark'. Excellent agreement has been found between XANES spectra of synthetic Pb-doped carbonated hydroxyapatite and spectra obtained in the tidemark region and trabecular bone of normal human samples, confirming that in both tissues Pb is incorporated into the hydroxyapatite crystal structure of bone. During this study the µ-XANES set-up at the SUL-X beamline at ANKA was tested and has proven to be well suited for speciation of lead in human mineralized tissue samples.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY ABSORPTION SPECTROSCOPY; PB L3-EDGE XANES; HUMAN BONE; TIDEMARK; TRABECULAR BONE</dc:subject>
    <dc:description>A highly specific accumulation of the toxic element lead was recently measured in the transition zone between non-calcified and calcified normal human articular cartilage. This transition zone, the so-called `tidemark', is considered to be an active calcification front of great clinical importance. However, little is known about the mechanisms of accumulation and the chemical form of Pb in calcified cartilage and bone. Using spatially resolved X-ray absorption near-edge structure analysis (µ-XANES) at the Pb L3-edge, the chemical state of Pb in the osteochondral region was investigated. The feasibility of the µ-XANES set-up at the SUL-X beamline (ANKA synchrotron light source) was tested and confirmed by comparing XANES spectra of bulk Pb-reference compounds recorded at both the XAS and the SUL-X beamline at ANKA. The µ-XANES set-up was then used to investigate the tidemark region of human bone (two patella samples and one femoral head sample). The spectra recorded at the tidemark and at the trabecular bone were found to be highly correlated with the spectra of synthetic Pb-doped carbonated hydroxyapatite, suggesting that in both of these very different tissues Pb is incorporated into the hydroxyapatite structure.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Assessment of chemical species of lead accumulated in tidemarks of human articular cartilage by X-ray absorption near-edge structure analysis</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>238</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>244</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wa5016">
    <title>Coherent diffraction microscopy at SPring-8: instrumentation, data acquisition and data analysis</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wa5016</link>
    <description>Since the first demonstration of coherent diffraction microscopy in 1999, this lensless imaging technique has been experimentally refined by continued developments. Here, instrumentation and experimental procedures for measuring oversampled diffraction patterns from non-crystalline specimens using an undulator beamline (BL29XUL) at SPring-8 are presented. In addition, detailed post-experimental data analysis is provided that yields high-quality image reconstructions. As the acquisition of high-quality diffraction patterns is at least as important as the phase-retrieval procedure to guarantee successful image reconstructions, this work will be of interest for those who want to apply this imaging technique to materials science and biological samples.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Xu, R.</dc:creator>
    <dc:creator>Salha, S.</dc:creator>
    <dc:creator>Raines, K.S.</dc:creator>
    <dc:creator>Jiang, H.</dc:creator>
    <dc:creator>Chen, C.-C.</dc:creator>
    <dc:creator>Takahashi, Y.</dc:creator>
    <dc:creator>Kohmura, Y.</dc:creator>
    <dc:creator>Nishino, Y.</dc:creator>
    <dc:creator>Song, C.</dc:creator>
    <dc:creator>Ishikawa, T.</dc:creator>
    <dc:creator>Miao, J.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510051733</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An instrumentation and data analysis review of coherent diffraction microscopy at SPring-8 is given. This work will be of interest to those who want to apply coherent diffraction imaging to studies of materials science and biological samples.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COHERENT DIFFRACTION MICROSCOPY; COHERENT DIFFRACTION IMAGING; LENSLESS IMAGING; OVERSAMPLING; PHASE RETRIEVAL</dc:subject>
    <dc:description>Since the first demonstration of coherent diffraction microscopy in 1999, this lensless imaging technique has been experimentally refined by continued developments. Here, instrumentation and experimental procedures for measuring oversampled diffraction patterns from non-crystalline specimens using an undulator beamline (BL29XUL) at SPring-8 are presented. In addition, detailed post-experimental data analysis is provided that yields high-quality image reconstructions. As the acquisition of high-quality diffraction patterns is at least as important as the phase-retrieval procedure to guarantee successful image reconstructions, this work will be of interest for those who want to apply this imaging technique to materials science and biological samples.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Coherent diffraction microscopy at SPring-8: instrumentation, data acquisition and data analysis</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>293</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>298</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0440">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0440</link>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510051599</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>92</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>93</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5089">
    <title>A simplified description of X-ray free-electron lasers</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5089</link>
    <description>It is shown that an elementary semi-quantitative approach explains essential features of the X-ray free-electron laser mechanism, in particular those of the gain and saturation lengths. Using mathematical methods and derivations simpler than complete theories, this treatment reveals the basic physics that dominates the mechanism and makes it difficult to realise free-electron lasers for short wavelengths. This approach can be specifically useful for teachers at different levels and for colleagues interested in presenting X-ray free-electron lasers to non-specialized audiences.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Margaritondo, G.</dc:creator>
    <dc:creator>Rebernik Ribic, P.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951004896X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An elementary derivation of fundamental properties of X-ray free-electron lasers is presented, including gain and saturation. Because of its simplicity, this approach is particularly suitable for teaching at different levels and for presentations to non-specialized audiences.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FREE-ELECTRON LASER; SASE; X-RAY LASER</dc:subject>
    <dc:description>It is shown that an elementary semi-quantitative approach explains essential features of the X-ray free-electron laser mechanism, in particular those of the gain and saturation lengths. Using mathematical methods and derivations simpler than complete theories, this treatment reveals the basic physics that dominates the mechanism and makes it difficult to realise free-electron lasers for short wavelengths. This approach can be specifically useful for teachers at different levels and for colleagues interested in presenting X-ray free-electron lasers to non-specialized audiences.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A simplified description of X-ray free-electron lasers</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>101</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>108</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ms9010">
    <title>MicroGISAXS of Langmuir–Blodgett protein films: effect of temperature on long-range order. Addendum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ms9010</link>
    <description>An extra acknowledgment is published for the paper by Pechkova et al. [(2009), J. Synchrotron Rad. 16, 330–335].</description>
    <dc:rights>Copyright (c) 2011 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Pechkova, E.</dc:creator>
    <dc:creator>Tripathi, S.</dc:creator>
    <dc:creator>Nicolini, C.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510049344</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An extra acknowledgment is published for the paper by Pechkova et al. [(2009), J. Synchrotron Rad. 16, 330–335].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>An extra acknowledgment is published for the paper by Pechkova et al. [(2009), J. Synchrotron Rad. 16, 330–335].</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>MicroGISAXS of Langmuir–Blodgett protein films: effect of temperature on long-range order. Addendum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2011 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>307</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>307</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pp5008">
    <title>High-throughput full-automatic synchrotron-based tomographic microscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pp5008</link>
    <description>At the TOMCAT (TOmographic Microscopy and Coherent rAdiology experimenTs) beamline of the Swiss Light Source with an energy range of 8–45 keV and voxel size from 0.37 µm to 7.4 µm, full tomographic datasets are typically acquired in 5 to 10 min. To exploit the speed of the system and enable high-throughput studies to be performed in a fully automatic manner, a package of automation tools has been developed. The samples are automatically exchanged, aligned, moved to the correct region of interest, and scanned. This task is accomplished through the coordination of Python scripts, a robot-based sample-exchange system, sample positioning motors and a CCD camera. The tools are suited for any samples that can be mounted on a standard SEM stub, and require no specific environmental conditions. Up to 60 samples can be analyzed at a time without user intervention. The throughput of the system is dependent on resolution, energy and sample size, but rates of four samples per hour have been achieved with 0.74 µm voxel size at 17.5 keV. The maximum intervention-free scanning time is theoretically unlimited, and in practice experiments have been running unattended as long as 53 h (the average beam time allocation at TOMCAT is 48 h per user). The system is the first fully automated high-throughput tomography station: mounting samples, finding regions of interest, scanning and reconstructing can be performed without user intervention. The system also includes many features which accelerate and simplify the process of tomographic microscopy.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Mader, K.</dc:creator>
    <dc:creator>Marone, F.</dc:creator>
    <dc:creator>Hintermüller, C.</dc:creator>
    <dc:creator>Mikuljan, G.</dc:creator>
    <dc:creator>Isenegger, A.</dc:creator>
    <dc:creator>Stampanoni, M.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510047370</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The automatization tools for high-throughput tomographic microscopy developed at the TOMCAT beamline of the Swiss Light Source are described</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TOMOGRAPHY; AUTOMATION; HIGH-THROUGHPUT; IMAGE PROCESSING; ALIGNMENT</dc:subject>
    <dc:description>At the TOMCAT (TOmographic Microscopy and Coherent rAdiology experimenTs) beamline of the Swiss Light Source with an energy range of 8–45 keV and voxel size from 0.37 µm to 7.4 µm, full tomographic datasets are typically acquired in 5 to 10 min. To exploit the speed of the system and enable high-throughput studies to be performed in a fully automatic manner, a package of automation tools has been developed. The samples are automatically exchanged, aligned, moved to the correct region of interest, and scanned. This task is accomplished through the coordination of Python scripts, a robot-based sample-exchange system, sample positioning motors and a CCD camera. The tools are suited for any samples that can be mounted on a standard SEM stub, and require no specific environmental conditions. Up to 60 samples can be analyzed at a time without user intervention. The throughput of the system is dependent on resolution, energy and sample size, but rates of four samples per hour have been achieved with 0.74 µm voxel size at 17.5 keV. The maximum intervention-free scanning time is theoretically unlimited, and in practice experiments have been running unattended as long as 53 h (the average beam time allocation at TOMCAT is 48 h per user). The system is the first fully automated high-throughput tomography station: mounting samples, finding regions of interest, scanning and reconstructing can be performed without user intervention. The system also includes many features which accelerate and simplify the process of tomographic microscopy.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>High-throughput full-automatic synchrotron-based tomographic microscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>117</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>124</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hf5176">
    <title>Quick-EXAFS implementation on the general purpose EXAFS beamline at ESRF</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hf5176</link>
    <description>The new implementation of QEXAFS acquisition on the general purpose EXAFS beamline BM29 at the European Synchrotron Radiation Facility is presented. By adopting a continuous-scan mode, a high signal-to-noise ratio can be maintained, together with a fixed exit beam and full compatibility with step-by-step operation, while reducing acquisition times to a few seconds. The new equipment implemented on the beamline is described and the potential of this application is demonstrated with a few examples.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Prestipino, C.</dc:creator>
    <dc:creator>Mathon, O.</dc:creator>
    <dc:creator>Hino, R.</dc:creator>
    <dc:creator>Beteva, A.</dc:creator>
    <dc:creator>Pascarelli, S.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510046546</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The new implementation of QEXAFS acquisition on the general purpose EXAFS beamline BM29 at the European Synchrotron Radiation Facility is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TIME-RESOLVED XAFS; HETEROGENEOUS CATALYSIS; POWDERS; CHEMICAL PROCESSES</dc:subject>
    <dc:description>The new implementation of QEXAFS acquisition on the general purpose EXAFS beamline BM29 at the European Synchrotron Radiation Facility is presented. By adopting a continuous-scan mode, a high signal-to-noise ratio can be maintained, together with a fixed exit beam and full compatibility with step-by-step operation, while reducing acquisition times to a few seconds. The new equipment implemented on the beamline is described and the potential of this application is demonstrated with a few examples.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Quick-EXAFS implementation on the general purpose EXAFS beamline at ESRF</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>176</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>182</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi5614">
    <title>Phosphorus K-edge XANES spectroscopy of mineral standards</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi5614</link>
    <description>Phosphorus K-edge X-ray absorption near-edge structure (XANES) spectroscopy was performed on phosphate mineral specimens including (a) twelve specimens from the apatite group covering a range of compositional variation and crystallinity; (b) six non-apatite calcium-rich phosphate minerals; (c) 15 aluminium-rich phosphate minerals; (d) ten phosphate minerals rich in either reduced iron or manganese; (e) four phosphate minerals rich in either oxidized iron or manganese; (f) eight phosphate minerals rich in either magnesium, copper, lead, zinc or rare-earth elements; and (g) four uranium phosphate minerals. The identity of all minerals examined in this study was independently confirmed using X-ray powder diffraction. Minerals were distinguished using XANES spectra with a combination of pre-edge features, edge position, peak shapes and post-edge features. Shared spectral features were observed in minerals with compositions dominated by the same specific cation. Analyses of apatite-group minerals indicate that XANES spectral patterns are not strongly affected by variations in composition and crystallinity typical of natural mineral specimens.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ingall, E.D.</dc:creator>
    <dc:creator>Brandes, J.A.</dc:creator>
    <dc:creator>Diaz, J.M.</dc:creator>
    <dc:creator>Jonge, M.D.de</dc:creator>
    <dc:creator>Paterson, D.</dc:creator>
    <dc:creator>McNulty, I.</dc:creator>
    <dc:creator>Elliott, W.C.</dc:creator>
    <dc:creator>Northrup, P.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510045322</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Phosphorus K-edge XANES spectra are presented for a diverse set of 44 phosphate minerals.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>XANES; PHOSPHORUS; PHOSPHATE MINERALS</dc:subject>
    <dc:description>Phosphorus K-edge X-ray absorption near-edge structure (XANES) spectroscopy was performed on phosphate mineral specimens including (a) twelve specimens from the apatite group covering a range of compositional variation and crystallinity; (b) six non-apatite calcium-rich phosphate minerals; (c) 15 aluminium-rich phosphate minerals; (d) ten phosphate minerals rich in either reduced iron or manganese; (e) four phosphate minerals rich in either oxidized iron or manganese; (f) eight phosphate minerals rich in either magnesium, copper, lead, zinc or rare-earth elements; and (g) four uranium phosphate minerals. The identity of all minerals examined in this study was independently confirmed using X-ray powder diffraction. Minerals were distinguished using XANES spectra with a combination of pre-edge features, edge position, peak shapes and post-edge features. Shared spectral features were observed in minerals with compositions dominated by the same specific cation. Analyses of apatite-group minerals indicate that XANES spectral patterns are not strongly affected by variations in composition and crystallinity typical of natural mineral specimens.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Phosphorus K-edge XANES spectroscopy of mineral standards</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>189</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>197</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?gf5031">
    <title>Comparison of lens- and fiber-coupled CCD detectors for X-ray computed tomography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?gf5031</link>
    <description>X-ray imaging detectors with an identical phosphor and a CCD chip but employing lens- and fiber-coupling between them have been compared. These are designed for X-ray imaging experiments, especially computed tomography, at the medium-length beamline at the SPring-8 synchrotron radiation facility. It was found that the transmittance of light to the CCD is about four times higher in the fiber-coupled detector. The uniformity of response in the lens-coupled detector has a global shading of up to 40%, while pixel-to-pixel variation owing to a chicken-wire pattern was dominant in the fiber-coupled detector. Apart from the higher transmittance, the fiber-coupled detector has a few characteristics that require attention when it is used for computed tomography, which are browning of the fiber, discontinuity in the image, image distortion, and dark spots in the chicken-wire pattern. Thus, it is most suitable for high-speed tomography of samples that tend to deform, for example biological and soft materials.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Uesugi, K.</dc:creator>
    <dc:creator>Hoshino, M.</dc:creator>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510044523</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Lens- and fiber-coupled X-ray detectors with identical CCD chips were compared in their performance in high-resolution computed tomography experiments.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY IMAGING; FIBER-COUPLED CCD; LENS-COUPLED CCD; MICROTOMOGRAPHY</dc:subject>
    <dc:description>X-ray imaging detectors with an identical phosphor and a CCD chip but employing lens- and fiber-coupling between them have been compared. These are designed for X-ray imaging experiments, especially computed tomography, at the medium-length beamline at the SPring-8 synchrotron radiation facility. It was found that the transmittance of light to the CCD is about four times higher in the fiber-coupled detector. The uniformity of response in the lens-coupled detector has a global shading of up to 40%, while pixel-to-pixel variation owing to a chicken-wire pattern was dominant in the fiber-coupled detector. Apart from the higher transmittance, the fiber-coupled detector has a few characteristics that require attention when it is used for computed tomography, which are browning of the fiber, discontinuity in the image, image distortion, and dark spots in the chicken-wire pattern. Thus, it is most suitable for high-speed tomography of samples that tend to deform, for example biological and soft materials.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Comparison of lens- and fiber-coupled CCD detectors for X-ray computed tomography</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>217</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>223</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5084">
    <title>X-ray transfocators: focusing devices based on compound refractive lenses</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5084</link>
    <description>This paper describes a tunable X-ray focusing apparatus, referred to as a transfocator, based on compound refractive lenses. By varying the number of lenses in the beam, the X-ray energy focused and the focal length can be varied continuously throughout a large range of energies and distances. The instrument can be used in both white and monochromatic beams to focus, pre-focus or collimate the beam. The transfocator can be used with other monochromators and/or other focusing elements, leading to significant increases in flux. Furthermore, the chromatic nature of the focusing means the transfocator suppresses harmonics and can also be used as an extremely high flux broad-band-pass monochromator. These devices have been installed in the first optics and second experimental hutches at the ID11 beamline at the ESRF.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Vaughan, G.B.M.</dc:creator>
    <dc:creator>Wright, J.P.</dc:creator>
    <dc:creator>Bytchkov, A.</dc:creator>
    <dc:creator>Rossat, M.</dc:creator>
    <dc:creator>Gleyzolle, H.</dc:creator>
    <dc:creator>Snigireva, I.</dc:creator>
    <dc:creator>Snigirev, A.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510044365</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A tunable X-ray focusing and/or monochromating device, called a transfocator, is described. Examples of its implementation on ID11 at the ESRF are given.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COMPOUND REFRACTIVE LENS; X-RAY OPTICS; MONOCHROMATOR; MICROFOCUS</dc:subject>
    <dc:description>This paper describes a tunable X-ray focusing apparatus, referred to as a transfocator, based on compound refractive lenses. By varying the number of lenses in the beam, the X-ray energy focused and the focal length can be varied continuously throughout a large range of energies and distances. The instrument can be used in both white and monochromatic beams to focus, pre-focus or collimate the beam. The transfocator can be used with other monochromators and/or other focusing elements, leading to significant increases in flux. Furthermore, the chromatic nature of the focusing means the transfocator suppresses harmonics and can also be used as an extremely high flux broad-band-pass monochromator. These devices have been installed in the first optics and second experimental hutches at the ID11 beamline at the ESRF.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray transfocators: focusing devices based on compound refractive lenses</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>125</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>133</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys0036">
    <title>Diffraction structural biology – introductory overview</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys0036</link>
    <description>An introductory overview to the special issue papers on diffraction structural biology in this issue of the journal.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Fourme, R.</dc:creator>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:creator>Johnson, J.E.</dc:creator>
    <dc:creator>Sakabe, N.</dc:creator>
    <dc:creator>Yasuoka, N.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510044912</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An introductory overview to the special issue papers on diffraction structural biology in this issue of the journal.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>An introductory overview to the special issue papers on diffraction structural biology in this issue of the journal.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Diffraction structural biology – introductory overview</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>1</prism:startingPage>
    <prism:section>editorial</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5055">
    <title>A new paradigm for macromolecular crystallography beamlines derived from high-pressure methodology and results</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5055</link>
    <description>Biological structures can now be investigated at high resolution by high-pressure X-ray macromolecular crystallography (HPMX). The number of HPMX studies is growing, with applications to polynucleotides, monomeric and multimeric proteins, complex assemblies and even a virus capsid. Investigations of the effects of pressure perturbation have encompassed elastic compression of the native state, study of proteins from extremophiles and trapping of higher-energy conformers that are often of biological interest; measurements of the compressibility of crystals and macromolecules were also performed. HPMX results were an incentive to investigate short and ultra-short wavelengths for standard biocrystallography. On cryocooled lysozyme crystals it was found that the data collection efficiency using 33 keV photons is increased with respect to 18 keV photons. This conclusion was extended from 33 keV down to 6.5 keV by exploiting previously published data. To be fully exploited, the potential of higher-energy photons requires detectors with a good efficiency. Accordingly, a new paradigm for MX beamlines was suggested, using conventional short and ultra-short wavelengths, aiming at the collection of very high accuracy data on crystals under standard conditions or under high pressure. The main elements of such beamlines are outlined.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Fourme, R.</dc:creator>
    <dc:creator>Girard, E.</dc:creator>
    <dc:creator>Dhaussy, A.-C.</dc:creator>
    <dc:creator>Medjoubi, K.</dc:creator>
    <dc:creator>Prangé, T.</dc:creator>
    <dc:creator>Ascone, I.</dc:creator>
    <dc:creator>Mezouar, M.</dc:creator>
    <dc:creator>Kahn, R.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510041695</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Macromolecular crystallography at high pressure (HPMX) is a mature technique. Shorter X-ray wavelengths increase data collection efficiency on cryocooled crystals. Extending applications and exploiting spin-off of HPMX will require dedicated synchrotron radiation beamlines based on a new paradigm.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; HIGH PRESSURE; SHORT X-RAY WAVELENGTH</dc:subject>
    <dc:description>Biological structures can now be investigated at high resolution by high-pressure X-ray macromolecular crystallography (HPMX). The number of HPMX studies is growing, with applications to polynucleotides, monomeric and multimeric proteins, complex assemblies and even a virus capsid. Investigations of the effects of pressure perturbation have encompassed elastic compression of the native state, study of proteins from extremophiles and trapping of higher-energy conformers that are often of biological interest; measurements of the compressibility of crystals and macromolecules were also performed. HPMX results were an incentive to investigate short and ultra-short wavelengths for standard biocrystallography. On cryocooled lysozyme crystals it was found that the data collection efficiency using 33 keV photons is increased with respect to 18 keV photons. This conclusion was extended from 33 keV down to 6.5 keV by exploiting previously published data. To be fully exploited, the potential of higher-energy photons requires detectors with a good efficiency. Accordingly, a new paradigm for MX beamlines was suggested, using conventional short and ultra-short wavelengths, aiming at the collection of very high accuracy data on crystals under standard conditions or under high pressure. The main elements of such beamlines are outlined.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A new paradigm for macromolecular crystallography beamlines derived from high-pressure methodology and results</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>31</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>36</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pp5007">
    <title>Three-dimensional X-ray micro-velocimetry</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pp5007</link>
    <description>A direct measurement of three-dimensional X-ray velocimetry with micrometer spatial resolution is presented. The key to this development is the use of a Laue crystal as an X-ray beam splitter and mirror. Three-dimensional flow velocities in a 0.4 mm-diameter tubing were recorded, with &lt;5 µm spatial resolution and speeds of 0.7 mm s−1. This development paves the way for three-dimensional velocimetry in many cases where visible-light techniques are not effective, such as multiphase flow or flow of optically opaque liquids.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Lee, W.-K.</dc:creator>
    <dc:creator>Fezzaa, K.</dc:creator>
    <dc:creator>Uemura, T.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510040434</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Three-dimensional X-ray velocimetry with micrometer-level resolution is demonstrated.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY IMAGING; 3D VELOCIMETRY; STEREO IMAGING; 3D PARTICLE TRACKING; 3D FLOW VELOCIMETRY</dc:subject>
    <dc:description>A direct measurement of three-dimensional X-ray velocimetry with micrometer spatial resolution is presented. The key to this development is the use of a Laue crystal as an X-ray beam splitter and mirror. Three-dimensional flow velocities in a 0.4 mm-diameter tubing were recorded, with &lt;5 µm spatial resolution and speeds of 0.7 mm s−1. This development paves the way for three-dimensional velocimetry in many cases where visible-light techniques are not effective, such as multiphase flow or flow of optically opaque liquids.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Three-dimensional X-ray micro-velocimetry</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>302</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>304</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0427">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0427</link>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2010-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510040896</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-11-01</prism:publicationDate>
    <prism:startingPage>821</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>822</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5046">
    <title>Synchrotron Mössbauer spectroscopy using high-speed shutters</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5046</link>
    <description>A new method of performing Mössbauer spectroscopy with synchrotron radiation is demonstrated that involves using a high-speed periodic shutter near the focal spot of a microfocused X-ray beam. This fast microshuttering technique operates without a high-resolution monochromator and has the potential to produce much higher signal rates. It also offers orders of magnitude more suppression of unwanted electronic charge scattering. Measurement results are shown that prove the principle of the method and improvements are discussed to deliver a very pure beam of Mössbauer photons (E/ΔE ≃ 1012) with previously unavailable spectral brightness. Such a source will allow both Mössbauer spectroscopy in the energy domain with the many advantageous characteristics of synchrotron radiation and new opportunities for measurements using X-rays with ultra-high energy resolution.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Toellner, T.S.</dc:creator>
    <dc:creator>Alp, E.E.</dc:creator>
    <dc:creator>Graber, T.</dc:creator>
    <dc:creator>Henning, R.W.</dc:creator>
    <dc:creator>Shastri, S.D.</dc:creator>
    <dc:creator>Shenoy, G.</dc:creator>
    <dc:creator>Sturhahn, W.</dc:creator>
    <dc:date>2011-03-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951003863X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A new method of performing Mössbauer spectroscopy using a fast shutter in combination with microfocused synchrotron radiation is demonstrated.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MOSSBAUER SPECTROSCOPY; NUCLEAR RESONANT SCATTERING; X-RAY SHUTTER</dc:subject>
    <dc:description>A new method of performing Mössbauer spectroscopy with synchrotron radiation is demonstrated that involves using a high-speed periodic shutter near the focal spot of a microfocused X-ray beam. This fast microshuttering technique operates without a high-resolution monochromator and has the potential to produce much higher signal rates. It also offers orders of magnitude more suppression of unwanted electronic charge scattering. Measurement results are shown that prove the principle of the method and improvements are discussed to deliver a very pure beam of Mössbauer photons (E/ΔE ≃ 1012) with previously unavailable spectral brightness. Such a source will allow both Mössbauer spectroscopy in the energy domain with the many advantageous characteristics of synchrotron radiation and new opportunities for measurements using X-rays with ultra-high energy resolution.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Synchrotron Mössbauer spectroscopy using high-speed shutters</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-03-01</prism:publicationDate>
    <prism:startingPage>183</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>188</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wa5015">
    <title>Indirectly illuminated X-ray area detector for X-ray photon correlation spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wa5015</link>
    <description>An indirectly illuminated X-ray area detector is employed for X-ray photon correlation spectroscopy (XPCS). The detector consists of a phosphor screen, an image intensifier (microchannel plate), a coupling lens and either a CCD or CMOS image sensor. By changing the gain of the image intensifier, both photon-counting and integrating measurements can be performed. Speckle patterns with a high signal-to-noise ratio can be observed in a single shot in the integrating mode, while XPCS measurement can be performed with much fewer photons in the photon-counting mode. By switching the image sensor, various combinations of frame rate, dynamic range and active area can be obtained. By virtue of these characteristics, this detector can be used for XPCS measurements of various types of samples that show slow or fast dynamics, a high or low scattering intensity, and a wide or narrow range of scattering angles.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Shinohara, Y.</dc:creator>
    <dc:creator>Imai, R.</dc:creator>
    <dc:creator>Kishimoto, H.</dc:creator>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:creator>Amemiya, Y.</dc:creator>
    <dc:date>2010-11-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951003726X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An indirectly illuminated X-ray area detector employed for X-ray photon correlation spectroscopy is discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>INDIRECTLY ILLUMINATED X-RAY DETECTORS; X-RAY PHOTON CORRELATION SPECTROSCOPY</dc:subject>
    <dc:description>An indirectly illuminated X-ray area detector is employed for X-ray photon correlation spectroscopy (XPCS). The detector consists of a phosphor screen, an image intensifier (microchannel plate), a coupling lens and either a CCD or CMOS image sensor. By changing the gain of the image intensifier, both photon-counting and integrating measurements can be performed. Speckle patterns with a high signal-to-noise ratio can be observed in a single shot in the integrating mode, while XPCS measurement can be performed with much fewer photons in the photon-counting mode. By switching the image sensor, various combinations of frame rate, dynamic range and active area can be obtained. By virtue of these characteristics, this detector can be used for XPCS measurements of various types of samples that show slow or fast dynamics, a high or low scattering intensity, and a wide or narrow range of scattering angles.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Indirectly illuminated X-ray area detector for X-ray photon correlation spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-11-01</prism:publicationDate>
    <prism:startingPage>737</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>742</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5061">
    <title>Improvement in the quality of hematopoietic prostaglandin D synthase crystals in a microgravity environment</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5061</link>
    <description>Human hematopoietic prostaglandin synthase, one of the better therapeutic target enzymes for allergy and inflammation, was crystallized with 22 inhibitors and in three inhibitor-free conditions in microgravity. Most of the space-grown crystals showed better X-ray diffraction patterns than the terrestrially grown ones, indicating the advantage of a microgravity environment on protein crystallization, especially in the case of this protein.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Tanaka, H.</dc:creator>
    <dc:creator>Tsurumura, T.</dc:creator>
    <dc:creator>Aritake, K.</dc:creator>
    <dc:creator>Furubayashi, N.</dc:creator>
    <dc:creator>Takahashi, S.</dc:creator>
    <dc:creator>Yamanaka, M.</dc:creator>
    <dc:creator>Hirota, E.</dc:creator>
    <dc:creator>Sano, S.</dc:creator>
    <dc:creator>Sato, M.</dc:creator>
    <dc:creator>Kobayashi, T.</dc:creator>
    <dc:creator>Tanaka, T.</dc:creator>
    <dc:creator>Inaka, K.</dc:creator>
    <dc:creator>Urade, Y.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510037076</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Crystals of hematopoietic prostaglandin D synthase grown in microgravity show improved quality.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROSTAGLANDIN D SYNTHASE; HEMATOPOIETIC; H-PGDS; CRYSTAL; MICROGRAVITY; SPACE EXPERIMENT; ANTI-INFLAMMATION; ANTI-ALLERGY; JAXA; COUNTER-DIFFUSION</dc:subject>
    <dc:description>Human hematopoietic prostaglandin synthase, one of the better therapeutic target enzymes for allergy and inflammation, was crystallized with 22 inhibitors and in three inhibitor-free conditions in microgravity. Most of the space-grown crystals showed better X-ray diffraction patterns than the terrestrially grown ones, indicating the advantage of a microgravity environment on protein crystallization, especially in the case of this protein.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Improvement in the quality of hematopoietic prostaglandin D synthase crystals in a microgravity environment</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>88</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>91</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5053">
    <title>Using lanthanoid complexes to phase large macromolecular assemblies</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5053</link>
    <description>Lanthanoid ions exhibit extremely large anomalous X-ray scattering at their LIII absorption edge. They are thus well suited for anomalous diffraction experiments. A novel class of lanthanoid complexes has been developed that combines the physical properties of lanthanoid atoms with functional chemical groups that allow non-covalent binding to proteins. Two structures of large multimeric proteins have already been determined by using such complexes. Here the use of the luminescent europium tris-dipicolinate complex [Eu(DPA)3]3− to solve the low-resolution structure of a 444 kDa homo­dodecameric aminopeptidase, called PhTET1-12s from the archaea Pyrococcus horikoshii, is reported. Surprisingly, considering the low resolution of the data, the experimental electron density map is very well defined. Experimental phases obtained by using the lanthanoid complex lead to maps displaying particular structural features usually observed in higher-resolution maps. Such complexes open a new way for solving the structure of large molecular assemblies, even with low-resolution data.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Talon, R.</dc:creator>
    <dc:creator>Kahn, R.</dc:creator>
    <dc:creator>Durá, M.A.</dc:creator>
    <dc:creator>Maury, O.</dc:creator>
    <dc:creator>Vellieux, F.M.D.</dc:creator>
    <dc:creator>Franzetti, B.</dc:creator>
    <dc:creator>Girard, E.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510036824</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A lanthanoid complex, [Eu(DPA)3]3−, was used to obtain experimental phases at 4.0 Å resolution of PhTET1-12s, a large self-compartmentalized homo-dodecameric protease complex of 444 kDa.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>LANTHANOID COMPLEXES; EXPERIMENTAL PHASING; LARGE MACROMOLECULAR ASSEMBLIES; TET AMINOPEPTIDASE</dc:subject>
    <dc:description>Lanthanoid ions exhibit extremely large anomalous X-ray scattering at their LIII absorption edge. They are thus well suited for anomalous diffraction experiments. A novel class of lanthanoid complexes has been developed that combines the physical properties of lanthanoid atoms with functional chemical groups that allow non-covalent binding to proteins. Two structures of large multimeric proteins have already been determined by using such complexes. Here the use of the luminescent europium tris-dipicolinate complex [Eu(DPA)3]3− to solve the low-resolution structure of a 444 kDa homo­dodecameric aminopeptidase, called PhTET1-12s from the archaea Pyrococcus horikoshii, is reported. Surprisingly, considering the low resolution of the data, the experimental electron density map is very well defined. Experimental phases obtained by using the lanthanoid complex lead to maps displaying particular structural features usually observed in higher-resolution maps. Such complexes open a new way for solving the structure of large molecular assemblies, even with low-resolution data.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Using lanthanoid complexes to phase large macromolecular assemblies</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>74</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>78</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5051">
    <title>Three-dimensional structural analysis of eukaryotic flagella/cilia by electron cryo-tomography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5051</link>
    <description>Electron cryo-tomography is a potential approach to analyzing the three-dimensional conformation of frozen hydrated biological macromolecules using electron microscopy. Since projections of each individual object illuminated from different orientations are merged, electron tomography is capable of structural analysis of such heterogeneous environments as in vivo or with polymorphism, although radiation damage and the missing wedge are severe problems. Here, recent results on the structure of eukaryotic flagella, which is an ATP-driven bending organelle, from green algae Chlamydomonas are presented. Tomographic analysis reveals asymmetric molecular arrangements, especially that of the dynein motor proteins, in flagella, giving insight into the mechanism of planar asymmetric bending motion. Methodological challenges to obtaining higher-resolution structures from this technique are also discussed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Bui, K.H.</dc:creator>
    <dc:creator>Pigino, G.</dc:creator>
    <dc:creator>Ishikawa, T.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510036812</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Based on the molecular architecture revealed by electron cryo-tomography, the mechanism of the bending motion of eukaryotic flagella/cilia is discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DYNEIN; FLAGELLA; AXONEME; TOMOGRAPHY; CRYO-EM</dc:subject>
    <dc:description>Electron cryo-tomography is a potential approach to analyzing the three-dimensional conformation of frozen hydrated biological macromolecules using electron microscopy. Since projections of each individual object illuminated from different orientations are merged, electron tomography is capable of structural analysis of such heterogeneous environments as in vivo or with polymorphism, although radiation damage and the missing wedge are severe problems. Here, recent results on the structure of eukaryotic flagella, which is an ATP-driven bending organelle, from green algae Chlamydomonas are presented. Tomographic analysis reveals asymmetric molecular arrangements, especially that of the dynein motor proteins, in flagella, giving insight into the mechanism of planar asymmetric bending motion. Methodological challenges to obtaining higher-resolution structures from this technique are also discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Three-dimensional structural analysis of eukaryotic flagella/cilia by electron cryo-tomography</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>2</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>5</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5059">
    <title>Biomolecular solution X-ray scattering at the National Synchrotron Light Source</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5059</link>
    <description>In recent years there has been a growing interest in the application of X-ray scattering techniques to biomolecules in solution. At NSLS, a new undulator-based beamline, X9, has been constructed to address the oversubscribed user demand for X-ray scattering. Beamline X9 has the capability to perform small/wide-angle X-ray scattering (SAXS/WAXS) all in one single instrument. This is accomplished by utilizing a vacuum sample/detector chamber that is an integral part of the SAXS scattering flight path. This vacuum chamber allows a WAXS detector to be positioned at a close distance from the sample, while not interfering with scattered X-rays at small angles from reaching the SAXS detector. A regular training program, the X9 workbench, has also been established to allow users to become familiar with beamline X9 for solution X-ray scattering.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Allaire, M.</dc:creator>
    <dc:creator>Yang, L.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510036022</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A new beamline for simultaneous SAXS/WAXS of biomolecules in solution is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; WAXS; BEAMLINE; PROTEINS; DNA/RNA</dc:subject>
    <dc:description>In recent years there has been a growing interest in the application of X-ray scattering techniques to biomolecules in solution. At NSLS, a new undulator-based beamline, X9, has been constructed to address the oversubscribed user demand for X-ray scattering. Beamline X9 has the capability to perform small/wide-angle X-ray scattering (SAXS/WAXS) all in one single instrument. This is accomplished by utilizing a vacuum sample/detector chamber that is an integral part of the SAXS scattering flight path. This vacuum chamber allows a WAXS detector to be positioned at a close distance from the sample, while not interfering with scattered X-rays at small angles from reaching the SAXS detector. A regular training program, the X9 workbench, has also been established to allow users to become familiar with beamline X9 for solution X-ray scattering.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Biomolecular solution X-ray scattering at the National Synchrotron Light Source</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>41</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>44</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5054">
    <title>Structural insights and ab initio sequencing within the DING proteins family</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5054</link>
    <description>DING proteins constitute an intriguing family of phosphate-binding proteins that was identified in a wide range of organisms, from prokaryotes and archae to eukaryotes. Despite their seemingly ubiquitous occurrence in eukaryotes, their encoding genes are missing from sequenced genomes. Such a lack has considerably hampered functional studies. In humans, these proteins have been related to several diseases, like atherosclerosis, kidney stones, inflammation processes and HIV inhibition. The human phosphate binding protein is a human representative of the DING family that was serendipitously discovered from human plasma. An original approach was developed to determine ab initio the complete and exact sequence of this 38 kDa protein by utilizing mass spectrometry and X-ray data in tandem. Taking advantage of this first complete eukaryotic DING sequence, a immunohistochemistry study was undertaken to check the presence of DING proteins in various mice tissues, revealing that these proteins are widely expressed. Finally, the structure of a bacterial representative from Pseudomonas fluorescens was solved at sub-angstrom resolution, allowing the molecular mechanism of the phosphate binding in these high-affinity proteins to be elucidated.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Elias, M.</dc:creator>
    <dc:creator>Liebschner, D.</dc:creator>
    <dc:creator>Gotthard, G.</dc:creator>
    <dc:creator>Chabriere, E.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510036009</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>DING proteins constitute a recently discovered protein family that is ubiquitous in eukaryotes. The structural insights and the physiological involvements of these intriguing proteins are hereby deciphered.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SERENDIPITY; DING PROTEIN; AB INITIO SEQUENCING; SUB-ANGSTROM CRYSTALLOGRAPHY; HIV INHIBITION</dc:subject>
    <dc:description>DING proteins constitute an intriguing family of phosphate-binding proteins that was identified in a wide range of organisms, from prokaryotes and archae to eukaryotes. Despite their seemingly ubiquitous occurrence in eukaryotes, their encoding genes are missing from sequenced genomes. Such a lack has considerably hampered functional studies. In humans, these proteins have been related to several diseases, like atherosclerosis, kidney stones, inflammation processes and HIV inhibition. The human phosphate binding protein is a human representative of the DING family that was serendipitously discovered from human plasma. An original approach was developed to determine ab initio the complete and exact sequence of this 38 kDa protein by utilizing mass spectrometry and X-ray data in tandem. Taking advantage of this first complete eukaryotic DING sequence, a immunohistochemistry study was undertaken to check the presence of DING proteins in various mice tissues, revealing that these proteins are widely expressed. Finally, the structure of a bacterial representative from Pseudomonas fluorescens was solved at sub-angstrom resolution, allowing the molecular mechanism of the phosphate binding in these high-affinity proteins to be elucidated.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structural insights and ab initio sequencing within the DING proteins family</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>45</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>49</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5052">
    <title>Optimization of salt concentration in PEG-based crystallization solutions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5052</link>
    <description>Although polyethylene glycol (PEG) is the most widely used precipitant in protein crystallization, the concentration of co-existing salt in the solution has not been well discussed. To determine the optimum salt concentration range, several kinds of protein were crystallized in a 30% PEG 4000 solution at various NaCl concentrations with various pH levels. It was found that, if crystallization occurred, the lowest effective salt concentration depended on the pH of the protein solution and the pI of the protein molecule; that is, higher salt concentrations were required for crystal growth if the difference between pH and pI was increasing. The linear relationship between the charge density of the protein and the ionic strength of the crystallization solution was further verified. These results suggested that the lowest effective concentration of salt in a crystallization solution can be predicted before performing a crystallization experiment. Our results can be a tip for tuning crystallization conditions by the vapor-diffusion method.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yamanaka, M.</dc:creator>
    <dc:creator>Inaka, K.</dc:creator>
    <dc:creator>Furubayashi, N.</dc:creator>
    <dc:creator>Matsushima, M.</dc:creator>
    <dc:creator>Takahashi, S.</dc:creator>
    <dc:creator>Tanaka, H.</dc:creator>
    <dc:creator>Sano, S.</dc:creator>
    <dc:creator>Sato, M.</dc:creator>
    <dc:creator>Kobayashi, T.</dc:creator>
    <dc:creator>Tanaka, T.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510035995</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Optimal salt concentration in a PEG-based crystallization solution is important for successful crystal growth and can be predicted prior to performing crystallization experiments.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROTEIN CRYSTALLIZATION; OPTIMIZATION; SALT CONCENTRATION; POLYETHYLENE GLYCOL; IONIC STRENGTH</dc:subject>
    <dc:description>Although polyethylene glycol (PEG) is the most widely used precipitant in protein crystallization, the concentration of co-existing salt in the solution has not been well discussed. To determine the optimum salt concentration range, several kinds of protein were crystallized in a 30% PEG 4000 solution at various NaCl concentrations with various pH levels. It was found that, if crystallization occurred, the lowest effective salt concentration depended on the pH of the protein solution and the pI of the protein molecule; that is, higher salt concentrations were required for crystal growth if the difference between pH and pI was increasing. The linear relationship between the charge density of the protein and the ionic strength of the crystallization solution was further verified. These results suggested that the lowest effective concentration of salt in a crystallization solution can be predicted before performing a crystallization experiment. Our results can be a tip for tuning crystallization conditions by the vapor-diffusion method.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Optimization of salt concentration in PEG-based crystallization solutions</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>84</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>87</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5060">
    <title>Microcrystallography, high-pressure cryocooling and BioSAXS at MacCHESS</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5060</link>
    <description>The Macromolecular Diffraction Facility at the Cornell High Energy Synchrotron Source (MacCHESS) is a national research resource supported by the National Center for Research Resources of the US National Institutes of Health. MacCHESS is pursuing several research initiatives designed to benefit both CHESS users and the wider structural biology community. Three initiatives are presented in further detail: microcrystallography, which aims to improve the collection of diffraction data from crystals a few micrometers across, or small well diffracting regions of inhomogeneous crystals, so as to obtain high-resolution structures; pressure cryocooling, which can stabilize transient structures and reduce lattice damage during the cooling process; and BioSAXS (small-angle X-ray scattering on biological solutions), which can extract molecular shape and other structural information from macromolecules in solution.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Englich, U.</dc:creator>
    <dc:creator>Kriksunov, I.A.</dc:creator>
    <dc:creator>Cerione, R.A.</dc:creator>
    <dc:creator>Cook, M.J.</dc:creator>
    <dc:creator>Gillilan, R.</dc:creator>
    <dc:creator>Gruner, S.M.</dc:creator>
    <dc:creator>Huang, Q.</dc:creator>
    <dc:creator>Kim, C.U.</dc:creator>
    <dc:creator>Miller, W.</dc:creator>
    <dc:creator>Nielsen, S.</dc:creator>
    <dc:creator>Schuller, D.</dc:creator>
    <dc:creator>Smith, S.</dc:creator>
    <dc:creator>Szebenyi, D.M.E.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510036010</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Three research initiatives pursued by the Macromolecular Diffraction Facility at the Cornell High Energy Synchrotron Source (MacCHESS) are presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROTEIN CRYSTALLOGRAPHY; MICROCRYSTALLOGRAPHY; BIOSAXS; CRYO; PRESSURE</dc:subject>
    <dc:description>The Macromolecular Diffraction Facility at the Cornell High Energy Synchrotron Source (MacCHESS) is a national research resource supported by the National Center for Research Resources of the US National Institutes of Health. MacCHESS is pursuing several research initiatives designed to benefit both CHESS users and the wider structural biology community. Three initiatives are presented in further detail: microcrystallography, which aims to improve the collection of diffraction data from crystals a few micrometers across, or small well diffracting regions of inhomogeneous crystals, so as to obtain high-resolution structures; pressure cryocooling, which can stabilize transient structures and reduce lattice damage during the cooling process; and BioSAXS (small-angle X-ray scattering on biological solutions), which can extract molecular shape and other structural information from macromolecules in solution.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Microcrystallography, high-pressure cryocooling and BioSAXS at MacCHESS</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>70</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>73</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5046">
    <title>Detection of the reaction intermediates catalyzed by a copper amine oxidase</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5046</link>
    <description>To reveal the chemical changes and geometry changes of active-site residues that cooperate with a reaction is important for understanding the functional mechanism of proteins. Consecutive temporal analyses of enzyme structures have been performed during reactions to clarify structure-based reaction mechanisms. Phenylethylamine oxidase from Arthrobacter globiformis (AGAO) contains a copper ion and topaquinone (TPQox). The catalytic reaction of AGAO catalyzes oxidative deaminations of phenylethylamine and consists of reductive and oxidative half-reactions. In the reduction step, TPQox reacts with a phenylethylamine (PEA) substrate giving rise to a topasemiquinone (TPQsq) formed Schiff-base and produces phenylacetaldehyde. To elucidate the mechanism of the reductive half-reaction, an attempt was made to trap the reaction intermediates in order to analyze their structures. The reaction proceeded within the crystals when AGAO crystals were soaked in a PEA solution and freeze-trapped in liquid nitrogen. The reaction stage of each crystal was confirmed by single-crystal microspectrometry, before X-ray diffraction measurements were made of four reaction intermediates. The structure at 15 min after the onset of the reaction was analyzed at atomic resolution, and it was shown that TPQox and some residues in the substrate channel were alternated via catalytic reductive half-reactions.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Kataoka, M.</dc:creator>
    <dc:creator>Oya, H.</dc:creator>
    <dc:creator>Tominaga, A.</dc:creator>
    <dc:creator>Otsu, M.</dc:creator>
    <dc:creator>Okajima, T.</dc:creator>
    <dc:creator>Tanizawa, K.</dc:creator>
    <dc:creator>Yamaguchi, H.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510034989</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Consecutive temporal analyses of enzyme structure have been performed during reactions in order to clarify the structure-based reaction mechanism. Four intermediate structures have been determined.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COPPER AMINE OXIDASE; AGAO; TOPAQUINONE; REACTION INTERMEDIATE; SINGLE-CRYSTAL MICROSPECTROSCOPY; X-RAY CRYSTAL STRUCTURE ANALYSIS</dc:subject>
    <dc:description>To reveal the chemical changes and geometry changes of active-site residues that cooperate with a reaction is important for understanding the functional mechanism of proteins. Consecutive temporal analyses of enzyme structures have been performed during reactions to clarify structure-based reaction mechanisms. Phenylethylamine oxidase from Arthrobacter globiformis (AGAO) contains a copper ion and topaquinone (TPQox). The catalytic reaction of AGAO catalyzes oxidative deaminations of phenylethylamine and consists of reductive and oxidative half-reactions. In the reduction step, TPQox reacts with a phenylethylamine (PEA) substrate giving rise to a topasemiquinone (TPQsq) formed Schiff-base and produces phenylacetaldehyde. To elucidate the mechanism of the reductive half-reaction, an attempt was made to trap the reaction intermediates in order to analyze their structures. The reaction proceeded within the crystals when AGAO crystals were soaked in a PEA solution and freeze-trapped in liquid nitrogen. The reaction stage of each crystal was confirmed by single-crystal microspectrometry, before X-ray diffraction measurements were made of four reaction intermediates. The structure at 15 min after the onset of the reaction was analyzed at atomic resolution, and it was shown that TPQox and some residues in the substrate channel were alternated via catalytic reductive half-reactions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Detection of the reaction intermediates catalyzed by a copper amine oxidase</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>58</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>61</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5057">
    <title>Deriving the ultrastructure of α-crustacyanin using lower-resolution structural and biophysical methods</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5057</link>
    <description>The low-resolution structure of α-crustacyanin has been determined to 30 Å resolution using negative-stain electron microscopy (EM) with single-particle averaging. The protein, which is an assembly of eight β-crustacyanin dimers, appears asymmetrical and rather open in layout. A model was built to the EM map using the X-ray crystallographic structure of β-crustacyanin guided by PISA interface analyses. The model has a theoretical sedimentation coefficient that matches well with the experimentally derived value from sedimentation velocity analytical ultracentrifugation. Additionally, the EM model has similarities to models calculated independently by rigid-body modelling to small-angle X-ray scattering (SAXS) data and extracted in silico from the β-crustacyanin crystal lattice. Theoretical X-ray scattering from each of these models is in reasonable agreement with the experimental SAXS data and together suggest an overall design for the α-crustacyanin assembly.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Rhys, N.H.</dc:creator>
    <dc:creator>Wang, M.-C.</dc:creator>
    <dc:creator>Jowitt, T.A.</dc:creator>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:creator>Grossmann, J.G.</dc:creator>
    <dc:creator>Baldock, C.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510034977</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The structure of α-crustacyanin has been determined to 30 Å resolution using negative-stain electron microscopy (EM) single-particle averaging and modelling with the β-crustacyanin dimer from the crystal structure (Protein Data Bank code 1gka), guided by PISA protein subunit interface calculations for 1gka, and compared with the protein arrangements observed in the crystal lattice of 1gka. This α-crustacyanin EM model has been checked against SAXS experimental data, including comparison with rigid-body models calculated from the SAXS data, and finally with analytical ultracentrifugation measurements.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>[ALPHA]-CRUSTACYANIN; EM; SAXS; CRYSTAL PACKING OF 1GKA; PISA; ANALYTICAL ULTRACENTRIFUGATION</dc:subject>
    <dc:description>The low-resolution structure of α-crustacyanin has been determined to 30 Å resolution using negative-stain electron microscopy (EM) with single-particle averaging. The protein, which is an assembly of eight β-crustacyanin dimers, appears asymmetrical and rather open in layout. A model was built to the EM map using the X-ray crystallographic structure of β-crustacyanin guided by PISA interface analyses. The model has a theoretical sedimentation coefficient that matches well with the experimentally derived value from sedimentation velocity analytical ultracentrifugation. Additionally, the EM model has similarities to models calculated independently by rigid-body modelling to small-angle X-ray scattering (SAXS) data and extracted in silico from the β-crustacyanin crystal lattice. Theoretical X-ray scattering from each of these models is in reasonable agreement with the experimental SAXS data and together suggest an overall design for the α-crustacyanin assembly.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Deriving the ultrastructure of α-crustacyanin using lower-resolution structural and biophysical methods</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>79</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>83</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5047">
    <title>Approach for growth of high-quality and large protein crystals</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5047</link>
    <description>Three crystallization methods for growing large high-quality protein crystals, i.e. crystallization in the presence of a semi-solid agarose gel, top-seeded solution growth (TSSG) and a large-scale hanging-drop method, have previously been presented. In this study the effectiveness of crystallization in the presence of a semi-solid agarose gel has been further evaluated by crystallizing additional proteins in the presence of 2.0% (w/v) agarose gel, resulting in complete gelification with high mechanical strength. In TSSG the seed crystals are hung by a seed holder protruding from the top of the growth vessel to prevent polycrystallization. In the large-scale hanging-drop method, a cut pipette tip was used to maintain large-scale droplets consisting of protein–precipitant solution. Here a novel crystallization method that combines TSSG and the large-scale hanging-drop method is reported. A large and single crystal of lysozyme was obtained by this method.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Matsumura, H.</dc:creator>
    <dc:creator>Sugiyama, S.</dc:creator>
    <dc:creator>Hirose, M.</dc:creator>
    <dc:creator>Kakinouchi, K.</dc:creator>
    <dc:creator>Maruyama, M.</dc:creator>
    <dc:creator>Murai, R.</dc:creator>
    <dc:creator>Adachi, H.</dc:creator>
    <dc:creator>Takano, K.</dc:creator>
    <dc:creator>Murakami, S.</dc:creator>
    <dc:creator>Mori, Y.</dc:creator>
    <dc:creator>Inoue, T.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951003445X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Three crystallization methods, including crystallization in the presence of a semi-solid agarose gel, top-seeded solution growth (TSSG) and a large-scale hanging-drop method, have previously been presented. In this study, crystallization has been further evaluated in the presence of a semi-solid agarose gel by crystallizing additional proteins. A novel crystallization method combining TSSG and the large-scale hanging-drop method has also been developed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SEMI-SOLID AGAROSE GELS; TOP-SEEDED SOLUTION GROWTH; LARGE-SCALE HANGING-DROP METHOD; X-RAY CRYSTALLOGRAPHY; NEUTRON CRYSTALLOGRAPHY</dc:subject>
    <dc:description>Three crystallization methods for growing large high-quality protein crystals, i.e. crystallization in the presence of a semi-solid agarose gel, top-seeded solution growth (TSSG) and a large-scale hanging-drop method, have previously been presented. In this study the effectiveness of crystallization in the presence of a semi-solid agarose gel has been further evaluated by crystallizing additional proteins in the presence of 2.0% (w/v) agarose gel, resulting in complete gelification with high mechanical strength. In TSSG the seed crystals are hung by a seed holder protruding from the top of the growth vessel to prevent polycrystallization. In the large-scale hanging-drop method, a cut pipette tip was used to maintain large-scale droplets consisting of protein–precipitant solution. Here a novel crystallization method that combines TSSG and the large-scale hanging-drop method is reported. A large and single crystal of lysozyme was obtained by this method.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Approach for growth of high-quality and large protein crystals</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>16</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>19</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5049">
    <title>Structure of the inhibitor complex of old yellow enzyme from Trypanosoma cruzi</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5049</link>
    <description>Old yellow enzyme (OYE) is an NADPH oxidoreductase which contains flavin mononucleotide as prosthetic group. The X-ray structures of OYE from Trypanosoma cruzi (TcOYE) which produces prostaglandin (PG) F2α from PGH2 have been determined in the presence or absence of menadione. The binding motif of menadione, known as one of the inhibitors for TcOYE, should accelerate the structure-based development of novel anti-chagasic drugs that inhibit PGF2α production specifically.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yamaguchi, K.</dc:creator>
    <dc:creator>Okamoto, N.</dc:creator>
    <dc:creator>Tokuoka, K.</dc:creator>
    <dc:creator>Sugiyama, S.</dc:creator>
    <dc:creator>Uchiyama, N.</dc:creator>
    <dc:creator>Matsumura, H.</dc:creator>
    <dc:creator>Inaka, K.</dc:creator>
    <dc:creator>Urade, Y.</dc:creator>
    <dc:creator>Inoue, T.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510033595</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The structures of old yellow enzyme from Trypanosoma cruzi which produces prostaglandin F2α from PGH2 have been determined in the presence or absence of menadione.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY STRUCTURE; INHIBITOR COMPLEX; PROSTAGLANDIN SYNTHASE</dc:subject>
    <dc:description>Old yellow enzyme (OYE) is an NADPH oxidoreductase which contains flavin mononucleotide as prosthetic group. The X-ray structures of OYE from Trypanosoma cruzi (TcOYE) which produces prostaglandin (PG) F2α from PGH2 have been determined in the presence or absence of menadione. The binding motif of menadione, known as one of the inhibitors for TcOYE, should accelerate the structure-based development of novel anti-chagasic drugs that inhibit PGF2α production specifically.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structure of the inhibitor complex of old yellow enzyme from Trypanosoma cruzi</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>66</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>69</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5058">
    <title>Single-crystal Raman spectroscopy and X-ray crystallography at beamline X26-C of the NSLS</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5058</link>
    <description>Three-dimensional structures derived from X-ray diffraction of protein crystals provide a wealth of information. Features and interactions important for the function of macromolecules can be deduced and catalytic mechanisms postulated. Still, many questions can remain, for example regarding metal oxidation states and the interpretation of `mystery density', i.e. ambiguous or unknown features within the electron density maps, especially at ∼2 Å resolutions typical of most macromolecular structures. Beamline X26-C at the National Synchrotron Light Source (NSLS), Brookhaven National Laboratory (BNL), provides researchers with the opportunity to not only determine the atomic structure of their samples but also to explore the electronic and vibrational characteristics of the sample before, during and after X-ray diffraction data collection. When samples are maintained under cryo-conditions, an opportunity to promote and follow photochemical reactions in situ as a function of X-ray exposure is also provided. Plans are in place to further expand the capabilities at beamline X26-C and to develop beamlines at NSLS-II, currently under construction at BNL, which will provide users access to a wide array of complementary spectroscopic methods in addition to high-quality X-ray diffraction data.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Stoner-Ma, D.</dc:creator>
    <dc:creator>Skinner, J.M.</dc:creator>
    <dc:creator>Schneider, D.K.</dc:creator>
    <dc:creator>Cowan, M.</dc:creator>
    <dc:creator>Sweet, R.M.</dc:creator>
    <dc:creator>Orville, A.M.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510033601</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The collection of absorption and Raman spectroscopic data correlated with X-ray diffraction data allows investigators to understand the atomic structure as well as the electronic and vibrational characteristics of their samples, to identify transiently formed intermediates and to explore mechanistic questions. Raman spectroscopy instrumentation at beamline X26-C at the NSLS is currently available to the general user population.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RAMAN; SINGLE-CRYSTAL SPECTROSCOPY; X-RAY DIFFRACTION</dc:subject>
    <dc:description>Three-dimensional structures derived from X-ray diffraction of protein crystals provide a wealth of information. Features and interactions important for the function of macromolecules can be deduced and catalytic mechanisms postulated. Still, many questions can remain, for example regarding metal oxidation states and the interpretation of `mystery density', i.e. ambiguous or unknown features within the electron density maps, especially at ∼2 Å resolutions typical of most macromolecular structures. Beamline X26-C at the National Synchrotron Light Source (NSLS), Brookhaven National Laboratory (BNL), provides researchers with the opportunity to not only determine the atomic structure of their samples but also to explore the electronic and vibrational characteristics of the sample before, during and after X-ray diffraction data collection. When samples are maintained under cryo-conditions, an opportunity to promote and follow photochemical reactions in situ as a function of X-ray exposure is also provided. Plans are in place to further expand the capabilities at beamline X26-C and to develop beamlines at NSLS-II, currently under construction at BNL, which will provide users access to a wide array of complementary spectroscopic methods in addition to high-quality X-ray diffraction data.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Single-crystal Raman spectroscopy and X-ray crystallography at beamline X26-C of the NSLS</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>37</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>40</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0423">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0423</link>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2010-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510032899</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-09-01</prism:publicationDate>
    <prism:startingPage>708</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>709</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5050">
    <title>Protein surface shielding agents in protein crystallization</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5050</link>
    <description>The molecules adhering temporarily on the surface of protein molecules change the propensity of protein molecules to deposit on the crystal surface in a definite position and orientation. The concepts of competitive adhesion modes and protein surface shielding agents acting on the surface of molecules in a non-equilibrium process of protein crystallization provide a useful platform for the control of crystallization. The desirable goal, i.e. a transient preference of a single dominating adhesion mode between protein molecules during crystallization, leads to uniform deposition of proteins in a crystal. This condition is the most important factor for diffraction quality and thus also for the accuracy of protein structure determination. The presented hypothesis is a generalization of the experimentally well proven behaviour of hydrophilic polymers on the surface of protein molecules of other compounds.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hašek, J.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510032450</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The crystallization process can be controlled by protein surface shielding agents blocking undesirable competitive adhesion modes during non-equilibrium processes of deposition of protein molecules on the surface of growing crystalline blocks. The hypothesis is based on a number of experimental proofs from diffraction experiments and also retrieved from the Protein Data Bank.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROTEIN ADHESION; PROTEIN SURFACE SHIELDING AGENTS; INTERMOLECULAR INTERACTIONS; COMPETITIVE ADHESION MODES; POLYMER CRYSTALLIZATION SCREENS</dc:subject>
    <dc:description>The molecules adhering temporarily on the surface of protein molecules change the propensity of protein molecules to deposit on the crystal surface in a definite position and orientation. The concepts of competitive adhesion modes and protein surface shielding agents acting on the surface of molecules in a non-equilibrium process of protein crystallization provide a useful platform for the control of crystallization. The desirable goal, i.e. a transient preference of a single dominating adhesion mode between protein molecules during crystallization, leads to uniform deposition of proteins in a crystal. This condition is the most important factor for diffraction quality and thus also for the accuracy of protein structure determination. The presented hypothesis is a generalization of the experimentally well proven behaviour of hydrophilic polymers on the surface of protein molecules of other compounds.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Protein surface shielding agents in protein crystallization</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>50</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>52</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ms5026">
    <title>Software for the high-throughput collection of SAXS data using an enhanced Blu-Ice/DCS control system</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ms5026</link>
    <description>Biological small-angle X-ray scattering (SAXS) provides powerful complementary data for macromolecular crystallography (MX) by defining shape, conformation and assembly in solution. Although SAXS is in principle the highest throughput technique for structural biology, data collection is limited in practice by current data collection software. Here the adaption of beamline control software, historically developed for MX beamlines, for the efficient operation and high-throughput data collection at synchrotron SAXS beamlines is reported. The Blu-Ice GUI and Distributed Control System (DCS) developed in the Macromolecular Crystallography Group at the Stanford Synchrotron Radiation Laboratory has been optimized, extended and enhanced to suit the specific needs of the biological SAXS endstation at the SIBYLS beamline at the Advanced Light Source. The customizations reported here provide a potential route for other SAXS beamlines in need of robust and efficient beamline control software. As a great deal of effort and optimization has gone into crystallographic software, the adaption and extension of crystallographic software may prove to be a general strategy to provide advanced SAXS software for the synchrotron community. In this way effort can be put into optimizing features for SAXS rather than reproducing those that have already been successfully implemented for the crystallographic community.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Classen, S.</dc:creator>
    <dc:creator>Rodic, I.</dc:creator>
    <dc:creator>Holton, J.</dc:creator>
    <dc:creator>Hura, G.L.</dc:creator>
    <dc:creator>Hammel, M.</dc:creator>
    <dc:creator>Tainer, J.A.</dc:creator>
    <dc:date>2010-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510028566</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The Blu-Ice GUI and Distributed Control System (DCS) developed in the Macromolecular Crystallography Group at the Stanford Synchrotron Radiation Laboratory has been optimized, extended and enhanced to suit the specific needs of the SAXS endstation at the SIBYLS beamline at the Advanced Light Source. The customizations reported here provide one potential route for other SAXS beamlines in need of robust and efficient beamline control software.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; SOFTWARE; BEAMLINE; CONTROL SYSTEM; BLU-ICE; DCS; SIBYLS; GUI</dc:subject>
    <dc:description>Biological small-angle X-ray scattering (SAXS) provides powerful complementary data for macromolecular crystallography (MX) by defining shape, conformation and assembly in solution. Although SAXS is in principle the highest throughput technique for structural biology, data collection is limited in practice by current data collection software. Here the adaption of beamline control software, historically developed for MX beamlines, for the efficient operation and high-throughput data collection at synchrotron SAXS beamlines is reported. The Blu-Ice GUI and Distributed Control System (DCS) developed in the Macromolecular Crystallography Group at the Stanford Synchrotron Radiation Laboratory has been optimized, extended and enhanced to suit the specific needs of the biological SAXS endstation at the SIBYLS beamline at the Advanced Light Source. The customizations reported here provide a potential route for other SAXS beamlines in need of robust and efficient beamline control software. As a great deal of effort and optimization has gone into crystallographic software, the adaption and extension of crystallographic software may prove to be a general strategy to provide advanced SAXS software for the synchrotron community. In this way effort can be put into optimizing features for SAXS rather than reproducing those that have already been successfully implemented for the crystallographic community.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Software for the high-throughput collection of SAXS data using an enhanced Blu-Ice/DCS control system</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-11-01</prism:publicationDate>
    <prism:startingPage>774</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>781</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5044">
    <title>Structure analysis of group I plant nucleases</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5044</link>
    <description>Anticancer drugs attacking nucleic acids of the target cells have so far been based on animal or fungal ribonucleases. Plant nucleases have been proved to exhibit decreased cytotoxic side effects. Tomato bifunctional nuclease 1 with activity against both single-stranded and double-stranded RNA and DNA was produced in tobacco leaves as recombinant protein. The enzyme crystallizes under several different crystallization conditions. The presence of Zn2+ ions was confirmed by X-ray fluorescence. First crystallographic data were obtained.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Dohnálek, J.</dc:creator>
    <dc:creator>Koval', T.</dc:creator>
    <dc:creator>Lipovová, P.</dc:creator>
    <dc:creator>Podzimek, T.</dc:creator>
    <dc:creator>Matoušek, J.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510030700</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Structural properties of plant nuclease TBN1 are studied using synchrotron radiation to explain its specificity, role of glycosylation and to contribute to potential application in cancer treatment.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>NUCLEASE; PROTEIN STRUCTURE; CRYSTAL STRUCTURE; GLYCOSYLATION; ANTICANCER DRUGS</dc:subject>
    <dc:description>Anticancer drugs attacking nucleic acids of the target cells have so far been based on animal or fungal ribonucleases. Plant nucleases have been proved to exhibit decreased cytotoxic side effects. Tomato bifunctional nuclease 1 with activity against both single-stranded and double-stranded RNA and DNA was produced in tobacco leaves as recombinant protein. The enzyme crystallizes under several different crystallization conditions. The presence of Zn2+ ions was confirmed by X-ray fluorescence. First crystallographic data were obtained.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structure analysis of group I plant nucleases</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>29</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>30</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5056">
    <title>The alternating access mechanism of transport as observed in the sodium-hydantoin transporter Mhp1</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5056</link>
    <description>Secondary active transporters move molecules across cell membranes by coupling this process to the energetically favourable downhill movement of ions or protons along an electrochemical gradient. They function by the alternating access model of transport in which, through conformational changes, the substrate binding site alternately faces either side of the membrane. Owing to the difficulties in obtaining the crystal structure of a single transporter in different conformational states, relatively little structural information is known to explain how this process occurs. Here, the structure of the sodium-benzylhydantoin transporter, Mhp1, from Microbacterium liquefaciens, has been determined in three conformational states; from this a mechanism is proposed for switching from the outward-facing open conformation through an occluded structure to the inward-facing open state.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Weyand, S.</dc:creator>
    <dc:creator>Shimamura, T.</dc:creator>
    <dc:creator>Beckstein, O.</dc:creator>
    <dc:creator>Sansom, M.S.P.</dc:creator>
    <dc:creator>Iwata, S.</dc:creator>
    <dc:creator>Henderson, P.J.F.</dc:creator>
    <dc:creator>Cameron, A.D.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510032449</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Crystal structures of a membrane protein transporter in three different conformational states provide insights into the transport mechanism.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MEMBRANE TRANSPORT; TRANSPORT PROTEIN; ALTERNATING ACCESS; HYDANTOINS</dc:subject>
    <dc:description>Secondary active transporters move molecules across cell membranes by coupling this process to the energetically favourable downhill movement of ions or protons along an electrochemical gradient. They function by the alternating access model of transport in which, through conformational changes, the substrate binding site alternately faces either side of the membrane. Owing to the difficulties in obtaining the crystal structure of a single transporter in different conformational states, relatively little structural information is known to explain how this process occurs. Here, the structure of the sodium-benzylhydantoin transporter, Mhp1, from Microbacterium liquefaciens, has been determined in three conformational states; from this a mechanism is proposed for switching from the outward-facing open conformation through an occluded structure to the inward-facing open state.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The alternating access mechanism of transport as observed in the sodium-hydantoin transporter Mhp1</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>20</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>23</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5048">
    <title>Research and development of an electron beam focusing system for a high-brightness X-ray generator</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5048</link>
    <description>A new type of rotating anticathode X-ray generator, where an electron beam of up to 60 keV irradiates the inner surface of a U-shaped Cu anticathode, has achieved a beam brilliance of 130 kW mm−2 (at 2.3 kW). A higher-flux electron beam is expected from simulation by optimizing the geometry of a combined-function-type magnet instead of the fringing field of the bending magnet. In order to minimize the size of the X-ray source the electron beam has been focused over a short distance by a new combined-function bending magnet, whose geometrical shape was determined by simulation using the Opera-3D, General Particle Tracer and CST-STUDIO codes. The result of the simulation clearly shows that the role of combined functions in both the bending and the steering magnets is important for focusing the beam to a small size. FWHM sizes of the beam are predicted by simulation to be 0.45 mm (horizontal) and 0.05 mm (vertical) for a 120 keV/75 mA beam, of which the effective brilliance is about 500 kW mm−2 on the supposition of a two-dimensional Gaussian distribution. High-power tests have begun using a high-voltage 120 kV/75 mA power supply for the X-ray generator instead of 60 kV/100 mA. The beam focus size on the target will be verified in the experiments.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sakai, T.</dc:creator>
    <dc:creator>Ohsawa, S.</dc:creator>
    <dc:creator>Sakabe, N.</dc:creator>
    <dc:creator>Sugimura, T.</dc:creator>
    <dc:creator>Ikeda, M.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510029948</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>In order to minimize the size of the X-ray source for a U-shaped rotating anticathode X-ray generator, the electron beam is focused over a short distance by a combined-function bending magnet. Simulation predicts that the beam brightness will reach almost 500 kW mm−2 for a 120 keV/75 mA beam.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY GENERATOR; HIGH-FLUX ELECTRON BEAM; DC ELECTRON GUN; COMBINED-FUNCTION BENDING MAGNET</dc:subject>
    <dc:description>A new type of rotating anticathode X-ray generator, where an electron beam of up to 60 keV irradiates the inner surface of a U-shaped Cu anticathode, has achieved a beam brilliance of 130 kW mm−2 (at 2.3 kW). A higher-flux electron beam is expected from simulation by optimizing the geometry of a combined-function-type magnet instead of the fringing field of the bending magnet. In order to minimize the size of the X-ray source the electron beam has been focused over a short distance by a new combined-function bending magnet, whose geometrical shape was determined by simulation using the Opera-3D, General Particle Tracer and CST-STUDIO codes. The result of the simulation clearly shows that the role of combined functions in both the bending and the steering magnets is important for focusing the beam to a small size. FWHM sizes of the beam are predicted by simulation to be 0.45 mm (horizontal) and 0.05 mm (vertical) for a 120 keV/75 mA beam, of which the effective brilliance is about 500 kW mm−2 on the supposition of a two-dimensional Gaussian distribution. High-power tests have begun using a high-voltage 120 kV/75 mA power supply for the X-ray generator instead of 60 kV/100 mA. The beam focus size on the target will be verified in the experiments.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Research and development of an electron beam focusing system for a high-brightness X-ray generator</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>53</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>57</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5042">
    <title>Crystal structure of stable protein CutA1 from psychrotrophic bacterium Shewanella sp. SIB1</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5042</link>
    <description>CutA1 is widely found in bacteria, plants and animals, including humans. The functions of CutA1, however, have not been well clarified. It is known that CutA1s from Pyrococcus horikoshii, Thermus thermophilus and Oryza sativa unfold at temperatures remarkably higher than the growth temperatures of the host organisms. In this work the crystal structure of CutA1 from the psychrotrophic bacterium Shewanella sp. SIB1 (SIB1–CutA1) in a trimeric form was determined at 2.7 Å resolution. This is the first crystal structure of a psychrotrophic CutA1. The overall structure of SIB1–CutA1 is similar to those of CutA1 from Homo sapiens, Escherichia coli, Pyrococcus horikoshii, Thermus thermophilus, Termotoga maritima, Oryza sativa and Rattus norvergicus. A peculiarity is observed in the β2 strand. The β2 strand is divided into two short β strands, β2a and β2b, in SIB1–CutA1. A thermal denaturation experiment revealed that SIB1–CutA1 does not unfold completely at 363 K at pH 7.0, although Shewanella sp. SIB1 cannot grow at temperatures exceeding 303 K. These results indicate that the trimeric structural motif of CutA1 is the critical factor in its unusually high stability and suggest that CutA1 needs to maintain its high stability in order to function, even in psychrotrophs.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sato, A.</dc:creator>
    <dc:creator>Yokotani, S.</dc:creator>
    <dc:creator>Tadokoro, T.</dc:creator>
    <dc:creator>Tanaka, S.</dc:creator>
    <dc:creator>Angkawidjaja, C.</dc:creator>
    <dc:creator>Koga, Y.</dc:creator>
    <dc:creator>Takano, K.</dc:creator>
    <dc:creator>Kanaya, S.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510028669</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The crystal structure of CutA1 from the psychrotrophic bacterium Shewanella sp. SIB1 in a trimeric form was determined at 2.7 Å resolution. This is the first crystal structure of a psychrotrophic CutA1.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CUTA1; SHEWANELLA SP. SIB1; CRYSTAL STRUCTURE; THERMAL DENATURATION; TRIMERIC STRUCTURAL MOTIF</dc:subject>
    <dc:description>CutA1 is widely found in bacteria, plants and animals, including humans. The functions of CutA1, however, have not been well clarified. It is known that CutA1s from Pyrococcus horikoshii, Thermus thermophilus and Oryza sativa unfold at temperatures remarkably higher than the growth temperatures of the host organisms. In this work the crystal structure of CutA1 from the psychrotrophic bacterium Shewanella sp. SIB1 (SIB1–CutA1) in a trimeric form was determined at 2.7 Å resolution. This is the first crystal structure of a psychrotrophic CutA1. The overall structure of SIB1–CutA1 is similar to those of CutA1 from Homo sapiens, Escherichia coli, Pyrococcus horikoshii, Thermus thermophilus, Termotoga maritima, Oryza sativa and Rattus norvergicus. A peculiarity is observed in the β2 strand. The β2 strand is divided into two short β strands, β2a and β2b, in SIB1–CutA1. A thermal denaturation experiment revealed that SIB1–CutA1 does not unfold completely at 363 K at pH 7.0, although Shewanella sp. SIB1 cannot grow at temperatures exceeding 303 K. These results indicate that the trimeric structural motif of CutA1 is the critical factor in its unusually high stability and suggest that CutA1 needs to maintain its high stability in order to function, even in psychrotrophs.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Crystal structure of stable protein CutA1 from psychrotrophic bacterium Shewanella sp. SIB1</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>6</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>10</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5043">
    <title>UV LED lighting for automated crystal centring</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5043</link>
    <description>A direct outcome of the exponential growth of macromolecular crystallography is the continuously increasing demand for synchrotron beam time, both from academic and industrial users. As more and more projects entail screening a profusion of sample crystals, fully automated procedures at every level of the experiments are being implemented at all synchrotron facilities. One of the major obstacles to achieving such automation lies in the sample recognition and centring in the X-ray beam. The capacity of UV light to specifically react with aromatic residues present in proteins or with DNA base pairs is at the basis of UV-assisted crystal centring. Although very efficient, a well known side effect of illuminating biological samples with strong UV sources is the damage induced on the irradiated samples. In the present study the effectiveness of a softer UV light for crystal centring by taking advantage of low-power light-emitting diode (LED) sources has been investigated. The use of UV LEDs represents a low-cost solution for crystal centring with high specificity.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Chavas, L.M.G.</dc:creator>
    <dc:creator>Yamada, Y.</dc:creator>
    <dc:creator>Hiraki, M.</dc:creator>
    <dc:creator>Igarashi, N.</dc:creator>
    <dc:creator>Matsugaki, N.</dc:creator>
    <dc:creator>Wakatsuki, S.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510028670</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A low-cost light-emitting diode (LED) UV source has been developed for facilitating macromolecular sample centring in the X-ray beam.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>UV LIGHT; LED; MACROMOLECULAR CRYSTALLOGRAPHY; AUTOMATION; HIGH THROUGHPUT; CRYSTAL CENTRING</dc:subject>
    <dc:description>A direct outcome of the exponential growth of macromolecular crystallography is the continuously increasing demand for synchrotron beam time, both from academic and industrial users. As more and more projects entail screening a profusion of sample crystals, fully automated procedures at every level of the experiments are being implemented at all synchrotron facilities. One of the major obstacles to achieving such automation lies in the sample recognition and centring in the X-ray beam. The capacity of UV light to specifically react with aromatic residues present in proteins or with DNA base pairs is at the basis of UV-assisted crystal centring. Although very efficient, a well known side effect of illuminating biological samples with strong UV sources is the damage induced on the irradiated samples. In the present study the effectiveness of a softer UV light for crystal centring by taking advantage of low-power light-emitting diode (LED) sources has been investigated. The use of UV LEDs represents a low-cost solution for crystal centring with high specificity.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>UV LED lighting for automated crystal centring</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>11</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>15</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5005">
    <title>Beam-induced damage on diffractive hard X-ray optics</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5005</link>
    <description>The issue of beam-induced damage on diffractive hard X-ray optics is addressed. For this purpose a systematic study on the radiation damage induced by a high-power X-ray beam is carried out in both ambient and inert atmospheres. Diffraction gratings fabricated by three different techniques are considered: electroplated Au gratings both with and without the polymer mold, and Ir-coated Si gratings. The beam-induced damage is monitored by X-ray diffraction and evaluated using scanning electron microscopy.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Nygård, K.</dc:creator>
    <dc:creator>Gorelick, S.</dc:creator>
    <dc:creator>Vila-Comamala, J.</dc:creator>
    <dc:creator>Färm, E.</dc:creator>
    <dc:creator>Bergamaschi, A.</dc:creator>
    <dc:creator>Cervellino, A.</dc:creator>
    <dc:creator>Gozzo, F.</dc:creator>
    <dc:creator>Patterson, B.D.</dc:creator>
    <dc:creator>Ritala, M.</dc:creator>
    <dc:creator>David, C.</dc:creator>
    <dc:date>2010-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510028487</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Beam-induced damage on diffractive hard X-ray optics is studied by means of X-ray diffraction and scanning electron microscopy.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DIFFRACTIVE X-RAY OPTICS; RADIATION DAMAGE</dc:subject>
    <dc:description>The issue of beam-induced damage on diffractive hard X-ray optics is addressed. For this purpose a systematic study on the radiation damage induced by a high-power X-ray beam is carried out in both ambient and inert atmospheres. Diffraction gratings fabricated by three different techniques are considered: electroplated Au gratings both with and without the polymer mold, and Ir-coated Si gratings. The beam-induced damage is monitored by X-ray diffraction and evaluated using scanning electron microscopy.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Beam-induced damage on diffractive hard X-ray optics</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-11-01</prism:publicationDate>
    <prism:startingPage>786</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>790</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ms5027">
    <title>A new technique to examine individual pollutant particle and fibre deposition and transit behaviour in live mouse trachea</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ms5027</link>
    <description>During respiration, particles suspended in the air are inhaled and unless cleared by airway defences they can remain and affect lung health. Their size precludes the use of standard imaging modalities so we have developed synchrotron phase-contrast X-ray imaging (PCXI) methods to non-invasively monitor the behaviour of individual particles in live mouse airways. In this study we used these techniques to examine post-deposition particle behaviour in the trachea. PCXI was used to monitor the deposition and subsequent behaviour of particles of quarry dust and lead ore; fibres of asbestos and fibreglass; and hollow glass micro-spheres. Visibility was examined in vitro and ex vivo to avoid the complicating effects of surrounding tissue and respiratory or cardiac motion. Particle behaviour was then examined after deposition onto the tracheal airway surfaces of live mice. Each particle and fibre looked and behaved differently on the airway surface. Particles lodged on the airway shortly after deposition, and the rate at which this occurred was dependent on the particle type and size. After the live-imaging experiments, excised airway samples were examined using light and electron microscopy. Evidence of particle capture into the airway surface fluids and the epithelial cell layer was found. PCXI is a valuable tool for examining post-deposition particulate behaviour in the tracheal airway. These first indications that the interaction between airways and individual particles may depend on the particle type and size should provide a novel approach to studying the early effects of respired particles on airway health.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Donnelley, M.</dc:creator>
    <dc:creator>Siu, K.K.W.</dc:creator>
    <dc:creator>Morgan, K.S.</dc:creator>
    <dc:creator>Skinner, W.</dc:creator>
    <dc:creator>Suzuki, Y.</dc:creator>
    <dc:creator>Takeuchi, A.</dc:creator>
    <dc:creator>Uesugi, K.</dc:creator>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:creator>Parsons, D.W.</dc:creator>
    <dc:date>2010-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510028451</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>This experiment established synchrotron phase-contrast X-ray imaging techniques to non-invasively examine pollutant particulate deposition and mucociliary transit in live mouse trachea. In this report the behaviour of individual particles of quarry dust, fibreglass, lead ore and reference hollow silver-coated glass beads was examined in live and intact animals.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PARTICLES; POLLUTION; AIRWAY SURFACE; LUNG; TRACHEA; MUCOCILIARY TRANSIT; NON-INVASIVE; X-RAY IMAGING; MOUSE</dc:subject>
    <dc:description>During respiration, particles suspended in the air are inhaled and unless cleared by airway defences they can remain and affect lung health. Their size precludes the use of standard imaging modalities so we have developed synchrotron phase-contrast X-ray imaging (PCXI) methods to non-invasively monitor the behaviour of individual particles in live mouse airways. In this study we used these techniques to examine post-deposition particle behaviour in the trachea. PCXI was used to monitor the deposition and subsequent behaviour of particles of quarry dust and lead ore; fibres of asbestos and fibreglass; and hollow glass micro-spheres. Visibility was examined in vitro and ex vivo to avoid the complicating effects of surrounding tissue and respiratory or cardiac motion. Particle behaviour was then examined after deposition onto the tracheal airway surfaces of live mice. Each particle and fibre looked and behaved differently on the airway surface. Particles lodged on the airway shortly after deposition, and the rate at which this occurred was dependent on the particle type and size. After the live-imaging experiments, excised airway samples were examined using light and electron microscopy. Evidence of particle capture into the airway surface fluids and the epithelial cell layer was found. PCXI is a valuable tool for examining post-deposition particulate behaviour in the tracheal airway. These first indications that the interaction between airways and individual particles may depend on the particle type and size should provide a novel approach to studying the early effects of respired particles on airway health.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A new technique to examine individual pollutant particle and fibre deposition and transit behaviour in live mouse trachea</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-11-01</prism:publicationDate>
    <prism:startingPage>719</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>729</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ms5024">
    <title>Raster microdiffraction with synchrotron radiation of hydrated biopolymers with nanometre step-resolution: case study of starch granules</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ms5024</link>
    <description>X-ray radiation damage propagation is explored for hydrated starch granules in order to reduce the step resolution in raster-microdiffraction experiments to the nanometre range. Radiation damage was induced by synchrotron radiation microbeams of 5, 1 and 0.3 µm size with ∼0.1 nm wavelength in B-type potato, Canna edulis and Phajus grandifolius starch granules. A total loss of crystallinity of granules immersed in water was found at a dose of ∼1.3 photons nm−3. The temperature dependence of radiation damage suggests that primary radiation damage prevails up to about 120 K while secondary radiation damage becomes effective at higher temperatures. Primary radiation damage remains confined to the beam track at 100 K. Propagation of radiation damage beyond the beam track at room temperature is assumed to be due to reactive species generated principally by water radiolysis induced by photoelectrons. By careful dose selection during data collection, raster scans with 500 nm step-resolution could be performed for granules immersed in water.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Riekel, C.</dc:creator>
    <dc:creator>Burghammer, M.</dc:creator>
    <dc:creator>Davies, R.J.</dc:creator>
    <dc:creator>Di Cola, E.</dc:creator>
    <dc:creator>König, C.</dc:creator>
    <dc:creator>Lemke, H.T.</dc:creator>
    <dc:creator>Putaux, J.-L.</dc:creator>
    <dc:creator>Schöder, S.</dc:creator>
    <dc:date>2010-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510028335</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Radiation damage propagation was examined in starch granules by synchrotron radiation micro- and nano-diffraction techniques from cryo- to room temperatures. Careful dose limitation allowed raster-diffraction experiments with 500 nm step resolution to be performed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>BIOPOLYMERS; NANOMETRE RASTER-DIFFRACTION; RADIATION DAMAGE; STARCH GRANULES</dc:subject>
    <dc:description>X-ray radiation damage propagation is explored for hydrated starch granules in order to reduce the step resolution in raster-microdiffraction experiments to the nanometre range. Radiation damage was induced by synchrotron radiation microbeams of 5, 1 and 0.3 µm size with ∼0.1 nm wavelength in B-type potato, Canna edulis and Phajus grandifolius starch granules. A total loss of crystallinity of granules immersed in water was found at a dose of ∼1.3 photons nm−3. The temperature dependence of radiation damage suggests that primary radiation damage prevails up to about 120 K while secondary radiation damage becomes effective at higher temperatures. Primary radiation damage remains confined to the beam track at 100 K. Propagation of radiation damage beyond the beam track at room temperature is assumed to be due to reactive species generated principally by water radiolysis induced by photoelectrons. By careful dose selection during data collection, raster scans with 500 nm step-resolution could be performed for granules immersed in water.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Raster microdiffraction with synchrotron radiation of hydrated biopolymers with nanometre step-resolution: case study of starch granules</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-11-01</prism:publicationDate>
    <prism:startingPage>743</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>750</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5041">
    <title>Crystallization and preliminary structural analysis of the giant haemoglobin from Glossoscolex paulistus at 3.2 Å</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5041</link>
    <description>Glossoscolex paulistus is a free-living earthworm encountered in south-east Brazil. Its oxygen transport requirements are undertaken by a giant extracellular haemoglobin, or erythrocruorin (HbGp), which has an approximate molecular mass of 3.6 MDa and, by analogy with its homologue from Lumbricus terrestris (HbLt), is believed to be composed of a total of 180 polypeptide chains. In the present work the full 3.6 MDa particle in its cyanomet state was purified and crystallized using sodium citrate or PEG8000 as precipitant. The crystals contain one-quarter of the full particle in the asymmetric unit of the I222 cell and have parameters of a = 270.8 Å, b = 320.3 Å and c = 332.4 Å. Diffraction data were collected to 3.15 Å using synchrotron radiation on beamline X29A at the Brookhaven National Laboratory and represent the highest resolution data described to date for similar erythrocruorins. The structure was solved by molecular replacement using a search model corresponding to one-twelfth of its homologue from HbLt. This revealed that HbGp belongs to the type I class of erythrocruorins and provided an interpretable initial electron density map in which many features including the haem groups and disulfide bonds could be identified.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Bachega, J.F.R.</dc:creator>
    <dc:creator>Bleicher, L.</dc:creator>
    <dc:creator>Horjales, E.R.</dc:creator>
    <dc:creator>Santiago, P.S.</dc:creator>
    <dc:creator>Garratt, R.C.</dc:creator>
    <dc:creator>Tabak, M.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S090904951002772X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Diffraction data to 3.2 Å from crystals of the 3.6 MDa erythrocruorin from a Brazilian earthworm represent the highest resolution reported to date for similar complexes. An unambiguous molecular replacement solution shows the particle to belong to the type I class.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HAEMOGLOBIN; ERYTHROCRUORIN; CRYSTALLIZATION; EARTHWORM</dc:subject>
    <dc:description>Glossoscolex paulistus is a free-living earthworm encountered in south-east Brazil. Its oxygen transport requirements are undertaken by a giant extracellular haemoglobin, or erythrocruorin (HbGp), which has an approximate molecular mass of 3.6 MDa and, by analogy with its homologue from Lumbricus terrestris (HbLt), is believed to be composed of a total of 180 polypeptide chains. In the present work the full 3.6 MDa particle in its cyanomet state was purified and crystallized using sodium citrate or PEG8000 as precipitant. The crystals contain one-quarter of the full particle in the asymmetric unit of the I222 cell and have parameters of a = 270.8 Å, b = 320.3 Å and c = 332.4 Å. Diffraction data were collected to 3.15 Å using synchrotron radiation on beamline X29A at the Brookhaven National Laboratory and represent the highest resolution data described to date for similar erythrocruorins. The structure was solved by molecular replacement using a search model corresponding to one-twelfth of its homologue from HbLt. This revealed that HbGp belongs to the type I class of erythrocruorins and provided an interpretable initial electron density map in which many features including the haem groups and disulfide bonds could be identified.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Crystallization and preliminary structural analysis of the giant haemoglobin from Glossoscolex paulistus at 3.2 Å</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>24</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>28</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5040">
    <title>Purine nucleoside phosphorylase from Schistosoma mansoni in complex with ribose-1-phosphate</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5040</link>
    <description>Schistosomes are blood flukes which cause schistosomiasis, a disease affecting approximately 200 million people worldwide. Along with several other important human parasites including trypanosomes and Plasmodium, schistosomes lack the de novo pathway for purine synthesis and depend exclusively on the salvage pathway for their purine requirements, making the latter an attractive target for drug development. Part of the pathway involves the conversion of inosine (or guanosine) into hypoxanthine (or guanine) together with ribose-1-phosphate (R1P) or vice versa. This inter-conversion is undertaken by the enzyme purine nucleoside phosphorylase (PNP) which has been used as the basis for the development of novel anti-malarials, conceptually validating this approach. It has been suggested that, during the reverse reaction, R1P binding to the enzyme would occur only as a consequence of conformational changes induced by hypoxanthine, thus making a binary PNP–R1P complex unlikely. Contradictory to this statement, a crystal structure of just such a binary complex involving the Schistosoma mansoni enzyme has been successfully obtained. The ligand shows an intricate hydrogen-bonding network in the phosphate and ribose binding sites and adds a further chapter to our knowledge which could be of value in the future development of selective inhibitors.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>D'Muniz Pereira, H.</dc:creator>
    <dc:creator>Oliva, G.</dc:creator>
    <dc:creator>Garratt, R.C.</dc:creator>
    <dc:date>2011-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510027718</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A binary complex between a low-molecular-weight purine nucleoside phosphorylase and ribose-1-phosphate is described for the first time and comparisons with known ternary complexes are drawn.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SCHISTOSOMIASIS; PURINE NUCLEOSIDE PHOSPHORYLASE; RIBOSE-1-PHOSPHATE</dc:subject>
    <dc:description>Schistosomes are blood flukes which cause schistosomiasis, a disease affecting approximately 200 million people worldwide. Along with several other important human parasites including trypanosomes and Plasmodium, schistosomes lack the de novo pathway for purine synthesis and depend exclusively on the salvage pathway for their purine requirements, making the latter an attractive target for drug development. Part of the pathway involves the conversion of inosine (or guanosine) into hypoxanthine (or guanine) together with ribose-1-phosphate (R1P) or vice versa. This inter-conversion is undertaken by the enzyme purine nucleoside phosphorylase (PNP) which has been used as the basis for the development of novel anti-malarials, conceptually validating this approach. It has been suggested that, during the reverse reaction, R1P binding to the enzyme would occur only as a consequence of conformational changes induced by hypoxanthine, thus making a binary PNP–R1P complex unlikely. Contradictory to this statement, a crystal structure of just such a binary complex involving the Schistosoma mansoni enzyme has been successfully obtained. The ligand shows an intricate hydrogen-bonding network in the phosphate and ribose binding sites and adds a further chapter to our knowledge which could be of value in the future development of selective inhibitors.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Purine nucleoside phosphorylase from Schistosoma mansoni in complex with ribose-1-phosphate</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>18</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2011-01-01</prism:publicationDate>
    <prism:startingPage>62</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>65</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?gf5028">
    <title>The MYTHEN detector for X-ray powder diffraction experiments at the Swiss Light Source</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?gf5028</link>
    <description>The MYTHEN single-photon-counting silicon microstrip detector has been developed at the Swiss Light Source for time-resolved powder diffraction experiments. An upgraded version of the detector has been installed at the SLS powder diffraction station allowing the acquisition of diffraction patterns over 120° in 2θ in fractions of seconds. Thanks to the outstanding performance of the detector and to the calibration procedures developed, the quality of the data obtained is now comparable with that of traditional high-resolution point detectors in terms of FWHM resolution and peak profile shape, with the additional advantage of fast and simultaneous acquisition of the full diffraction pattern. MYTHEN is therefore optimal for time-resolved or dose-critical measurements. The characteristics of the MYTHEN detector together with the calibration procedures implemented for the optimization of the data are described in detail. The refinements of two known standard powders are discussed together with a remarkable application of MYTHEN to organic compounds in relation to the problem of radiation damage.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Bergamaschi, A.</dc:creator>
    <dc:creator>Cervellino, A.</dc:creator>
    <dc:creator>Dinapoli, R.</dc:creator>
    <dc:creator>Gozzo, F.</dc:creator>
    <dc:creator>Henrich, B.</dc:creator>
    <dc:creator>Johnson, I.</dc:creator>
    <dc:creator>Kraft, P.</dc:creator>
    <dc:creator>Mozzanica, A.</dc:creator>
    <dc:creator>Schmitt, B.</dc:creator>
    <dc:creator>Shi, X.</dc:creator>
    <dc:date>2010-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510026051</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A report on the characterization, calibration and performances of the MYTHEN photon-counting silicon microstrip detector at the powder diffraction station at the Swiss Light Source is given.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DETECTORS; POWDER DIFFRACTION</dc:subject>
    <dc:description>The MYTHEN single-photon-counting silicon microstrip detector has been developed at the Swiss Light Source for time-resolved powder diffraction experiments. An upgraded version of the detector has been installed at the SLS powder diffraction station allowing the acquisition of diffraction patterns over 120° in 2θ in fractions of seconds. Thanks to the outstanding performance of the detector and to the calibration procedures developed, the quality of the data obtained is now comparable with that of traditional high-resolution point detectors in terms of FWHM resolution and peak profile shape, with the additional advantage of fast and simultaneous acquisition of the full diffraction pattern. MYTHEN is therefore optimal for time-resolved or dose-critical measurements. The characteristics of the MYTHEN detector together with the calibration procedures implemented for the optimization of the data are described in detail. The refinements of two known standard powders are discussed together with a remarkable application of MYTHEN to organic compounds in relation to the problem of radiation damage.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The MYTHEN detector for X-ray powder diffraction experiments at the Swiss Light Source</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-09-01</prism:publicationDate>
    <prism:startingPage>653</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>668</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5041">
    <title>The role of single element errors in planar parabolic compound refractive lenses</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5041</link>
    <description>The propagation of X-rays through a compound refractive lens (CRL) with imperfect CRL elements is investigated. The trajectories of random rays within the geometrical optics regime are calculated in one plane using Monte Carlo methods. Three different lenses were simulated: Be, Al and Ni lenses designed for photon energies of 20 keV, 60 keV and 175 keV, respectively. The results show that while transverse displacements of single elements in a CRL do not influence imaging resolution, rotational errors can be important. Systematic calculations of aberrations owing to the deviation of the element's surface from a perfect parabolic shape are also presented.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Andrejczuk, A.</dc:creator>
    <dc:creator>Krzywiński, J.</dc:creator>
    <dc:creator>Sakurai, Y.</dc:creator>
    <dc:creator>Itou, M.</dc:creator>
    <dc:date>2010-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510022454</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>It is shown how the misalignment of conical surface axes of single lenses in a compound refractive lens array can influence the focusing resolution.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COMPOUND REFRACTIVE LENS; X-RAY OPTICS; ERRORS IN THE LENS; RAY-TRACING</dc:subject>
    <dc:description>The propagation of X-rays through a compound refractive lens (CRL) with imperfect CRL elements is investigated. The trajectories of random rays within the geometrical optics regime are calculated in one plane using Monte Carlo methods. Three different lenses were simulated: Be, Al and Ni lenses designed for photon energies of 20 keV, 60 keV and 175 keV, respectively. The results show that while transverse displacements of single elements in a CRL do not influence imaging resolution, rotational errors can be important. Systematic calculations of aberrations owing to the deviation of the element's surface from a perfect parabolic shape are also presented.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The role of single element errors in planar parabolic compound refractive lenses</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-09-01</prism:publicationDate>
    <prism:startingPage>616</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>623</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0421">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0421</link>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2010-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510022296</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-07-01</prism:publicationDate>
    <prism:startingPage>567</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>568</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?bf5031">
    <title>MxCuBE: a synchrotron beamline control environment customized for macromolecular crystallography experiments</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?bf5031</link>
    <description>The design and features of a beamline control software system for macromolecular crystallography (MX) experiments developed at the European Synchrotron Radiation Facility (ESRF) are described. This system, MxCuBE, allows users to easily and simply interact with beamline hardware components and provides automated routines for common tasks in the operation of a synchrotron beamline dedicated to experiments in MX. Additional functionality is provided through intuitive interfaces that enable the assessment of the diffraction characteristics of samples, experiment planning, automatic data collection and the on-line collection and analysis of X-ray emission spectra. The software can be run in a tandem client-server mode that allows for remote control and relevant experimental parameters and results are automatically logged in a relational database, ISPyB. MxCuBE is modular, flexible and extensible and is currently deployed on eight macromolecular crystallography beamlines at the ESRF. Additionally, the software is installed at MAX-lab beamline I911-3 and at BESSY beamline BL14.1.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Gabadinho, J.</dc:creator>
    <dc:creator>Beteva, A.</dc:creator>
    <dc:creator>Guijarro, M.</dc:creator>
    <dc:creator>Rey-Bakaikoa, V.</dc:creator>
    <dc:creator>Spruce, D.</dc:creator>
    <dc:creator>Bowler, M.W.</dc:creator>
    <dc:creator>Brockhauser, S.</dc:creator>
    <dc:creator>Flot, D.</dc:creator>
    <dc:creator>Gordon, E.J.</dc:creator>
    <dc:creator>Hall, D.R.</dc:creator>
    <dc:creator>Lavault, B.</dc:creator>
    <dc:creator>McCarthy, A.A.</dc:creator>
    <dc:creator>McCarthy, J.</dc:creator>
    <dc:creator>Mitchell, E.</dc:creator>
    <dc:creator>Monaco, S.</dc:creator>
    <dc:creator>Mueller-Dieckmann, C.</dc:creator>
    <dc:creator>Nurizzo, D.</dc:creator>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:creator>Thibault, X.</dc:creator>
    <dc:creator>Walsh, M.A.</dc:creator>
    <dc:creator>Leonard, G.A.</dc:creator>
    <dc:creator>McSweeney, S.M.</dc:creator>
    <dc:date>2010-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510020005</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>MxCuBE is a beamline control environment optimized for the needs of macromolecular crystallography. This paper describes the design of the software and the features that MxCuBE currently provides.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AUTOMATION; MACROMOLECULAR CRYSTALLOGRAPHY; SYNCHROTRON BEAMLINE CONTROL; GRAPHICAL USER INTERFACE</dc:subject>
    <dc:description>The design and features of a beamline control software system for macromolecular crystallography (MX) experiments developed at the European Synchrotron Radiation Facility (ESRF) are described. This system, MxCuBE, allows users to easily and simply interact with beamline hardware components and provides automated routines for common tasks in the operation of a synchrotron beamline dedicated to experiments in MX. Additional functionality is provided through intuitive interfaces that enable the assessment of the diffraction characteristics of samples, experiment planning, automatic data collection and the on-line collection and analysis of X-ray emission spectra. The software can be run in a tandem client-server mode that allows for remote control and relevant experimental parameters and results are automatically logged in a relational database, ISPyB. MxCuBE is modular, flexible and extensible and is currently deployed on eight macromolecular crystallography beamlines at the ESRF. Additionally, the software is installed at MAX-lab beamline I911-3 and at BESSY beamline BL14.1.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>MxCuBE: a synchrotron beamline control environment customized for macromolecular crystallography experiments</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-09-01</prism:publicationDate>
    <prism:startingPage>700</prism:startingPage>
    <prism:section>computer programs</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>707</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?bf5029">
    <title>High-resolution soft X-ray beamline ADRESS at the Swiss Light Source for resonant inelastic X-ray scattering and angle-resolved photoelectron spectroscopies</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?bf5029</link>
    <description>The concepts and technical realisation of the high-resolution soft X-ray beamline ADRESS operating in the energy range from 300 to 1600 eV and intended for resonant inelastic X-ray scattering (RIXS) and angle-resolved photoelectron spectroscopy (ARPES) are described. The photon source is an undulator of novel fixed-gap design where longitudinal movement of permanent magnetic arrays controls not only the light polarization (including circular and 0–180° rotatable linear polarizations) but also the energy without changing the gap. The beamline optics is based on the well established scheme of plane-grating monochromator operating in collimated light. The ultimate resolving power E/ΔE is above 33000 at 1 keV photon energy. The choice of blazed versus lamellar gratings and optimization of their profile parameters is described. Owing to glancing angles on the mirrors as well as optimized groove densities and profiles of the gratings, the beamline is capable of delivering high photon flux up to 1 × 1013 photons s−1 (0.01% BW)−1 at 1 keV. Ellipsoidal refocusing optics used for the RIXS endstation demagnifies the vertical spot size down to 4 µm, which allows slitless operation and thus maximal transmission of the high-resolution RIXS spectrometer delivering E/ΔE &gt; 11000 at 1 keV photon energy. Apart from the beamline optics, an overview of the control system is given, the diagnostics and software tools are described, and strategies used for the optical alignment are discussed. An introduction to the concepts and instrumental realisation of the ARPES and RIXS endstations is given.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Strocov, V.N.</dc:creator>
    <dc:creator>Schmitt, T.</dc:creator>
    <dc:creator>Flechsig, U.</dc:creator>
    <dc:creator>Schmidt, T.</dc:creator>
    <dc:creator>Imhof, A.</dc:creator>
    <dc:creator>Chen, Q.</dc:creator>
    <dc:creator>Raabe, J.</dc:creator>
    <dc:creator>Betemps, R.</dc:creator>
    <dc:creator>Zimoch, D.</dc:creator>
    <dc:creator>Krempasky, J.</dc:creator>
    <dc:creator>Wang, X.</dc:creator>
    <dc:creator>Grioni, M.</dc:creator>
    <dc:creator>Piazzalunga, A.</dc:creator>
    <dc:creator>Patthey, L.</dc:creator>
    <dc:date>2010-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510019862</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Concepts and technical realization of the high-resolution soft X-ray beamline ADRESS at the Swiss Light Source are described. Optimization of the optical scheme for high resolution and photon flux as well as diagnostics tools and alignment strategies are discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SWISS LIGHT SOURCE; FIXED-GAP UNDULATOR; SOFT X-RAY BEAMLINE; X-RAY OPTICS; PLANE-GRATING MONOCHROMATOR; GRATING OPTIMIZATION; ELLIPSOIDAL REFOCUSING OPTICS; RESONANT INELASTIC X-RAY SCATTERING; ANGLE-RESOLVED PHOTOELECTRON SPECTROSCOPY</dc:subject>
    <dc:description>The concepts and technical realisation of the high-resolution soft X-ray beamline ADRESS operating in the energy range from 300 to 1600 eV and intended for resonant inelastic X-ray scattering (RIXS) and angle-resolved photoelectron spectroscopy (ARPES) are described. The photon source is an undulator of novel fixed-gap design where longitudinal movement of permanent magnetic arrays controls not only the light polarization (including circular and 0–180° rotatable linear polarizations) but also the energy without changing the gap. The beamline optics is based on the well established scheme of plane-grating monochromator operating in collimated light. The ultimate resolving power E/ΔE is above 33000 at 1 keV photon energy. The choice of blazed versus lamellar gratings and optimization of their profile parameters is described. Owing to glancing angles on the mirrors as well as optimized groove densities and profiles of the gratings, the beamline is capable of delivering high photon flux up to 1 × 1013 photons s−1 (0.01% BW)−1 at 1 keV. Ellipsoidal refocusing optics used for the RIXS endstation demagnifies the vertical spot size down to 4 µm, which allows slitless operation and thus maximal transmission of the high-resolution RIXS spectrometer delivering E/ΔE &gt; 11000 at 1 keV photon energy. Apart from the beamline optics, an overview of the control system is given, the diagnostics and software tools are described, and strategies used for the optical alignment are discussed. An introduction to the concepts and instrumental realisation of the ARPES and RIXS endstations is given.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>High-resolution soft X-ray beamline ADRESS at the Swiss Light Source for resonant inelastic X-ray scattering and angle-resolved photoelectron spectroscopies</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-09-01</prism:publicationDate>
    <prism:startingPage>631</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>643</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pp5004">
    <title>Radiation dose optimized lateral expansion of the field of view in synchrotron radiation X-ray tomographic microscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pp5004</link>
    <description>Volumetric data at micrometer level resolution can be acquired within a few minutes using synchrotron-radiation-based tomographic microscopy. The field of view along the rotation axis of the sample can easily be increased by stacking several tomograms, allowing the investigation of long and thin objects at high resolution. On the contrary, an extension of the field of view in the perpendicular direction is non-trivial. This paper presents an acquisition protocol which increases the field of view of the tomographic dataset perpendicular to its rotation axis. The acquisition protocol can be tuned as a function of the reconstruction quality and scanning time. Since the scanning time is proportional to the radiation dose imparted to the sample, this method can be used to increase the field of view of tomographic microscopy instruments while optimizing the radiation dose for radiation-sensitive samples and keeping the quality of the tomographic dataset on the required level. This approach, dubbed wide-field synchrotron radiation tomographic microscopy, can increase the lateral field of view up to five times. The method has been successfully applied for the three-dimensional imaging of entire rat lung acini with a diameter of 4.1 mm at a voxel size of 1.48 µm.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Haberthür, D.</dc:creator>
    <dc:creator>Hintermüller, C.</dc:creator>
    <dc:creator>Marone, F.</dc:creator>
    <dc:creator>Schittny, J.C.</dc:creator>
    <dc:creator>Stampanoni, M.</dc:creator>
    <dc:date>2010-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510019618</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Increasing the lateral field of view of tomography-based imaging methods greatly increases the acquisition time. This article presents scanning protocols to obtain high-resolution tomographic scans with large lateral field of view at greatly decreased acquisition time and thus reduced radiation dose while resulting in high-quality three-dimensional tomographic datasets.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY IMAGING; COMPUTED TOMOGRAPHY; SYNCHROTRON MICROTOMOGRAPHY; SRXTM; FIELD OF VIEW; RADIATION DOSE; LUNG; LUNG DEVELOPMENT; ALVEOLI; ACINUS</dc:subject>
    <dc:description>Volumetric data at micrometer level resolution can be acquired within a few minutes using synchrotron-radiation-based tomographic microscopy. The field of view along the rotation axis of the sample can easily be increased by stacking several tomograms, allowing the investigation of long and thin objects at high resolution. On the contrary, an extension of the field of view in the perpendicular direction is non-trivial. This paper presents an acquisition protocol which increases the field of view of the tomographic dataset perpendicular to its rotation axis. The acquisition protocol can be tuned as a function of the reconstruction quality and scanning time. Since the scanning time is proportional to the radiation dose imparted to the sample, this method can be used to increase the field of view of tomographic microscopy instruments while optimizing the radiation dose for radiation-sensitive samples and keeping the quality of the tomographic dataset on the required level. This approach, dubbed wide-field synchrotron radiation tomographic microscopy, can increase the lateral field of view up to five times. The method has been successfully applied for the three-dimensional imaging of entire rat lung acini with a diameter of 4.1 mm at a voxel size of 1.48 µm.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Radiation dose optimized lateral expansion of the field of view in synchrotron radiation X-ray tomographic microscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-09-01</prism:publicationDate>
    <prism:startingPage>590</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>599</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5077">
    <title>X-ray reflectivity theory for determining the density profile of a liquid under nanometre confinement</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5077</link>
    <description>An X-ray reflectivity theory on the determination of the density profile of a molecular liquid under nanometre confinement is presented. The confinement geometry acts like an X-ray interferometer, which consists of two opposing atomically flat single-crystal mica membranes with an intervening thin liquid film of variable thickness. The X-rays reflected from the parallel crystal planes (of known structure) and the layered liquid in between them (of unknown structure) interfere with one another, making X-ray reflectivity highly sensitive to the liquid's density profile along the confinement direction. An expression for the reflected intensity as a function of momentum transfer is given. The total structure factor intensity for the liquid-filled confinement device is derived as a sum of contributions from the inner and outer crystal terminations. The method presented readily distinguishes the confined liquid from the liquid adsorbed on the outer mica surfaces. It is illustrated for the molecular liquid tetrakis(trimethyl)siloxysilane, confined by two mica surfaces at a distance of 8.6 nm.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Perret, E.</dc:creator>
    <dc:creator>Nygård, K.</dc:creator>
    <dc:creator>Satapathy, D.K.</dc:creator>
    <dc:creator>Balmer, T.E.</dc:creator>
    <dc:creator>Bunk, O.</dc:creator>
    <dc:creator>Heuberger, M.</dc:creator>
    <dc:creator>van der Veen, J.F.</dc:creator>
    <dc:date>2010-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510014858</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The determination of out-of-plane density profiles of a confined molecular liquid by synchrotron X-ray reflectivity is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY REFLECTIVITY; CONFINED FLUIDS</dc:subject>
    <dc:description>An X-ray reflectivity theory on the determination of the density profile of a molecular liquid under nanometre confinement is presented. The confinement geometry acts like an X-ray interferometer, which consists of two opposing atomically flat single-crystal mica membranes with an intervening thin liquid film of variable thickness. The X-rays reflected from the parallel crystal planes (of known structure) and the layered liquid in between them (of unknown structure) interfere with one another, making X-ray reflectivity highly sensitive to the liquid's density profile along the confinement direction. An expression for the reflected intensity as a function of momentum transfer is given. The total structure factor intensity for the liquid-filled confinement device is derived as a sum of contributions from the inner and outer crystal terminations. The method presented readily distinguishes the confined liquid from the liquid adsorbed on the outer mica surfaces. It is illustrated for the molecular liquid tetrakis(trimethyl)siloxysilane, confined by two mica surfaces at a distance of 8.6 nm.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray reflectivity theory for determining the density profile of a liquid under nanometre confinement</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-07-01</prism:publicationDate>
    <prism:startingPage>465</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>472</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ia5052">
    <title>Quantification of phosphorus in single cells using synchrotron X-ray fluorescence</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ia5052</link>
    <description>Phosphorus is required for numerous cellular compounds and as a result can serve as a useful proxy for total cell biomass in studies of cell elemental composition. Single-cell analysis by synchrotron X-ray fluorescence (SXRF) enables quantitative and qualitative analyses of cell elemental composition with high elemental sensitivity. Element standards are required to convert measured X-ray fluorescence intensities into element concentrations, but few appropriate standards are available, particularly for the biologically important element P. Empirical P conversion factors derived from other elements contained in certified thin-film standards were used to quantify P in the model diatom Thalassiosira pseudonana, and the measured cell quotas were compared with those measured in bulk by spectrophotometry. The mean cellular P quotas quantified with SXRF for cells on Au, Ni and nylon grids using this approach were not significantly different from each other or from those measured spectrophotometrically. Inter-cell variability typical of cell populations was observed. Additionally, the grid substrates were compared for their suitability to P quantification based on the potential for spectral interferences with P. Nylon grids were found to have the lowest background concentrations and limits of detection for P, while background concentrations in Ni and Au grids were 1.8- and 6.3-fold higher. The advantages and disadvantages of each grid type for elemental analysis of individual phytoplankton cells are discussed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Núñez-Milland, D.R.</dc:creator>
    <dc:creator>Baines, S.B.</dc:creator>
    <dc:creator>Vogt, S.</dc:creator>
    <dc:creator>Twining, B.S.</dc:creator>
    <dc:date>2010-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510014020</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Phosphorus abundance was quantified in individual phytoplankton cells by synchrotron X-ray fluorescence and compared with bulk spectrophotometric measurements to confirm accuracy of quantification. Figures of merit for P quantification on three different types of transmission electron microscopy grids are compared to assess possible interferences.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PHYTOPLANKTON; DIATOM; TEM GRID; SINGLE-CELL ANALYSIS; THALASSIOSIRA PSEUDONANA</dc:subject>
    <dc:description>Phosphorus is required for numerous cellular compounds and as a result can serve as a useful proxy for total cell biomass in studies of cell elemental composition. Single-cell analysis by synchrotron X-ray fluorescence (SXRF) enables quantitative and qualitative analyses of cell elemental composition with high elemental sensitivity. Element standards are required to convert measured X-ray fluorescence intensities into element concentrations, but few appropriate standards are available, particularly for the biologically important element P. Empirical P conversion factors derived from other elements contained in certified thin-film standards were used to quantify P in the model diatom Thalassiosira pseudonana, and the measured cell quotas were compared with those measured in bulk by spectrophotometry. The mean cellular P quotas quantified with SXRF for cells on Au, Ni and nylon grids using this approach were not significantly different from each other or from those measured spectrophotometrically. Inter-cell variability typical of cell populations was observed. Additionally, the grid substrates were compared for their suitability to P quantification based on the potential for spectral interferences with P. Nylon grids were found to have the lowest background concentrations and limits of detection for P, while background concentrations in Ni and Au grids were 1.8- and 6.3-fold higher. The advantages and disadvantages of each grid type for elemental analysis of individual phytoplankton cells are discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Quantification of phosphorus in single cells using synchrotron X-ray fluorescence</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-07-01</prism:publicationDate>
    <prism:startingPage>560</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>566</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0420">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0420</link>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2010-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510013476</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-05-01</prism:publicationDate>
    <prism:startingPage>430</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>431</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ia5058">
    <title>Simultaneous measurement of X-ray specular reflection and off-specular diffuse scattering from liquid surfaces using a two-dimensional pixel array detector: the liquid-interface reflectometer of BL37XU at SPring-8</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ia5058</link>
    <description>An X-ray reflectometer for simultaneous measurement of specular and off-specular reflection of liquid surfaces is described. The reflectometer, equipped with a two-dimensional single X-ray photon-counting pixel array detector obtained the full range of X-ray specular and off-specular reflections in an extremely short time (1 s). Both the specular and off-specular reflection of water exhibited good agreement with the predicted capillary-wave theory within the appropriate instrumental resolution. The approach is also demonstrated on an aqueous solution of 1-dodecyl-3-methylimidazolium chloride. The monolayer in which the dodecyl chain faces upwards and the Cl− anion locates next to the imidazolium ring formed on the water surface was found to be laterally homogeneous. The use of a pixel array detector will be particularly powerful for in situ measurements to investigate both out-of-plane and in-plane structures simultaneously, not only for liquid surfaces but also for other thin films.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yano, Y.F.</dc:creator>
    <dc:creator>Uruga, T.</dc:creator>
    <dc:creator>Tanida, H.</dc:creator>
    <dc:creator>Toyokawa, H.</dc:creator>
    <dc:creator>Terada, Y.</dc:creator>
    <dc:creator>Yamada, H.</dc:creator>
    <dc:date>2010-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510013087</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>X-ray reflectivity measurements of liquid surfaces were performed using a recently developed liquid-interface reflectometer at SPring-8. The full range of X-ray specular and off-specular reflections was obtained in an extremely short time by a two-dimensional single X-ray photon-counting pixel array detector, which offers enormous potential to determine the out-of-plane and in-plane structures at an interface simultaneously.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY REFLECTIVITY; OFF-SPECULAR DIFFUSE SCATTERING; PILATUS; AIR/WATER INTERFACE; IONIC LIQUIDS</dc:subject>
    <dc:description>An X-ray reflectometer for simultaneous measurement of specular and off-specular reflection of liquid surfaces is described. The reflectometer, equipped with a two-dimensional single X-ray photon-counting pixel array detector obtained the full range of X-ray specular and off-specular reflections in an extremely short time (1 s). Both the specular and off-specular reflection of water exhibited good agreement with the predicted capillary-wave theory within the appropriate instrumental resolution. The approach is also demonstrated on an aqueous solution of 1-dodecyl-3-methylimidazolium chloride. The monolayer in which the dodecyl chain faces upwards and the Cl− anion locates next to the imidazolium ring formed on the water surface was found to be laterally homogeneous. The use of a pixel array detector will be particularly powerful for in situ measurements to investigate both out-of-plane and in-plane structures simultaneously, not only for liquid surfaces but also for other thin films.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Simultaneous measurement of X-ray specular reflection and off-specular diffuse scattering from liquid surfaces using a two-dimensional pixel array detector: the liquid-interface reflectometer of BL37XU at SPring-8</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-07-01</prism:publicationDate>
    <prism:startingPage>511</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>516</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5078">
    <title>Impact of synchrotron radiation on macromolecular crystallography: a personal view</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5078</link>
    <description>The introduction of synchrotron radiation sources almost four decades ago has led to a revolutionary change in the way that diffraction data from macromolecular crystals are being collected. Here a brief history of the development of methodologies that took advantage of the availability of synchrotron sources are presented, and some personal experiences with the utilization of synchrotrons in the early days are recalled.</description>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Dauter, Z.</dc:creator>
    <dc:creator>Jaskolski, M.</dc:creator>
    <dc:creator>Wlodawer, A.</dc:creator>
    <dc:date>2010-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510011611</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>This article, largely based on personal experiences of the authors, reviews the early history of the application of synchrotron radiation to structural biology, and particularly protein crystallography, to show the tremendous impact that this experimental innovation has had on these disciplines.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; STRUCTURAL BIOLOGY; SCIENCE HISTORY</dc:subject>
    <dc:description>The introduction of synchrotron radiation sources almost four decades ago has led to a revolutionary change in the way that diffraction data from macromolecular crystals are being collected. Here a brief history of the development of methodologies that took advantage of the availability of synchrotron sources are presented, and some personal experiences with the utilization of synchrotrons in the early days are recalled.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Impact of synchrotron radiation on macromolecular crystallography: a personal view</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-07-01</prism:publicationDate>
    <prism:startingPage>433</prism:startingPage>
    <prism:section>feature articles</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>444</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ia5057">
    <title>Wavelength-dispersive spectrometer for X-ray microfluorescence analysis at the X-ray microscopy beamline ID21 (ESRF)</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ia5057</link>
    <description>The development of a wavelength-dispersive spectrometer for microfluorescence analysis at the X-ray Microscopy ID21 beamline of the European Synchrotron Radiation Facility (ESRF) is reported. The spectrometer is based on a polycapillary optic for X-ray fluorescence collection and is operated in a flat-crystal geometry. The design considerations as well as operation characteristics of the spectrometer are presented. The achieved performances, in particular the energy resolution, are compared with the results of Monte Carlo simulations. Further improvement in the energy resolution, down to ∼eV range, by employing a double-crystal geometry is examined. Finally, examples of applications requiring both spatial and spectral resolutions are presented.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Szlachetko, J.</dc:creator>
    <dc:creator>Cotte, M.</dc:creator>
    <dc:creator>Morse, J.</dc:creator>
    <dc:creator>Salomé, M.</dc:creator>
    <dc:creator>Jagodzinski, P.</dc:creator>
    <dc:creator>Dousse, J.-C.</dc:creator>
    <dc:creator>Hoszowska, J.</dc:creator>
    <dc:creator>Kayser, Y.</dc:creator>
    <dc:creator>Susini, J.</dc:creator>
    <dc:date>2010-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510010691</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A polycapillary-based wavelength-dispersive spectrometer is reported. The design consideration as well as operation characteristics are presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY SPECTROSCOPY; WAVELENGTH-DISPERSIVE SPECTROMETER; X-RAY IMAGING</dc:subject>
    <dc:description>The development of a wavelength-dispersive spectrometer for microfluorescence analysis at the X-ray Microscopy ID21 beamline of the European Synchrotron Radiation Facility (ESRF) is reported. The spectrometer is based on a polycapillary optic for X-ray fluorescence collection and is operated in a flat-crystal geometry. The design considerations as well as operation characteristics of the spectrometer are presented. The achieved performances, in particular the energy resolution, are compared with the results of Monte Carlo simulations. Further improvement in the energy resolution, down to ∼eV range, by employing a double-crystal geometry is examined. Finally, examples of applications requiring both spatial and spectral resolutions are presented.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Wavelength-dispersive spectrometer for X-ray microfluorescence analysis at the X-ray microscopy beamline ID21 (ESRF)</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-05-01</prism:publicationDate>
    <prism:startingPage>400</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>408</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5079">
    <title>European Synchrotron User Organization established</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5079</link>
    <description>A report on the establishment of the European Synchrotron User Organization (ESUO), a body representing the interests of synchrotron radiation users across Europe.</description>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Pietsch, U.</dc:creator>
    <dc:creator>Cooper, M.J.</dc:creator>
    <dc:date>2010-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510010484</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A report on the establishment of the European Synchrotron User Organization (ESUO), a body representing the interests of synchrotron radiation users across Europe.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>A report on the establishment of the European Synchrotron User Organization (ESUO), a body representing the interests of synchrotron radiation users across Europe.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>European Synchrotron User Organization established</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-05-01</prism:publicationDate>
    <prism:startingPage>428</prism:startingPage>
    <prism:section>meeting reports</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>429</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5034">
    <title>Density measurement of samples under high pressure using synchrotron microtomography and diamond anvil cell techniques</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5034</link>
    <description>Accurate mass density information is critical in high-pressure studies of materials. It is, however, very difficult to measure the mass densities of amorphous materials under high pressure with a diamond anvil cell (DAC). Employing tomography to measure mass density of amorphous samples under high pressure in a DAC has recently been reported. In reality, the tomography data of a sample in a DAC suffers from not only noise but also from the missing angle problem owing to the geometry of the DAC. An algorithm that can suppress noise and overcome the missing angle problem has been developed to obtain accurate mass density information from such ill-posed data. The validity of the proposed methods was supported with simulations.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Xiao, X.</dc:creator>
    <dc:creator>Liu, H.</dc:creator>
    <dc:creator>Wang, L.</dc:creator>
    <dc:creator>De Carlo, F.</dc:creator>
    <dc:date>2010-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510008502</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An algorithm is developed to extract accurate mass density information from tomography data of a sample embedded in a diamond anvil cell in a high-pressure environment.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HIGH PRESSURE; EQUATION OF STATE; MICROTOMOGRAPHY; INCOMPLETE DATA</dc:subject>
    <dc:description>Accurate mass density information is critical in high-pressure studies of materials. It is, however, very difficult to measure the mass densities of amorphous materials under high pressure with a diamond anvil cell (DAC). Employing tomography to measure mass density of amorphous samples under high pressure in a DAC has recently been reported. In reality, the tomography data of a sample in a DAC suffers from not only noise but also from the missing angle problem owing to the geometry of the DAC. An algorithm that can suppress noise and overcome the missing angle problem has been developed to obtain accurate mass density information from such ill-posed data. The validity of the proposed methods was supported with simulations.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Density measurement of samples under high pressure using synchrotron microtomography and diamond anvil cell techniques</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-05-01</prism:publicationDate>
    <prism:startingPage>360</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>366</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5002">
    <title>In vivo pink-beam imaging and fast alignment procedure for rat brain lesion microbeam radiation therapy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5002</link>
    <description>A fast 50 µm-accuracy alignment procedure has been developed for the radiosurgery of brain lesions in rats, using microbeam radiation therapy. In vivo imaging was performed using the pink beam (35–60 keV) produced by the ID17 wiggler at the ESRF opened at 120 mm and filtered. A graphical user interface has been developed in order to define the irradiation field size and to position the target with respect to the skull structures observed in X-ray images. The method proposed here allows tremendous time saving by skipping the swap from white beam to monochromatic beam and vice versa. To validate the concept, the somatosensory cortex or thalamus of GAERS rats were irradiated under several ports using this alignment procedure. The magnetic resonance images acquired after contrast agent injection showed that the irradiations were selectively performed in these two expected brain regions. Image-guided microbeam irradiations have therefore been realised for the first time ever, and, thanks to this new development, the ID17 biomedical beamline provides a major tool allowing brain radiosurgery trials on animal patients.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Serduc, R.</dc:creator>
    <dc:creator>Berruyer, G.</dc:creator>
    <dc:creator>Brochard, T.</dc:creator>
    <dc:creator>Renier, M.</dc:creator>
    <dc:creator>Nemoz, C.</dc:creator>
    <dc:date>2010-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510006667</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A fast 50 µm-accuracy alignment procedure has been developed for the radiosurgery of brain lesions in rats, using microbeam radiation therapy.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SYNCHROTRON MICROBEAM RADIATION THERAPY; PINK-BEAM IMAGING; ALIGNMENT PROCEDURE; PRECLINICAL BRAIN RADIOSURGERY</dc:subject>
    <dc:description>A fast 50 µm-accuracy alignment procedure has been developed for the radiosurgery of brain lesions in rats, using microbeam radiation therapy. In vivo imaging was performed using the pink beam (35–60 keV) produced by the ID17 wiggler at the ESRF opened at 120 mm and filtered. A graphical user interface has been developed in order to define the irradiation field size and to position the target with respect to the skull structures observed in X-ray images. The method proposed here allows tremendous time saving by skipping the swap from white beam to monochromatic beam and vice versa. To validate the concept, the somatosensory cortex or thalamus of GAERS rats were irradiated under several ports using this alignment procedure. The magnetic resonance images acquired after contrast agent injection showed that the irradiations were selectively performed in these two expected brain regions. Image-guided microbeam irradiations have therefore been realised for the first time ever, and, thanks to this new development, the ID17 biomedical beamline provides a major tool allowing brain radiosurgery trials on animal patients.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>In vivo pink-beam imaging and fast alignment procedure for rat brain lesion microbeam radiation therapy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-05-01</prism:publicationDate>
    <prism:startingPage>325</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>331</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5615">
    <title>X-ray magnetic circular dichroism measurements using an X-ray phase retarder on the BM25 A-SpLine beamline at the ESRF</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5615</link>
    <description>Circularly polarized X-rays produced by a diamond X-ray phase retarder of thickness 0.5 mm in the Laue transmission configuration have been used for recording X-ray magnetic circular dichroism (XMCD) on the bending-magnet beamline BM25A (SpLine) at the ESRF. Field reversal and helicity reversal techniques have been used to carry out the measurements. The performance of the experimental set-up has been demonstrated by recording XMCD in the energy range from 7 to 11 keV.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Boada, R.</dc:creator>
    <dc:creator>Laguna-Marco, M.Á.</dc:creator>
    <dc:creator>Gallastegui, J.A.</dc:creator>
    <dc:creator>Castro, G.R.</dc:creator>
    <dc:creator>Chaboy, J.</dc:creator>
    <dc:date>2010-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510005881</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The experimental set-up at SpLine (BM25A, ESRF) to measure XMCD by using a diamond X-ray phase retarder to obtain circularly polarized X-rays is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY MAGNETIC CIRCULAR DICHROISM; X-RAY PHASE RETARDER; POLARIZATION TUNABILITY; MAGNETIC POLARIZATION</dc:subject>
    <dc:description>Circularly polarized X-rays produced by a diamond X-ray phase retarder of thickness 0.5 mm in the Laue transmission configuration have been used for recording X-ray magnetic circular dichroism (XMCD) on the bending-magnet beamline BM25A (SpLine) at the ESRF. Field reversal and helicity reversal techniques have been used to carry out the measurements. The performance of the experimental set-up has been demonstrated by recording XMCD in the energy range from 7 to 11 keV.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray magnetic circular dichroism measurements using an X-ray phase retarder on the BM25 A-SpLine beamline at the ESRF</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-05-01</prism:publicationDate>
    <prism:startingPage>308</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>313</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0418">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0418</link>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2010-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510004954</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-03-01</prism:publicationDate>
    <prism:startingPage>295</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>297</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?bf5028">
    <title>Silicon saw-tooth refractive lens for high-energy X-rays made using a diamond saw</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?bf5028</link>
    <description>Silicon is a material well suited for refractive lenses operating at high X-ray energies (&gt;50 keV), particularly if implemented in a single-crystal form to minimize small-angle scattering. A single-crystal silicon saw-tooth refractive lens, fabricated by a dicing process using a thin diamond wheel, was tested with 115 keV X-rays, giving an ideal 17 µm line focus width in a long focal length, 2:1 ratio demagnification geometry, with a source-to-focus distance of 58.5 m. The fabrication is simple, using resources typically available at any synchrotron facility's optics shop.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Said, A.H.</dc:creator>
    <dc:creator>Shastri, S.D.</dc:creator>
    <dc:date>2010-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510003584</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A Si saw-tooth refractive lens, fabricated by a dicing process, is demonstrated to focus a 115 keV X-ray beam.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAW-TOOTH LENSES; REFRACTIVE LENSES; HIGH-ENERGY X-RAYS; X-RAY OPTICS</dc:subject>
    <dc:description>Silicon is a material well suited for refractive lenses operating at high X-ray energies (&gt;50 keV), particularly if implemented in a single-crystal form to minimize small-angle scattering. A single-crystal silicon saw-tooth refractive lens, fabricated by a dicing process using a thin diamond wheel, was tested with 115 keV X-rays, giving an ideal 17 µm line focus width in a long focal length, 2:1 ratio demagnification geometry, with a source-to-focus distance of 58.5 m. The fabrication is simple, using resources typically available at any synchrotron facility's optics shop.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Silicon saw-tooth refractive lens for high-energy X-rays made using a diamond saw</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-05-01</prism:publicationDate>
    <prism:startingPage>425</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>427</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xt0011">
    <title>Synchrotron radiation in soil and geosciences</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xt0011</link>
    <description>This special issue is the outcome of the Session SSS24 `Synchrotron radiation in soil and geosciences' that was held on 21 April 2009 in Vienna during the EGU (European Geosciences Union) General Assembly 2009, within the Soil System Sciences (SSS) program. In this special issue ten papers are presented, chosen after a selection among 19 written contributions that were received after the scientific Session at EGU.</description>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Terzano, R.</dc:creator>
    <dc:creator>Denecke, M.A.</dc:creator>
    <dc:creator>Medici, L.</dc:creator>
    <dc:date>2010-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510003535</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Introductory overview to the special issue papers on synchrotron radiation in soil and geosciences.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>This special issue is the outcome of the Session SSS24 `Synchrotron radiation in soil and geosciences' that was held on 21 April 2009 in Vienna during the EGU (European Geosciences Union) General Assembly 2009, within the Soil System Sciences (SSS) program. In this special issue ten papers are presented, chosen after a selection among 19 written contributions that were received after the scientific Session at EGU.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Synchrotron radiation in soil and geosciences</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-03-01</prism:publicationDate>
    <prism:startingPage>147</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>148</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5076">
    <title>In vitro synchrotron-based radiography of micro-gap formation at the implant–abutment interface of two-piece dental implants</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5076</link>
    <description>Micro-gap formation at the implant–abutment interface of two-piece dental implants was investigated in vitro using high-resolution radiography in combination with hard X-ray synchrotron radiation. Images were taken with the specimen under different mechanical loads of up to 100 N. The aim of this investigation was to prove the existence of micro-gaps for implants with conical connections as well as to study the mechanical behavior of the mating zone of conical implants during loading. Synchrotron-based radiography in comparison with classical laboratory radiography yields high spatial resolution in combination with high contrast even when exploiting micro-sized features in highly attenuating objects. The first illustration of a micro-gap which was previously indistinguishable by laboratory methods underlines that the complex micro-mechanical behavior of implants requires further in vitro investigations where synchrotron-based micro-imaging is one of the prerequisites.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Rack, A.</dc:creator>
    <dc:creator>Rack, T.</dc:creator>
    <dc:creator>Stiller, M.</dc:creator>
    <dc:creator>Riesemeier, H.</dc:creator>
    <dc:creator>Zabler, S.</dc:creator>
    <dc:creator>Nelson, K.</dc:creator>
    <dc:date>2010-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510001834</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Micro-radiography using hard X-ray synchrotron radiation is the first potential tool to allow an evaluation of the mechanical behavior of the dental implant–abutment complex during force application, thus enabling the enhancement of the design of dental implants which has been based on theoretical analysis to date.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY IMAGING; DENTAL IMPLANTS; DIGITAL RADIOGRAPHY; IMPLANT-ABUTMENT INTERFACE</dc:subject>
    <dc:description>Micro-gap formation at the implant–abutment interface of two-piece dental implants was investigated in vitro using high-resolution radiography in combination with hard X-ray synchrotron radiation. Images were taken with the specimen under different mechanical loads of up to 100 N. The aim of this investigation was to prove the existence of micro-gaps for implants with conical connections as well as to study the mechanical behavior of the mating zone of conical implants during loading. Synchrotron-based radiography in comparison with classical laboratory radiography yields high spatial resolution in combination with high contrast even when exploiting micro-sized features in highly attenuating objects. The first illustration of a micro-gap which was previously indistinguishable by laboratory methods underlines that the complex micro-mechanical behavior of implants requires further in vitro investigations where synchrotron-based micro-imaging is one of the prerequisites.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>In vitro synchrotron-based radiography of micro-gap formation at the implant–abutment interface of two-piece dental implants</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-03-01</prism:publicationDate>
    <prism:startingPage>289</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>294</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?mo5001">
    <title>Synchrotron radiation computed laminography for polymer composite failure studies</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?mo5001</link>
    <description>Synchrotron radiation computed laminography is applied to the three-dimensional micro-imaging of damage in large polymer composite plates with high spatial resolution. The influence of different experimental conditions is studied with respect to measurement time optimization, dose minimization and reduction of artefacts in the reconstructed images. Failures like delaminations, transverse ply cracks and splits are observed under in situ loads. The propagation of up to 2 mm-long cracks is non-destructively followed in situ and investigated in detail. By phase retrieval using a single detector distance, the failures can be easily visualized in three dimensions.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Xu, F.</dc:creator>
    <dc:creator>Helfen, L.</dc:creator>
    <dc:creator>Moffat, A.J.</dc:creator>
    <dc:creator>Johnson, G.</dc:creator>
    <dc:creator>Sinclair, I.</dc:creator>
    <dc:creator>Baumbach, T.</dc:creator>
    <dc:date>2010-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049510001512</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Failures of laterally extended polymer composite panels are imaged using 3D computed laminography. The experimental parameters and capability of the method are studied.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>LAMINOGRAPHY; IN SITU LOADING; POLYMER COMPOSITES; PHASE RETRIEVAL</dc:subject>
    <dc:description>Synchrotron radiation computed laminography is applied to the three-dimensional micro-imaging of damage in large polymer composite plates with high spatial resolution. The influence of different experimental conditions is studied with respect to measurement time optimization, dose minimization and reduction of artefacts in the reconstructed images. Failures like delaminations, transverse ply cracks and splits are observed under in situ loads. The propagation of up to 2 mm-long cracks is non-destructively followed in situ and investigated in detail. By phase retrieval using a single detector distance, the failures can be easily visualized in three dimensions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Synchrotron radiation computed laminography for polymer composite failure studies</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-03-01</prism:publicationDate>
    <prism:startingPage>222</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>226</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0407">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0407</link>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2010-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509053230</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-01-01</prism:publicationDate>
    <prism:startingPage>139</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>140</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5611">
    <title>Development of a differential pumping system for soft X-ray beamlines for windowless experiments under normal atmospheric conditions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5611</link>
    <description>A novel design for a differential pumping system has been investigated. This system allows windowless experiments in a soft X-ray beamline under normal atmospheric conditions. The new design consists of an aperture-based four-stage differential pumping system, based on a simple model calculation. A prototype system with a total length of 600 mm was constructed to confirm the validity of the design concept. Relatively short conductance-limiting components allow easy installation and alignment of the system on a synchrotron beamline. The fabricated system was installed on a beamline to test the transmission of soft X-rays through atmospheric helium.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Tamenori, Y.</dc:creator>
    <dc:date>2010-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509052571</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A differential pumping system has been constructed for the windowless connection of a soft X-ray high-vacuum beamline and an experimental chamber under normal atmospheric conditions.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>VACUUM; DIFFERENTIAL PUMP; WINDOWLESS CONNECTION; HELIUM PATH; SOFT X-RAYS</dc:subject>
    <dc:description>A novel design for a differential pumping system has been investigated. This system allows windowless experiments in a soft X-ray beamline under normal atmospheric conditions. The new design consists of an aperture-based four-stage differential pumping system, based on a simple model calculation. A prototype system with a total length of 600 mm was constructed to confirm the validity of the design concept. Relatively short conductance-limiting components allow easy installation and alignment of the system on a synchrotron beamline. The fabricated system was installed on a beamline to test the transmission of soft X-rays through atmospheric helium.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Development of a differential pumping system for soft X-ray beamlines for windowless experiments under normal atmospheric conditions</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-03-01</prism:publicationDate>
    <prism:startingPage>243</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>249</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5070">
    <title>X-ray microdiffraction analysis of radiation-induced defects in single grains of polycrystalline Fe</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5070</link>
    <description>Single-crystal diffuse X-ray scattering was used to characterize radiation-induced defects in individual grains of a polycrystalline proton-irradiated Fe foil. The grains were probed with an intense 1 µm X-ray beam to demonstrate that both polycrystalline and micrometer-scale samples can be studied with single-crystal-like signal-to-noise. Scattering was measured with an X-ray-sensitive area detector, which measures intensity over a surface in reciprocal space. By scanning the X-ray energy, the intensity was measured over reciprocal-space volumes. Since the sample is not rotated, the real-space scattering volume does not change. Methods to minimize experimental artifacts arising from the use of an area detector are described.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Specht, E.D.</dc:creator>
    <dc:creator>Walker, F.J.</dc:creator>
    <dc:creator>Liu, W.</dc:creator>
    <dc:date>2010-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509052078</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Single-crystal diffuse X-ray microdiffraction was used to characterize radiation-induced defects in individual grains of a polycrystalline proton-irradiated Fe foil.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MICRODIFFRACTION; IRRADIATION; DIFFUSE SCATTERING</dc:subject>
    <dc:description>Single-crystal diffuse X-ray scattering was used to characterize radiation-induced defects in individual grains of a polycrystalline proton-irradiated Fe foil. The grains were probed with an intense 1 µm X-ray beam to demonstrate that both polycrystalline and micrometer-scale samples can be studied with single-crystal-like signal-to-noise. Scattering was measured with an X-ray-sensitive area detector, which measures intensity over a surface in reciprocal space. By scanning the X-ray energy, the intensity was measured over reciprocal-space volumes. Since the sample is not rotated, the real-space scattering volume does not change. Methods to minimize experimental artifacts arising from the use of an area detector are described.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray microdiffraction analysis of radiation-induced defects in single grains of polycrystalline Fe</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-03-01</prism:publicationDate>
    <prism:startingPage>250</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>256</prism:endingPage>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wa9008">
    <title>X-ray spectroscopic approaches to the investigation and characterization of photochemical processes. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wa9008</link>
    <description>An error in the paper by Kennepohl et al. [(2009), J. Synchrotron Rad. 16, 484–488] is corrected.</description>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Kennepohl, P.</dc:creator>
    <dc:creator>Wasinger, E.C.</dc:creator>
    <dc:creator>DeBeer George, S.</dc:creator>
    <dc:date>2010-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509048237</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An error in the paper by Kennepohl et al. [(2009), J. Synchrotron Rad. 16, 484–488] is corrected.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>An error in the paper by Kennepohl et al. [(2009), J. Synchrotron Rad. 16, 484–488] is corrected.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray spectroscopic approaches to the investigation and characterization of photochemical processes. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-01-01</prism:publicationDate>
    <prism:startingPage>138</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>138</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5614">
    <title>Facing the challenge of biosample imaging by FTIR with a synchrotron radiation source</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5614</link>
    <description>Fourier-transform infrared (FTIR) synchrotron radiation (SR) microspectroscopy is a powerful molecular probe of biological samples at cellular resolution (&lt;10 µm). As the brilliance of SR is 100–1000 times higher than that of a conventional Globar source, FTIR microscopes are now available in almost all advanced SR facilities around the world. However, in spite of this superior performance, the expected advances in IR SR microscopy have not yet been realised, particularly with regard to bio-analytical studies of single cells and soft tissues. In recent decades solid-state array detectors have revolutionized the fields of molecular spectroscopy and chemical imaging, and now new IR focal plane array detectors implemented at ultra-bright SR facilities will extend the performance and overcome the existing limitations, possibly allowing IR SR instrumentation to achieve the highest sensitivity and resolution of molecular imaging. The impact of IR imaging on large tissue area and the complexity of the analysis are discussed. In view of the high brilliance of SR sources, a comparison of published microscope images is given. Finally, it is briefly outlined how an optimized combination of IR instrumentation and SR optical systems could reach the expected advantages of a SR-based FTIR imaging system.</description>
    <dc:rights>Copyright (c) 2010 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Petibois, C.</dc:creator>
    <dc:creator>Piccinini, M.</dc:creator>
    <dc:creator>Guidi, M.C.</dc:creator>
    <dc:creator>Marcelli, A.</dc:creator>
    <dc:date>2010-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509046056</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Fourier-transform infrared synchrotron radiation microspectroscopy is a powerful molecular probe of biological samples at cellular resolution (&lt;10 µm). The impact of IR imaging on large tissue area and the complexity of the analysis are discussed, and, in view of the high brilliance of SR sources, a comparison of published microscope images is given.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FTIR MICROSCOPY; BIOLOGICAL TISSUE; MOLECULAR IMAGING</dc:subject>
    <dc:description>Fourier-transform infrared (FTIR) synchrotron radiation (SR) microspectroscopy is a powerful molecular probe of biological samples at cellular resolution (&lt;10 µm). As the brilliance of SR is 100–1000 times higher than that of a conventional Globar source, FTIR microscopes are now available in almost all advanced SR facilities around the world. However, in spite of this superior performance, the expected advances in IR SR microscopy have not yet been realised, particularly with regard to bio-analytical studies of single cells and soft tissues. In recent decades solid-state array detectors have revolutionized the fields of molecular spectroscopy and chemical imaging, and now new IR focal plane array detectors implemented at ultra-bright SR facilities will extend the performance and overcome the existing limitations, possibly allowing IR SR instrumentation to achieve the highest sensitivity and resolution of molecular imaging. The impact of IR imaging on large tissue area and the complexity of the analysis are discussed. In view of the high brilliance of SR sources, a comparison of published microscope images is given. Finally, it is briefly outlined how an optimized combination of IR instrumentation and SR optical systems could reach the expected advantages of a SR-based FTIR imaging system.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Facing the challenge of biosample imaging by FTIR with a synchrotron radiation source</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2010 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-01-01</prism:publicationDate>
    <prism:startingPage>1</prism:startingPage>
    <prism:section>feature articles</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>11</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5596">
    <title>Synchrotron-radiation-stimulated etching of polydimethylsiloxane using XeF2 as a reaction gas</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5596</link>
    <description>The synchrotron radiation (SR) stimulated etching of silicon elastomer polydimethylsiloxane (PDMS) using XeF2 as an etching gas has been demonstrated. An etching system with differential pumps and two parabolic focusing mirrors was constructed to perform the etching. The PDMS was found to be effectively etched by the SR irradiation under the XeF2 gas flow, and the etching process was area-selective and anisotropic. An extremely high etching rate of 40–50 µm (10 min)−1 was easily obtained at an XeF2 gas pressure of 0.2–0.4 torr. This suggests that SR etching using XeF2 gas provides a new microfabrication technology for thick PDMS membranes, which can open new applications such as the formation of three-dimensional microfluidic circuits.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Chiang, T.-Y.</dc:creator>
    <dc:creator>Makimura, T.</dc:creator>
    <dc:creator>He, T.</dc:creator>
    <dc:creator>Torii, S.</dc:creator>
    <dc:creator>Yoshida, T.</dc:creator>
    <dc:creator>Tero, R.</dc:creator>
    <dc:creator>Wang, C.</dc:creator>
    <dc:creator>Urisu, T.</dc:creator>
    <dc:date>2010-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509045658</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Synchrotron-radiation-stimulated etching of silicon elastomer polydimethylsiloxane using XeF2 as an etching gas is demonstrated.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PDMS; SYNCHROTRON RADIATION ETCHING; XEF2; ANISOTROPY</dc:subject>
    <dc:description>The synchrotron radiation (SR) stimulated etching of silicon elastomer polydimethylsiloxane (PDMS) using XeF2 as an etching gas has been demonstrated. An etching system with differential pumps and two parabolic focusing mirrors was constructed to perform the etching. The PDMS was found to be effectively etched by the SR irradiation under the XeF2 gas flow, and the etching process was area-selective and anisotropic. An extremely high etching rate of 40–50 µm (10 min)−1 was easily obtained at an XeF2 gas pressure of 0.2–0.4 torr. This suggests that SR etching using XeF2 gas provides a new microfabrication technology for thick PDMS membranes, which can open new applications such as the formation of three-dimensional microfluidic circuits.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Synchrotron-radiation-stimulated etching of polydimethylsiloxane using XeF2 as a reaction gas</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-01-01</prism:publicationDate>
    <prism:startingPage>69</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>74</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5607">
    <title>Temperature gradient analyzers for compact high-resolution X-ray spectrometers</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5607</link>
    <description>Compact high-resolution X-ray spectrometers with a one-dimensional temperature gradient at the analyzer crystal are considered. This gradient, combined with the use of a position-sensitive detector, makes it possible to relax the usual Rowland-circle condition, allowing increased space at the sample position for a given energy resolution or arm radius. Thus, for example, it is estimated that ∼meV resolution is possible with a 3 m analyzer arm and 200 mm clearance between the sample and detector. Simple analytic formulae are provided, supported by excellent agreement with ray-tracing simulations. One variation of this method also allows the detector position sensitivity to be used to determine momentum transfer, effectively improving momentum resolution without reducing (slitting down) the analyzer size. Application to medium-resolution (∼10–100 meV) inelastic X-ray scattering spectrometers with large angular acceptance is discussed, where this method also allows increased space at the sample. In some cases the application of a temperature gradient can improve the energy resolution even with a single-element detector.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ishikawa, D.</dc:creator>
    <dc:creator>Baron, A.Q.R.</dc:creator>
    <dc:date>2010-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509043167</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A temperature gradient applied to analyzer crystals allows relaxation of the Roland-circle geometry for meV-resolution spectrometers.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY SPECTROMETERS; ANALYZER CRYSTALS; INELASTIC X-RAY SCATTERING; ATOMIC DYNAMICS; ELECTRONIC DYNAMICS</dc:subject>
    <dc:description>Compact high-resolution X-ray spectrometers with a one-dimensional temperature gradient at the analyzer crystal are considered. This gradient, combined with the use of a position-sensitive detector, makes it possible to relax the usual Rowland-circle condition, allowing increased space at the sample position for a given energy resolution or arm radius. Thus, for example, it is estimated that ∼meV resolution is possible with a 3 m analyzer arm and 200 mm clearance between the sample and detector. Simple analytic formulae are provided, supported by excellent agreement with ray-tracing simulations. One variation of this method also allows the detector position sensitivity to be used to determine momentum transfer, effectively improving momentum resolution without reducing (slitting down) the analyzer size. Application to medium-resolution (∼10–100 meV) inelastic X-ray scattering spectrometers with large angular acceptance is discussed, where this method also allows increased space at the sample. In some cases the application of a temperature gradient can improve the energy resolution even with a single-element detector.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Temperature gradient analyzers for compact high-resolution X-ray spectrometers</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-01-01</prism:publicationDate>
    <prism:startingPage>12</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>24</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0393">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0393</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2009-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509041922</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-11-01</prism:publicationDate>
    <prism:startingPage>880</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>882</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xl5015">
    <title>Advances and synergy of high-pressure sciences at synchrotron sources</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xl5015</link>
    <description>Introductory overview to the special issue papers on high-pressure sciences and synchrotron radiation.</description>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Liu, H.</dc:creator>
    <dc:creator>Duffy, T.</dc:creator>
    <dc:creator>Ehm, L.</dc:creator>
    <dc:creator>Crichton, W.</dc:creator>
    <dc:creator>Aoki, K.</dc:creator>
    <dc:date>2009-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509041946</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Introductory overview to the special issue papers on high-pressure sciences and synchrotron radiation.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>Introductory overview to the special issue papers on high-pressure sciences and synchrotron radiation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Advances and synergy of high-pressure sciences at synchrotron sources</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-11-01</prism:publicationDate>
    <prism:startingPage>697</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>698</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi5601">
    <title>The ID23-2 structural biology microfocus beamline at the ESRF</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi5601</link>
    <description>The first phase of the ESRF beamline ID23 to be constructed was ID23-1, a tunable MAD-capable beamline which opened to users in early 2004. The second phase of the beamline to be constructed is ID23-2, a monochromatic microfocus beamline dedicated to macromolecular crystallography experiments. Beamline ID23-2 makes use of well characterized optical elements: a single-bounce silicon (111) monochromator and two mirrors in Kirkpatrick–Baez geometry to focus the X-ray beam. A major design goal of the ID23-2 beamline is to provide a reliable, easy-to-use and routine microfocus beam. ID23-2 started operation in November 2005, as the first beamline dedicated to microfocus macromolecular crystallography. The beamline has taken the standard automated ESRF macromolecular crystallography environment (both hardware and software), allowing users of ID23-2 to be rapidly familiar with the microfocus environment. This paper describes the beamline design, the special considerations taken into account given the microfocus beam, and summarizes the results of the first years of the beamline operation.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Flot, D.</dc:creator>
    <dc:creator>Mairs, T.</dc:creator>
    <dc:creator>Giraud, T.</dc:creator>
    <dc:creator>Guijarro, M.</dc:creator>
    <dc:creator>Lesourd, M.</dc:creator>
    <dc:creator>Rey, V.</dc:creator>
    <dc:creator>van Brussel, D.</dc:creator>
    <dc:creator>Morawe, C.</dc:creator>
    <dc:creator>Borel, C.</dc:creator>
    <dc:creator>Hignette, O.</dc:creator>
    <dc:creator>Chavanne, J.</dc:creator>
    <dc:creator>Nurizzo, D.</dc:creator>
    <dc:creator>McSweeney, S.</dc:creator>
    <dc:creator>Mitchell, E.</dc:creator>
    <dc:date>2010-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509041168</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Beamline ID23-2, the first dedicated and highly automated high-throughput monochromatic macromolecular crystallography microfocus beamline, is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; AUTOMATION; MICROFOCUS</dc:subject>
    <dc:description>The first phase of the ESRF beamline ID23 to be constructed was ID23-1, a tunable MAD-capable beamline which opened to users in early 2004. The second phase of the beamline to be constructed is ID23-2, a monochromatic microfocus beamline dedicated to macromolecular crystallography experiments. Beamline ID23-2 makes use of well characterized optical elements: a single-bounce silicon (111) monochromator and two mirrors in Kirkpatrick–Baez geometry to focus the X-ray beam. A major design goal of the ID23-2 beamline is to provide a reliable, easy-to-use and routine microfocus beam. ID23-2 started operation in November 2005, as the first beamline dedicated to microfocus macromolecular crystallography. The beamline has taken the standard automated ESRF macromolecular crystallography environment (both hardware and software), allowing users of ID23-2 to be rapidly familiar with the microfocus environment. This paper describes the beamline design, the special considerations taken into account given the microfocus beam, and summarizes the results of the first years of the beamline operation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The ID23-2 structural biology microfocus beamline at the ESRF</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>17</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2010-01-01</prism:publicationDate>
    <prism:startingPage>107</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>118</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5033">
    <title>Use of a hexapod in diffraction measurements of substrate-supported crystals of organic semiconductors</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5033</link>
    <description>Thin films of organic semiconductor prepared on substrates generally contain crystals that have one common crystal plane parallel to the substrate but random in-plane orientations. In diffraction measurements of these structures, it is often required to anchor the X-ray beam on a fixed spot on the sample, such as an optically visible crystallite or island. Here, a hexapod is used in place of a traditional multi-circle diffractometer to perform area-detector-based diffraction measurements on an actual device that contains 6,13-bis(triisopropyl­silyethynyl)-pentacene (TIPS-pentacene) crystals. The hexapod allows for sample rotations about any user-defined rotation center. Two types of complex sample motions have been programmed to characterize the structure of the TIPS-pentacene crystal: an in-plane powder average has been performed at a fixed grazing-incident angle to determine the lattice parameters of the crystal; then the in-plane component of the scattering vector was continuously rotated in transmission geometry to determine the local crystal orientation.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yang, L.</dc:creator>
    <dc:creator>Yang, H.</dc:creator>
    <dc:date>2009-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509037911</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The use of a hexapod in X-ray diffraction measurements of substrate-supported TIPS-pentacene crystals has been demonstrated to determine the lattice constants and the local orientation of the crystals.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY DIFFRACTION; HEXAPOD; TRANSMISSION; GRAZING INCIDENCE</dc:subject>
    <dc:description>Thin films of organic semiconductor prepared on substrates generally contain crystals that have one common crystal plane parallel to the substrate but random in-plane orientations. In diffraction measurements of these structures, it is often required to anchor the X-ray beam on a fixed spot on the sample, such as an optically visible crystallite or island. Here, a hexapod is used in place of a traditional multi-circle diffractometer to perform area-detector-based diffraction measurements on an actual device that contains 6,13-bis(triisopropyl­silyethynyl)-pentacene (TIPS-pentacene) crystals. The hexapod allows for sample rotations about any user-defined rotation center. Two types of complex sample motions have been programmed to characterize the structure of the TIPS-pentacene crystal: an in-plane powder average has been performed at a fixed grazing-incident angle to determine the lattice parameters of the crystal; then the in-plane component of the scattering vector was continuously rotated in transmission geometry to determine the local crystal orientation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Use of a hexapod in diffraction measurements of substrate-supported crystals of organic semiconductors</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-11-01</prism:publicationDate>
    <prism:startingPage>788</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>795</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wa5013">
    <title>A decade of user operation on the macromolecular crystallography MAD beamline ID14-4 at the ESRF</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wa5013</link>
    <description>ID14-4 at the ESRF is the first tunable undulator-based macromolecular crystallography beamline that can celebrate a decade of user service. During this time ID14-4 has not only been instrumental in the determination of the structures of biologically important molecules but has also contributed significantly to the development of various instruments, novel data collection schemes and pioneering radiation damage studies on biological samples. Here, the evolution of ID14-4 over the last decade is presented, and some of the major improvements that were carried out in order to maintain its status as one of the most productive macromolecular crystallography beamlines are highlighted. The experimental hutch has been upgraded to accommodate a high-precision diffractometer, a sample changer and a large CCD detector. More recently, the optical hutch has been refurbished in order to improve the X-ray beam quality on ID14-4 and to incorporate the most modern and robust optical elements used at other ESRF beamlines. These new optical elements will be described and their effect on beam stability discussed. These studies may be useful in the design, construction and maintenance of future X-ray beamlines for macromolecular crystallography and indeed other applications, such as those planned for the ESRF upgrade.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>McCarthy, A.A.</dc:creator>
    <dc:creator>Brockhauser, S.</dc:creator>
    <dc:creator>Nurizzo, D.</dc:creator>
    <dc:creator>Theveneau, P.</dc:creator>
    <dc:creator>Mairs, T.</dc:creator>
    <dc:creator>Spruce, D.</dc:creator>
    <dc:creator>Guijarro, M.</dc:creator>
    <dc:creator>Lesourd, M.</dc:creator>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:creator>McSweeney, S.</dc:creator>
    <dc:date>2009-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509035377</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The improvement of the X-ray beam quality achieved on ID14-4 by the installation of new X-ray optical elements is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; X-RAY BEAM QUALITY; BEAMLINE DIAGNOSTICS; BEAMLINE AUTOMATION</dc:subject>
    <dc:description>ID14-4 at the ESRF is the first tunable undulator-based macromolecular crystallography beamline that can celebrate a decade of user service. During this time ID14-4 has not only been instrumental in the determination of the structures of biologically important molecules but has also contributed significantly to the development of various instruments, novel data collection schemes and pioneering radiation damage studies on biological samples. Here, the evolution of ID14-4 over the last decade is presented, and some of the major improvements that were carried out in order to maintain its status as one of the most productive macromolecular crystallography beamlines are highlighted. The experimental hutch has been upgraded to accommodate a high-precision diffractometer, a sample changer and a large CCD detector. More recently, the optical hutch has been refurbished in order to improve the X-ray beam quality on ID14-4 and to incorporate the most modern and robust optical elements used at other ESRF beamlines. These new optical elements will be described and their effect on beam stability discussed. These studies may be useful in the design, construction and maintenance of future X-ray beamlines for macromolecular crystallography and indeed other applications, such as those planned for the ESRF upgrade.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A decade of user operation on the macromolecular crystallography MAD beamline ID14-4 at the ESRF</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-11-01</prism:publicationDate>
    <prism:startingPage>803</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>812</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0391">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0391</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2009-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509031501</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-09-01</prism:publicationDate>
    <prism:startingPage>693</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>694</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5067">
    <title>Comments on Determination of X-ray flux using silicon pin diodes by R. L. Owen et al. (2009). J. Synchrotron Rad. 16, 143–151</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5067</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Krumrey, M.</dc:creator>
    <dc:date>2009-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509023887</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Comments on Owen et al. [J. Synchrotron Rad. (2009). 16, 143–151].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Comments on Determination of X-ray flux using silicon pin diodes by R. L. Owen et al. (2009). J. Synchrotron Rad. 16, 143–151</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-09-01</prism:publicationDate>
    <prism:startingPage>690</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>690</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv0003">
    <title>Response to Krumrey's Comments on Determination of X-ray flux using silicon pin diodes by R. L. Owen et al. (2009). J. Synchrotron Rad. 16, 143–153</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv0003</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Owen, R.L.</dc:creator>
    <dc:creator>Holton, J.M.</dc:creator>
    <dc:creator>Schulze-Briese, C.</dc:creator>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:date>2009-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509023644</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Response to Krumrey's comments in the previous paper.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Response to Krumrey's Comments on Determination of X-ray flux using silicon pin diodes by R. L. Owen et al. (2009). J. Synchrotron Rad. 16, 143–153</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-09-01</prism:publicationDate>
    <prism:startingPage>691</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>692</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0390">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0390</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2009-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509021748</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-07-01</prism:publicationDate>
    <prism:startingPage>597</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>599</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0388">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0388</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2009-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509013910</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-05-01</prism:publicationDate>
    <prism:startingPage>440</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>441</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5059">
    <title>Performance of single-photon-counting PILATUS detector modules</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5059</link>
    <description>PILATUS is a silicon hybrid pixel detector system, operating in single-photon-counting mode, that has been developed at the Paul Scherrer Institut for the needs of macromolecular crystallography at the Swiss Light Source (SLS). A calibrated PILATUS module has been characterized with monochromatic synchrotron radiation. The influence of charge sharing on the count rate and the overall energy resolution of the detector were investigated. The dead-time of the system was determined using the attenuated direct synchrotron beam. A single module detector was also tested in surface diffraction experiments at the SLS, whereby its performance regarding fluorescence suppression and saturation tolerance were evaluated, and have shown to greatly improve the sensitivity, reliability and speed of surface diffraction data acquisition.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Kraft, P.</dc:creator>
    <dc:creator>Bergamaschi, A.</dc:creator>
    <dc:creator>Broennimann, Ch.</dc:creator>
    <dc:creator>Dinapoli, R.</dc:creator>
    <dc:creator>Eikenberry, E.F.</dc:creator>
    <dc:creator>Henrich, B.</dc:creator>
    <dc:creator>Johnson, I.</dc:creator>
    <dc:creator>Mozzanica, A.</dc:creator>
    <dc:creator>Schlepütz, C.M.</dc:creator>
    <dc:creator>Willmott, P.R.</dc:creator>
    <dc:creator>Schmitt, B.</dc:creator>
    <dc:date>2009-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509009911</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Characterization of PILATUS single-photon-counting X-ray detector modules regarding charge sharing, energy resolution and rate capability is presented. The performance of the detector was tested with surface diffraction experiments at the synchrotron.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HYBRID PIXEL DETECTOR; SINGLE PHOTON COUNTING; ENERGY RESOLUTION; CHARGE SHARING; DEAD-TIME; SURFACE X-RAY DIFFRACTION</dc:subject>
    <dc:description>PILATUS is a silicon hybrid pixel detector system, operating in single-photon-counting mode, that has been developed at the Paul Scherrer Institut for the needs of macromolecular crystallography at the Swiss Light Source (SLS). A calibrated PILATUS module has been characterized with monochromatic synchrotron radiation. The influence of charge sharing on the count rate and the overall energy resolution of the detector were investigated. The dead-time of the system was determined using the attenuated direct synchrotron beam. A single module detector was also tested in surface diffraction experiments at the SLS, whereby its performance regarding fluorescence suppression and saturation tolerance were evaluated, and have shown to greatly improve the sensitivity, reliability and speed of surface diffraction data acquisition.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Performance of single-photon-counting PILATUS detector modules</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-05-01</prism:publicationDate>
    <prism:startingPage>368</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>375</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ia5038">
    <title>X-ray diffractometry for the structure determination of a submicrometre single powder grain</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ia5038</link>
    <description>A high-precision diffractometer has been developed for the structure analysis of a submicrometre-scale single grain of a powder sample at the SPring-8 BL40XU undulator beamline. The key design concept is the combination of a stable focused synchrotron radiation beam and the precise axis control of the diffractometer, which allows accurate diffraction intensity data of a submicrometre-scale single powder grain to be measured. The phase zone plate was designed to create a high-flux focused synchrotron radiation beam. A low-eccentric goniometer and high-precision sample positioning stages were adopted to ensure the alignment of a micrometre-scale focused synchrotron radiation beam onto the submicrometre-scale single powder grain. In order to verify the diffractometer performance, the diffraction pattern data of several powder grains of BaTiO3, of dimensions ∼600 × 600 × 300 nm, were measured. By identifying the diffraction data set of one single powder grain, the crystal structure was successfully determined with a reliable factor of 5.24%.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yasuda, N.</dc:creator>
    <dc:creator>Murayama, H.</dc:creator>
    <dc:creator>Fukuyama, Y.</dc:creator>
    <dc:creator>Kim, J.E.</dc:creator>
    <dc:creator>Kimura, S.</dc:creator>
    <dc:creator>Toriumi, K.</dc:creator>
    <dc:creator>Tanaka, Y.</dc:creator>
    <dc:creator>Moritomo, Y.</dc:creator>
    <dc:creator>Kuroiwa, Y.</dc:creator>
    <dc:creator>Kato, K.</dc:creator>
    <dc:creator>Tanaka, H.</dc:creator>
    <dc:creator>Takata, M.</dc:creator>
    <dc:date>2009-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950900675X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A high-precision diffractometer with a synchrotron radiation microfocusing technique has been developed to investigate the crystal structure of a submicrometre-scale single grain of powder sample. The structure of a BaTiO3 single powder grain, of dimensions ∼600 × 600 × 300 nm, was determined.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SUBMICROMETRE X-RAY BEAM; PHASE ZONE PLATE; X-RAY DIFFRACTION; SINGLE-CRYSTAL STRUCTURE ANALYSIS; POWDER DIFFRACTION</dc:subject>
    <dc:description>A high-precision diffractometer has been developed for the structure analysis of a submicrometre-scale single grain of a powder sample at the SPring-8 BL40XU undulator beamline. The key design concept is the combination of a stable focused synchrotron radiation beam and the precise axis control of the diffractometer, which allows accurate diffraction intensity data of a submicrometre-scale single powder grain to be measured. The phase zone plate was designed to create a high-flux focused synchrotron radiation beam. A low-eccentric goniometer and high-precision sample positioning stages were adopted to ensure the alignment of a micrometre-scale focused synchrotron radiation beam onto the submicrometre-scale single powder grain. In order to verify the diffractometer performance, the diffraction pattern data of several powder grains of BaTiO3, of dimensions ∼600 × 600 × 300 nm, were measured. By identifying the diffraction data set of one single powder grain, the crystal structure was successfully determined with a reliable factor of 5.24%.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray diffractometry for the structure determination of a submicrometre single powder grain</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-05-01</prism:publicationDate>
    <prism:startingPage>352</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>357</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi5590">
    <title>100 ps time-resolved solution scattering utilizing a wide-bandwidth X-ray beam from multilayer optics</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi5590</link>
    <description>100 ps time-resolved X-ray solution-scattering capabilities have been developed using multilayer optics at the beamline NW14A, Photon Factory Advanced Ring, KEK. X-ray pulses with an energy bandwidth of ΔE/E = 1–5% are generated by reflecting X-ray pulses (ΔE/E = 15%) through multilayer optics, made of W/B4C or depth-graded Ru/C on silicon substrate. This tailor-made wide-bandwidth X-ray pulse provides high-quality solution-scattering data for obtaining photo-induced molecular reaction dynamics. The time-resolved solution scattering of CH2I2 in methanol is demonstrated as a typical example.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ichiyanagi, K.</dc:creator>
    <dc:creator>Sato, T.</dc:creator>
    <dc:creator>Nozawa, S.</dc:creator>
    <dc:creator>Kim, K.H.</dc:creator>
    <dc:creator>Lee, J.H.</dc:creator>
    <dc:creator>Choi, J.</dc:creator>
    <dc:creator>Tomita, A.</dc:creator>
    <dc:creator>Ichikawa, H.</dc:creator>
    <dc:creator>Adachi, S.</dc:creator>
    <dc:creator>Ihee, H.</dc:creator>
    <dc:creator>Koshihara, S.</dc:creator>
    <dc:date>2009-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509005986</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A new method of time-resolved solution scattering utilizing X-ray multilayer optics is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TIME-RESOLVED SOLUTION SCATTERING; PHOTODISSOCIATION REACTION; LIQUIDOGRAPHY; MULTILAYERS</dc:subject>
    <dc:description>100 ps time-resolved X-ray solution-scattering capabilities have been developed using multilayer optics at the beamline NW14A, Photon Factory Advanced Ring, KEK. X-ray pulses with an energy bandwidth of ΔE/E = 1–5% are generated by reflecting X-ray pulses (ΔE/E = 15%) through multilayer optics, made of W/B4C or depth-graded Ru/C on silicon substrate. This tailor-made wide-bandwidth X-ray pulse provides high-quality solution-scattering data for obtaining photo-induced molecular reaction dynamics. The time-resolved solution scattering of CH2I2 in methanol is demonstrated as a typical example.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>100 ps time-resolved solution scattering utilizing a wide-bandwidth X-ray beam from multilayer optics</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-05-01</prism:publicationDate>
    <prism:startingPage>391</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>394</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5586">
    <title>Comments on Migration of mercury from dental amalgam through human teeth by H. H. Harris et al. (2008). J. Synchrotron Rad. 15, 123–128</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5586</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Guzzi, G.</dc:creator>
    <dc:creator>Pigatto, P.D.</dc:creator>
    <dc:date>2009-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950900212X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Comments on Harris et al. [J. Synchrotron Rad. (2008). 15, 123–128].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Comments on Migration of mercury from dental amalgam through human teeth by H. H. Harris et al. (2008). J. Synchrotron Rad. 15, 123–128</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-05-01</prism:publicationDate>
    <prism:startingPage>435</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>436</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh0007">
    <title>Radiation damage in protein crystals examined under various conditions by different methods</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh0007</link>
    <description>Investigation of radiation damage in protein crystals has progressed in several directions over the past couple of years. There have been improvements in the basic procedures such as calibration of the incident X-ray intensity and calculation of the dose likely to be deposited in a crystal of known size and composition with this intensity. There has been increased emphasis on using additional techniques such as optical, Raman or X-ray spectroscopy to complement X-ray diffraction. Apparent discrepancies between the results of different techniques can be explained by the fact that they are sensitive to different length scales or to changes in the electronic state rather than to movement of atoms. Investigations have been carried out at room temperature as well as cryo-temperatures and, in both cases, with the introduction of potential scavenger molecules. These and other studies are leading to an overall description of the changes which can occur when a protein crystal is irradiated with X-rays at both cryo- and room temperatures. Results from crystallographic and spectroscopic radiation-damage experiments can be reconciled with other studies in the field of radiation physics and chemistry.</description>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:creator>Nave, C.</dc:creator>
    <dc:date>2009-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509005238</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The current understanding of radiation damage in protein crystals is reviewed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; PROTEIN CRYSTALS; SCAVENGERS; MICROSPECTROSCOPY</dc:subject>
    <dc:description>Investigation of radiation damage in protein crystals has progressed in several directions over the past couple of years. There have been improvements in the basic procedures such as calibration of the incident X-ray intensity and calculation of the dose likely to be deposited in a crystal of known size and composition with this intensity. There has been increased emphasis on using additional techniques such as optical, Raman or X-ray spectroscopy to complement X-ray diffraction. Apparent discrepancies between the results of different techniques can be explained by the fact that they are sensitive to different length scales or to changes in the electronic state rather than to movement of atoms. Investigations have been carried out at room temperature as well as cryo-temperatures and, in both cases, with the introduction of potential scavenger molecules. These and other studies are leading to an overall description of the changes which can occur when a protein crystal is irradiated with X-rays at both cryo- and room temperatures. Results from crystallographic and spectroscopic radiation-damage experiments can be reconciled with other studies in the field of radiation physics and chemistry.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Radiation damage in protein crystals examined under various conditions by different methods</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-03-01</prism:publicationDate>
    <prism:startingPage>129</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>132</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5015">
    <title>A beginner's guide to radiation damage</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5015</link>
    <description>Many advances in the understanding of radiation damage to protein crystals, particularly at cryogenic temperatures, have been made in recent years, but with this comes an expanding literature, and, to the new breed of protein crystallographer who is not really interested in X-ray physics or radiation chemistry but just wants to solve a biologically relevant structure, the technical nature and breadth of this literature can be daunting. The purpose of this paper is to serve as a rough guide to radiation damage issues, and to provide references to the more exacting and detailed work. No attempt has been made to report precise numbers (a factor of two is considered satisfactory), and, since there are aspects of radiation damage that are demonstrably unpredictable, the `worst case scenario' as well as the `average crystal' are discussed in terms of the practicalities of data collection.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Holton, J.M.</dc:creator>
    <dc:date>2009-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509004361</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Radiation damage considerations affecting data collection by more than a factor of two are summarized and damage avoidance strategies are suggested.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; MINIMUM CRYSTAL SIZE; PROTEIN MACROMOLECULAR CRYSTALLOGRAPHY; DOSE DOUBLING; RADIOPROTECTANT; DATA COLLECTION STRATEGY</dc:subject>
    <dc:description>Many advances in the understanding of radiation damage to protein crystals, particularly at cryogenic temperatures, have been made in recent years, but with this comes an expanding literature, and, to the new breed of protein crystallographer who is not really interested in X-ray physics or radiation chemistry but just wants to solve a biologically relevant structure, the technical nature and breadth of this literature can be daunting. The purpose of this paper is to serve as a rough guide to radiation damage issues, and to provide references to the more exacting and detailed work. No attempt has been made to report precise numbers (a factor of two is considered satisfactory), and, since there are aspects of radiation damage that are demonstrably unpredictable, the `worst case scenario' as well as the `average crystal' are discussed in terms of the practicalities of data collection.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A beginner's guide to radiation damage</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-03-01</prism:publicationDate>
    <prism:startingPage>133</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>142</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv9050">
    <title>Classification of Fe-bearing species from K-edge XANES data using two-parameter correlation plots. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv9050</link>
    <description>In the paper by Marcus et al. [(2008), J. Synchrotron Rad. 15, 463–468], an incorrect version of Table 1 was published. The correct version is given here.</description>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Marcus, M.A.</dc:creator>
    <dc:creator>Westphal, A.J.</dc:creator>
    <dc:creator>Fakra, S.C.</dc:creator>
    <dc:date>2009-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509007328</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An erratum to the paper by Marcus et al. [(2008), J. Synchrotron Rad. 15, 463–468].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>K-EDGE XANES; IRON; STARDUST MINERALS; ENVIRONMENT</dc:subject>
    <dc:description>In the paper by Marcus et al. [(2008), J. Synchrotron Rad. 15, 463–468], an incorrect version of Table 1 was published. The correct version is given here.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Classification of Fe-bearing species from K-edge XANES data using two-parameter correlation plots. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-05-01</prism:publicationDate>
    <prism:startingPage>439</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>439</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot0001">
    <title>Response to Guzzi &amp; Pigatto's Comments on Migration of mercury from dental amalgam through human teeth by H. H. Harris et al. (2008). J. Synchrotron Rad. 15, 123–128</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot0001</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Harris, H.H.</dc:creator>
    <dc:creator>Vogt, S.</dc:creator>
    <dc:creator>Lay, P.A.</dc:creator>
    <dc:date>2009-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509005706</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Response to Guzzi &amp; Pigatto's comments in the previous paper.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Response to Guzzi &amp; Pigatto's Comments on Migration of mercury from dental amalgam through human teeth by H. H. Harris et al. (2008). J. Synchrotron Rad. 15, 123–128</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-05-01</prism:publicationDate>
    <prism:startingPage>437</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>438</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5057">
    <title>Synchrotron-based radioscopy employing spatio-temporal micro-resolution for studying fast phenomena in liquid metal foams</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5057</link>
    <description>Investigations of pore coalescence and individual cell wall collapse in an expanding liquid metal foam by means of X-ray radioscopy with spatio-temporal micro-resolution are reported. By using white synchrotron radiation for imaging, the rupture of a film and the subsequent merger of two neighbouring bubbles could be recorded with a time sampling rate of 40000 frames s−1 (25 µs exposure time) and a spatial sampling rate of 20 µm. The rupture time of a cell wall was found to be in the range of 300 µs. This value is in agreement with theoretical considerations which assume an inertia-dominated rupture time of cell walls in liquid metal foams.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Rack, A.</dc:creator>
    <dc:creator>García-Moreno, F.</dc:creator>
    <dc:creator>Baumbach, T.</dc:creator>
    <dc:creator>Banhart, J.</dc:creator>
    <dc:date>2009-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509001939</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>High-speed synchrotron-based radioscopy is applied to study a coalescence event (which lasts ∼2 ms) in situ in a liquid metal foam.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY RADIOSCOPY; METAL FOAMS; COALESCENCE; CMOS; MICRO-RADIOGRAPHY; LIQUID FILMS; METALLIC THIN FILMS; VISCOSITY; FRACTURE; ALUMINIUM ALLOYS; BUBBLES</dc:subject>
    <dc:description>Investigations of pore coalescence and individual cell wall collapse in an expanding liquid metal foam by means of X-ray radioscopy with spatio-temporal micro-resolution are reported. By using white synchrotron radiation for imaging, the rupture of a film and the subsequent merger of two neighbouring bubbles could be recorded with a time sampling rate of 40000 frames s−1 (25 µs exposure time) and a spatial sampling rate of 20 µm. The rupture time of a cell wall was found to be in the range of 300 µs. This value is in agreement with theoretical considerations which assume an inertia-dominated rupture time of cell walls in liquid metal foams.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Synchrotron-based radioscopy employing spatio-temporal micro-resolution for studying fast phenomena in liquid metal foams</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-05-01</prism:publicationDate>
    <prism:startingPage>432</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>434</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5016">
    <title>Colouring cryo-cooled crystals: online microspectrophotometry</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5016</link>
    <description>X-rays can produce a high concentration of radicals within cryo-cooled macromolecular crystals. Some radicals have large extinction coefficients in the visible (VIS) range of the electromagnetic spectrum, and can be observed optically and spectrally. An online microspectrophotometer with high temporal resolution has been constructed that is capable of measuring UV/VIS absorption spectra (200–1100 nm) during X-ray data collection. The typical X-ray-induced blue colour that is characteristic of a wide range of cryo-conditions has been identified as trapped solvated electrons. Disulphide-containing proteins are shown to form disulphide radicals at millimolar concentrations, with absorption maxima around 400 nm. The solvated electrons and the disulphide radicals seem to have a lifetime in the range of seconds up to minutes at 100 K. The temperature dependence of the kinetics of X-ray-induced radical formation is different for the solvated electrons compared with the disulphide radicals. The online microspectrophotometer provides a technique complementary to X-ray diffraction for analysing and characterizing intermediates and redox states of proteins and enzymes.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>McGeehan, J.</dc:creator>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:creator>Murray, J.W.</dc:creator>
    <dc:creator>Owen, R.L.</dc:creator>
    <dc:creator>Cipriani, F.</dc:creator>
    <dc:creator>McSweeney, S.</dc:creator>
    <dc:creator>Weik, M.</dc:creator>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:date>2009-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509001629</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A portable and readily aligned online microspectrophotometer that can be easily installed on macromolecular crystallography beamlines is described. It allows measurement of the spectral characteristics of macromolecular crystals prior, during, and after the X-ray diffraction experiment.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; MACROMOLECULAR CRYSTALLOGRAPHY; ONLINE MICROSPECTROPHOTOMETRY</dc:subject>
    <dc:description>X-rays can produce a high concentration of radicals within cryo-cooled macromolecular crystals. Some radicals have large extinction coefficients in the visible (VIS) range of the electromagnetic spectrum, and can be observed optically and spectrally. An online microspectrophotometer with high temporal resolution has been constructed that is capable of measuring UV/VIS absorption spectra (200–1100 nm) during X-ray data collection. The typical X-ray-induced blue colour that is characteristic of a wide range of cryo-conditions has been identified as trapped solvated electrons. Disulphide-containing proteins are shown to form disulphide radicals at millimolar concentrations, with absorption maxima around 400 nm. The solvated electrons and the disulphide radicals seem to have a lifetime in the range of seconds up to minutes at 100 K. The temperature dependence of the kinetics of X-ray-induced radical formation is different for the solvated electrons compared with the disulphide radicals. The online microspectrophotometer provides a technique complementary to X-ray diffraction for analysing and characterizing intermediates and redox states of proteins and enzymes.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Colouring cryo-cooled crystals: online microspectrophotometry</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-03-01</prism:publicationDate>
    <prism:startingPage>163</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>172</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0382">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0382</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2009-01-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950804199X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-01-01</prism:publicationDate>
    <prism:startingPage>119</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>121</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0387">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0387</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2009-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049509004610</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-03-01</prism:publicationDate>
    <prism:startingPage>314</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>315</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh0001">
    <title>A new on-axis multimode spectrometer for the macromolecular crystallography beamlines of the Swiss Light Source</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh0001</link>
    <description>X-ray crystallography at third-generation synchrotron sources permits tremendous insight into the three-dimensional structure of macromolecules. Additional information is, however, often required to aid the transition from structure to function. In situ spectroscopic methods such as UV–Vis absorption and (resonance) Raman can provide this, and can also provide a means of detecting X-ray-induced changes. Here, preliminary results are introduced from an on-axis UV–Vis absorption and Raman multimode spectrometer currently being integrated into the beamline environment at X10SA of the Swiss Light Source. The continuing development of the spectrometer is also outlined.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Owen, R.L.</dc:creator>
    <dc:creator>Pearson, A.R.</dc:creator>
    <dc:creator>Meents, A.</dc:creator>
    <dc:creator>Boehler, P.</dc:creator>
    <dc:creator>Thominet, V.</dc:creator>
    <dc:creator>Schulze-Briese, C.</dc:creator>
    <dc:date>2009-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508040120</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Complementary techniques greatly aid the interpretation of macromolecule structures to yield functional information, and can also help to track radiation-induced changes. A new on-axis spectrometer being integrated into the macromolecular crystallography beamlines of the Swiss Light Source is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SINGLE-CRYSTAL MICROSPECTROPHOTOMETRY; KINETIC CRYSTALLOGRAPHY; STRUCTURAL ENZYMOLOGY; RADIATION DAMAGE; MACROMOLECULAR CRYSTALLOGRAPHY; COMPLEMENTARY TECHNIQUES</dc:subject>
    <dc:description>X-ray crystallography at third-generation synchrotron sources permits tremendous insight into the three-dimensional structure of macromolecules. Additional information is, however, often required to aid the transition from structure to function. In situ spectroscopic methods such as UV–Vis absorption and (resonance) Raman can provide this, and can also provide a means of detecting X-ray-induced changes. Here, preliminary results are introduced from an on-axis UV–Vis absorption and Raman multimode spectrometer currently being integrated into the beamline environment at X10SA of the Swiss Light Source. The continuing development of the spectrometer is also outlined.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A new on-axis multimode spectrometer for the macromolecular crystallography beamlines of the Swiss Light Source</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-03-01</prism:publicationDate>
    <prism:startingPage>173</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>182</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh0002">
    <title>Determination of X-ray flux using silicon pin diodes</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh0002</link>
    <description>Accurate measurement of photon flux from an X-ray source, a parameter required to calculate the dose absorbed by the sample, is not yet routinely available at macromolecular crystallography beamlines. The development of a model for determining the photon flux incident on pin diodes is described here, and has been tested on the macromolecular crystallography beamlines at both the Swiss Light Source, Villigen, Switzerland, and the Advanced Light Source, Berkeley, USA, at energies between 4 and 18 keV. These experiments have shown that a simple model based on energy deposition in silicon is sufficient for determining the flux incident on high-quality silicon pin diodes. The derivation and validation of this model is presented, and a web-based tool for the use of the macromolecular crystallography and wider synchrotron community is introduced.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Owen, R.L.</dc:creator>
    <dc:creator>Holton, J.M.</dc:creator>
    <dc:creator>Schulze-Briese, C.</dc:creator>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:date>2009-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508040429</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Accurate measurement of photon flux from an X-ray source is a parameter required to calculate the dose absorbed by a sample. The development of a model for determining the photon flux incident on pin diodes, and experiments to test this model, are described for incident energies between 4 and 18 keV used in macromolecular crystallography.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; FLUX DETERMINATION; SILICON PIN DIODE; ABSORBED DOSE</dc:subject>
    <dc:description>Accurate measurement of photon flux from an X-ray source, a parameter required to calculate the dose absorbed by the sample, is not yet routinely available at macromolecular crystallography beamlines. The development of a model for determining the photon flux incident on pin diodes is described here, and has been tested on the macromolecular crystallography beamlines at both the Swiss Light Source, Villigen, Switzerland, and the Advanced Light Source, Berkeley, USA, at energies between 4 and 18 keV. These experiments have shown that a simple model based on energy deposition in silicon is sufficient for determining the flux incident on high-quality silicon pin diodes. The derivation and validation of this model is presented, and a web-based tool for the use of the macromolecular crystallography and wider synchrotron community is introduced.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Determination of X-ray flux using silicon pin diodes</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-03-01</prism:publicationDate>
    <prism:startingPage>143</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>151</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi5593">
    <title>Capturing molecular structural dynamics by 100 ps time-resolved X-ray absorption spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi5593</link>
    <description>An experimental set-up for time-resolved X-ray absorption spectroscopy with 100 ps time resolution at beamline NW14A at the Photon Factory Advanced Ring is presented. The X-ray positional active feedback to crystals in a monochromator combined with a figure-of-merit scan of the laser beam position has been utilized as an essential tool to stabilize the spatial overlap of the X-ray and laser beams at the sample position. As a typical example, a time-resolved XAFS measurement of a photo-induced spin crossover reaction of the tris(1,10-phenanthrorine)iron(II) complex in water is presented.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sato, T.</dc:creator>
    <dc:creator>Nozawa, S.</dc:creator>
    <dc:creator>Ichiyanagi, K.</dc:creator>
    <dc:creator>Tomita, A.</dc:creator>
    <dc:creator>Chollet, M.</dc:creator>
    <dc:creator>Ichikawa, H.</dc:creator>
    <dc:creator>Fujii, H.</dc:creator>
    <dc:creator>Adachi, S.</dc:creator>
    <dc:creator>Koshihara, S.</dc:creator>
    <dc:date>2009-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508034596</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An experimental set-up for time-resolved X-ray absorption spectroscopy with 100 ps time resolution at beamline NW14A at the Photon Factory Advanced Ring is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TIME-RESOLVED X-RAY ABSORPTION; SPIN CROSSOVER; TRIS(1,10-PHENANTHRORINE)IRON(II)</dc:subject>
    <dc:description>An experimental set-up for time-resolved X-ray absorption spectroscopy with 100 ps time resolution at beamline NW14A at the Photon Factory Advanced Ring is presented. The X-ray positional active feedback to crystals in a monochromator combined with a figure-of-merit scan of the laser beam position has been utilized as an essential tool to stabilize the spatial overlap of the X-ray and laser beams at the sample position. As a typical example, a time-resolved XAFS measurement of a photo-induced spin crossover reaction of the tris(1,10-phenanthrorine)iron(II) complex in water is presented.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Capturing molecular structural dynamics by 100 ps time-resolved X-ray absorption spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>16</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2009-01-01</prism:publicationDate>
    <prism:startingPage>110</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>115</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0380">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0380</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2008-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508032755</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-11-01</prism:publicationDate>
    <prism:startingPage>663</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>665</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0370">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0370</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2008-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508025600</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-09-01</prism:publicationDate>
    <prism:startingPage>539</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>541</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0371">
    <title>PI-MTE cameras now twice as fast with 2 MHz readout</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0371</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Flint-Baum, D.</dc:creator>
    <dc:date>2008-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508026162</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>PI-MTE cameras now twice as fast with 2 MHz readout</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-09-01</prism:publicationDate>
    <prism:startingPage>538</prism:startingPage>
    <prism:section>new commercial products</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>538</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wl5146">
    <title>A coherent synchrotron X-ray microradiology investigation of bubble and droplet coalescence</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wl5146</link>
    <description>A quantitative application of microradiology with coherent X-rays to the real-time study of microbubble and microdroplet coalescence phenomena, with specific emphasis on the size relations in three-body events, is presented. The results illustrate the remarkable effectiveness of coherent X-ray imaging in delineating interfaces in multiphase systems, in accurately measuring their geometric properties and in monitoring their dynamics.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Weon, B.M.</dc:creator>
    <dc:creator>Je, J.H.</dc:creator>
    <dc:creator>Hwu, Y.</dc:creator>
    <dc:creator>Margaritondo, G.</dc:creator>
    <dc:date>2008-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508025363</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Microradiology with coherent X-rays is shown to be very effective in revealing interfaces in multiphase systems and in particular gas bubbles. Its use has been tested in the study of bubble colescence validating the results with a simple theoretical analysis based on mass conservation.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COHERENT SYNCHROTRON X-RAY; MICRORADIOLOGY; COALESCENCE; BUBBLES; DROPLETS</dc:subject>
    <dc:description>A quantitative application of microradiology with coherent X-rays to the real-time study of microbubble and microdroplet coalescence phenomena, with specific emphasis on the size relations in three-body events, is presented. The results illustrate the remarkable effectiveness of coherent X-ray imaging in delineating interfaces in multiphase systems, in accurately measuring their geometric properties and in monitoring their dynamics.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A coherent synchrotron X-ray microradiology investigation of bubble and droplet coalescence</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>http://creativecommons.org/licenses/by/2.0/uk</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-11-01</prism:publicationDate>
    <prism:startingPage>660</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>662</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0369">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0369</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2008-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508017330</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-07-01</prism:publicationDate>
    <prism:startingPage>423</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>424</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0368">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0368</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508009175</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>319</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>321</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5026">
    <title>Development of an X-ray HARP–FEA detector system for high-throughput protein crystallography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5026</link>
    <description>A new detector system for protein crystallography is now being developed based on an X-ray HARP–FEA (high-gain avalanche rushing amorphous photoconductor–field emitter array), which consists of an amorphous selenium membrane and a matrix field emitter array. The combination of the membrane avalanche effect with a single driven FEA has several advantages over currently available area detectors, including higher sensitivity, higher spatial resolution and a higher frame rate. Preliminary evaluation of the detector has been carried out and its effectiveness has been confirmed. Next, diffraction images were measured with continuous rotation of a protein crystal, and the images were compared with those measured by the existing CCD detector; the system successfully obtained high-spatial-resolution images. Using shutterless measurement, the total measurement time can be reduced significantly, making the method appropriate for high-throughput protein crystallography. The X-ray HARP–FEA detector is an attractive candidate for the next generation of X-ray area detectors.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Miyoshi, T.</dc:creator>
    <dc:creator>Igarashi, N.</dc:creator>
    <dc:creator>Matsugaki, N.</dc:creator>
    <dc:creator>Yamada, Y.</dc:creator>
    <dc:creator>Hirano, K.</dc:creator>
    <dc:creator>Hyodo, K.</dc:creator>
    <dc:creator>Tanioka, K.</dc:creator>
    <dc:creator>Egami, N.</dc:creator>
    <dc:creator>Namba, M.</dc:creator>
    <dc:creator>Kubota, M.</dc:creator>
    <dc:creator>Kawai, T.</dc:creator>
    <dc:creator>Wakatsuki, S.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508006584</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A new detector system for protein crystallography based on an X-ray HARP–FEA is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HARP; SEMICONDUCTOR; AMORPHOUS SELENIUM; AVALANCHE MULTIPLICATION; IMAGING DEVICE; PROTEIN CRYSTALLOGRAPHY</dc:subject>
    <dc:description>A new detector system for protein crystallography is now being developed based on an X-ray HARP–FEA (high-gain avalanche rushing amorphous photoconductor–field emitter array), which consists of an amorphous selenium membrane and a matrix field emitter array. The combination of the membrane avalanche effect with a single driven FEA has several advantages over currently available area detectors, including higher sensitivity, higher spatial resolution and a higher frame rate. Preliminary evaluation of the detector has been carried out and its effectiveness has been confirmed. Next, diffraction images were measured with continuous rotation of a protein crystal, and the images were compared with those measured by the existing CCD detector; the system successfully obtained high-spatial-resolution images. Using shutterless measurement, the total measurement time can be reduced significantly, making the method appropriate for high-throughput protein crystallography. The X-ray HARP–FEA detector is an attractive candidate for the next generation of X-ray area detectors.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Development of an X-ray HARP–FEA detector system for high-throughput protein crystallography</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>281</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>284</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5019">
    <title>Structure of six-transmembrane cation channels revealed by single-particle analysis from electron microscopic images</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5019</link>
    <description>Six-transmembrane (6-TM) cation channels are plasma membrane-integral components of cellular signaling pathways conserved in almost all species, including animals, plants and some kinds of prokaryotes. These channels selectively permeate cations in response to various signals. In excitable and non-excitable mammalian cells, 6-TM cation channels play fundamental roles, including the generation of action potential and its transmission, the regulation of intracellular ion concentrations, and the activation of signaling cascades by humoral or mechanical pathways. Recently, the structures of three different 6-TM-type cation channels have been determined using single-particle analysis from cryo-electron microscopy images: the voltage-sensitive sodium channel, the IP3 receptor and the TRPC3 channel. The basic structure of the molecules is similar: a bell-like shape comprising a relatively small extracellular (or luminal) domain, a protein-dense transmembrane domain and an expanded cytoplasmic domain. However, in detail, the cytoplasmic architectures are different from one another and are diversely evolved to their specific physiological functions.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Mio, K.</dc:creator>
    <dc:creator>Ogura, T.</dc:creator>
    <dc:creator>Sato, C.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508004640</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Single-particle analysis is a computer-aided method for determining protein structure using projection images obtained by electron microscopy. Recently reconstructed 6-TM-type cation channels demonstrate the structural similarities and divergence of the family.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ELECTRON MICROSCOPY; ION CHANNEL STRUCTURE; SIX-TRANSMEMBRANE; SINGLE PARTICLES</dc:subject>
    <dc:description>Six-transmembrane (6-TM) cation channels are plasma membrane-integral components of cellular signaling pathways conserved in almost all species, including animals, plants and some kinds of prokaryotes. These channels selectively permeate cations in response to various signals. In excitable and non-excitable mammalian cells, 6-TM cation channels play fundamental roles, including the generation of action potential and its transmission, the regulation of intracellular ion concentrations, and the activation of signaling cascades by humoral or mechanical pathways. Recently, the structures of three different 6-TM-type cation channels have been determined using single-particle analysis from cryo-electron microscopy images: the voltage-sensitive sodium channel, the IP3 receptor and the TRPC3 channel. The basic structure of the molecules is similar: a bell-like shape comprising a relatively small extracellular (or luminal) domain, a protein-dense transmembrane domain and an expanded cytoplasmic domain. However, in detail, the cytoplasmic architectures are different from one another and are diversely evolved to their specific physiological functions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structure of six-transmembrane cation channels revealed by single-particle analysis from electron microscopic images</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>211</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>214</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5027">
    <title>Mutagenesis of the crystal contact of acidic fibroblast growth factor</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5027</link>
    <description>An attempt has been made to improve a crystal contact of human acidic fibroblast growth factor (haFGF; 140 amino acids) to control the crystal growth, because haFGF crystallizes only as a thin-plate form, yielding crystals suitable for X-ray but not neutron diffraction. X-ray crystal analysis of haFGF showed that the Glu81 side chain, located at a crystal contact between haFGF molecules, is in close proximity with an identical residue related by crystallographic symmetry, suggesting that charge repulsion may disrupt suitable crystal-packing interactions. To investigate whether the Glu residue affects the crystal-packing interactions, haFGF mutants in which Glu81 was replaced by Ala, Val, Leu, Ser and Thr were constructed. Although crystals of the Ala and Leu mutants were grown as a thin-plate form by the same precipitant (formate) as the wild type, crystals of the Ser and Thr mutants were grown with increased thickness, yielding a larger overall crystal volume. X-ray structural analysis of the Ser mutant determined at 1.35 Å resolution revealed that the hydroxy groups of Ser are linked by hydrogen bonds mediated by the formate used as a precipitant. This approach to engineering crystal contacts may contribute to the development of large protein crystals for neutron crystallography.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Honjo, E.</dc:creator>
    <dc:creator>Tamada, T.</dc:creator>
    <dc:creator>Adachi, M.</dc:creator>
    <dc:creator>Kuroki, R.</dc:creator>
    <dc:creator>Meher, A.</dc:creator>
    <dc:creator>Blaber, M.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508004470</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Several mutations at Glu81 located on the crystal contact of human acidic fibroblast growth factor were studied in an effort to improve crystal growth. Mutation to Ser and Thr resulted in crystallization of a rather bulky form of the wild type, whereas mutation to Val prohibited crystallization. These results suggest that crystal growth may be controlled by designing a new interface by protein engineering.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ACIDIC FIBROBLAST GROWTH FACTOR; CRYSTAL CONTACTS; MUTAGENESIS</dc:subject>
    <dc:description>An attempt has been made to improve a crystal contact of human acidic fibroblast growth factor (haFGF; 140 amino acids) to control the crystal growth, because haFGF crystallizes only as a thin-plate form, yielding crystals suitable for X-ray but not neutron diffraction. X-ray crystal analysis of haFGF showed that the Glu81 side chain, located at a crystal contact between haFGF molecules, is in close proximity with an identical residue related by crystallographic symmetry, suggesting that charge repulsion may disrupt suitable crystal-packing interactions. To investigate whether the Glu residue affects the crystal-packing interactions, haFGF mutants in which Glu81 was replaced by Ala, Val, Leu, Ser and Thr were constructed. Although crystals of the Ala and Leu mutants were grown as a thin-plate form by the same precipitant (formate) as the wild type, crystals of the Ser and Thr mutants were grown with increased thickness, yielding a larger overall crystal volume. X-ray structural analysis of the Ser mutant determined at 1.35 Å resolution revealed that the hydroxy groups of Ser are linked by hydrogen bonds mediated by the formate used as a precipitant. This approach to engineering crystal contacts may contribute to the development of large protein crystals for neutron crystallography.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Mutagenesis of the crystal contact of acidic fibroblast growth factor</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>285</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>287</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0364">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0364</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2008-03-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950800407X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-03-01</prism:publicationDate>
    <prism:startingPage>195</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>197</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5031">
    <title>Implementation of remote monitoring and diffraction evaluation systems at the Photon Factory macromolecular crystallography beamlines</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5031</link>
    <description>Owing to recent advances in high-throughput technology in macromolecular crystallography beamlines, such as high-brilliant X-ray sources, high-speed readout detectors and robotics, the number of samples that can be examined in a single visit to the beamline has increased dramatically. In order to make these experiments more efficient, two functions, remote monitoring and diffraction image evaluation, have been implemented in the macromolecular crystallography beamlines at the Photon Factory (PF). Remote monitoring allows scientists to participate in the experiment by watching from their laboratories, without having to come to the beamline. Diffraction image evaluation makes experiments easier, especially when using the sample exchange robot. To implement these two functions, two independent clients have been developed that work specifically for remote monitoring and diffraction image evaluation. In the macromolecular crystallography beamlines at PF, beamline control is performed using STARS (simple transmission and retrieval system). The system adopts a client–server style in which client programs communicate with each other through a server process using the STARS protocol. This is an advantage of the extension of the system; implementation of these new functions required few modifications of the existing system.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yamada, Y.</dc:creator>
    <dc:creator>pHonda, N.</dc:creator>
    <dc:creator>Matsugaki, N.</dc:creator>
    <dc:creator>Igarashi, N.</dc:creator>
    <dc:creator>Hiraki, M.</dc:creator>
    <dc:creator>Wakatsuki, S.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508004019</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>At the Photon Factory macromolecular crystallography beamlines, two new functions, remote monitoring and diffraction image evaluation, have been developed and installed on the beamline controlling system STARS (simple transmission and retrieval system).</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; BEAMLINE CONTROL SYSTEM; REMOTE MONITORING; DIFFRACTION IMAGE EVALUATION</dc:subject>
    <dc:description>Owing to recent advances in high-throughput technology in macromolecular crystallography beamlines, such as high-brilliant X-ray sources, high-speed readout detectors and robotics, the number of samples that can be examined in a single visit to the beamline has increased dramatically. In order to make these experiments more efficient, two functions, remote monitoring and diffraction image evaluation, have been implemented in the macromolecular crystallography beamlines at the Photon Factory (PF). Remote monitoring allows scientists to participate in the experiment by watching from their laboratories, without having to come to the beamline. Diffraction image evaluation makes experiments easier, especially when using the sample exchange robot. To implement these two functions, two independent clients have been developed that work specifically for remote monitoring and diffraction image evaluation. In the macromolecular crystallography beamlines at PF, beamline control is performed using STARS (simple transmission and retrieval system). The system adopts a client–server style in which client programs communicate with each other through a server process using the STARS protocol. This is an advantage of the extension of the system; implementation of these new functions required few modifications of the existing system.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Implementation of remote monitoring and diffraction evaluation systems at the Photon Factory macromolecular crystallography beamlines</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>296</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>299</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5039">
    <title>Highly bright X-ray generator using heat of fusion with a specially designed rotating anticathode</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5039</link>
    <description>A new type of rotating anticathode X-ray generator has been developed, in which the electron beam irradiates the inner surface of a U-shaped anticathode (Cu). A high-flux electron beam is focused on the inner surface by optimizing the shape of the bending magnet. The power of the electron beam can be increased to the point at which the irradiated part of the inner surface is melted, because a strong centrifugal force fixes the melted part on the inner surface. When the irradiated part is melted, a large amount of energy is stored as the heat of fusion, resulting in emission of X-rays 4.3 times more brilliant than can be attained by a conventional rotating anticathode. Oscillating translation of the irradiated position on the inner surface during use is expected to be very advantageous for extending the target life. A carbon film coating on the inner surface is considered to suppress evaporation of the target metal and will be an important technique in further realization of highly bright X-ray generation.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sakabe, N.</dc:creator>
    <dc:creator>Ohsawa, S.</dc:creator>
    <dc:creator>Sugimura, T.</dc:creator>
    <dc:creator>Ikeda, M.</dc:creator>
    <dc:creator>Tawada, M.</dc:creator>
    <dc:creator>Watanabe, N.</dc:creator>
    <dc:creator>Sasaki, K.</dc:creator>
    <dc:creator>Ohshima, K.</dc:creator>
    <dc:creator>Wakatsuki, M.</dc:creator>
    <dc:creator>Sakabe, K.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508003993</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A very compact X-ray generator, 4.3 times more brilliant than can be attained by a conventional rotating-anticathode X-ray generator, has been developed using a U-shaped rotating anticathode and a high-flux electron gun with focusing bending magnet.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>BRIGHT X-RAY GENERATORS; U-SHAPE ANTICATHODES; HEAT OF FUSION; TARGET LIFE EXTENSION; LOW EMITTANCE; DC/PULSE GUNS; FOCUSING BENDING MAGNETS</dc:subject>
    <dc:description>A new type of rotating anticathode X-ray generator has been developed, in which the electron beam irradiates the inner surface of a U-shaped anticathode (Cu). A high-flux electron beam is focused on the inner surface by optimizing the shape of the bending magnet. The power of the electron beam can be increased to the point at which the irradiated part of the inner surface is melted, because a strong centrifugal force fixes the melted part on the inner surface. When the irradiated part is melted, a large amount of energy is stored as the heat of fusion, resulting in emission of X-rays 4.3 times more brilliant than can be attained by a conventional rotating anticathode. Oscillating translation of the irradiated position on the inner surface during use is expected to be very advantageous for extending the target life. A carbon film coating on the inner surface is considered to suppress evaporation of the target metal and will be an important technique in further realization of highly bright X-ray generation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Highly bright X-ray generator using heat of fusion with a specially designed rotating anticathode</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>231</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>234</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5002">
    <title>High-resolution X-ray microdiffraction analysis of natural teeth</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5002</link>
    <description>The main component of natural teeth was determined many years ago as calcium phosphate, mostly in the form of hydroxyapatite with different crystallites. In the past, the method used in tooth crystal investigation has been mainly powder X-ray diffraction analysis, but this method has its drawbacks, i.e. the destruction of the natural tooth structure and the difficulty in examining the preferred orientation in different layers of the tooth. During the last century, microzone X-ray diffraction on the tooth surface was carried out, but, as the technology was less sophisticated, the results obtained were not very detailed. The newly developed microdiffraction equipment permits analysis of the microzone of teeth in situ. To test this new microdiffraction equipment, microdiffraction analysis of one natural healthy deciduous molar tooth and one carious deciduous molar tooth has been performed, using a Bruker D8 instrument. Phase analysis of the two teeth was performed; the crystal size at six test points in the natural healthy tooth was calculated by reflection (211), and the crystal preferred orientation of reflection (300) and reflection (002) at six test points in the natural healthy tooth were compared. The results showed that the tooth was a kind of biological mixed crystal composed of several crystal phases, the main crystal phase being hydroxyapatite. The crystal size grew larger going from the dentin to the enamel. The crystal preferred orientation mainly existed in the enamel, especially in the reflection (002). From our experiment, layer orientation and continuous crystal variations in teeth could be conveniently studied using fast online measurements by high-resolution X-ray microdiffraction equipment.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Xue, J.</dc:creator>
    <dc:creator>Zhang, L.</dc:creator>
    <dc:creator>Zou, L.</dc:creator>
    <dc:creator>Liao, Y.</dc:creator>
    <dc:creator>Li, J.</dc:creator>
    <dc:creator>Xiao, L.</dc:creator>
    <dc:creator>Li, W.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508003397</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>In situ microzone X-ray diffraction analysis of natural teeth is presented. From our experiment, layer orientation and continuous crystal variations in teeth could be conveniently studied using fast online measurements by high-resolution X-ray microdiffraction equipment.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY MICRODIFFRACTION; ENAMEL; CARIES; TEXTURE; CRYSTAL</dc:subject>
    <dc:description>The main component of natural teeth was determined many years ago as calcium phosphate, mostly in the form of hydroxyapatite with different crystallites. In the past, the method used in tooth crystal investigation has been mainly powder X-ray diffraction analysis, but this method has its drawbacks, i.e. the destruction of the natural tooth structure and the difficulty in examining the preferred orientation in different layers of the tooth. During the last century, microzone X-ray diffraction on the tooth surface was carried out, but, as the technology was less sophisticated, the results obtained were not very detailed. The newly developed microdiffraction equipment permits analysis of the microzone of teeth in situ. To test this new microdiffraction equipment, microdiffraction analysis of one natural healthy deciduous molar tooth and one carious deciduous molar tooth has been performed, using a Bruker D8 instrument. Phase analysis of the two teeth was performed; the crystal size at six test points in the natural healthy tooth was calculated by reflection (211), and the crystal preferred orientation of reflection (300) and reflection (002) at six test points in the natural healthy tooth were compared. The results showed that the tooth was a kind of biological mixed crystal composed of several crystal phases, the main crystal phase being hydroxyapatite. The crystal size grew larger going from the dentin to the enamel. The crystal preferred orientation mainly existed in the enamel, especially in the reflection (002). From our experiment, layer orientation and continuous crystal variations in teeth could be conveniently studied using fast online measurements by high-resolution X-ray microdiffraction equipment.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>High-resolution X-ray microdiffraction analysis of natural teeth</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>235</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>238</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5034">
    <title>X-ray crystallographic and biochemical characterizations of a mutant photosystem II complex from Thermosynechococcus vulcanus with the psbTc gene inactivated by an insertion mutation</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5034</link>
    <description>The crystal structure of a photosystem II (PSII) dimer from Thermosynechococcus vulcanus with its psbTc gene inactivated by insertion mutation of an antibiotic cassette in a site in the C-terminal region was analyzed at 3.8 Å resolution. In the crystal structure of the mutant PSII, the transmembrane helix of PsbTc remains, whereas the C-terminal loop of PsbTc has disappeared. In addition, the PsbM subunit, which seemed to be lost in a PsbTc-deletion mutant PSII of T. elongatus, is still present. The deletion of the C-terminal loop of PsbTc in the mutant PSII was verified by mass spectrometry. Thus, the insertion mutation of psbTc eliminated only the C-terminal loop of this subunit. Nevertheless, some features of the mutant PSII, namely a destabilization of the dimeric form and a slight decrease of the oxygen-evolving activity, were observed in the mutant, indicating that the C-terminal loop of PsbTc functions to maintain the stability of the PSII dimer and the activity of oxygen evolution.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Henmi, T.</dc:creator>
    <dc:creator>Iwai, M.</dc:creator>
    <dc:creator>Ikeuchi, M.</dc:creator>
    <dc:creator>Kawakami, K.</dc:creator>
    <dc:creator>Shen, J.-R..</dc:creator>
    <dc:creator>Kamiya, N.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508002458</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The characterization of a PsbTc-truncated mutant photosystem II complex is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PHOTOSYSTEM II; PSBTC; OXYGEN EVOLUTION; MUTANT; THERMOSYNECHOCOCCUS VULCANUS</dc:subject>
    <dc:description>The crystal structure of a photosystem II (PSII) dimer from Thermosynechococcus vulcanus with its psbTc gene inactivated by insertion mutation of an antibiotic cassette in a site in the C-terminal region was analyzed at 3.8 Å resolution. In the crystal structure of the mutant PSII, the transmembrane helix of PsbTc remains, whereas the C-terminal loop of PsbTc has disappeared. In addition, the PsbM subunit, which seemed to be lost in a PsbTc-deletion mutant PSII of T. elongatus, is still present. The deletion of the C-terminal loop of PsbTc in the mutant PSII was verified by mass spectrometry. Thus, the insertion mutation of psbTc eliminated only the C-terminal loop of this subunit. Nevertheless, some features of the mutant PSII, namely a destabilization of the dimeric form and a slight decrease of the oxygen-evolving activity, were observed in the mutant, indicating that the C-terminal loop of PsbTc functions to maintain the stability of the PSII dimer and the activity of oxygen evolution.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray crystallographic and biochemical characterizations of a mutant photosystem II complex from Thermosynechococcus vulcanus with the psbTc gene inactivated by an insertion mutation</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>304</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>307</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5023">
    <title>Protein crystallization in a 100 nl solution with new stirring equipment</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5023</link>
    <description>To investigate quantitatively the effects of stirring on protein crystallization, a new stirring system which can agitate a protein solution, ∼100 nl, by providing Hagen–Poiseuille flow has been successfully developed. In addition, this new stirring system provides flow with a well defined pattern and velocity. Using this system, hen egg-white lysozyme was crystallized in 100–200 nl solutions while being stirred. The optimum stirring conditions for lysozyme crystals have been explored by evaluating the Reynolds (Re) number and the crystals obtained. Intermittent flow, as well as a low Re number, was found to contribute significantly to the growth of a smaller number of larger crystals.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Maki, S.</dc:creator>
    <dc:creator>Murai, R.</dc:creator>
    <dc:creator>Yoshikawa, H.Y.</dc:creator>
    <dc:creator>Kitatani, T.</dc:creator>
    <dc:creator>Nakata, S.</dc:creator>
    <dc:creator>Kawahara, H.</dc:creator>
    <dc:creator>Hasenaka, H.</dc:creator>
    <dc:creator>Kobayashi, A.</dc:creator>
    <dc:creator>Okada, S.</dc:creator>
    <dc:creator>Sugiyama, S.</dc:creator>
    <dc:creator>Adachi, H.</dc:creator>
    <dc:creator>Matsumura, H.</dc:creator>
    <dc:creator>Takano, K.</dc:creator>
    <dc:creator>Murakami, S.</dc:creator>
    <dc:creator>Inoue, T.</dc:creator>
    <dc:creator>Sasaki, T.</dc:creator>
    <dc:creator>Mori, Y.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508001842</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>To investigate quantitatively the effects of stirring on protein crystallization, a new stirring system which can agitate a protein solution, ∼100 nl, by providing Hagen–Poiseuille flow has been successfully developed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>LYSOZYME; LOW-REYNOLDS-NUMBER FLOW; STIRRING METHOD; SYRINGE PUMP; MICROCAPILLARY; THIXOTROPY</dc:subject>
    <dc:description>To investigate quantitatively the effects of stirring on protein crystallization, a new stirring system which can agitate a protein solution, ∼100 nl, by providing Hagen–Poiseuille flow has been successfully developed. In addition, this new stirring system provides flow with a well defined pattern and velocity. Using this system, hen egg-white lysozyme was crystallized in 100–200 nl solutions while being stirred. The optimum stirring conditions for lysozyme crystals have been explored by evaluating the Reynolds (Re) number and the crystals obtained. Intermittent flow, as well as a low Re number, was found to contribute significantly to the growth of a smaller number of larger crystals.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Protein crystallization in a 100 nl solution with new stirring equipment</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>269</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>272</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5020">
    <title>Protein structures by spallation neutron crystallography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5020</link>
    <description>The Protein Crystallography Station at Los Alamos Neutron Science Center is a high-performance beamline that forms the core of a capability for neutron macromolecular structure and function determination. This capability also includes the Macromolecular Neutron Crystallography (MNC) consortium between Los Alamos (LANL) and Lawrence Berkeley National Laboratories for developing computational tools for neutron protein crystallography, a biological deuteration laboratory, the National Stable Isotope Production Facility, and an MNC drug design consortium between LANL and Case Western Reserve University.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Langan, P.</dc:creator>
    <dc:creator>Fisher, Z.</dc:creator>
    <dc:creator>Kovalevsky, A.</dc:creator>
    <dc:creator>Mustyakimov, M.</dc:creator>
    <dc:creator>Sutcliffe Valone, A.</dc:creator>
    <dc:creator>Unkefer, C.</dc:creator>
    <dc:creator>Waltman, M.J.</dc:creator>
    <dc:creator>Coates, L.</dc:creator>
    <dc:creator>Adams, P.D.</dc:creator>
    <dc:creator>Afonine, P.V.</dc:creator>
    <dc:creator>Bennett, B.</dc:creator>
    <dc:creator>Dealwis, C.</dc:creator>
    <dc:creator>Schoenborn, B.P.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508000824</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The capabilities of the Protein Crystallography Station at Los Alamos Neutron Science Center for determining protein structures by spallation neutron crystallography are illustrated, and the methodological and technological advances that are emerging from the Macromolecular Neutron Crystallography consortium are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>NEUTRONS; PROTEINS; MACROMOLECULAR CRYSTALLOGRAPHY; DEUTERATION; ENZYME MECHANISMS; DRUG BINDING; HYDRATION; JOINT XN STRUCTURE REFINEMENT</dc:subject>
    <dc:description>The Protein Crystallography Station at Los Alamos Neutron Science Center is a high-performance beamline that forms the core of a capability for neutron macromolecular structure and function determination. This capability also includes the Macromolecular Neutron Crystallography (MNC) consortium between Los Alamos (LANL) and Lawrence Berkeley National Laboratories for developing computational tools for neutron protein crystallography, a biological deuteration laboratory, the National Stable Isotope Production Facility, and an MNC drug design consortium between LANL and Case Western Reserve University.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Protein structures by spallation neutron crystallography</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>215</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>218</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5017">
    <title>Structural studies on Helicobacter pylori ATP-dependent protease, FtsH</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5017</link>
    <description>The ATP-dependent protease, FtsH, degrades misassembled membrane proteins for quality control like SecY, subunit a of FoF1-ATPase, and YccA, and digests short-lived soluble proteins in order to control their cellular regulation, including σ32, LpxC and λcII. The FtsH protein has an N-terminal transmembrane segment and a large cytosolic region that consists of two domains, an ATPase and a protease domain. To provide a structural basis for the nucleotide-dependent domain motions and a better understanding of substrate translocation, the crystal structures of the Helicobacter pylori (Hp) FtsH ATPase domain in the nucleotide-free state and complexed with ADP, were determined. Two different structures of HpFtsH ATPase were observed, with the nucleotide-free state in an asymmetric unit, and these structures reveal the new forms and show other conformational differences between the nucleotide-free and ADP-bound state compared with previous structures. In particular, one HpFtsH Apo structure has a considerable rotation difference compared with the HpFtsH ADP complex, and this large conformational change reveals that FtsH may have the mechanical force needed for substrate translocation.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Kim, S.H.</dc:creator>
    <dc:creator>Kang, G.B.</dc:creator>
    <dc:creator>Song, H.-E.</dc:creator>
    <dc:creator>Park, S.J.</dc:creator>
    <dc:creator>Bea, M.-H.</dc:creator>
    <dc:creator>Eom, S.H.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950706846X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The crystal structures of the Helicobacter pylori FtsH ATPase domain in the nucleotide-free state and complexed with ADP have been determined.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ATP-DEPENDENT PROTEASE; FTSH; HELICOBACTER PYLORI</dc:subject>
    <dc:description>The ATP-dependent protease, FtsH, degrades misassembled membrane proteins for quality control like SecY, subunit a of FoF1-ATPase, and YccA, and digests short-lived soluble proteins in order to control their cellular regulation, including σ32, LpxC and λcII. The FtsH protein has an N-terminal transmembrane segment and a large cytosolic region that consists of two domains, an ATPase and a protease domain. To provide a structural basis for the nucleotide-dependent domain motions and a better understanding of substrate translocation, the crystal structures of the Helicobacter pylori (Hp) FtsH ATPase domain in the nucleotide-free state and complexed with ADP, were determined. Two different structures of HpFtsH ATPase were observed, with the nucleotide-free state in an asymmetric unit, and these structures reveal the new forms and show other conformational differences between the nucleotide-free and ADP-bound state compared with previous structures. In particular, one HpFtsH Apo structure has a considerable rotation difference compared with the HpFtsH ADP complex, and this large conformational change reveals that FtsH may have the mechanical force needed for substrate translocation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structural studies on Helicobacter pylori ATP-dependent protease, FtsH</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>208</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>210</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wl5143">
    <title>Science experiments via telepresence at a synchrotron radiation source facility</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wl5143</link>
    <description>Station 9.8 is one of the most oversubscribed and high-throughput stations at the Synchrotron Radiation Source, Daresbury, whereby awarded experimental time is limited, data collections last normally no longer than an hour, user changeover is normally every 24 h, and familiarity with the station systems can be low. Therefore time lost owing to technical failures on the station has a dramatic impact on productivity. To provide 24 h support, the application of a turnkey communication system has been implemented, and is described along with additional applications including its use for inter-continental classroom instruction, user training and remote participation.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Warren, J.E.</dc:creator>
    <dc:creator>Diakun, G.</dc:creator>
    <dc:creator>Bushnell-Wye, G.</dc:creator>
    <dc:creator>Fisher, S.</dc:creator>
    <dc:creator>Thalal, A.</dc:creator>
    <dc:creator>Helliwell, M.</dc:creator>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:date>2008-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508000587</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The application of a turnkey communication system for telepresence at station 9.8 of the Synchrotron Radiation Source, Daresbury, is described and demonstrated, including its use for inter-continental classroom instruction and user training.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TELEPRESENCE; REMOTE TECHNICAL SUPPORT; WIDENING PARTICIPATION; GICSI INITIATIVE; USER TRAINING; STUDENT TEACHING; REMOTE USER PARTICIPATION</dc:subject>
    <dc:description>Station 9.8 is one of the most oversubscribed and high-throughput stations at the Synchrotron Radiation Source, Daresbury, whereby awarded experimental time is limited, data collections last normally no longer than an hour, user changeover is normally every 24 h, and familiarity with the station systems can be low. Therefore time lost owing to technical failures on the station has a dramatic impact on productivity. To provide 24 h support, the application of a turnkey communication system has been implemented, and is described along with additional applications including its use for inter-continental classroom instruction, user training and remote participation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Science experiments via telepresence at a synchrotron radiation source facility</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-03-01</prism:publicationDate>
    <prism:startingPage>191</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>194</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5006">
    <title>Ultrahigh-resolution crystallography and related electron density and electrostatic properties in proteins</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5006</link>
    <description>With an increasing number of biological macromolecular crystal structures measured at ultrahigh resolution (1 Å or better), it is necessary to extend to large systems the experimental valence electron density modelling that is applied to small molecules. A database of average multipole populations has been built, describing the electron density of chemical groups in all 20 amino acids found in proteins. It allows calculation of atomic aspherical scattering factors, which are the starting point for refinement of the protein electron density, using the MoPro software. It is shown that the use of non-spherical scattering factors has a major impact on crystallographic statistics and results in a more accurate crystal structure, notably in terms of thermal displacement parameters and bond distances involving H atoms. It is also possible to obtain a realistic valence electron density model, which is used in the calculation of the electrostatic potential and energetic properties of proteins.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Lecomte, C.</dc:creator>
    <dc:creator>Jelsch, C.</dc:creator>
    <dc:creator>Guillot, B.</dc:creator>
    <dc:creator>Fournier, B.</dc:creator>
    <dc:creator>Lagoutte, A.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049508000447</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Ultrahigh-resolution protein diffraction data allow valence electron density modelling and calculations of experimental electrostatic properties. Protein–ligand interaction energy may therefore be estimated.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ELECTRON DENSITY; PROTEIN REFINEMENT; HIGH-RESOLUTION CRYSTALLOGRAPHY</dc:subject>
    <dc:description>With an increasing number of biological macromolecular crystal structures measured at ultrahigh resolution (1 Å or better), it is necessary to extend to large systems the experimental valence electron density modelling that is applied to small molecules. A database of average multipole populations has been built, describing the electron density of chemical groups in all 20 amino acids found in proteins. It allows calculation of atomic aspherical scattering factors, which are the starting point for refinement of the protein electron density, using the MoPro software. It is shown that the use of non-spherical scattering factors has a major impact on crystallographic statistics and results in a more accurate crystal structure, notably in terms of thermal displacement parameters and bond distances involving H atoms. It is also possible to obtain a realistic valence electron density model, which is used in the calculation of the electrostatic potential and energetic properties of proteins.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Ultrahigh-resolution crystallography and related electron density and electrostatic properties in proteins</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>202</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>203</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5038">
    <title>Effect of amino acids and amino acid derivatives on crystallization of hemoglobin and ribonuclease A</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5038</link>
    <description>Determination of the appropriate conditions for protein crystallization remains a highly empirical process. Preventing protein aggregation is necessary for the formation of single crystals under aggregation-prone solution conditions. Because many amino acids and amino acid derivatives offer a unique combination of solubility and stabilizing properties, they open new avenues into the field of protein aggregation research. The use of amino acids and amino acid derivatives can potentially influence processes such as heat treatment and refolding reactions. The effect of the addition of several amino acids, such as lysine, and several amino acid derivatives, such as glycine ethyl ester and glycine amide, on the crystallization of equine hemoglobin and bovine pancreatic ribonuclease A has been examined. The addition of these amino acids and amino acid derivatives expanded the range of precipitant concentration in which crystals formed without aggregation. The addition of such additives appears to promote the crystallization of proteins.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ito, L.</dc:creator>
    <dc:creator>Kobayashi, T.</dc:creator>
    <dc:creator>Shiraki, K.</dc:creator>
    <dc:creator>Yamaguchi, H.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507068598</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The effect of the addition of amino acids and amino acid derivatives on the crystallization of hemoglobin and ribonuclease A has been evaluated. The results showed that certain types of additives expand the concentration conditions in which crystals are formed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROTEIN CRYSTALLIZATION; PROMOTION OF CRYSTALLIZATION; ADDITIVES; AMINO ACIDS; AMINO ACID DERIVATIVES; PROTEIN AGGREGATION</dc:subject>
    <dc:description>Determination of the appropriate conditions for protein crystallization remains a highly empirical process. Preventing protein aggregation is necessary for the formation of single crystals under aggregation-prone solution conditions. Because many amino acids and amino acid derivatives offer a unique combination of solubility and stabilizing properties, they open new avenues into the field of protein aggregation research. The use of amino acids and amino acid derivatives can potentially influence processes such as heat treatment and refolding reactions. The effect of the addition of several amino acids, such as lysine, and several amino acid derivatives, such as glycine ethyl ester and glycine amide, on the crystallization of equine hemoglobin and bovine pancreatic ribonuclease A has been examined. The addition of these amino acids and amino acid derivatives expanded the range of precipitant concentration in which crystals formed without aggregation. The addition of such additives appears to promote the crystallization of proteins.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Effect of amino acids and amino acid derivatives on crystallization of hemoglobin and ribonuclease A</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>316</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>318</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5003">
    <title>Interaction of HIV-1 aspartic protease with its inhibitor, by molecular dynamics and ab initio fragment molecular orbital method</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5003</link>
    <description>For the three complex crystal structures of HIV-1 aspartic protease (an enzyme of AIDS) with its inhibitor in the Protein Data Bank, molecular dynamics of the generalized Born surface area and the ab initio fragment molecular orbital of an ABINIT-MP calculation was performed to obtain the binding free energy, the molecular orbital energy, the interaction energy of residues with an inhibitor and the charge transfer at the active site. The inhibitors are five symmetric cyclic ureas, of which three were modelled, and an asymmetric dipeptide. The interaction energy of the inhibitor at the active sites of aspartic acid is as great as 50 kcal mol−1, coinciding with a tetrahedral transition state. For the inhibitor with a higher affinity, charge was transferred to the inhibitor from the active site. The difference in symmetry of the inhibitor was not evident. Binding free energy corresponds to the experimental value of the binding constant, while molecular orbital energy does not always, which is considered to be an entropy effect.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Koyano, K.</dc:creator>
    <dc:creator>Nakano, T.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507068586</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Molecular dynamics and the ab initio fragment molecular orbital method were applied to investigate the interaction of HIV-1 aspartic protease with its inhibitor. The interaction energy of the inhibitor at the active sites of aspartic acid obtained by the ab initio fragment molecular orbital method was as great as 50 kcal mol−1, coinciding with a tetrahedral transition state.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AIDS; ASPARTIC PROTEASE INHIBITOR; MOLECULAR DYNAMICS MM_GBSA; FRAGMENT MOLECULAR ORBITAL ABINIT-MP; TETRAHEDRAL TRANSITION STATES; ACTIVE SITES; INTERACTION ENERGY; CHARGE TRANSFER</dc:subject>
    <dc:description>For the three complex crystal structures of HIV-1 aspartic protease (an enzyme of AIDS) with its inhibitor in the Protein Data Bank, molecular dynamics of the generalized Born surface area and the ab initio fragment molecular orbital of an ABINIT-MP calculation was performed to obtain the binding free energy, the molecular orbital energy, the interaction energy of residues with an inhibitor and the charge transfer at the active site. The inhibitors are five symmetric cyclic ureas, of which three were modelled, and an asymmetric dipeptide. The interaction energy of the inhibitor at the active sites of aspartic acid is as great as 50 kcal mol−1, coinciding with a tetrahedral transition state. For the inhibitor with a higher affinity, charge was transferred to the inhibitor from the active site. The difference in symmetry of the inhibitor was not evident. Binding free energy corresponds to the experimental value of the binding constant, while molecular orbital energy does not always, which is considered to be an entropy effect.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Interaction of HIV-1 aspartic protease with its inhibitor, by molecular dynamics and ab initio fragment molecular orbital method</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>239</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>242</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5013">
    <title>Novel dimer structure of a membrane-bound protease with a catalytic Ser–Lys dyad and its linkage to stomatin</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5013</link>
    <description>Membrane-bound proteases are involved in various regulatory functions. A previous report indicates that the N-terminal region of PH1510 (1510-N) from the hyperthermophilic archaeon Pyrococcus horikoshii is a serine protease with a catalytic Ser–Lys dyad (Ser97 and Lys138), and specifically cleaves the C-terminal hydrophobic region of the p-stomatin PH1511. According to the crystal structure of the wild-type 1510-N in dimeric form, the active site around Ser97 is in a hydrophobic environment suitable for the hydrophobic substrates. This article reports the crystal structure of the K138A mutant of 1510-N at 2.3 Å resolution. The determined structure contains one molecule per asymmetric unit, but 1510-N is active in dimeric form. Two possible sets of dimer were found from the symmetry-related molecules. One dimer is almost the same as the wild-type 1510-N. Another dimer is probably in an inactive form. The L2 loop, which is disordered in the wild-type structure, is significantly kinked at around A-138 in the K138A mutant. Thus Lys138 probably has an important role on the conformation of L2.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yokoyama, H.</dc:creator>
    <dc:creator>Hamamatsu, S.</dc:creator>
    <dc:creator>Fujii, S.</dc:creator>
    <dc:creator>Matsui, I.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507068471</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The crystal structure of the K138A mutant of the 1510-N protease specific for p-stomatin was determined at 2.3 Å resolution. The structure shows a novel dimer form, and the kinked L2 loop indicates that Lys138 would probably have an important effect on the conformation of L2.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MEMBRANE-BOUND PROTEASE; STOMATIN; CLPP; DIMERS; PYROCOCCUS HORIKOSHII</dc:subject>
    <dc:description>Membrane-bound proteases are involved in various regulatory functions. A previous report indicates that the N-terminal region of PH1510 (1510-N) from the hyperthermophilic archaeon Pyrococcus horikoshii is a serine protease with a catalytic Ser–Lys dyad (Ser97 and Lys138), and specifically cleaves the C-terminal hydrophobic region of the p-stomatin PH1511. According to the crystal structure of the wild-type 1510-N in dimeric form, the active site around Ser97 is in a hydrophobic environment suitable for the hydrophobic substrates. This article reports the crystal structure of the K138A mutant of 1510-N at 2.3 Å resolution. The determined structure contains one molecule per asymmetric unit, but 1510-N is active in dimeric form. Two possible sets of dimer were found from the symmetry-related molecules. One dimer is almost the same as the wild-type 1510-N. Another dimer is probably in an inactive form. The L2 loop, which is disordered in the wild-type structure, is significantly kinked at around A-138 in the K138A mutant. Thus Lys138 probably has an important role on the conformation of L2.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Novel dimer structure of a membrane-bound protease with a catalytic Ser–Lys dyad and its linkage to stomatin</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>254</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>257</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5030">
    <title>X-ray beam stabilization at BL-17A, the protein microcrystallography beamline of the Photon Factory</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5030</link>
    <description>BL-17A is a new structural biology beamline at the Photon Factory, Japan. The high-brilliance beam, derived from the new short-gap undulator (SGU#17), allows for unique protein crystallographic experiments such as data collection from microcrystals and structural determination using softer X-rays. However, microcrystal experiments require robust beam stability during data collection and minor fluctuations could not be ignored. Initially, significant beam instability was observed at BL-17A. The causes of the beam instability were investigated and its various sources identified. Subsequently, several effective countermeasures have been implemented, and the fluctuation of the beam intensity successfully suppressed to within 1%. Here the instability reduction techniques used at BL-17A are presented.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Igarashi, N.</dc:creator>
    <dc:creator>Ikuta, K.</dc:creator>
    <dc:creator>Miyoshi, T.</dc:creator>
    <dc:creator>Matsugaki, N.</dc:creator>
    <dc:creator>Yamada, Y.</dc:creator>
    <dc:creator>Yousef, M.S.</dc:creator>
    <dc:creator>Wakatsuki, S.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507067118</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>BL-17A is a new structural biology beamline at the Photon Factory, dedicated to protein crystallography of microcrystals. Here the X-ray beam stabilization techniques used at BL-17A are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROTEIN MICROCRYSTALLOGRAPHY; PHOTON FACTORY; BEAMLINE DEVELOPMENT; X-RAY BEAM STABILIZATION</dc:subject>
    <dc:description>BL-17A is a new structural biology beamline at the Photon Factory, Japan. The high-brilliance beam, derived from the new short-gap undulator (SGU#17), allows for unique protein crystallographic experiments such as data collection from microcrystals and structural determination using softer X-rays. However, microcrystal experiments require robust beam stability during data collection and minor fluctuations could not be ignored. Initially, significant beam instability was observed at BL-17A. The causes of the beam instability were investigated and its various sources identified. Subsequently, several effective countermeasures have been implemented, and the fluctuation of the beam intensity successfully suppressed to within 1%. Here the instability reduction techniques used at BL-17A are presented.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray beam stabilization at BL-17A, the protein microcrystallography beamline of the Photon Factory</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>292</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>295</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5014">
    <title>Performance of an electron gun for a high-brightness X-ray generator</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5014</link>
    <description>A prototype thermionic electron gun for a high-brightness X-ray generator has been developed. Its extraction voltage and design current are 60 kV and 100 mA (DC), respectively. The X-ray generator aims towards a maximum brilliance of 60 kW mm−2. The beam sizes at the rotating anticathode must therefore be within 1.0 mm × 0.1 mm and a small beam emittance is required. The fabricated electron gun optimizes an aperture grid and a Whenelt electrode. The performance of the prototype electron gun measured using pulsed-beam tests is as follows: maximum beam current, 85.7 mA; beam focus size at the rotating anticathode, 0.79 mm × 0.13 mm. In DC beam tests, FWHM beam sizes were measured to be 0.65 mm × 0.08 mm at the rotating anticathode with a beam current of 45 mA. The beam current recently reached ∼60 mA with some thermal problems.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Sugimura, T.</dc:creator>
    <dc:creator>Ohsawa, S.</dc:creator>
    <dc:creator>Ikeda, M.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507066769</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The development of an electron gun for a high-brightness X-ray generator whose target brilliance is 60 kW mm−2 is reported.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ELECTRON GUN; DC BEAM; X-RAY GENERATOR</dc:subject>
    <dc:description>A prototype thermionic electron gun for a high-brightness X-ray generator has been developed. Its extraction voltage and design current are 60 kV and 100 mA (DC), respectively. The X-ray generator aims towards a maximum brilliance of 60 kW mm−2. The beam sizes at the rotating anticathode must therefore be within 1.0 mm × 0.1 mm and a small beam emittance is required. The fabricated electron gun optimizes an aperture grid and a Whenelt electrode. The performance of the prototype electron gun measured using pulsed-beam tests is as follows: maximum beam current, 85.7 mA; beam focus size at the rotating anticathode, 0.79 mm × 0.13 mm. In DC beam tests, FWHM beam sizes were measured to be 0.65 mm × 0.08 mm at the rotating anticathode with a beam current of 45 mA. The beam current recently reached ∼60 mA with some thermal problems.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Performance of an electron gun for a high-brightness X-ray generator</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>258</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>261</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5021">
    <title>Solution structures of RseA and its complex with RseB</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5021</link>
    <description>The bacterial envelope stress response, which is responsible for sensing stress signals in the envelope and for turning on the σE-dependent transcription, is modulated by the binding of RseB to RseA.  In this study, the solution structures of RseA and its complex with RseB were analyzed using circular dichroism and small-angle X-ray scattering. The periplasmic domain of RseA is unstructured and flexible when it is not bound to RseB. However, upon the formation of the stable complex with RseB, RseA induces conformational changes in RseB and, at the same time, RseA becomes more structured. Furthermore, it appears that some other undefined region of RseA, as well as the previously identified minimum region (amino acid 169–186), is also involved in RseB binding. It is thought that these conformational changes are relevant to the proteolytic cleavage of RseA and the modulation of envelope stress response.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Jin, K.S.</dc:creator>
    <dc:creator>Kim, D.Y.</dc:creator>
    <dc:creator>Rho, Y.</dc:creator>
    <dc:creator>Le, V.B.</dc:creator>
    <dc:creator>Kwon, E.</dc:creator>
    <dc:creator>Kim, K.K.</dc:creator>
    <dc:creator>Ree, M.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507066319</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Conformational changes of RseA and RseB were observed by circular dichroism and small-angle X-ray scattering upon the formation of their complex.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>[SIGMA]E SIGNALING PATHWAY; ENVELOPE STRESS RESPONSE; RSEA; RSEB; SMALL-ANGLE X-RAY SCATTERING; CIRCULAR DICHROISM</dc:subject>
    <dc:description>The bacterial envelope stress response, which is responsible for sensing stress signals in the envelope and for turning on the σE-dependent transcription, is modulated by the binding of RseB to RseA.  In this study, the solution structures of RseA and its complex with RseB were analyzed using circular dichroism and small-angle X-ray scattering. The periplasmic domain of RseA is unstructured and flexible when it is not bound to RseB. However, upon the formation of the stable complex with RseB, RseA induces conformational changes in RseB and, at the same time, RseA becomes more structured. Furthermore, it appears that some other undefined region of RseA, as well as the previously identified minimum region (amino acid 169–186), is also involved in RseB binding. It is thought that these conformational changes are relevant to the proteolytic cleavage of RseA and the modulation of envelope stress response.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Solution structures of RseA and its complex with RseB</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>219</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>222</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0358">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0358</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2008-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507066332</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-01-01</prism:publicationDate>
    <prism:startingPage>111</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>114</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5005">
    <title>Protein disulfide bond generation in Escherichia coli DsbB–DsbA</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5005</link>
    <description>Protein disulfide bond formation is catalyzed by a series of Dsb enzymes present in the periplasm of Escherichia coli. The crystal structure of the DsbB–DsbA–ubiquinone ternary complex provided important insights into mechanisms of the de novo disulfide bond generation cooperated by DsbB and ubiquinone and of the disulfide bond shuttle from DsbB to DsbA. The structural basis for prevention of the crosstalk between the DsbA–DsbB oxidative and the DsbC–DsbD reductive pathways has also been proposed.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Inaba, K.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950706061X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The crystal structure of the DsbB–DsbA–ubiquinone ternary complex has revealed a mechanism of protein disulfide bond generation in Escherichia coli.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROTEIN DISULFIDE BOND GENERATION; ESCHERICHIA COLI</dc:subject>
    <dc:description>Protein disulfide bond formation is catalyzed by a series of Dsb enzymes present in the periplasm of Escherichia coli. The crystal structure of the DsbB–DsbA–ubiquinone ternary complex provided important insights into mechanisms of the de novo disulfide bond generation cooperated by DsbB and ubiquinone and of the disulfide bond shuttle from DsbB to DsbA. The structural basis for prevention of the crosstalk between the DsbA–DsbB oxidative and the DsbC–DsbD reductive pathways has also been proposed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Protein disulfide bond generation in Escherichia coli DsbB–DsbA</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>199</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>201</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5015">
    <title>Crystal twinning of human MD-2 recognizing endotoxin cores of lipopolysaccharide</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5015</link>
    <description>Twinning of crystals causes overlapping of two or more reciprocal lattice points, and hence structure amplitudes for a single crystalline domain are hardly obtained from X-ray diffraction intensities. MD-2 protein forms a stable complex with Toll-like receptor 4 and recognizes bacterial lipopolysaccharide (LPS). Excessive immune responses activated by LPS cause septic shocks. Saccharide-trimmed human MD-2 crystallizes in the tetragonal form with apparent Laue symmetry of 4/mmm, and diffraction intensities from these crystals indicate crystal twinning. The crystal consists of two different domains, A and B. The cA axis of domain A coincides with the cB axis of domain B with a smaller lattice, and the aA axis corresponds to the (aB + bB) axis. This twinning severely imposes difficulty in structure determination. Through optimization of cryoprotectant, domain A was thoroughly transformed into domain B. The crystal containing only domain B is in space group P41212 with one MD-2 molecule in the asymmetric unit. The structure of this form of MD-2 as well as its complex with antiendotoxic lipid IVa was successfully determined using the multiple isomorphous replacement method.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ohto, U.</dc:creator>
    <dc:creator>Satow, Y.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507056531</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Twinned crystals of humaan MD-2 are transformed into single crystals with cryoprotectant optimization.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CRYSTAL TWINNING; INNATE IMMUNITY; ENDOTOXIN</dc:subject>
    <dc:description>Twinning of crystals causes overlapping of two or more reciprocal lattice points, and hence structure amplitudes for a single crystalline domain are hardly obtained from X-ray diffraction intensities. MD-2 protein forms a stable complex with Toll-like receptor 4 and recognizes bacterial lipopolysaccharide (LPS). Excessive immune responses activated by LPS cause septic shocks. Saccharide-trimmed human MD-2 crystallizes in the tetragonal form with apparent Laue symmetry of 4/mmm, and diffraction intensities from these crystals indicate crystal twinning. The crystal consists of two different domains, A and B. The cA axis of domain A coincides with the cB axis of domain B with a smaller lattice, and the aA axis corresponds to the (aB + bB) axis. This twinning severely imposes difficulty in structure determination. Through optimization of cryoprotectant, domain A was thoroughly transformed into domain B. The crystal containing only domain B is in space group P41212 with one MD-2 molecule in the asymmetric unit. The structure of this form of MD-2 as well as its complex with antiendotoxic lipid IVa was successfully determined using the multiple isomorphous replacement method.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Crystal twinning of human MD-2 recognizing endotoxin cores of lipopolysaccharide</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>262</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>265</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5032">
    <title>Fragment approaches in structure-based drug discovery</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5032</link>
    <description>There has been considerable interest recently in what is known as `fragment-based lead discovery'. The novel feature of the approach is to begin with small low-affinity compounds. The main advantage is that a larger potential chemical diversity can be sampled with fewer compounds, which is particularly important for new target classes. The approach relies on careful design of the fragment library, a method that can detect binding of the fragment to the protein target, determination of the structure of the fragment bound to the target, and the conventional use of structural information to guide compound optimization. In this article the methods are reviewed, and experiences in fragment-based discovery of lead series of compounds against kinases such as PDK1 and ATPases such as Hsp90 are discussed. The examples illustrate some of the key benefits and issues of the approach and also provide anecdotal examples of the patterns seen in selectivity and the binding mode of fragments across different protein targets.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hubbard, R.E.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950705666X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Fragment-based methods are successfully generating novel and selective drug-like inhibitors of protein targets, with a number of groups reporting compounds entering clinical trials. This paper summarizes the key features of the approach as one of the tools in structure-guided drug discovery.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>There has been considerable interest recently in what is known as `fragment-based lead discovery'. The novel feature of the approach is to begin with small low-affinity compounds. The main advantage is that a larger potential chemical diversity can be sampled with fewer compounds, which is particularly important for new target classes. The approach relies on careful design of the fragment library, a method that can detect binding of the fragment to the protein target, determination of the structure of the fragment bound to the target, and the conventional use of structural information to guide compound optimization. In this article the methods are reviewed, and experiences in fragment-based discovery of lead series of compounds against kinases such as PDK1 and ATPases such as Hsp90 are discussed. The examples illustrate some of the key benefits and issues of the approach and also provide anecdotal examples of the patterns seen in selectivity and the binding mode of fragments across different protein targets.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Fragment approaches in structure-based drug discovery</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>227</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>230</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5028">
    <title>Mail-in data collection at SPring-8 protein crystallography beamlines</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5028</link>
    <description>A mail-in data collection system makes it possible for beamline users to collect diffraction data without visiting a synchrotron facility. In the mail-in data collection system at SPring-8, users pack crystals into sample trays and send the trays to SPring-8 via a courier service as the first step. Next, the user specifies measurement conditions and checks the diffraction images via the Internet. The user can also collect diffraction data using an automated sample changer robot and beamline control software. For distant users there is a newly developed data management system, D-Cha. D-Cha provides a graphical user interface that enables the user to specify the experimental conditions for samples and to check and download the diffraction images using a web browser. This system is now in routine operation and is contributing to high-throughput beamline operation.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Okazaki, N.</dc:creator>
    <dc:creator>Hasegawa, K.</dc:creator>
    <dc:creator>Ueno, G.</dc:creator>
    <dc:creator>Murakami, H.</dc:creator>
    <dc:creator>Kumasaka, T.</dc:creator>
    <dc:creator>Yamamoto, M.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507064679</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A mail-in data collection system at SPring-8, which is a web application with automated beamline operation, has been developed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MAIL-IN DATA COLLECTION; HIGH-THROUGHPUT DATA COLLECTION; BEAMLINE AUTOMATION; WEB APPLICATION; DATABASE SYSTEM</dc:subject>
    <dc:description>A mail-in data collection system makes it possible for beamline users to collect diffraction data without visiting a synchrotron facility. In the mail-in data collection system at SPring-8, users pack crystals into sample trays and send the trays to SPring-8 via a courier service as the first step. Next, the user specifies measurement conditions and checks the diffraction images via the Internet. The user can also collect diffraction data using an automated sample changer robot and beamline control software. For distant users there is a newly developed data management system, D-Cha. D-Cha provides a graphical user interface that enables the user to specify the experimental conditions for samples and to check and download the diffraction images using a web browser. This system is now in routine operation and is contributing to high-throughput beamline operation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Mail-in data collection at SPring-8 protein crystallography beamlines</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>288</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>291</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5022">
    <title>An optimal exposure strategy for cryoprotected virus crystals with lattice constants greater than 1000 Å</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5022</link>
    <description>Studies of icosahedral virus capsids provide insights into the function of supramolecular machines. Virus capsid crystals have exceptionally large unit cells; as a result, they diffract weakly compared with protein crystals. HK97 is a dsDNA lambda-like bacteriophage whose 13 MDa capsid expands from 550 Å to 650 Å with large subunit conformational changes during virus maturation. The HK97 penultimate maturation intermediate was crystallized in a tetragonal unit cell that has lattice constants of 1010 Å × 1010 Å × 730 Å. The crystals could be cryoprotected, but diffracted to a modest resolution of 5 Å at a bending-magnet beamline. When these crystals were optimally exposed with two orders-of-magnitude more photons from a new insertion-device beamline, data extending to better than 3.8 Å resolution were obtained. Here, the strategies to collect and process such data are described. These strategies can be adapted for other crystals with large unit cells and for microcrystals.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Gan, L.</dc:creator>
    <dc:creator>Johnson, J.E.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507064813</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Many supramolecular complexes form crystals that have lattice constants of the order of 1000 Å. An optimized method for data collection and processing is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>VIRUS CRYSTALS; BACTERIOPHAGE HK97; INSERTION-DEVICE BEAMLINES</dc:subject>
    <dc:description>Studies of icosahedral virus capsids provide insights into the function of supramolecular machines. Virus capsid crystals have exceptionally large unit cells; as a result, they diffract weakly compared with protein crystals. HK97 is a dsDNA lambda-like bacteriophage whose 13 MDa capsid expands from 550 Å to 650 Å with large subunit conformational changes during virus maturation. The HK97 penultimate maturation intermediate was crystallized in a tetragonal unit cell that has lattice constants of 1010 Å × 1010 Å × 730 Å. The crystals could be cryoprotected, but diffracted to a modest resolution of 5 Å at a bending-magnet beamline. When these crystals were optimally exposed with two orders-of-magnitude more photons from a new insertion-device beamline, data extending to better than 3.8 Å resolution were obtained. Here, the strategies to collect and process such data are described. These strategies can be adapted for other crystals with large unit cells and for microcrystals.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>An optimal exposure strategy for cryoprotected virus crystals with lattice constants greater than 1000 Å</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>223</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>226</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5033">
    <title>High-throughput operation of sample-exchange robots with double tongs at the Photon Factory beamlines</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5033</link>
    <description>Sample-exchange robots that can exchange cryo-pins bearing protein crystals out of experimental hutches according to user instructions have been developed. The robots were designed based on the SAM (Stanford Synchrotron Research Laboratory automated mounting) system. In order to reduce the time required for the sample exchange, the single tongs of the SAM system were modified and a double-tongs system that can hold two cryo-pins at the same time was developed. Robots with double tongs can move to the goniometer head holding the next cryo-pin with one set of tongs, dismount the experimented cryo-pin with the other set, and then mount the next pin onto the goniometer head without leaving the diffractometer area. Two different types of tongs have been installed: single tongs at beamlines BL-5A and AR-NW12A, and a double-tongs system at beamline BL-17A of the Photon Factory. The same graphical user interface software for operation of the sample-exchange robots is used at all beamlines, however, so that users do not need to consider differences between the systems. In a trial, the robot with double tongs could exchange samples within 10 s.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hiraki, M.</dc:creator>
    <dc:creator>Watanabe, S.</dc:creator>
    <dc:creator>pHonda, N.</dc:creator>
    <dc:creator>Yamada, Y.</dc:creator>
    <dc:creator>Matsugaki, N.</dc:creator>
    <dc:creator>Igarashi, N.</dc:creator>
    <dc:creator>Gaponov, Y.</dc:creator>
    <dc:creator>Wakatsuki, S.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507064680</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Sample-exchange robots with a double-tongs system that could exchange samples within 10 s have been developed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAMPLE-EXCHANGE ROBOT; PROTEIN CRYSTALLOGRAPHY; AUTOMATED SYSTEM; DIFFRACTION EXPERIMENT</dc:subject>
    <dc:description>Sample-exchange robots that can exchange cryo-pins bearing protein crystals out of experimental hutches according to user instructions have been developed. The robots were designed based on the SAM (Stanford Synchrotron Research Laboratory automated mounting) system. In order to reduce the time required for the sample exchange, the single tongs of the SAM system were modified and a double-tongs system that can hold two cryo-pins at the same time was developed. Robots with double tongs can move to the goniometer head holding the next cryo-pin with one set of tongs, dismount the experimented cryo-pin with the other set, and then mount the next pin onto the goniometer head without leaving the diffractometer area. Two different types of tongs have been installed: single tongs at beamlines BL-5A and AR-NW12A, and a double-tongs system at beamline BL-17A of the Photon Factory. The same graphical user interface software for operation of the sample-exchange robots is used at all beamlines, however, so that users do not need to consider differences between the systems. In a trial, the robot with double tongs could exchange samples within 10 s.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>High-throughput operation of sample-exchange robots with double tongs at the Photon Factory beamlines</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>300</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>303</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5010">
    <title>Deduced catalytic mechanism of d-amino acid amidase from Ochrobactrum anthropi SV3</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5010</link>
    <description>d-Amino acid amidase (DAA) from Ochrobactrum anthropi SV3 catalyzes d-stereospecific hydrolysis of amino acid amides. DAA has attracted attention as a catalyst for the stereospecific production of d-amino acids, although the mechanism that drives the reaction has not been clear. Previously, the structure of DAA was classified into two types, a substrate-bound state with an ordered Ω loop, and a ground state with a disordered Ω loop. Because the binding of the substrate facilitates ordering, this transition was regarded to be induced fit motion. The angles and distances of hydrogen bonds at Tyr149 Oη, Ser60 Oγ and Lys63 Nζ revealed that Tyr149 Oη donates an H atom to a water molecule in the substrate-bound state, and that Tyr149 Oη donates an H atom to Ser60 Oγ or Lys63 Nζ in the ground state. Taking into consideration the locations of the H atoms of Tyr149 Oη, Ser60 Oγ and Lys63 Nζ, a catalytic mechanism of DAA activity is presented, wherein a shift of an H atom at Tyr149 Oη in the substrate-bound versus the ground state plays a significant role in the reaction. This mechanism explains well why acylation proceeds and deacylation does not proceed in the substrate-bound state.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Okazaki, S.</dc:creator>
    <dc:creator>Suzuki, A.</dc:creator>
    <dc:creator>Komeda, H.</dc:creator>
    <dc:creator>Asano, Y.</dc:creator>
    <dc:creator>Yamane, T.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507064655</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The catalytic mechanism of d-amino acid amidase from Ochrobactrum anthropi SV3 has been deduced.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CATALYTIC MECHANISMS; STEREOSPECIFIC HYDROLYSIS; D-AMINO ACID AMIDASE</dc:subject>
    <dc:description>d-Amino acid amidase (DAA) from Ochrobactrum anthropi SV3 catalyzes d-stereospecific hydrolysis of amino acid amides. DAA has attracted attention as a catalyst for the stereospecific production of d-amino acids, although the mechanism that drives the reaction has not been clear. Previously, the structure of DAA was classified into two types, a substrate-bound state with an ordered Ω loop, and a ground state with a disordered Ω loop. Because the binding of the substrate facilitates ordering, this transition was regarded to be induced fit motion. The angles and distances of hydrogen bonds at Tyr149 Oη, Ser60 Oγ and Lys63 Nζ revealed that Tyr149 Oη donates an H atom to a water molecule in the substrate-bound state, and that Tyr149 Oη donates an H atom to Ser60 Oγ or Lys63 Nζ in the ground state. Taking into consideration the locations of the H atoms of Tyr149 Oη, Ser60 Oγ and Lys63 Nζ, a catalytic mechanism of DAA activity is presented, wherein a shift of an H atom at Tyr149 Oη in the substrate-bound versus the ground state plays a significant role in the reaction. This mechanism explains well why acylation proceeds and deacylation does not proceed in the substrate-bound state.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Deduced catalytic mechanism of d-amino acid amidase from Ochrobactrum anthropi SV3</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>250</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>253</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5008">
    <title>Key steps in the structure-based optimization of the hepatitis C virus NS3/4A protease inhibitor SCH503034</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5008</link>
    <description>The structures of both native and S139A holo-HCV NS3/4A protease domain were solved to high resolution. Subsequently, structures were determined for a series of ketoamide inhibitors in complex with the protease. The changes in the inhibitor potency were correlated with changes in the buried surface area upon binding the inhibitor to the active site. The largest contributions to the binding energy arise from the hydrophobic interactions of the P1 and P2 groups as they bind to the S1 and S2 pockets. This correlation of the changes in potency with increased buried surface area contributed directly to the design of a potent tripeptide inhibitor of the HCV NS3/4A protease, which is currently in clinical trials.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Madison, V.</dc:creator>
    <dc:creator>Prongay, A.J.</dc:creator>
    <dc:creator>Guo, Z.</dc:creator>
    <dc:creator>Yao, N.</dc:creator>
    <dc:creator>Pichardo, J.</dc:creator>
    <dc:creator>Fischmann, T.</dc:creator>
    <dc:creator>Strickland, C.</dc:creator>
    <dc:creator>Myers Jr, J.</dc:creator>
    <dc:creator>Weber, P.C.</dc:creator>
    <dc:creator>Beyer, B.M.</dc:creator>
    <dc:creator>Ingram, R.</dc:creator>
    <dc:creator>Hong, Z.</dc:creator>
    <dc:creator>Prosise, W.W.</dc:creator>
    <dc:creator>Ramanathan, L.</dc:creator>
    <dc:creator>Taremi, S.S.</dc:creator>
    <dc:creator>Yarosh-Tomaine, T.</dc:creator>
    <dc:creator>Zhang, R.</dc:creator>
    <dc:creator>Senior, M.</dc:creator>
    <dc:creator>Yang, R.-S.</dc:creator>
    <dc:creator>Malcolm, B.</dc:creator>
    <dc:creator>Arasappan, A.</dc:creator>
    <dc:creator>Bennett, F.</dc:creator>
    <dc:creator>Bogen, S.L.</dc:creator>
    <dc:creator>Chen, K.</dc:creator>
    <dc:creator>Jao, E.</dc:creator>
    <dc:creator>Liu, Y.-T.</dc:creator>
    <dc:creator>Lovey, R.G.</dc:creator>
    <dc:creator>Saksena, A.K.</dc:creator>
    <dc:creator>Venkatraman, S.</dc:creator>
    <dc:creator>Girijavallabhan, V.</dc:creator>
    <dc:creator>Njoroge, F.G.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507064229</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Crystal structures of protease/inhibitor complexes guided optimization of the buried nonpolar surface area thereby maximizing hydrophobic binding. The resulting potent tripeptide inhibitor is in clinical trials.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HCV PROTEASE; STRUCTURE-BASED DESIGN; KETOAMIDES; HYDROPHOBIC BINDING</dc:subject>
    <dc:description>The structures of both native and S139A holo-HCV NS3/4A protease domain were solved to high resolution. Subsequently, structures were determined for a series of ketoamide inhibitors in complex with the protease. The changes in the inhibitor potency were correlated with changes in the buried surface area upon binding the inhibitor to the active site. The largest contributions to the binding energy arise from the hydrophobic interactions of the P1 and P2 groups as they bind to the S1 and S2 pockets. This correlation of the changes in potency with increased buried surface area contributed directly to the design of a potent tripeptide inhibitor of the HCV NS3/4A protease, which is currently in clinical trials.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Key steps in the structure-based optimization of the hepatitis C virus NS3/4A protease inhibitor SCH503034</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>204</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>207</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5009">
    <title>A degradation signal recognition in prokaryotes</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5009</link>
    <description>The degradation of ssrA-tagged substrates in prokaryotes is conducted by a subset of ATP-dependent proteases, including ClpXP complex. More than 630 sequences of ssrA have been identified from 514 species, and are conserved in a wide range of prokaryotes. SspB protein markedly stimulates the degradation of these ssrA-tagged substrates by the ClpXP proteolytic machine. The dimeric SspB protein is composed of a compact ssrA-binding domain, which has a dimerization surface and a flexible C-terminal tail with a ClpX-binding motif at its very end. Since SspB is an adaptor protein for the ClpXP complex, designed mutagenesis, fluorescence spectroscopy, biochemistry and X-ray crystallography have been used to investigate the mechanism of delivery of ssrA-tagged proteins. In this paper the structural basis of ssrA-tag recognition by ClpX and SspB, as well as SspB-tail recognition by ZBD, is described.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Park, E.Y.</dc:creator>
    <dc:creator>Song, H.K.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507062826</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Substrates tagged with ssrA are recognized and degraded by a subset of the Clp family, ATP-dependent proteases in prokaryotes. This paper describes the mechanism of intracellular breakdown of ssrA-tagged substrates by ClpXP and its adaptor protein, SspB.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ADAPTOR; CLPX; CLPXP COMPLEX; SSPB; SSRA; ZINC-BINDING DOMAIN</dc:subject>
    <dc:description>The degradation of ssrA-tagged substrates in prokaryotes is conducted by a subset of ATP-dependent proteases, including ClpXP complex. More than 630 sequences of ssrA have been identified from 514 species, and are conserved in a wide range of prokaryotes. SspB protein markedly stimulates the degradation of these ssrA-tagged substrates by the ClpXP proteolytic machine. The dimeric SspB protein is composed of a compact ssrA-binding domain, which has a dimerization surface and a flexible C-terminal tail with a ClpX-binding motif at its very end. Since SspB is an adaptor protein for the ClpXP complex, designed mutagenesis, fluorescence spectroscopy, biochemistry and X-ray crystallography have been used to investigate the mechanism of delivery of ssrA-tagged proteins. In this paper the structural basis of ssrA-tag recognition by ClpX and SspB, as well as SspB-tail recognition by ZBD, is described.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A degradation signal recognition in prokaryotes</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>246</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>249</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5035">
    <title>Complex of human neutrophil elastase with 1/2SLPI</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5035</link>
    <description>SLPI (secretory leukocyte protease inhibitor) is a 107-residue non-glycosylated protease inhibitor, which inhibits a wide range of serine proteases, trypsin, chymotrypsin, neutrophil elastase, chymase and cathepsin G. X-ray crystallographic analyses have shown that SLPI comprises two separate domains of similar architecture [Grütter, Fendrich, Huber &amp; Bode (1988), EMBO J. 7, 345–351] and the C-terminal domain interacts with bovine α-chymotrypsin. In order to understand SLPI's multiple functions against various serine proteases, the complex HNE (human neutrophil elastase) has been co-crystallized with 1/2SLPI (recombinant C-terminal domain of SLPI; Arg58–Ala107), which has a biological activity similar to full SLPI. The 1/2SLPI and HNE complex structure was solved at 1.7 Å resolution, and compared with the interaction mechanism of elafin, which is a specific inhibitor of elastase. It was found that P1 Leu72i and six hydrogen bonds between the main chains in the primary contact region have sufficient ability to inhibit HNE and PPE (porcine pancreatic elastase), and P5 Tyr68i is important in increasing the selectivity of 1/2SLPI against HNE. The mechanisms of the functions of SLPI are relatively unknown, but the current study could help understand the selectivity of SLPI against HNE and PPE.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Koizumi, M.</dc:creator>
    <dc:creator>Fujino, A.</dc:creator>
    <dc:creator>Fukushima, K.</dc:creator>
    <dc:creator>Kamimura, T.</dc:creator>
    <dc:creator>Takimoto-Kamimura, M.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507060670</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The 1/2SLPI and HNE complex structure was solved at 1.7 Å resolution and compared with the interaction mechanism of elafin.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ELASTASE INHIBITOR; CRYSTAL STRUCTURE; SLPI</dc:subject>
    <dc:description>SLPI (secretory leukocyte protease inhibitor) is a 107-residue non-glycosylated protease inhibitor, which inhibits a wide range of serine proteases, trypsin, chymotrypsin, neutrophil elastase, chymase and cathepsin G. X-ray crystallographic analyses have shown that SLPI comprises two separate domains of similar architecture [Grütter, Fendrich, Huber &amp; Bode (1988), EMBO J. 7, 345–351] and the C-terminal domain interacts with bovine α-chymotrypsin. In order to understand SLPI's multiple functions against various serine proteases, the complex HNE (human neutrophil elastase) has been co-crystallized with 1/2SLPI (recombinant C-terminal domain of SLPI; Arg58–Ala107), which has a biological activity similar to full SLPI. The 1/2SLPI and HNE complex structure was solved at 1.7 Å resolution, and compared with the interaction mechanism of elafin, which is a specific inhibitor of elastase. It was found that P1 Leu72i and six hydrogen bonds between the main chains in the primary contact region have sufficient ability to inhibit HNE and PPE (porcine pancreatic elastase), and P5 Tyr68i is important in increasing the selectivity of 1/2SLPI against HNE. The mechanisms of the functions of SLPI are relatively unknown, but the current study could help understand the selectivity of SLPI against HNE and PPE.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Complex of human neutrophil elastase with 1/2SLPI</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>308</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>311</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5037">
    <title>Crystallization and evaluation of hen egg-white lysozyme crystals for protein pH titration in the crystalline state</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5037</link>
    <description>To observe the ionized status of the amino acid residues in proteins at different pH (protein pH titration in the crystalline state) by neutron diffraction, hen egg-white lysozyme was crystallized over a wide pH range (2.5–8.0). Crystallization phase diagrams at pH 2.5, 6.0 and 7.5 were determined. At pH &lt; 4.5 the border between the metastable region and the nucleation region shifted to the left (lower precipitant concentration) in the phase diagram, and at pH &gt; 4.5 the border shifted to the right (higher precipitant concentration). The qualities of these crystals were characterized using the Wilson plot method. The qualities of all crystals at different pH were more or less equivalent (B-factor values within 25–40). It is expected that neutron diffraction analysis of these crystals of different pH provides equivalent data in quality for discussions of protein pH titration in the crystalline state of hen egg-white lysozyme.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Iwai, W.</dc:creator>
    <dc:creator>Yagi, D.</dc:creator>
    <dc:creator>Ishikawa, T.</dc:creator>
    <dc:creator>Ohnishi, Y.</dc:creator>
    <dc:creator>Tanaka, I.</dc:creator>
    <dc:creator>Niimura, N.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507059559</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Hen egg-white lysozyme was crystallized over a wide pH range (2.5–8.0) and the quality of the crystals was characterized. Crystallization phase diagrams at pH 2.5, 6.0 and 7.5 were determined</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>NEUTRON DIFFRACTION; CRYSTALLIZATION PHASE DIAGRAM; PH TITRATION; LYSOZYME; QUALITY OF CRYSTAL</dc:subject>
    <dc:description>To observe the ionized status of the amino acid residues in proteins at different pH (protein pH titration in the crystalline state) by neutron diffraction, hen egg-white lysozyme was crystallized over a wide pH range (2.5–8.0). Crystallization phase diagrams at pH 2.5, 6.0 and 7.5 were determined. At pH &lt; 4.5 the border between the metastable region and the nucleation region shifted to the left (lower precipitant concentration) in the phase diagram, and at pH &gt; 4.5 the border shifted to the right (higher precipitant concentration). The qualities of these crystals were characterized using the Wilson plot method. The qualities of all crystals at different pH were more or less equivalent (B-factor values within 25–40). It is expected that neutron diffraction analysis of these crystals of different pH provides equivalent data in quality for discussions of protein pH titration in the crystalline state of hen egg-white lysozyme.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Crystallization and evaluation of hen egg-white lysozyme crystals for protein pH titration in the crystalline state</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>312</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>315</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5025">
    <title>Hydrogen bonds of DsrD protein revealed by neutron crystallography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5025</link>
    <description>The features of hydrogen bonds in DsrD protein from sulfate-reducing bacteria have been investigated by neutron protein crystallography. The function of DsrD has not yet been elucidated clearly, but its X-ray crystal structure revealed that it comprises a winged-helix motif and shows the highest structural homology to the DNA-binding proteins. Since any neutron structure of a DNA recognition protein has not yet been obtained, here detailed information on the hydrogen bonds in the winged-helix-motif protein is given and the following features found. (i) The number of hydrogen bonds per amino acid of DsrD is relatively fewer than for other proteins for which neutron structures were determined previously. (ii) Hydrogen bonds are localized between main-chain and main-chain atoms; there are few hydrogen bonds between main-chain and side-chain atoms and between side-chain and side-chain atoms. (iii) Hydrogen bonds inducted by protonation of specific amino acid residues (Glu50) seem to play an essential role in the dimerization of DsrD. The former two points are related to the function of the DNA-binding protein; the three-dimensional structure was mainly constructed by hydrogen bonds in main chains, while the side chains appeared to be used for another role. The latter point would be expected to contribute to the crystal growth of DsrD.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Chatake, T.</dc:creator>
    <dc:creator>Higuchi, Y.</dc:creator>
    <dc:creator>Mizuno, N.</dc:creator>
    <dc:creator>Tanaka, I.</dc:creator>
    <dc:creator>Niimura, N.</dc:creator>
    <dc:creator>Morimoto, Y.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507058979</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Hydrogen bonds of DNA-binding protein DsrD have been determined by neutron diffraction. In terms of proton donors and acceptors, DsrD protein shows striking differences from other proteins.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DSRD; DNA-BINDING PROTEIN; HYDROGEN BOND; NEUTRON CRYSTALLOGRAPHY</dc:subject>
    <dc:description>The features of hydrogen bonds in DsrD protein from sulfate-reducing bacteria have been investigated by neutron protein crystallography. The function of DsrD has not yet been elucidated clearly, but its X-ray crystal structure revealed that it comprises a winged-helix motif and shows the highest structural homology to the DNA-binding proteins. Since any neutron structure of a DNA recognition protein has not yet been obtained, here detailed information on the hydrogen bonds in the winged-helix-motif protein is given and the following features found. (i) The number of hydrogen bonds per amino acid of DsrD is relatively fewer than for other proteins for which neutron structures were determined previously. (ii) Hydrogen bonds are localized between main-chain and main-chain atoms; there are few hydrogen bonds between main-chain and side-chain atoms and between side-chain and side-chain atoms. (iii) Hydrogen bonds inducted by protonation of specific amino acid residues (Glu50) seem to play an essential role in the dimerization of DsrD. The former two points are related to the function of the DNA-binding protein; the three-dimensional structure was mainly constructed by hydrogen bonds in main chains, while the side chains appeared to be used for another role. The latter point would be expected to contribute to the crystal growth of DsrD.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Hydrogen bonds of DsrD protein revealed by neutron crystallography</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>277</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>280</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ml5226">
    <title>Cost-effective upgrade of a focusing system for inelastic X-ray scattering experiments under high pressure</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ml5226</link>
    <description>Inelastic X-ray scattering (IXS) is a powerful technique capable of probing the dynamic behavior and electronic structure of materials. For IXS experiments under high pressure up to the megabar range using state-of-the-art diamond-anvil-cell technology, the sample volume is limited to the order of 1 × 10−3 mm3 for which a beam focus of the same order and less is often required. In this paper a scheme utilizing a set of low-cost and compact Kirkpatrick–Baez mirrors for upgrading the existing optical system of the Taiwan IXS beamline at SPring-8 is described. The scheme as implemented improves the focus to 13 µm × 16 µm (horizontal × vertical) with a transmission of up to 72% and a flux density gain of over 30 times, which has enhanced substantially the efficiency of the beamline for high-pressure research.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Huang, C.-Y.</dc:creator>
    <dc:creator>Cai, Y.Q.</dc:creator>
    <dc:creator>Hiraoka, N.</dc:creator>
    <dc:creator>Chen, C.-C.</dc:creator>
    <dc:creator>Chung, S.-C.</dc:creator>
    <dc:creator>Song, Y.-F.</dc:creator>
    <dc:creator>Tsang, K.-L.</dc:creator>
    <dc:date>2008-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507055884</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>This paper describes a scheme utilizing a set of low-cost and compact Kirkpatrick–Baez mirrors for upgrading the optical system of the Taiwan Inelastic X-ray Scattering beamline at SPring-8 for high-pressure experiments using diamond-anvil cells. The scheme as implemented improves the focus to 13 µm × 16 µm with transmission of up to 72%.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>KIRKPATRICK-BAEZ MIRRORS; INELASTIC X-RAY SCATTERING; DIAMOND-ANVIL CELL</dc:subject>
    <dc:description>Inelastic X-ray scattering (IXS) is a powerful technique capable of probing the dynamic behavior and electronic structure of materials. For IXS experiments under high pressure up to the megabar range using state-of-the-art diamond-anvil-cell technology, the sample volume is limited to the order of 1 × 10−3 mm3 for which a beam focus of the same order and less is often required. In this paper a scheme utilizing a set of low-cost and compact Kirkpatrick–Baez mirrors for upgrading the existing optical system of the Taiwan IXS beamline at SPring-8 is described. The scheme as implemented improves the focus to 13 µm × 16 µm (horizontal × vertical) with a transmission of up to 72% and a flux density gain of over 30 times, which has enhanced substantially the efficiency of the beamline for high-pressure research.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Cost-effective upgrade of a focusing system for inelastic X-ray scattering experiments under high pressure</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-01-01</prism:publicationDate>
    <prism:startingPage>50</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>54</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5016">
    <title>Crystallization of the Atg12–Atg5 conjugate bound to Atg16 by the free-interface diffusion method</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5016</link>
    <description>Autophagy mediates the bulk degradation of cytoplasmic components in lysosomes/vacuoles. Five autophagy-related (Atg) proteins are involved in a ubiquitin-like protein conjugation system. Atg12 is conjugated to its sole target, Atg5, by two enzymes, Atg7 and Atg10. The Atg12–Atg5 conjugates form a multimeric complex with Atg16. Formation of the Atg12–Atg5–Atg16 ternary complex is crucial for the functions of these proteins on autophagy. Here, the expression, purification and crystallization of the Atg12–Atg5 conjugate bound to the N-terminal region of Atg16 (Atg16N) are reported. The Atg12–Atg5 conjugates were formed by co-expressing Atg5, Atg7, Atg10 and Atg12 in Eschericia coli. The Atg12–Atg5–Atg16N ternary complex was formed by mixing purified Atg12–Atg5 conjugates and Atg16N, and was further purified by gel-filtration chromatography. Crystallization screening was performed by the free-interface diffusion method. Using obtained microcrystals as seeds, large crystals for diffraction data collection were obtained by the sitting-drop vapour-diffusion method. The crystal contained one ternary complex per asymmetric unit, and diffracted to 2.6 Å resolution.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Noda, N.N.</dc:creator>
    <dc:creator>Fujioka, Y.</dc:creator>
    <dc:creator>Ohsumi, Y.</dc:creator>
    <dc:creator>Inagaki, F.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507054799</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The Atg12–Atg5 conjugate was prepared by in vivo reconstitution and was crystallized with Atg16 using the free-interface diffusion method.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AUTOPHAGY; UBIQUITIN-LIKE CONJUGATION; CRYSTALLIZATION; FREE-INTERFACE DIFFUSION METHOD</dc:subject>
    <dc:description>Autophagy mediates the bulk degradation of cytoplasmic components in lysosomes/vacuoles. Five autophagy-related (Atg) proteins are involved in a ubiquitin-like protein conjugation system. Atg12 is conjugated to its sole target, Atg5, by two enzymes, Atg7 and Atg10. The Atg12–Atg5 conjugates form a multimeric complex with Atg16. Formation of the Atg12–Atg5–Atg16 ternary complex is crucial for the functions of these proteins on autophagy. Here, the expression, purification and crystallization of the Atg12–Atg5 conjugate bound to the N-terminal region of Atg16 (Atg16N) are reported. The Atg12–Atg5 conjugates were formed by co-expressing Atg5, Atg7, Atg10 and Atg12 in Eschericia coli. The Atg12–Atg5–Atg16N ternary complex was formed by mixing purified Atg12–Atg5 conjugates and Atg16N, and was further purified by gel-filtration chromatography. Crystallization screening was performed by the free-interface diffusion method. Using obtained microcrystals as seeds, large crystals for diffraction data collection were obtained by the sitting-drop vapour-diffusion method. The crystal contained one ternary complex per asymmetric unit, and diffracted to 2.6 Å resolution.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Crystallization of the Atg12–Atg5 conjugate bound to Atg16 by the free-interface diffusion method</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>266</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>268</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5004">
    <title>Trimeric structure and conformational equilibrium of M-ficolin fibrinogen-like domain</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5004</link>
    <description>Ficolins are pathogen-recognition molecules in innate immune systems. The crystal structure of the human M-ficolin recognition domain (FD1) has been determined at 1.9 Å resolution, and compared with that of the human fibrinogen γ fragment, tachylectin-5A, L-ficolin and H-ficolin. The overall structure of FD1 is similar to that of the other proteins, although the peptide bond between Asp282 and Cys283, which is in a predicted ligand-binding site, is a normal trans bond, unlike the cases of the other proteins. Analysis of the pH-dependent ligand-binding activity of FD1 in solution suggested that a conformational equilibrium between active and non-active forms in the ligand-binding region, involving cis-trans isomerization of the Asp282—Cys283 peptide bond, contributes to the discrimination between self and non-self, and that the pKa values of His284 are 6.1 and 6.3 in the active and non-active forms, respectively.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Tanio, M.</dc:creator>
    <dc:creator>Kondo, S.</dc:creator>
    <dc:creator>Sugio, S.</dc:creator>
    <dc:creator>Kohno, T.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507054325</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The crystal structure and ligand-binding study of M-ficolin provides an insight into its discrimination mechanism between self and non-self.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FICOLIN; INNATE IMMUNITY; CONFORMATIONAL EQUILIBRIUM</dc:subject>
    <dc:description>Ficolins are pathogen-recognition molecules in innate immune systems. The crystal structure of the human M-ficolin recognition domain (FD1) has been determined at 1.9 Å resolution, and compared with that of the human fibrinogen γ fragment, tachylectin-5A, L-ficolin and H-ficolin. The overall structure of FD1 is similar to that of the other proteins, although the peptide bond between Asp282 and Cys283, which is in a predicted ligand-binding site, is a normal trans bond, unlike the cases of the other proteins. Analysis of the pH-dependent ligand-binding activity of FD1 in solution suggested that a conformational equilibrium between active and non-active forms in the ligand-binding region, involving cis-trans isomerization of the Asp282—Cys283 peptide bond, contributes to the discrimination between self and non-self, and that the pKa values of His284 are 6.1 and 6.3 in the active and non-active forms, respectively.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Trimeric structure and conformational equilibrium of M-ficolin fibrinogen-like domain</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>243</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>245</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pf0055">
    <title>Engines of Discovery (A Century of Particle Accelerators). By Andrew Sessler and Edmund Wilson. Pp. ix + 212. Hackensack, NJ: World Scientific Publishing 2007. Price: (hardcover) GBP 29, USD 54. ISBN 978-981-270-070-4.</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pf0055</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Suller, V.P.</dc:creator>
    <dc:date>2008-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507052521</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Engines of Discovery (A Century of Particle Accelerators). By Andrew Sessler and Edmund Wilson. Pp. ix + 212. Hackensack, NJ: World Scientific Publishing 2007. Price: (hardcover) GBP 29, USD 54. ISBN 978-981-270-070-4.</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-01-01</prism:publicationDate>
    <prism:startingPage>109</prism:startingPage>
    <prism:section>book reviews</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>110</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys5024">
    <title>Structural insights into the similar modes of Nrf2 transcription factor recognition by the cytoplasmic repressor Keap1</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys5024</link>
    <description>The cytoplasmic repressor Keap1 regulates the function of transcription factor Nrf2 which plays critical roles in oxidative and xenobiotic stresses. The Neh2 domain of Nrf2 interacts with Keap1 at the bottom region of the Kelch/β-propeller domain which is formed by double-glycine repeat and C-terminal region domains (Keap1-DC). The structure of Keap1-DC complexed with an Nrf2 peptide containing a conserved DLG motif has been determined at 1.9 Å resolution. The Keap1-bound DLG peptide possesses a hairpin conformation, and it binds to the Keap1 protein at the bottom region of the β-propeller domain. The intermolecular interaction occurs through their complementary electrostatic interactions. Comparison of the present structure with the recently reported Keap1-DC complex structure suggests that the DLG and ETGE motifs of Neh2 in Nrf2 bind to Keap1 in a similar manner but with different binding potencies.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Padmanabhan, B.</dc:creator>
    <dc:creator>Tong, K.I.</dc:creator>
    <dc:creator>Kobayashi, A.</dc:creator>
    <dc:creator>Yamamoto, M.</dc:creator>
    <dc:creator>Yokoyama, S.</dc:creator>
    <dc:date>2008-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950705114X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The structure of mouse Keap1-DC complexed with the DLG motif peptide of Nrf2 transcription factor was determined at 1.9 Å resolution. The structure showed that the peptide binds to Keap1-DC at the bottom region of the β-propeller domain.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>OXIDATIVE STRESS; NRF2 TRANSCRIPTION FACTOR; KEAP1; [BETA]-PROPELLER DOMAIN; STRUCTURE OF THE COMPLEX</dc:subject>
    <dc:description>The cytoplasmic repressor Keap1 regulates the function of transcription factor Nrf2 which plays critical roles in oxidative and xenobiotic stresses. The Neh2 domain of Nrf2 interacts with Keap1 at the bottom region of the Kelch/β-propeller domain which is formed by double-glycine repeat and C-terminal region domains (Keap1-DC). The structure of Keap1-DC complexed with an Nrf2 peptide containing a conserved DLG motif has been determined at 1.9 Å resolution. The Keap1-bound DLG peptide possesses a hairpin conformation, and it binds to the Keap1 protein at the bottom region of the β-propeller domain. The intermolecular interaction occurs through their complementary electrostatic interactions. Comparison of the present structure with the recently reported Keap1-DC complex structure suggests that the DLG and ETGE motifs of Neh2 in Nrf2 bind to Keap1 in a similar manner but with different binding potencies.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structural insights into the similar modes of Nrf2 transcription factor recognition by the cytoplasmic repressor Keap1</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>15</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2008-05-01</prism:publicationDate>
    <prism:startingPage>273</prism:startingPage>
    <prism:section>short communications</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>276</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0348">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0348</link>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2007-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507049242</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-11-01</prism:publicationDate>
    <prism:startingPage>532</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>534</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0347">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0347</link>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2007-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507038897</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-09-01</prism:publicationDate>
    <prism:startingPage>449</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>450</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5043">
    <title>Coherent X-ray scattering and lensless imaging at the European XFEL Facility</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5043</link>
    <description>Coherent X-ray diffraction imaging is a rapidly advancing form of lensless microscopy. The phase information of the diffraction pattern is embedded in a sufficiently sampled coherent diffraction pattern. Using advanced computational methods, this diffraction pattern can be inverted to produce an image of a sample with diffraction-limited resolution. It is attractive to use high-power coherent X-ray beams produced by future X-ray free-electron lasers for imaging nanoscale condensed matter, materials and biological samples. Here, the scientific case, requirements and the possible realisation of the coherent X-ray diffraction imaging beamlines at the European XFEL Facility are presented.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Vartanyants, I.A.</dc:creator>
    <dc:creator>Robinson, I.K.</dc:creator>
    <dc:creator>McNulty, I.</dc:creator>
    <dc:creator>David, C.</dc:creator>
    <dc:creator>Wochner, P.</dc:creator>
    <dc:creator>Tschentscher, Th.</dc:creator>
    <dc:date>2007-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507037600</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>High-power coherent X-ray beams produced by future X-ray free-electron lasers are an ideal source for coherent X-ray diffraction imaging of nanoscale condensed matter, materials and biological samples. The scientific case, requirements and the possible realization of the coherent X-ray diffraction imaging experiments at the European XFEL Facility are presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY FREE-ELECTRON LASER; COHERENT X-RAY DIFFRACTION IMAGING; PHASE RETRIEVAL</dc:subject>
    <dc:description>Coherent X-ray diffraction imaging is a rapidly advancing form of lensless microscopy. The phase information of the diffraction pattern is embedded in a sufficiently sampled coherent diffraction pattern. Using advanced computational methods, this diffraction pattern can be inverted to produce an image of a sample with diffraction-limited resolution. It is attractive to use high-power coherent X-ray beams produced by future X-ray free-electron lasers for imaging nanoscale condensed matter, materials and biological samples. Here, the scientific case, requirements and the possible realisation of the coherent X-ray diffraction imaging beamlines at the European XFEL Facility are presented.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Coherent X-ray scattering and lensless imaging at the European XFEL Facility</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-11-01</prism:publicationDate>
    <prism:startingPage>453</prism:startingPage>
    <prism:section>feature articles</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>470</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0345">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0345</link>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2007-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507028270</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-07-01</prism:publicationDate>
    <prism:startingPage>392</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>393</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?fd5013">
    <title>Developing 100 ps-resolved X-ray structural analysis capabilities on beamline NW14A at the Photon Factory Advanced Ring</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?fd5013</link>
    <description>NW14A is a newly constructed undulator beamline for 100 ps time-resolved X-ray experiments at the Photon Factory Advanced Ring. This beamline was designed to conduct a wide variety of time-resolved X-ray measurements, such as time-resolved diffraction, scattering and X-ray absorption fine structure. Its versatility is allowed by various instruments, including two undulators, three diffractometers, two pulse laser systems and an X-ray chopper. The potential for the detection of structural changes on the 100 ps time scale at NW14A is demonstrated by two examples of photo-induced structural changes in an organic crystal and photodissociation in solution.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Nozawa, S.</dc:creator>
    <dc:creator>Adachi, S.</dc:creator>
    <dc:creator>Takahashi, J.</dc:creator>
    <dc:creator>Tazaki, R.</dc:creator>
    <dc:creator>Guérin, L.</dc:creator>
    <dc:creator>Daimon, M.</dc:creator>
    <dc:creator>Tomita, A.</dc:creator>
    <dc:creator>Sato, T.</dc:creator>
    <dc:creator>Chollet, M.</dc:creator>
    <dc:creator>Collet, E.</dc:creator>
    <dc:creator>Cailleau, H.</dc:creator>
    <dc:creator>Yamamoto, S.</dc:creator>
    <dc:creator>Tsuchiya, K.</dc:creator>
    <dc:creator>Shioya, T.</dc:creator>
    <dc:creator>Sasaki, H.</dc:creator>
    <dc:creator>Mori, T.</dc:creator>
    <dc:creator>Ichiyanagi, K.</dc:creator>
    <dc:creator>Sawa, H.</dc:creator>
    <dc:creator>Kawata, H.</dc:creator>
    <dc:creator>Koshihara, S.</dc:creator>
    <dc:date>2007-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507025496</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Beamline NW14A, a newly constructed undulator beamline for 100 ps time-resolved X-ray experiments at the Photon Factory Advanced Ring, is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PHOTO-INDUCED PHASE TRANSITION; TIME-RESOLVED DIFFRACTION; TIME-RESOLVED SCATTERING; TIME-RESOLVED XAFS; INSERTION DEVICE; PF-AR; TTF-CA; NITTP</dc:subject>
    <dc:description>NW14A is a newly constructed undulator beamline for 100 ps time-resolved X-ray experiments at the Photon Factory Advanced Ring. This beamline was designed to conduct a wide variety of time-resolved X-ray measurements, such as time-resolved diffraction, scattering and X-ray absorption fine structure. Its versatility is allowed by various instruments, including two undulators, three diffractometers, two pulse laser systems and an X-ray chopper. The potential for the detection of structural changes on the 100 ps time scale at NW14A is demonstrated by two examples of photo-induced structural changes in an organic crystal and photodissociation in solution.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Developing 100 ps-resolved X-ray structural analysis capabilities on beamline NW14A at the Photon Factory Advanced Ring</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-07-01</prism:publicationDate>
    <prism:startingPage>313</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>319</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?fh5376">
    <title>ID20: a beamline for magnetic and resonant X-ray scattering investigations under extreme conditions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?fh5376</link>
    <description>A new experimental station at ESRF beamline ID20 is presented which allows magnetic and resonant X-ray scattering experiments in the energy range 3–25 keV to be performed under extreme conditions. High magnetic field up to 10 T, high pressure up to 30 kbar combined with low temperatures down to 1.5 K are available and experiments can be performed at the M-edges of actinide elements, L-edges of lanthanides and K-edges of transition metals.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Paolasini, L.</dc:creator>
    <dc:creator>Detlefs, C.</dc:creator>
    <dc:creator>Mazzoli, C.</dc:creator>
    <dc:creator>Wilkins, S.</dc:creator>
    <dc:creator>Deen, P.P.</dc:creator>
    <dc:creator>Bombardi, A.</dc:creator>
    <dc:creator>Kernavanois, N.</dc:creator>
    <dc:creator>de Bergevin, F.</dc:creator>
    <dc:creator>Yakhou, F.</dc:creator>
    <dc:creator>Valade, J.P.</dc:creator>
    <dc:creator>Breslavetz, I.</dc:creator>
    <dc:creator>Fondacaro, A.</dc:creator>
    <dc:creator>Pepellin, G.</dc:creator>
    <dc:creator>Bernard, P.</dc:creator>
    <dc:date>2007-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507024879</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A new experimental station at ESRF beamline ID20 is presented which allows magnetic and resonant X-ray scattering experiments in the energy range 3–25 keV to be performed under extreme conditions.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RESONANT X-RAY MAGNETIC SCATTERING; HIGH MAGNETIC FIELDS; HIGH PRESSURE; STRONGLY CORRELATED ELECTRON SYSTEMS</dc:subject>
    <dc:description>A new experimental station at ESRF beamline ID20 is presented which allows magnetic and resonant X-ray scattering experiments in the energy range 3–25 keV to be performed under extreme conditions. High magnetic field up to 10 T, high pressure up to 30 kbar combined with low temperatures down to 1.5 K are available and experiments can be performed at the M-edges of actinide elements, L-edges of lanthanides and K-edges of transition metals.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>ID20: a beamline for magnetic and resonant X-ray scattering investigations under extreme conditions</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-07-01</prism:publicationDate>
    <prism:startingPage>301</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>312</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?fh9370">
    <title>The small-angle and wide-angle X-ray scattering set-up at beamline BL9 of DELTA. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?fh9370</link>
    <description>A correction is made to the equation in Krywka et al. (2007), J. Synchrotron Rad. 14, 244–251.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Krywka, C.</dc:creator>
    <dc:creator>Sternemann, C.</dc:creator>
    <dc:creator>Paulus, M.</dc:creator>
    <dc:creator>Javid, N.</dc:creator>
    <dc:creator>Winter, R.</dc:creator>
    <dc:creator>Al-Sawalmih, A.</dc:creator>
    <dc:creator>Yi, S.</dc:creator>
    <dc:creator>Raabe, D.</dc:creator>
    <dc:creator>Tolan, M.</dc:creator>
    <dc:date>2007-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507020729</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Erratum to Krywka et al. [J. Synchrotron Rad. (2007), 14, 244–251].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>A correction is made to the equation in Krywka et al. (2007), J. Synchrotron Rad. 14, 244–251.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The small-angle and wide-angle X-ray scattering set-up at beamline BL9 of DELTA. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-07-01</prism:publicationDate>
    <prism:startingPage>391</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>391</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0344">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0344</link>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2007-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950701583X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-05-01</prism:publicationDate>
    <prism:startingPage>297</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>298</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0342">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0342</link>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2007-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049507006097</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-03-01</prism:publicationDate>
    <prism:startingPage>229</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>231</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0335">
    <title>Progress in research into radiation damage in cryo-cooled macromolecular crystals</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0335</link>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:creator>McSweeney, S.M.</dc:creator>
    <dc:date>2007-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506053015</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Progress in research into radiation damage in cryo-cooled macromolecular crystals</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-01-01</prism:publicationDate>
    <prism:startingPage>1</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>3</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0337">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0337</link>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2007-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506053003</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-01-01</prism:publicationDate>
    <prism:startingPage>173</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>174</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wl5138">
    <title>Verifying DiffEXAFS measurements with differential X-ray diffraction</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wl5138</link>
    <description>Differential EXAFS (DiffEXAFS) is a novel technique for measuring atomic perturbations on a local scale. Here a complementary technique for such studies is presented: differential X-ray diffraction (DiffXRD), which may be used to independently verify DiffEXAFS results whilst using exactly the same experimental apparatus and measurement technique. A test experiment has been conducted to show that DiffXRD can be used to successfully determine the thermal expansion coefficient of SrF2.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ruffoni, M.P.</dc:creator>
    <dc:creator>Pettifer, R.F.</dc:creator>
    <dc:creator>Pascarelli, S.</dc:creator>
    <dc:creator>Mathon, O.</dc:creator>
    <dc:date>2007-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506049971</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Differential EXAFS (DiffEXAFS) is a novel technique for measuring atomic perturbations on a local scale. Here a complementary technique for such studies is presented: differential X-ray diffraction (DiffXRD), which may be used to independently verify DiffEXAFS results whilst using exactly the same experimental apparatus and measurement technique. A test experiment has been conducted to show that DiffXRD can be used to successfully determine the thermal expansion coefficient of SrF2.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DIFFXRD; DIFFEXAFS; ATOMIC STRAIN; THERMAL EXPANSION; STRONTIUM FLUORIDE</dc:subject>
    <dc:description>Differential EXAFS (DiffEXAFS) is a novel technique for measuring atomic perturbations on a local scale. Here a complementary technique for such studies is presented: differential X-ray diffraction (DiffXRD), which may be used to independently verify DiffEXAFS results whilst using exactly the same experimental apparatus and measurement technique. A test experiment has been conducted to show that DiffXRD can be used to successfully determine the thermal expansion coefficient of SrF2.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Verifying DiffEXAFS measurements with differential X-ray diffraction</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-01-01</prism:publicationDate>
    <prism:startingPage>169</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>172</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5004">
    <title>Dose dependence of radiation damage for protein crystals studied at various X-ray energies</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5004</link>
    <description>Radiation damage to protein crystals is the most serious problem in obtaining accurate structures from protein crystallography. In order to examine the photon energy dependence of radiation damage, 12 to 15 data sets from each of nine tetragonal lysozyme crystals were collected at nine different X-ray energies (6.5, 7.1, 8.3, 9.9, 12.4, 16.5, 20.0, 24.8 and 33.0 keV) using beamline BL41XU at SPring-8. All results were compared on the basis of absorbed dose, expressed in Gray (Gy). Crystallographic statistics, such as the values of lattice constants, Rmerge and I/σ(I), for each data set degraded at all nine energies as the exposure time for each crystal increased. In all data sets, radiation damage was observed after the absorbed dose exceeded 106 Gy. However, from the point of view of crystallographic statistics normalized to the absorbed dose, no clear dependence on photon energy was observed in these results. Structural refinement showed that the average B-factor for the last data set was larger than that for the first data set at all energies tested. However, no energy dependence of radiation damage on B-factor was found. Furthermore, disruption of disulfide bonds due to radiation damage was observed in electron density maps even at the highest photon energy (33 keV) used in this study. Therefore, these results suggest that radiation damage in the energy range investigated could be evaluated based on absorbed dose without energy dependence, and that it is important to minimize the absorbed dose in a crystal sample for obtaining an accurate protein structure.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Shimizu, N.</dc:creator>
    <dc:creator>Hirata, K.</dc:creator>
    <dc:creator>Hasegawa, K.</dc:creator>
    <dc:creator>Ueno, G.</dc:creator>
    <dc:creator>Yamamoto, M.</dc:creator>
    <dc:date>2007-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506049296</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A systematic study of radiation damage has been conducted for various X-ray energies at beamline BL41XU at SPring-8. The dependence of radiation damage on photon energy is discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; X-RAY ENERGY; DOSE DEPENDENCE</dc:subject>
    <dc:description>Radiation damage to protein crystals is the most serious problem in obtaining accurate structures from protein crystallography. In order to examine the photon energy dependence of radiation damage, 12 to 15 data sets from each of nine tetragonal lysozyme crystals were collected at nine different X-ray energies (6.5, 7.1, 8.3, 9.9, 12.4, 16.5, 20.0, 24.8 and 33.0 keV) using beamline BL41XU at SPring-8. All results were compared on the basis of absorbed dose, expressed in Gray (Gy). Crystallographic statistics, such as the values of lattice constants, Rmerge and I/σ(I), for each data set degraded at all nine energies as the exposure time for each crystal increased. In all data sets, radiation damage was observed after the absorbed dose exceeded 106 Gy. However, from the point of view of crystallographic statistics normalized to the absorbed dose, no clear dependence on photon energy was observed in these results. Structural refinement showed that the average B-factor for the last data set was larger than that for the first data set at all energies tested. However, no energy dependence of radiation damage on B-factor was found. Furthermore, disruption of disulfide bonds due to radiation damage was observed in electron density maps even at the highest photon energy (33 keV) used in this study. Therefore, these results suggest that radiation damage in the energy range investigated could be evaluated based on absorbed dose without energy dependence, and that it is important to minimize the absorbed dose in a crystal sample for obtaining an accurate protein structure.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Dose dependence of radiation damage for protein crystals studied at various X-ray energies</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-01-01</prism:publicationDate>
    <prism:startingPage>4</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>10</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5006">
    <title>XANES measurements of the rate of radiation damage to selenomethionine side chains</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5006</link>
    <description>The radiation-induced disordering of selenomethionine (SeMet) side chains represents a significant impediment to protein structure solution. Not only does the increased B-factor of these sites result in a serious drop in phasing power, but some sites decay much faster than others in the same unit cell. These radio-labile SeMet side chains decay faster than high-order diffraction spots with dose, making it difficult to detect this kind of damage by inspection of the diffraction pattern. The selenium X-ray absorbance near-edge spectrum (XANES) from samples containing SeMet was found to change significantly after application of X-ray doses of 10–100 MGy. Most notably, the sharp `white line' feature near the canonical Se edge disappears. The change was attributed to breakage of the Cγ—Se bond in SeMet. This spectral change was used as a probe to measure the decay rate of SeMet with X-ray dose in cryo-cooled samples. Two protein crystal types and 15 solutions containing free SeMet amino acid were examined. The damage rate was influenced by the chemical and physical condition of the sample, and the half-decaying dose for the selenium XANES signal ranged from 5 to 43 MGy. These decay rates were 34- to 3.8-fold higher than the rate at which the Se atoms interacted directly with X-ray photons, so the damage mechanism must be a secondary effect. Samples that cooled to a more crystalline state generally decayed faster than samples that cooled to an amorphous solid. The single exception was a protein crystal where a nanocrystalline cryoprotectant had a protective effect. Lowering the pH, especially with ascorbic or nitric acids, had a protective effect, and SeMet lifetime increased monotonically with decreasing sample temperature (down to 93 K). The SeMet lifetime in one protein crystal was the same as that of the free amino acid, and the longest SeMet lifetime measured was found in the other protein crystal type. This protection was found to arise from the folded structure of the protein molecule. A mechanism to explain observed decay rates involving the damaging species following the electric field lines around protein molecules is proposed.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Holton, J.M.</dc:creator>
    <dc:date>2007-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506048898</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The lifetime of selenomethionine in a protein crystallography X-ray beam was measured and the effects of varying sample parameters such as temperature, volume, physical state, Se concentration, chemical additives and protein structure were evaluated. Depending on the combination of these parameters, the dose required to damage half of the selenomethionine in a sample varied by as much as a factor of eight.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY DOSE; PROTECTIVE SOLUTES; PH AND TEMPERATURE EFFECTS; PROTEIN CRYSTAL STRUCTURE; MECHANISM OF RADIATION DAMAGE</dc:subject>
    <dc:description>The radiation-induced disordering of selenomethionine (SeMet) side chains represents a significant impediment to protein structure solution. Not only does the increased B-factor of these sites result in a serious drop in phasing power, but some sites decay much faster than others in the same unit cell. These radio-labile SeMet side chains decay faster than high-order diffraction spots with dose, making it difficult to detect this kind of damage by inspection of the diffraction pattern. The selenium X-ray absorbance near-edge spectrum (XANES) from samples containing SeMet was found to change significantly after application of X-ray doses of 10–100 MGy. Most notably, the sharp `white line' feature near the canonical Se edge disappears. The change was attributed to breakage of the Cγ—Se bond in SeMet. This spectral change was used as a probe to measure the decay rate of SeMet with X-ray dose in cryo-cooled samples. Two protein crystal types and 15 solutions containing free SeMet amino acid were examined. The damage rate was influenced by the chemical and physical condition of the sample, and the half-decaying dose for the selenium XANES signal ranged from 5 to 43 MGy. These decay rates were 34- to 3.8-fold higher than the rate at which the Se atoms interacted directly with X-ray photons, so the damage mechanism must be a secondary effect. Samples that cooled to a more crystalline state generally decayed faster than samples that cooled to an amorphous solid. The single exception was a protein crystal where a nanocrystalline cryoprotectant had a protective effect. Lowering the pH, especially with ascorbic or nitric acids, had a protective effect, and SeMet lifetime increased monotonically with decreasing sample temperature (down to 93 K). The SeMet lifetime in one protein crystal was the same as that of the free amino acid, and the longest SeMet lifetime measured was found in the other protein crystal type. This protection was found to arise from the folded structure of the protein molecule. A mechanism to explain observed decay rates involving the damaging species following the electric field lines around protein molecules is proposed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>XANES measurements of the rate of radiation damage to selenomethionine side chains</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-01-01</prism:publicationDate>
    <prism:startingPage>51</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>72</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5010">
    <title>Radioprotectant screening for cryocrystallography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5010</link>
    <description>Radiation damage continues to present a problem to crystallographers using cryocooled protein crystals at third-generation synchrotrons. Free-radical scavengers have been suggested as a possible means of reducing the rate of this damage. The screening of a large number of potential radioprotectants was undertaken with an online microspectrophotometer using cystine and cysteine to model protein disulfide bonds and thiol groups, respectively. Oxidized α-lipoic acid was tested as a possible model disulfide bond. The evidence for the effectiveness of ascorbate as a radioprotectant was strengthened, and quinone, 2,2,6,6-tetramethyl-4-piperidone, and reduced dithiothreitol showed promise as radioprotectants.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Southworth-Davies, R.J.</dc:creator>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:date>2007-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506044177</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A range of radioprotectants have been tested as a possible means of reducing radiation damage in protein cryocrystallography, using an online microspectrophotometer.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIOPROTECTANTS; RADIATION DAMAGE; MACROMOLECULAR CRYOCRYSTALLOGRAPHY</dc:subject>
    <dc:description>Radiation damage continues to present a problem to crystallographers using cryocooled protein crystals at third-generation synchrotrons. Free-radical scavengers have been suggested as a possible means of reducing the rate of this damage. The screening of a large number of potential radioprotectants was undertaken with an online microspectrophotometer using cystine and cysteine to model protein disulfide bonds and thiol groups, respectively. Oxidized α-lipoic acid was tested as a possible model disulfide bond. The evidence for the effectiveness of ascorbate as a radioprotectant was strengthened, and quinone, 2,2,6,6-tetramethyl-4-piperidone, and reduced dithiothreitol showed promise as radioprotectants.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Radioprotectant screening for cryocrystallography</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-01-01</prism:publicationDate>
    <prism:startingPage>73</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>83</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5011">
    <title>X-ray radiation-induced damage in DNA monitored by online Raman</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5011</link>
    <description>High-quality Raman spectra have been collected on single DNA crystals kept at 100 K in a flow of cold nitrogen gas prior, during and after macromolecular crystallography (MX) data collection. The non-symmetric bending vibration for C—Br bonds in 8-bromo-2′-deoxyguanosine has been unambiguously identified at 293 cm−1 in the non-resonant Raman spectra. The breakage of this bond could be monitored by the continuous recording of Raman spectra during X-ray exposure, and its decay versus dose could be directly correlated with the loss of the bromide definition within the electron-density maps as determined with MX.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>McGeehan, J.E.</dc:creator>
    <dc:creator>Carpentier, P.</dc:creator>
    <dc:creator>Royant, A.</dc:creator>
    <dc:creator>Bourgeois, D.</dc:creator>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:date>2007-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506043251</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Raman spectra have been collected from cryocooled DNA crystals in combination with macromolecular cystallography data collection. The specific X-ray-induced breakage of a C—Br bond could be monitored in detail by both techniques.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; RADIATION-DAMAGE-INDUCED PHASING; RAMAN SPECTROSCOPY; DNA</dc:subject>
    <dc:description>High-quality Raman spectra have been collected on single DNA crystals kept at 100 K in a flow of cold nitrogen gas prior, during and after macromolecular crystallography (MX) data collection. The non-symmetric bending vibration for C—Br bonds in 8-bromo-2′-deoxyguanosine has been unambiguously identified at 293 cm−1 in the non-resonant Raman spectra. The breakage of this bond could be monitored by the continuous recording of Raman spectra during X-ray exposure, and its decay versus dose could be directly correlated with the loss of the bromide definition within the electron-density maps as determined with MX.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray radiation-induced damage in DNA monitored by online Raman</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-01-01</prism:publicationDate>
    <prism:startingPage>99</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>108</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xh5012">
    <title>Plastic-embedded protein crystals</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xh5012</link>
    <description>Rapid vitrification followed by the replacement of the vitrified water by a solvent (freeze substitution) and then resin is a widely used procedure for preparing biological samples for electron microscopy. The resulting plastic-embedded samples permit convenient room-temperature sectioning (micro­tomy) and can yield well preserved cellular structures. Here this procedure has been applied to crystalline protein samples, and it is shown that it is possible to freeze-substitute vitrified crystals while preserving some of their original diffraction properties. The plastic-embedded crystals were used to collect a series of complete room-temperature data sets at a powerful macromolecular crystallography synchrotron beamline. Whereas one normally observes specific damage to disulfide bonds upon X-ray radiation, no such damage was seen for the plastic-embedded sample. The X-ray diffraction data allowed an initial atomic analysis to be made of the effects of freeze-substitution and plastic embedding on biological samples.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:creator>Haselmann-Weiss, U.</dc:creator>
    <dc:creator>McGeehan, J.E.</dc:creator>
    <dc:creator>McCarthy, A.A.</dc:creator>
    <dc:creator>Marquez, J.A.</dc:creator>
    <dc:creator>Antony, C.</dc:creator>
    <dc:creator>Frangakis, A.S.</dc:creator>
    <dc:creator>Stranzl, G.</dc:creator>
    <dc:date>2007-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506043111</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The technique of freeze-substitution, commonly used in electron microscopy, has been applied to vitrified protein crystals. These plastic-embedded crystals have been examined in terms of X-ray diffraction properties and radiation hardness.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; FREEZE SUBSTITUTION; RESIN EMBEDDING</dc:subject>
    <dc:description>Rapid vitrification followed by the replacement of the vitrified water by a solvent (freeze substitution) and then resin is a widely used procedure for preparing biological samples for electron microscopy. The resulting plastic-embedded samples permit convenient room-temperature sectioning (micro­tomy) and can yield well preserved cellular structures. Here this procedure has been applied to crystalline protein samples, and it is shown that it is possible to freeze-substitute vitrified crystals while preserving some of their original diffraction properties. The plastic-embedded crystals were used to collect a series of complete room-temperature data sets at a powerful macromolecular crystallography synchrotron beamline. Whereas one normally observes specific damage to disulfide bonds upon X-ray radiation, no such damage was seen for the plastic-embedded sample. The X-ray diffraction data allowed an initial atomic analysis to be made of the effects of freeze-substitution and plastic embedding on biological samples.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Plastic-embedded protein crystals</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>14</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2007-01-01</prism:publicationDate>
    <prism:startingPage>128</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>132</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0328">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0328</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2006-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506042464</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-11-01</prism:publicationDate>
    <prism:startingPage>494</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>495</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?fh5368">
    <title>Calibration of spectra from dispersive XAS beamlines</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?fh5368</link>
    <description>The DXAS Calibration computer program provides a quantitative and automated solution to the problem of calibrating spectra from dispersive XAS beamlines. Such spectra, obtained in arbitrary energy units, are calibrated with respect to the absorption features of a supplied reference spectrum, which has been obtained under similar conditions on a calibrated beamline. In addition to basic energy coordinate transformation parameters, DXAS Calibration supplies instrument corrections to compensate for mismatches in instrument response functions between the dispersive and reference beamlines.</description>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ruffoni, M.P.</dc:creator>
    <dc:creator>Pettifer, R.F.</dc:creator>
    <dc:date>2006-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506039215</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The DXAS Calibration computer program provides a quantitative and automated solution to the problem of calibrating spectra from dispersive XAS beamlines.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DISPERSIVE XAS; CALIBRATION; INSTRUMENT RESPONSE FUNCTIONS</dc:subject>
    <dc:description>The DXAS Calibration computer program provides a quantitative and automated solution to the problem of calibrating spectra from dispersive XAS beamlines. Such spectra, obtained in arbitrary energy units, are calibrated with respect to the absorption features of a supplied reference spectrum, which has been obtained under similar conditions on a calibrated beamline. In addition to basic energy coordinate transformation parameters, DXAS Calibration supplies instrument corrections to compensate for mismatches in instrument response functions between the dispersive and reference beamlines.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Calibration of spectra from dispersive XAS beamlines</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-11-01</prism:publicationDate>
    <prism:startingPage>489</prism:startingPage>
    <prism:section>computer programs</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>493</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0325">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0325</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2006-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506030470</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-09-01</prism:publicationDate>
    <prism:startingPage>411</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>412</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wr5003">
    <title>Stable top-up operation at SPring-8</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wr5003</link>
    <description>Top-up operation allows SPring-8 to provide highly stable X-ray beams with arbitrary filling patterns. The implementation of top-up operation is described, with a focus on the simultaneous achievement of stability of stored current, beam orbit, purity of an isolated single bunch, and beam injection efficiency. Stored-current fluctuations have been routinely reduced to a level of 10−3. Stored-beam oscillation on frequent beam injection, which was originally regarded as the most serious problem, has been successfully suppressed to a sufficiently low level that it never perturbs imaging experiments. Current impurities in nominally empty buckets have been reduced to a level of 10−9 over more than one week of operation, making possible the measurement of time-resolved spectra using high-current bunches. Finally, excellent injection efficiency, higher than 80%, is routinely obtained, even for small undulator gaps, which is critical for preventing radiation damage to insertion-device magnets and to reduce leakage radiation. The process of achieving highly stabilized top-up operation at SPring-8 and its utility for user experiments are described.</description>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Tanaka, H.</dc:creator>
    <dc:creator>Adachi, M.</dc:creator>
    <dc:creator>Aoki, T.</dc:creator>
    <dc:creator>Asaka, T.</dc:creator>
    <dc:creator>Baron, A.</dc:creator>
    <dc:creator>Daté, S.</dc:creator>
    <dc:creator>Fukami, K.</dc:creator>
    <dc:creator>Furukawa, Y.</dc:creator>
    <dc:creator>Hanaki, H.</dc:creator>
    <dc:creator>Hosoda, N.</dc:creator>
    <dc:creator>Ishikawa, T.</dc:creator>
    <dc:creator>Kimura, H.</dc:creator>
    <dc:creator>Kobayashi, K.</dc:creator>
    <dc:creator>Kobayashi, T.</dc:creator>
    <dc:creator>Kohara, S.</dc:creator>
    <dc:creator>Kumagai, N.</dc:creator>
    <dc:creator>Masaki, M.</dc:creator>
    <dc:creator>Masuda, T.</dc:creator>
    <dc:creator>Matsui, S.</dc:creator>
    <dc:creator>Mizuno, A.</dc:creator>
    <dc:creator>Nakamura, T.</dc:creator>
    <dc:creator>Nakatani, T.</dc:creator>
    <dc:creator>Noda, T.</dc:creator>
    <dc:creator>Ohata, T.</dc:creator>
    <dc:creator>Ohkuma, H.</dc:creator>
    <dc:creator>Ohshima, T.</dc:creator>
    <dc:creator>Oishi, M.</dc:creator>
    <dc:creator>Sasaki, S.</dc:creator>
    <dc:creator>Schimizu, J.</dc:creator>
    <dc:creator>Shoji, M.</dc:creator>
    <dc:creator>Soutome, K.</dc:creator>
    <dc:creator>Suzuki, M.</dc:creator>
    <dc:creator>Suzuki, S.</dc:creator>
    <dc:creator>Suzuki, Y.</dc:creator>
    <dc:creator>Takano, S.</dc:creator>
    <dc:creator>Takao, M.</dc:creator>
    <dc:creator>Takashima, T.</dc:creator>
    <dc:creator>Takebe, H.</dc:creator>
    <dc:creator>Takeuchi, A.</dc:creator>
    <dc:creator>Tamura, K.</dc:creator>
    <dc:creator>Tanaka, R.</dc:creator>
    <dc:creator>Tanaka, Y.</dc:creator>
    <dc:creator>Taniuchi, T.</dc:creator>
    <dc:creator>Taniuchi, Y.</dc:creator>
    <dc:creator>Tsumaki, K.</dc:creator>
    <dc:creator>Yamashita, A.</dc:creator>
    <dc:creator>Yanagida, K.</dc:creator>
    <dc:creator>Yoda, Y.</dc:creator>
    <dc:creator>Yonehara, H.</dc:creator>
    <dc:creator>Yorita, T.</dc:creator>
    <dc:creator>Yoshioka, M.</dc:creator>
    <dc:creator>Takata, M.</dc:creator>
    <dc:date>2006-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506022862</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>SPring-8 has succeeded in achieving extremely stable top-up operation by retrofitting. Here the process of retrofitting is discussed, presenting key technical factors for stabilization of top-up operation. Examples are provided showing the value of top-up operation in various experiments.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TOP-UP OPERATION; INJECTION-BEAM LOSS; PURITY; STABILITY; THERMAL EQUILIBRIUM; HEAT LOAD</dc:subject>
    <dc:description>Top-up operation allows SPring-8 to provide highly stable X-ray beams with arbitrary filling patterns. The implementation of top-up operation is described, with a focus on the simultaneous achievement of stability of stored current, beam orbit, purity of an isolated single bunch, and beam injection efficiency. Stored-current fluctuations have been routinely reduced to a level of 10−3. Stored-beam oscillation on frequent beam injection, which was originally regarded as the most serious problem, has been successfully suppressed to a sufficiently low level that it never perturbs imaging experiments. Current impurities in nominally empty buckets have been reduced to a level of 10−9 over more than one week of operation, making possible the measurement of time-resolved spectra using high-current bunches. Finally, excellent injection efficiency, higher than 80%, is routinely obtained, even for small undulator gaps, which is critical for preventing radiation damage to insertion-device magnets and to reduce leakage radiation. The process of achieving highly stabilized top-up operation at SPring-8 and its utility for user experiments are described.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Stable top-up operation at SPring-8</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-09-01</prism:publicationDate>
    <prism:startingPage>378</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>391</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0323">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0323</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2006-07-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950602262X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-07-01</prism:publicationDate>
    <prism:startingPage>347</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>348</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ie5003">
    <title>Sharp-focusing Bragg–Fresnel zone plate with Laue diffraction geometry</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ie5003</link>
    <description>The impact of decreased zone height on the focal properties of hard X-ray Bragg–Fresnel zone plates has been studied by numerical simulation. Decreased zone height allows for smaller zone widths and, although the efficiency of the lens is decreased, the signal-to-background ratio in the focal plane of the lens remains at a comparatively high level. This is distinct from an analogous case of ordinary phase zone plates.</description>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Haroutunyan, L.</dc:creator>
    <dc:creator>Hovhannisyan, G.</dc:creator>
    <dc:date>2006-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506018449</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The focal sharpness of a Bragg–Fresnel lens (Laue diffraction geometry) can be improved by decreasing the height, and hence the width, of the Fresnel zones. The impact of this approach on the signal-to-background ratio of the focused spot and other properties is explored and found to be less than with ordinary Fresnel lens optics (in the absence of Bragg diffraction).</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY OPTICS; X-RAY DIFFRACTION; X-RAY FOCUSING; X-RAY DYNAMICAL DIFFRACTION; BRAGG-FRESNEL OPTICS; FRESNEL ZONE PLATE</dc:subject>
    <dc:description>The impact of decreased zone height on the focal properties of hard X-ray Bragg–Fresnel zone plates has been studied by numerical simulation. Decreased zone height allows for smaller zone widths and, although the efficiency of the lens is decreased, the signal-to-background ratio in the focal plane of the lens remains at a comparatively high level. This is distinct from an analogous case of ordinary phase zone plates.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Sharp-focusing Bragg–Fresnel zone plate with Laue diffraction geometry</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-07-01</prism:publicationDate>
    <prism:startingPage>343</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>345</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv9026">
    <title>Reciprocal space mapping and single-crystal scattering rods. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv9026</link>
    <description>While assembling the high-resolution graphics for Fig. 2 of Smilgies et al. [J. Synchrotron Rad. (2005). 12, 807–811], the curve from the bottom panel was erroneously repeated in the top panel. Below is the corrected figure.</description>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Smilgies, D.-M.</dc:creator>
    <dc:creator>Blasini, D.R.</dc:creator>
    <dc:creator>Hotta, S.</dc:creator>
    <dc:creator>Yanagi, H.</dc:creator>
    <dc:date>2006-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506015810</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Erratum to J. Synchrotron Rad. (2005). 12, 807–811.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>While assembling the high-resolution graphics for Fig. 2 of Smilgies et al. [J. Synchrotron Rad. (2005). 12, 807–811], the curve from the bottom panel was erroneously repeated in the top panel. Below is the corrected figure.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Reciprocal space mapping and single-crystal scattering rods. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-07-01</prism:publicationDate>
    <prism:startingPage>346</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>346</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0320">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0320</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:date>2006-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506012969</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-05-01</prism:publicationDate>
    <prism:startingPage>289</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>290</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0317">
    <title>Multiple-pass monochromators</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0317</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schoeffel, E.</dc:creator>
    <dc:date>2006-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506009861</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Multiple-pass monochromators</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-05-01</prism:publicationDate>
    <prism:startingPage>288</prism:startingPage>
    <prism:section>new commercial products</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>288</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?wl5133">
    <title>Evaluation of imaging performance of a taper optics CCD `FReLoN' camera designed for medical imaging</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?wl5133</link>
    <description>The purpose of this work was to assess the imaging performance of an indirect conversion detector (taper optics CCD `FReLoN' camera) in terms of the modulation transfer function (MTF), normalized noise power spectrum (NNPS) and detective quantum efficiency (DQE). Measurements were made with a synchrotron radiation laminar beam at various monochromatic energies in the 20–51.5 keV range for a gadolinium-based fluorescent screen varying in thickness; data acquisition and analysis were made by adapting to this beam geometry protocols used for conventional cone beams. The presampled MTFs of the systems were measured using an edge method. The NNPS of the systems were determined for a range of exposure levels by two-dimensional Fourier analysis of uniformly exposed radiographs. The DQEs were assessed from the measured MTF, NNPS, exposure and incoming number of photons. The MTF, for a given screen, was found to be almost energy independent and, for a given energy, higher for the thinnest screen. At 33 keV and for the 40 (100) µm screen, at 10% the MTF is 9.2 (8.6) line-pairs mm−1. The NNPS was found to be different in the two analyzed directions in relation to frequency. Highest DQE values were found for the combination 100 µm and 25 keV (0.5); it was still equal to 0.4 at 51.5 keV (above the gadolinium K-edge). The DQE is limited by the phosphor screen conversion yield and by the CCD efficiency. At the end of the manuscript the results of the FReLoN characterization and those from a selected number of detectors presented in the literature are compared.</description>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Coan, P.</dc:creator>
    <dc:creator>Peterzol, A.</dc:creator>
    <dc:creator>Fiedler, S.</dc:creator>
    <dc:creator>Ponchut, C.</dc:creator>
    <dc:creator>Labiche, J.C.</dc:creator>
    <dc:creator>Bravin, A.</dc:creator>
    <dc:date>2006-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506008983</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Full characterization in terms of modulation transfer function, normalized noise power spectrum and detective quantum efficiency of a fast-readout low-noise (FReLoN) CCD camera coupled to a fiberoptical taper, a detector developed at the European Synchrotron Radiation Facility.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MEDICAL IMAGING; IMAGE DETECTORS; IMAGE QUALITY</dc:subject>
    <dc:description>The purpose of this work was to assess the imaging performance of an indirect conversion detector (taper optics CCD `FReLoN' camera) in terms of the modulation transfer function (MTF), normalized noise power spectrum (NNPS) and detective quantum efficiency (DQE). Measurements were made with a synchrotron radiation laminar beam at various monochromatic energies in the 20–51.5 keV range for a gadolinium-based fluorescent screen varying in thickness; data acquisition and analysis were made by adapting to this beam geometry protocols used for conventional cone beams. The presampled MTFs of the systems were measured using an edge method. The NNPS of the systems were determined for a range of exposure levels by two-dimensional Fourier analysis of uniformly exposed radiographs. The DQEs were assessed from the measured MTF, NNPS, exposure and incoming number of photons. The MTF, for a given screen, was found to be almost energy independent and, for a given energy, higher for the thinnest screen. At 33 keV and for the 40 (100) µm screen, at 10% the MTF is 9.2 (8.6) line-pairs mm−1. The NNPS was found to be different in the two analyzed directions in relation to frequency. Highest DQE values were found for the combination 100 µm and 25 keV (0.5); it was still equal to 0.4 at 51.5 keV (above the gadolinium K-edge). The DQE is limited by the phosphor screen conversion yield and by the CCD efficiency. At the end of the manuscript the results of the FReLoN characterization and those from a selected number of detectors presented in the literature are compared.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Evaluation of imaging performance of a taper optics CCD `FReLoN' camera designed for medical imaging</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-05-01</prism:publicationDate>
    <prism:startingPage>260</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>270</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ml5214">
    <title>Comments on A new model for statistical error analysis in XAS: about the distribution function of the absorption coefficient by E. Curis &amp; S. Bénazeth (2001). J. Synchrotron Rad. 8, 264–266</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ml5214</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Nadarajah, S.</dc:creator>
    <dc:creator>Kotz, S.</dc:creator>
    <dc:date>2006-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506008958</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Comment on Curis &amp; Bénazeth [J. Synchrotron Rad. (2001), 8, 264–266].</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>LETTERS TO THE EDITOR</dc:subject>
    <dc:format>text/html</dc:format>
    <dc:title>Comments on A new model for statistical error analysis in XAS: about the distribution function of the absorption coefficient by E. Curis &amp; S. Bénazeth (2001). J. Synchrotron Rad. 8, 264–266</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-05-01</prism:publicationDate>
    <prism:startingPage>285</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>285</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ml0022">
    <title>Response to S. Nadarajah &amp; S. Kotz's Comments on A new model for statistical error analysis in XAS: about the distribution function of the absorption coefficient by E. Curis &amp; S. Bénazeth (2001). J. Synchrotron Rad. 8, 264–266</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ml0022</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Curis, E.</dc:creator>
    <dc:creator>Bénazeth, S.</dc:creator>
    <dc:date>2006-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950600896X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Response to Nadarajah &amp; Kotz's comments in the previous paper.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>LETTERS TO THE EDITOR</dc:subject>
    <dc:format>text/html</dc:format>
    <dc:title>Response to S. Nadarajah &amp; S. Kotz's Comments on A new model for statistical error analysis in XAS: about the distribution function of the absorption coefficient by E. Curis &amp; S. Bénazeth (2001). J. Synchrotron Rad. 8, 264–266</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-05-01</prism:publicationDate>
    <prism:startingPage>286</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>286</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pf0024">
    <title>Structure Determination by X-ray Crystallography. By Mark Ladd and Rex Palmer. Pp. xlii + 819. New York: Kluwer Academic/Plenum, 4th ed., 2003. Price (paperback) GBP 41, ISBN 0-306-47454-9.</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pf0024</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ohashi, Y.</dc:creator>
    <dc:date>2006-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506008910</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:subject>BOOK REVIEW</dc:subject>
    <dc:format>text/html</dc:format>
    <dc:title>Structure Determination by X-ray Crystallography. By Mark Ladd and Rex Palmer. Pp. xlii + 819. New York: Kluwer Academic/Plenum, 4th ed., 2003. Price (paperback) GBP 41, ISBN 0-306-47454-9.</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-05-01</prism:publicationDate>
    <prism:startingPage>287</prism:startingPage>
    <prism:section>book reviews</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>287</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0315">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0315</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:date>2006-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506004808</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-03-01</prism:publicationDate>
    <prism:startingPage>225</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>225</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0313">
    <title>Introduction to the Special Issue on Detectors</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0313</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Graafsma, H.</dc:creator>
    <dc:date>2006-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049506004274</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Introduction to the Special Issue on Detectors</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-03-01</prism:publicationDate>
    <prism:startingPage>97</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>98</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0312">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0312</link>
    <dc:rights>Copyright (c) 2006 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:date>2006-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505041415</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>13</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2006 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2006-01-01</prism:publicationDate>
    <prism:startingPage>88</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>89</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0303">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0303</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2005-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505032590</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-11-01</prism:publicationDate>
    <prism:startingPage>836</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>837</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0301">
    <title>Deep UV and vacuum ultraviolet spectrophotometer</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0301</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schoeffel, E.</dc:creator>
    <dc:date>2005-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505031687</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Deep UV and vacuum ultraviolet spectrophotometer</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-11-01</prism:publicationDate>
    <prism:startingPage>835</prism:startingPage>
    <prism:section>new commercial products</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>835</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?he5339">
    <title>A transparent two-dimensional in situ beam-position and profile monitor for synchrotron X-ray beamlines</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?he5339</link>
    <description>A compact, inexpensive and easy-to-construct two-dimensional in situ beam-position and profile monitor for synchrotron X-ray beamlines is presented. The device is based on the collection of spatially resolved scattered radiation from a polyimide foil. The X-ray beam passes through a foil placed in the path of the beam, which absorbs no more than 3% of the beam at 12 keV. The scattered radiation is collected at an angle of 90° through a collimator located below the foil onto a CCD sensor. The device was tested on bending-magnet beamline BM26 at the ESRF synchrotron radiation source and has a positional sensitivity better than 10 µm with a large working range of 25 mm × 25 mm. Although the device is optimized for use in the range 10–12 keV, it can easily be modified for use with higher-energy beams by using a suitably chosen scattering foil.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Kyele, N.R.</dc:creator>
    <dc:creator>Decanniere, K.</dc:creator>
    <dc:creator>Silfhout, R.G. van</dc:creator>
    <dc:date>2005-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505031250</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A CCD-based two-dimensional in situ beam-position and profile monitor for synchrotron X-ray beamlines is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAYS; BEAM-POSITION MONITOR; BEAM-PROFILE MONITOR; CCD-BASED; DETECTORS</dc:subject>
    <dc:description>A compact, inexpensive and easy-to-construct two-dimensional in situ beam-position and profile monitor for synchrotron X-ray beamlines is presented. The device is based on the collection of spatially resolved scattered radiation from a polyimide foil. The X-ray beam passes through a foil placed in the path of the beam, which absorbs no more than 3% of the beam at 12 keV. The scattered radiation is collected at an angle of 90° through a collimator located below the foil onto a CCD sensor. The device was tested on bending-magnet beamline BM26 at the ESRF synchrotron radiation source and has a positional sensitivity better than 10 µm with a large working range of 25 mm × 25 mm. Although the device is optimized for use in the range 10–12 keV, it can easily be modified for use with higher-energy beams by using a suitably chosen scattering foil.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A transparent two-dimensional in situ beam-position and profile monitor for synchrotron X-ray beamlines</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-11-01</prism:publicationDate>
    <prism:startingPage>800</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>806</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0299">
    <title>Synchrotron radiation and nanobiosciences – introductory overview</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0299</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Pechkova, E.</dc:creator>
    <dc:creator>Nicolini, C.</dc:creator>
    <dc:date>2005-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505029390</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Synchrotron radiation and nanobiosciences – introductory overview</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-11-01</prism:publicationDate>
    <prism:startingPage>711</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>711</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0300">
    <title>Some introductory remarks on microbeam diffraction in nanobiosciences</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0300</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Paris, O.</dc:creator>
    <dc:creator>Riekel, C.</dc:creator>
    <dc:date>2005-11-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950502950X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Some introductory remarks on microbeam diffraction in nanobiosciences</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-11-01</prism:publicationDate>
    <prism:startingPage>712</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>712</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0298">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0298</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2005-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505025513</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-09-01</prism:publicationDate>
    <prism:startingPage>708</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>709</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0297">
    <title>1 m vacuum monochromator</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0297</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schoeffel, E.</dc:creator>
    <dc:date>2005-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505025331</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>1 m vacuum monochromator</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-09-01</prism:publicationDate>
    <prism:startingPage>707</prism:startingPage>
    <prism:section>new commercial products</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>707</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0296">
    <title>Structure determination by single-crystal X-ray diffraction (SXD) at megabar pressures</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0296</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Dera, P.</dc:creator>
    <dc:creator>Prewitt, C.T.</dc:creator>
    <dc:creator>Jacobsen, S.D.</dc:creator>
    <dc:date>2005-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505024945</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Structure determination by single-crystal X-ray diffraction (SXD) at megabar pressures</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-09-01</prism:publicationDate>
    <prism:startingPage>547</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>548</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xd5006">
    <title>Structures from powders and poor-quality single crystals at high pressure</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xd5006</link>
    <description>The use of single-crystal techniques and quasi-single-crystal samples in solving and refining complex crystal structures at high pressure is reviewed. In particular, recent studies of the incommensurate and modulated structures found in a number of elemental metals at high pressure are focused on.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>McMahon, M.I.</dc:creator>
    <dc:date>2005-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505022788</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The use of data from poor-quality single crystals, and from combined powder/single-crystal studies, to determine crystal structures at high pressure is reviewed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HIGH-PRESSURE; SINGLE CRYSTAL; INCOMMENSURATE</dc:subject>
    <dc:description>The use of single-crystal techniques and quasi-single-crystal samples in solving and refining complex crystal structures at high pressure is reviewed. In particular, recent studies of the incommensurate and modulated structures found in a number of elemental metals at high pressure are focused on.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structures from powders and poor-quality single crystals at high pressure</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-09-01</prism:publicationDate>
    <prism:startingPage>549</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>553</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xd5010">
    <title>Advances in array detectors for X-ray diffraction techniques</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xd5010</link>
    <description>Improved focal plane array detector systems are described which can provide improved readout speeds, random addressing and even be employed to simultaneously measure position, intensity and energy. This latter capability promises to rekindle interests in Laue techniques. Simulations of three varieties of foil mask spectrometer in both on- and off-axis configurations indicate that systems of stacked silicon detectors can provide energy measurements within 1% of the true value based on the use of single `foils' and ∼10000 photons. An eight-detector hybrid design can provide energy coverage from 4 to 60 keV. Energy resolution can be improved by increased integration time or higher flux experiments. An off-axis spectrometer design in which the angle between the incident beam and the detector system is 45° results in a shift in the optimum energy response of the spectrometer system. In the case of a 200 µm-thick silicon absorber, the energy optimum shifts from 8.7 keV to 10.3 keV as the angle of incidence goes from 0 to 45°. These new designs make better use of incident photons, lower the impact of source flicker through simultaneous rather than sequential collection of intensities, and improve the energy range relative to previously reported systems.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hanley, Q.S.</dc:creator>
    <dc:creator>Denton, M.B.</dc:creator>
    <dc:date>2005-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505022600</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Recent developments in solid-state imaging technologies have provided a framework for faster, lower noise and larger format systems than previously available. Advances which have not found widespread use in instrumentation for X-ray diffraction include highly parallel readout amplifiers, hybrid imaging technologies and improved CMOS imagers. These advances are discussed and simulations are presented of selected devices incorporated into a new generation of instrumentation for Laue diffraction applications.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CCD; CID; CMOS; LAUE DIFFRACTION; SPECTROMETER</dc:subject>
    <dc:description>Improved focal plane array detector systems are described which can provide improved readout speeds, random addressing and even be employed to simultaneously measure position, intensity and energy. This latter capability promises to rekindle interests in Laue techniques. Simulations of three varieties of foil mask spectrometer in both on- and off-axis configurations indicate that systems of stacked silicon detectors can provide energy measurements within 1% of the true value based on the use of single `foils' and ∼10000 photons. An eight-detector hybrid design can provide energy coverage from 4 to 60 keV. Energy resolution can be improved by increased integration time or higher flux experiments. An off-axis spectrometer design in which the angle between the incident beam and the detector system is 45° results in a shift in the optimum energy response of the spectrometer system. In the case of a 200 µm-thick silicon absorber, the energy optimum shifts from 8.7 keV to 10.3 keV as the angle of incidence goes from 0 to 45°. These new designs make better use of incident photons, lower the impact of source flicker through simultaneous rather than sequential collection of intensities, and improve the energy range relative to previously reported systems.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Advances in array detectors for X-ray diffraction techniques</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-09-01</prism:publicationDate>
    <prism:startingPage>618</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>625</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xd5001">
    <title>High-pressure polymorphism of cyclopentanol (C5H10O): the structure of cyclopentanol phase-V at 1.5 GPa</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xd5001</link>
    <description>The fully ordered high-pressure crystal structure of cyclopentanol (C5H10O) has been solved using single-crystal X-ray diffraction techniques on station 9.8 at the SRS Daresbury Laboratory. At pressures above 1.5 GPa, cyclopentanol crystallizes in the monoclinic P21/c space group with a = 17.882 (3), b = 5.4573 (3), c = 9.6817 (14) Å, β = 104.699 (8)° and Z′ = 2. The crystal structure is characterized by the formation of hydrogen-bonded molecular chains, denoted C_2^2(4) in graph set notation, which lie parallel to the crystallographic c-axis, with the molecules adopting a pseudo fourfold arrangement around the central core of hydrogen bonds.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Moggach, S.A.</dc:creator>
    <dc:creator>Allan, D.R.</dc:creator>
    <dc:creator>Lozano-Casal, P.</dc:creator>
    <dc:creator>Parsons, S.</dc:creator>
    <dc:date>2005-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505021461</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The fully ordered high-pressure crystal structure of cyclopentanol (C5H10O) has been solved using single-crystal X-ray diffraction techniques on station 9.8 at the SRS Daresbury Laboratory. The crystal structure is characterized by the formation of molecular chains, denoted C_2^2(4) in graph set notation, with the molecules adopting a pseudo fourfold arrangement around the central core of hydrogen bonds.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HIGH PRESSURE; SINGLE-CRYSTAL DIFFRACTION; SMALL-MOLECULE</dc:subject>
    <dc:description>The fully ordered high-pressure crystal structure of cyclopentanol (C5H10O) has been solved using single-crystal X-ray diffraction techniques on station 9.8 at the SRS Daresbury Laboratory. At pressures above 1.5 GPa, cyclopentanol crystallizes in the monoclinic P21/c space group with a = 17.882 (3), b = 5.4573 (3), c = 9.6817 (14) Å, β = 104.699 (8)° and Z′ = 2. The crystal structure is characterized by the formation of hydrogen-bonded molecular chains, denoted C_2^2(4) in graph set notation, which lie parallel to the crystallographic c-axis, with the molecules adopting a pseudo fourfold arrangement around the central core of hydrogen bonds.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>High-pressure polymorphism of cyclopentanol (C5H10O): the structure of cyclopentanol phase-V at 1.5 GPa</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-09-01</prism:publicationDate>
    <prism:startingPage>590</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>597</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xd5007">
    <title>The effect of pressure on the crystal structure of hexagonal l-cystine</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xd5007</link>
    <description>The crystal structure of hexagonal l-cystine has been determined at room temperature at pressures between 0.4 and 3.7 GPa; unit-cell dimensions were measured up to 6.4 GPa. The structure of this phase consists of molecules in their zwitterionic form, and crystallizes in the hexagonal space group P6122. The structure consists of hydrogen-bonded layers which are strongly reminiscent of those seen in α-glycine, and consist of R_4^4(16) hydrogen-bonded ring motifs. These layers are connected on one side by the disulfide bridges within the cystine molecules, and on the other by NH⋯O hydrogen bonds to other glycine-like layers. The most compressible unit-cell dimension, and the direction of greatest strain in the structure, is along the c-axis, and application of pressure pushes the layers closer together. The compression occurs approximately equally in the regions of the interlayer hydrogen bonds and the disulfide bridges; in the latter, changes in the C—S—S—C torsion angles allow the cystine molecules to act like springs. The effects of pressure can be interpreted in terms of closing-up of voids in the structure, and this leads to (i) a lessening of the N—C—C—O and C—S—S—C torsional angles, (ii) shortening of the N—H⋯O hydrogen bonds by 0.10–0.60 Å and (iii) a further shortening of an already short S⋯S contact from 3.444 (4) Å to 3.264 (4) Å.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Moggach, S.A.</dc:creator>
    <dc:creator>Allan, D.R.</dc:creator>
    <dc:creator>Parsons, S.</dc:creator>
    <dc:creator>Sawyer, L.</dc:creator>
    <dc:creator>Warren, J.E.</dc:creator>
    <dc:date>2005-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505019850</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The structure of hexagonal l-cystine consists of pairs of hydrogen-bonded layers connected by disulfide bridges. The conformation about the bridges changes on compression to 3.7 GPa as the C—S—S—C units act like springs; other changes can be understood by examination of the distribution of voids in the ambient pressure structure.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AMINO ACID; HYDROGEN BONDING; HIGH-PRESSURE SINGLE-CRYSTAL DIFFRACTION</dc:subject>
    <dc:description>The crystal structure of hexagonal l-cystine has been determined at room temperature at pressures between 0.4 and 3.7 GPa; unit-cell dimensions were measured up to 6.4 GPa. The structure of this phase consists of molecules in their zwitterionic form, and crystallizes in the hexagonal space group P6122. The structure consists of hydrogen-bonded layers which are strongly reminiscent of those seen in α-glycine, and consist of R_4^4(16) hydrogen-bonded ring motifs. These layers are connected on one side by the disulfide bridges within the cystine molecules, and on the other by NH⋯O hydrogen bonds to other glycine-like layers. The most compressible unit-cell dimension, and the direction of greatest strain in the structure, is along the c-axis, and application of pressure pushes the layers closer together. The compression occurs approximately equally in the regions of the interlayer hydrogen bonds and the disulfide bridges; in the latter, changes in the C—S—S—C torsion angles allow the cystine molecules to act like springs. The effects of pressure can be interpreted in terms of closing-up of voids in the structure, and this leads to (i) a lessening of the N—C—C—O and C—S—S—C torsional angles, (ii) shortening of the N—H⋯O hydrogen bonds by 0.10–0.60 Å and (iii) a further shortening of an already short S⋯S contact from 3.444 (4) Å to 3.264 (4) Å.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The effect of pressure on the crystal structure of hexagonal l-cystine</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-09-01</prism:publicationDate>
    <prism:startingPage>598</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>607</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0295">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0295</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>,</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505018741</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>543</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>544</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ml0021">
    <title>Variable-period undulators as synchrotron radiation sources. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ml0021</link>
    <description>Citations are added to the paper by Shenoy et al. [J. Synchrotron Rad. (2003). 10, 205–213].</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Shenoy, G.K.</dc:creator>
    <dc:creator>Lewellen, J.W.</dc:creator>
    <dc:creator>Shu, D.</dc:creator>
    <dc:creator>Vinokurov, N.A.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505017814</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Erratum to J. Synchrotron Rad. (2003). 10, 205–213.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>VARIABLE-PERIOD UNDULATORS; SYNCHROTRON RADIATION SOURCES; RADIATION DAMAGE</dc:subject>
    <dc:description>Citations are added to the paper by Shenoy et al. [J. Synchrotron Rad. (2003). 10, 205–213].</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Variable-period undulators as synchrotron radiation sources. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>542</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>542</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv0001">
    <title>Application notes on the use of softer X-rays for anomalous powder diffraction</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv0001</link>
    <description>An in-vacuum diffractometer has been modified to collect powder diffraction data from a sample of promazine hydrochloride. Strong anomalous contrast has been observed at, or close to, the sulphur edge. Based on the data collected, a bespoke diffractometer has been designed that, together with minor changes to the geometry of the experiment, will enable the routine collection of powder data at absorption edges below 5.5 keV.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Cernik, R.J.</dc:creator>
    <dc:creator>Husheer, S.</dc:creator>
    <dc:creator>Smith, A.D.</dc:creator>
    <dc:creator>Roper, M.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505015414</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The practical aspects of studying powder samples with softer X-rays for indexing or structure solution applications are discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY INSTRUMENTATION; POWDER DIFFRACTION</dc:subject>
    <dc:description>An in-vacuum diffractometer has been modified to collect powder diffraction data from a sample of promazine hydrochloride. Strong anomalous contrast has been observed at, or close to, the sulphur edge. Based on the data collected, a bespoke diffractometer has been designed that, together with minor changes to the geometry of the experiment, will enable the routine collection of powder data at absorption edges below 5.5 keV.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Application notes on the use of softer X-rays for anomalous powder diffraction</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>431</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>433</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0294">
    <title>The uses of softer X-rays in structural studies</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0294</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Cernik, R.J.</dc:creator>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:creator>Helliwell, M.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505017243</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>The uses of softer X-rays in structural studies</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>391</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>391</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5013">
    <title>Nanoarchitectures of the animal extracellular matrix: opportunities for synchrotron radiation studies on collagen and fibrillin</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5013</link>
    <description>The extracellular matrix comprises structures that support the architectural organization of virtually all animal tissues. Within this architecture, two classes of protein assemblies found as long slender fibrils (collagen and fibrillin) characterize the bulk of the extracellular matrix. In both classes of fibrous protein, the molecular organization within a fibril ensures that the properties of the individual molecules transcend to the nanostructural and mesoscopic levels of structural organization and thence the tissue itself. The composition of the fibrils, in conjunction with other biomolecules and their suprafibrillar architecture, facilitates the formation of tissues as diverse as skin, tendon, cornea ciliary zonules and aorta. Here the relative tear resistance, strength, transparency and optical properties are paramount for proper function. Many structural investigations of fibrous protein structure have relied heavily on the use of synchrotron radiation in order to elucidate molecular packing, primarily due to the distinct benefits that X-ray diffraction provides, such as minimal sample preparation, rapid data collection and in situ mechanical testing. In this paper, an overview of the investigations that have revealed different levels of molecular architecture in fibril-based tissues is presented. Emerging future technology and how this can be matched with the pressing questions in extracellular matrix biology are also discussed.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Wess, T.J.</dc:creator>
    <dc:creator>Cairns, D.E.</dc:creator>
    <dc:date>2005-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505012306</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An overview of synchrotron-radiation-based X-ray diffraction experiments regarding different levels of molecular architecture in fibril-based tissues is presented. Specific reference is given to collagen and fibrillin, two important fibrous proteins that comprise the bulk of the extracellular matrix in the animal kingdom.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COLLAGEN; FIBRIL; FIBRILLIN; STRUCTURE; X-RAYS</dc:subject>
    <dc:description>The extracellular matrix comprises structures that support the architectural organization of virtually all animal tissues. Within this architecture, two classes of protein assemblies found as long slender fibrils (collagen and fibrillin) characterize the bulk of the extracellular matrix. In both classes of fibrous protein, the molecular organization within a fibril ensures that the properties of the individual molecules transcend to the nanostructural and mesoscopic levels of structural organization and thence the tissue itself. The composition of the fibrils, in conjunction with other biomolecules and their suprafibrillar architecture, facilitates the formation of tissues as diverse as skin, tendon, cornea ciliary zonules and aorta. Here the relative tear resistance, strength, transparency and optical properties are paramount for proper function. Many structural investigations of fibrous protein structure have relied heavily on the use of synchrotron radiation in order to elucidate molecular packing, primarily due to the distinct benefits that X-ray diffraction provides, such as minimal sample preparation, rapid data collection and in situ mechanical testing. In this paper, an overview of the investigations that have revealed different levels of molecular architecture in fibril-based tissues is presented. Emerging future technology and how this can be matched with the pressing questions in extracellular matrix biology are also discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Nanoarchitectures of the animal extracellular matrix: opportunities for synchrotron radiation studies on collagen and fibrillin</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-11-01</prism:publicationDate>
    <prism:startingPage>751</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>757</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0292">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0292</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:date>2005-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505011192</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-05-01</prism:publicationDate>
    <prism:startingPage>386</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>388</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ol5287">
    <title>A high-throughput structural biology/proteomics beamline at the SRS on a new multipole wiggler</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ol5287</link>
    <description>The North West Structural Genomics Centre's beamline, MAD10, at the SRS receives the central part of the radiation fan (0.5 mrad vertically, 4 mrad horizontally) produced by a new 2.46 T ten-pole wiggler. The optical arrangement of the beamline consists of a Rh-coated collimating Si mirror, a fixed-exit-beam double-crystal monochromator with sagittal bending for horizontal focusing and a second Rh-coated Si mirror for vertical focusing. The double-crystal Si (111) monochromator allows data collection in the 5–13.5 keV photon energy range with rapid (subsecond) tunability and high energy resolution. The monochromatic beam is optimized through a 200 µm collimator. The beamline end station has been designed around a Mar desktop beamline with high-throughput cryogenic sample changer, Mar225 CCD detector, liquid-N2 autofill system and an ORTEC C-TRAIN-04 energy-resolving high-count-rate X-ray fluorescence detector. The instrument is optimized for MAD/SAD applications in protein crystallography with the additional mode of operation of online single-crystal EXAFS studies on the same crystals. Thus, screening of metals/Se in the crystal can be performed quickly prior to MAD/SAD data collection by exciting the crystal with X-rays of appropriate energy and recording an energy-dispersive fluorescence spectrum. In addition, this experimental set-up allows for parallel XAFS measurements on the same crystal to monitor `radiation-induced' changes, if any, in e.g. the redox state of metal centres to be detected for a `metallic' functional group during crystallographic data collection. Moreover, careful minimization of the thickness of the Be window maximizes the intensity performance for the 2.0–2.5 Å softer wavelength range. This range also covers the K-edges of a number of important 3d transition metals as well as the L-edges of xenon and iodine and enhanced sulfur f ′′.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Cianci, M.</dc:creator>
    <dc:creator>Antonyuk, S.</dc:creator>
    <dc:creator>Bliss, N.</dc:creator>
    <dc:creator>Bailey, M.W.</dc:creator>
    <dc:creator>Buffey, S.G.</dc:creator>
    <dc:creator>Cheung, K.C.</dc:creator>
    <dc:creator>Clarke, J.A.</dc:creator>
    <dc:creator>Derbyshire, G.E.</dc:creator>
    <dc:creator>Ellis, M.J.</dc:creator>
    <dc:creator>Enderby, M.J.</dc:creator>
    <dc:creator>Grant, A.F.</dc:creator>
    <dc:creator>Holbourn, M.P.</dc:creator>
    <dc:creator>Laundy, D.</dc:creator>
    <dc:creator>Nave, C.</dc:creator>
    <dc:creator>Ryder, R.</dc:creator>
    <dc:creator>Stephenson, P.</dc:creator>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:creator>Hasnain, S.S.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505009131</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A new MAD beamline at the SRS (UK) for structural genomics and proteomics has been recently commissioned. The beamline is based on a 20 mm external gap, 2.46 T ten-pole wiggler with highly optimized optics to provide rapid (subsecond) tunability over an edge and the highest intensity radiation over 5 to 13.5 keV. An energy-dispersive high-count-rate fluorescence detector with large active area is also integrated into the crystallographic set-up providing unique capabilities to this MAD station.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>STRUCTURAL GENOMICS; HIGH THROUGHPUT; MACROMOLECULAR CRYSTALLOGRAPHY; SINGLE-CRYSTAL EXAFS; MAD; SAD; SOFTER X-RAYS; METALLOPROTEIN; X-RAY FLUORESCENCE</dc:subject>
    <dc:description>The North West Structural Genomics Centre's beamline, MAD10, at the SRS receives the central part of the radiation fan (0.5 mrad vertically, 4 mrad horizontally) produced by a new 2.46 T ten-pole wiggler. The optical arrangement of the beamline consists of a Rh-coated collimating Si mirror, a fixed-exit-beam double-crystal monochromator with sagittal bending for horizontal focusing and a second Rh-coated Si mirror for vertical focusing. The double-crystal Si (111) monochromator allows data collection in the 5–13.5 keV photon energy range with rapid (subsecond) tunability and high energy resolution. The monochromatic beam is optimized through a 200 µm collimator. The beamline end station has been designed around a Mar desktop beamline with high-throughput cryogenic sample changer, Mar225 CCD detector, liquid-N2 autofill system and an ORTEC C-TRAIN-04 energy-resolving high-count-rate X-ray fluorescence detector. The instrument is optimized for MAD/SAD applications in protein crystallography with the additional mode of operation of online single-crystal EXAFS studies on the same crystals. Thus, screening of metals/Se in the crystal can be performed quickly prior to MAD/SAD data collection by exciting the crystal with X-rays of appropriate energy and recording an energy-dispersive fluorescence spectrum. In addition, this experimental set-up allows for parallel XAFS measurements on the same crystal to monitor `radiation-induced' changes, if any, in e.g. the redox state of metal centres to be detected for a `metallic' functional group during crystallographic data collection. Moreover, careful minimization of the thickness of the Be window maximizes the intensity performance for the 2.0–2.5 Å softer wavelength range. This range also covers the K-edges of a number of important 3d transition metals as well as the L-edges of xenon and iodine and enhanced sulfur f ′′.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A high-throughput structural biology/proteomics beamline at the SRS on a new multipole wiggler</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>455</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>466</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5008">
    <title>Resonant soft X-ray diffraction – in extremis</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5008</link>
    <description>The use of softer-energy X-rays produced by synchrotron radiation for diffraction is an area of current interest. In this paper, experiments exploiting resonant scattering at the L absorption edges of 3d transition metal elements are reported. Such energies, typically 500–1000 eV, are at the extreme limit of soft X-ray diffraction where absorption effects are so severe that the sample and diffractometer must be placed in a windowless high-vacuum vessel. In addition, the Ewald sphere is so small as to likely contain, at most, only a single Bragg reflection. Advantages of using such radiation for the study of weak diffraction effects such as anomalous scattering, charge ordering, magnetic diffraction and orbital ordering are reported.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hatton, P.D.</dc:creator>
    <dc:creator>Wilkins, S.B.</dc:creator>
    <dc:creator>Beale, T.A.W.</dc:creator>
    <dc:creator>Johal, T.K.</dc:creator>
    <dc:creator>Prabhakaran, D.</dc:creator>
    <dc:creator>Boothroyd, A.T.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505009167</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Recent advances in the new technique of soft X-ray single-crystal diffraction are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SOFT X-RAYS; MAGNETIC DIFFRACTION; ORBITAL ORDERING; RESONANCE EFFECTS</dc:subject>
    <dc:description>The use of softer-energy X-rays produced by synchrotron radiation for diffraction is an area of current interest. In this paper, experiments exploiting resonant scattering at the L absorption edges of 3d transition metal elements are reported. Such energies, typically 500–1000 eV, are at the extreme limit of soft X-ray diffraction where absorption effects are so severe that the sample and diffractometer must be placed in a windowless high-vacuum vessel. In addition, the Ewald sphere is so small as to likely contain, at most, only a single Bragg reflection. Advantages of using such radiation for the study of weak diffraction effects such as anomalous scattering, charge ordering, magnetic diffraction and orbital ordering are reported.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Resonant soft X-ray diffraction – in extremis</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>434</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>441</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5560">
    <title>Overcoming protein denaturation caused by irradiation in a high-flux synchrotron radiation circular dichroism beamline</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5560</link>
    <description>It has been established that the new circular dichroism beamline CD12 has sufficiently high flux at low wavelengths to cause apparent irradiation problems with protein samples while their synchrotron radiation circular dichroism (SRCD) spectra are being collected. The cause of this effect has been extensively investigated and is reported in an accompanying paper [Wien et al. (2005). J. Synchrotron Rad. 12, 517–523.]. Experiments suggest that localized heating of the protein sample, leading to denaturation, is the probable cause. Methods to circumvent this problem by limiting the beam flux are reported. This was achieved using either an attenuation cell of water placed beam-side of the sample cell, or limiting the beam cross-sectional area hitting the sample. Such methods are shown to result in substantial reduction or apparent complete removal of this protein denaturation over the course of collecting three successive spectra. Elimination of this denaturation problem enables multiple SRCD scans for protein samples to be collected, which are vital both for good practice and for statistically valid results.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Janes, R.W.</dc:creator>
    <dc:creator>Cuff, A.L.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505007703</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Methods are described by which the deterioration of the synchrotron radiation circular dichroism signal of proteins in high-flux beamlines can be minimized.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CIRCULAR DICHROISM; VACUUM ULTRAVIOLET; PROTEIN DENATURATION; ATTENUATION; PROTEIN STRUCTURE</dc:subject>
    <dc:description>It has been established that the new circular dichroism beamline CD12 has sufficiently high flux at low wavelengths to cause apparent irradiation problems with protein samples while their synchrotron radiation circular dichroism (SRCD) spectra are being collected. The cause of this effect has been extensively investigated and is reported in an accompanying paper [Wien et al. (2005). J. Synchrotron Rad. 12, 517–523.]. Experiments suggest that localized heating of the protein sample, leading to denaturation, is the probable cause. Methods to circumvent this problem by limiting the beam flux are reported. This was achieved using either an attenuation cell of water placed beam-side of the sample cell, or limiting the beam cross-sectional area hitting the sample. Such methods are shown to result in substantial reduction or apparent complete removal of this protein denaturation over the course of collecting three successive spectra. Elimination of this denaturation problem enables multiple SRCD scans for protein samples to be collected, which are vital both for good practice and for statistically valid results.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Overcoming protein denaturation caused by irradiation in a high-flux synchrotron radiation circular dichroism beamline</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>524</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>529</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xn0001">
    <title>Towards an understanding of radiation damage in cryocooled macromolecular crystals</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xn0001</link>
    <description>Interest in radiation damage is growing rapidly owing to the surge in macromolecular crystallography experiments carried out at modern brilliant synchrotron macromolecular crystallography beamlines. Work on the characterization of radiation damage in cryocooled protein crystals is starting to have some impact on our understanding of the problem and of how damage might be affecting both the process of structure solution and the actual structure obtained. A brief review of the most recent developments is given together with an assessment of the remaining problems. Although progress is being made, the understanding of radiation damage is far from complete. Methods for recognizing the damage and treating the data are being made available but they are still at an early stage of development.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Nave, C.</dc:creator>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:date>2005-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505007132</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The current understanding of radiation damage in cryocooled macromolecular crystals is reviewed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; PROTEIN CRYSTALS; CRYOCOOLING</dc:subject>
    <dc:description>Interest in radiation damage is growing rapidly owing to the surge in macromolecular crystallography experiments carried out at modern brilliant synchrotron macromolecular crystallography beamlines. Work on the characterization of radiation damage in cryocooled protein crystals is starting to have some impact on our understanding of the problem and of how damage might be affecting both the process of structure solution and the actual structure obtained. A brief review of the most recent developments is given together with an assessment of the remaining problems. Although progress is being made, the understanding of radiation damage is far from complete. Methods for recognizing the damage and treating the data are being made available but they are still at an early stage of development.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Towards an understanding of radiation damage in cryocooled macromolecular crystals</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-05-01</prism:publicationDate>
    <prism:startingPage>257</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>260</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5561">
    <title>VUV irradiation effects on proteins in high-flux synchrotron radiation circular dichroism spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5561</link>
    <description>Synchrotron radiation circular dichroism (SRCD) spectroscopy is emerging as an important new tool in structural molecular biology. Previously we had shown that in lower-flux SRCD instruments, such as UV1 at ISA and beamline 3.1 at the SRS, vacuum ultraviolet (VUV) radiation damage to proteins was not evident after exposure over a period of hours. No effects were detected in either the protein primary or the secondary structures. However, with the development of high-flux beamlines, such as CD12 at the SRS, this issue has been revisited because of changes observed in the SRCD spectra of consecutive scans of protein samples obtained on this high-flux beamline. Experiments have been designed to distinguish between two different possible mechanisms: (i) photoionization causing free radicals or secondary electrons producing degradation of the protein, and (ii) local heating of the sample resulting in protein denaturation. The latter appears to be the principal source of the signal deterioration.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Wien, F.</dc:creator>
    <dc:creator>Miles, A.J.</dc:creator>
    <dc:creator>Lees, J.G.</dc:creator>
    <dc:creator>Hoffmann, S.V.</dc:creator>
    <dc:creator>Wallace, B.A.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505006953</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The effects of very intense synchrotron radiation vacuum ultraviolet light on the circular dichroism spectra and chemical integrity of proteins are discussed. Experiments have been chosen to distinguish between possible degradation and denaturation effects; local heating of the sample resulting in denaturation appears to be the primary factor producing the observed spectral changes.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>VACUUM ULTRAVIOLET; CIRCULAR DICHROISM SPECTROSCOPY; SYNCHROTRON RADIATION CIRCULAR DICHROISM SPECTROSCOPY; PROTEIN STRUCTURE; SECONDARY STRUCTURE; STRUCTURAL GENOMICS; CALIBRATION; MEMBRANE PROTEIN; PROTEIN DENATURATION</dc:subject>
    <dc:description>Synchrotron radiation circular dichroism (SRCD) spectroscopy is emerging as an important new tool in structural molecular biology. Previously we had shown that in lower-flux SRCD instruments, such as UV1 at ISA and beamline 3.1 at the SRS, vacuum ultraviolet (VUV) radiation damage to proteins was not evident after exposure over a period of hours. No effects were detected in either the protein primary or the secondary structures. However, with the development of high-flux beamlines, such as CD12 at the SRS, this issue has been revisited because of changes observed in the SRCD spectra of consecutive scans of protein samples obtained on this high-flux beamline. Experiments have been designed to distinguish between two different possible mechanisms: (i) photoionization causing free radicals or secondary electrons producing degradation of the protein, and (ii) local heating of the sample resulting in protein denaturation. The latter appears to be the principal source of the signal deterioration.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>VUV irradiation effects on proteins in high-flux synchrotron radiation circular dichroism spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>517</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>523</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?es0344">
    <title>Brightness, spectral brightness or brilliance – Report of the Working Group on Synchrotron Radiation Nomenclature</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?es0344</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Mills, D.M.</dc:creator>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:creator>Kvick, Å.</dc:creator>
    <dc:creator>Ohta, T.</dc:creator>
    <dc:creator>Robinson, I.A.</dc:creator>
    <dc:creator>Authier, A.</dc:creator>
    <dc:date>2005-05-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950500796X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Brightness, spectral brightness or brilliance – Report of the Working Group on Synchrotron Radiation Nomenclature</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-05-01</prism:publicationDate>
    <prism:startingPage>385</prism:startingPage>
    <prism:section>international union of crystallography</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>385</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0291">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0291</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:date>2005-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505004462</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-03-01</prism:publicationDate>
    <prism:startingPage>254</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>255</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0290">
    <title>Applications of synchrotron radiation to materials research</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0290</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Shenoy, G.</dc:creator>
    <dc:creator>Viccaro, P.J.</dc:creator>
    <dc:date>2005-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505003894</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Applications of synchrotron radiation to materials research</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-03-01</prism:publicationDate>
    <prism:startingPage>123</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>123</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5014">
    <title>Microfocus X-ray scattering investigations of eggshell nanotexture</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5014</link>
    <description>The avian eggshell is a highly ordered calcitic bioceramic composite, with both inorganic and organic constituents. The interactions between the inorganic and organic components within the structure are poorly understood but are likely to occur at the nanometre level. Thus structural variation at this level may impinge on the overall structural integrity and mechanical performance of the eggshell, and therefore analysis at this level is fundamental in fully understanding this ordered structure. In this study, structural changes in the mineral crystallites were investigated by microfocus small-angle X-ray scattering (µSAXS) using synchrotron radiation. Small-angle X-ray scattering (SAXS) can be used to investigate structures on the nanometre scale such as size, shape, arrangement and internal porosity. A microfocused X-ray beam, 1.5 µm vertically by 7 µm, was used to produce vertical linear scans of the eggshell section. SAXS patterns were taken from the eggshell membrane (inner surface of the eggshell) to the cuticle (outer surface of the eggshell). This allowed textural variations within the eggshell to be mapped. The scattering intensity profile was then used to derive the dimension of scattering objects that define the nanotexture. The nanotexture observed may result from the presence of the organic matrix, which is embedded as intracrystalline particles producing voids within the calcified framework of large (&gt;1 µm) calcite crystals. Porod analysis revealed the average size of a scattering interface to be approximately 4.5 nm with small changes that had a depth-dependent variation. These were largest at the mammillary layer/membrane boundary. The palisade layer displayed a small upward trend in size of scattering object. Parallel scans showed that the textural variations observed within the palisade layer are significant and indicate local subtextures. In addition, many of the patterns exhibit diffuse scattering streaks that could result from reflectivity from the larger crystallite interfaces. Changes in the orientation of diffuse streaks were observed within the different layers, the membranes, mammillary layer, palisade layer, vertical crystal layer and cuticle, indicating certain preferred orientations of the crystallites within the layers. The nanotextural variations that are apparent could have implications at the macroscopic level of the resulting eggshell.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Lammie, D.</dc:creator>
    <dc:creator>Bain, M.M.</dc:creator>
    <dc:creator>Wess, T.J.</dc:creator>
    <dc:date>2005-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505003547</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An investigation of the calcified eggshell nanotexture by microfocus small-angle X-ray scattering using synchrotron radiation is reported.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MICROFOCUS SMALL-ANGLE X-RAY SCATTERING; EGGSHELL; STRUCTURE; NANOTEXTURE</dc:subject>
    <dc:description>The avian eggshell is a highly ordered calcitic bioceramic composite, with both inorganic and organic constituents. The interactions between the inorganic and organic components within the structure are poorly understood but are likely to occur at the nanometre level. Thus structural variation at this level may impinge on the overall structural integrity and mechanical performance of the eggshell, and therefore analysis at this level is fundamental in fully understanding this ordered structure. In this study, structural changes in the mineral crystallites were investigated by microfocus small-angle X-ray scattering (µSAXS) using synchrotron radiation. Small-angle X-ray scattering (SAXS) can be used to investigate structures on the nanometre scale such as size, shape, arrangement and internal porosity. A microfocused X-ray beam, 1.5 µm vertically by 7 µm, was used to produce vertical linear scans of the eggshell section. SAXS patterns were taken from the eggshell membrane (inner surface of the eggshell) to the cuticle (outer surface of the eggshell). This allowed textural variations within the eggshell to be mapped. The scattering intensity profile was then used to derive the dimension of scattering objects that define the nanotexture. The nanotexture observed may result from the presence of the organic matrix, which is embedded as intracrystalline particles producing voids within the calcified framework of large (&gt;1 µm) calcite crystals. Porod analysis revealed the average size of a scattering interface to be approximately 4.5 nm with small changes that had a depth-dependent variation. These were largest at the mammillary layer/membrane boundary. The palisade layer displayed a small upward trend in size of scattering object. Parallel scans showed that the textural variations observed within the palisade layer are significant and indicate local subtextures. In addition, many of the patterns exhibit diffuse scattering streaks that could result from reflectivity from the larger crystallite interfaces. Changes in the orientation of diffuse streaks were observed within the different layers, the membranes, mammillary layer, palisade layer, vertical crystal layer and cuticle, indicating certain preferred orientations of the crystallites within the layers. The nanotextural variations that are apparent could have implications at the macroscopic level of the resulting eggshell.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Microfocus X-ray scattering investigations of eggshell nanotexture</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-11-01</prism:publicationDate>
    <prism:startingPage>721</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>726</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xn0006">
    <title>Phasing in the presence of radiation damage</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xn0006</link>
    <description>In the accurate estimation of small signals, redundancy of observations is often seen as an essential tool for the experimenter. This is particularly true during macromolecular structure determination by single-wavelength anomalous dispersion (SAD), where the exploitable signal can be less than a few percent. At the most intense undulator synchrotron beamlines, the effect of radiation damage can be such that all usable signal is obscured. Here the magnitude of this effect in experiments performed at the Se K-edge is quantified. Six successive data sets were collected on the same crystal, interspersed with two exposures to the X-ray beam during which data were not collected. It is shown that the very first data set has excellent phasing statistics, whereas these statistics degrade for the later data sets. Merging several data sets into one, highly redundant, data set only gave moderate improvements as a result of the presence of radiation damage. Part of the damage could be corrected for using a linear interpolation scheme. Interpolation of the data to a low-dose as well as to a high-dose data set allowed us to combine the SAD method with the radiation-damage induced phasing (RIP) technique, which further improved the experimental phases, especially after density modification. Some recommendations are given on how to mitigate the effect of radiation damage during structure determination.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:creator>Nanao, M.H.</dc:creator>
    <dc:creator>Lovering, A.</dc:creator>
    <dc:creator>White, S.</dc:creator>
    <dc:creator>McSweeney, S.</dc:creator>
    <dc:date>2005-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505003286</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The trade-off between redundancy and radiation damage for single-wavelength anomalous dispersion (SAD) experiments is discussed using an Se K-edge SAD data series collected on a third-generation synchrotron undulator MX beamline.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RADIATION DAMAGE; DATA REDUNDANCY; RADIATION-DAMAGE INDUCED PHASING (RIP); MULTIWAVELENGTH ANOMALOUS DISPERSION (MAD); SINGLE-WAVELENGTH ANOMALOUS DISPERSION (SAD)</dc:subject>
    <dc:description>In the accurate estimation of small signals, redundancy of observations is often seen as an essential tool for the experimenter. This is particularly true during macromolecular structure determination by single-wavelength anomalous dispersion (SAD), where the exploitable signal can be less than a few percent. At the most intense undulator synchrotron beamlines, the effect of radiation damage can be such that all usable signal is obscured. Here the magnitude of this effect in experiments performed at the Se K-edge is quantified. Six successive data sets were collected on the same crystal, interspersed with two exposures to the X-ray beam during which data were not collected. It is shown that the very first data set has excellent phasing statistics, whereas these statistics degrade for the later data sets. Merging several data sets into one, highly redundant, data set only gave moderate improvements as a result of the presence of radiation damage. Part of the damage could be corrected for using a linear interpolation scheme. Interpolation of the data to a low-dose as well as to a high-dose data set allowed us to combine the SAD method with the radiation-damage induced phasing (RIP) technique, which further improved the experimental phases, especially after density modification. Some recommendations are given on how to mitigate the effect of radiation damage during structure determination.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Phasing in the presence of radiation damage</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-05-01</prism:publicationDate>
    <prism:startingPage>276</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>284</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xn0007">
    <title>Beam-size effects in radiation damage in insulin and thaumatin crystals</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xn0007</link>
    <description>Cryocooled insulin and thaumatin crystals were irradiated in a series of alternating data collections and high-dose-rate exposures using either a vertically focused or vertically defocused beam. The main result is that the radiation damage is limited to the exposed region, which can be explained by the short range of the photoelectrons and the Auger electron cascade produced by light elements. Consequently, the unexposed angular range provides significantly improved data quality and electron density compared with previously exposed angular wedges of the crystal when a vertically focused beam is used, while no differences are observed between a fresh wedge and an exposed region for the vertically defocused beam. On the other hand, the focused beam provides higher I/σI ratios at high resolution than homogeneous sample illumination but also causes more rapid sample deterioration.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schulze-Briese, C.</dc:creator>
    <dc:creator>Wagner, A.</dc:creator>
    <dc:creator>Tomizaki, T.</dc:creator>
    <dc:creator>Oetiker, M.</dc:creator>
    <dc:date>2005-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505003298</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Radiation damage to insulin and thaumatin is limited to the irradiated volume. This has important implications for data collection strategies.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; RADIATION DAMAGE; DATA COLLECTION STRATEGY</dc:subject>
    <dc:description>Cryocooled insulin and thaumatin crystals were irradiated in a series of alternating data collections and high-dose-rate exposures using either a vertically focused or vertically defocused beam. The main result is that the radiation damage is limited to the exposed region, which can be explained by the short range of the photoelectrons and the Auger electron cascade produced by light elements. Consequently, the unexposed angular range provides significantly improved data quality and electron density compared with previously exposed angular wedges of the crystal when a vertically focused beam is used, while no differences are observed between a fresh wedge and an exposed region for the vertically defocused beam. On the other hand, the focused beam provides higher I/σI ratios at high resolution than homogeneous sample illumination but also causes more rapid sample deterioration.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Beam-size effects in radiation damage in insulin and thaumatin crystals</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-05-01</prism:publicationDate>
    <prism:startingPage>261</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>267</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?xn0004">
    <title>Parameters affecting the X-ray dose absorbed by macromolecular crystals</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?xn0004</link>
    <description>The lifetime of a macromolecular crystal in an X-ray beam is assumed to be limited by the absorbed dose. This dose, expressed in Gray (Gy = J kg−1), is a function of a number of parameters: the absorption coefficients of the constituent atoms of the crystal, the number of molecules per asymmetric unit, the beam energy, flux, size and profile, the crystal size, and the total irradiation time. The effects of these variables on the predicted absorbed dose, calculated using the program RADDOSE, are discussed and are illustrated with reference to the irradiation of a selenomethionine protein crystal of unknown structure. The results of RADDOSE can and will in the future be used to inform the data collection procedure as it sets a theoretical upper limit on the total exposure time at a certain X-ray source. However, as illustrated with an example for which the experimental data are compared with prediction, the actual lifetime of a crystal could become shorter in those cases where specific damage breaks down crucial crystal contacts.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Murray, J.W.</dc:creator>
    <dc:creator>Rudiño-Piñera, E.</dc:creator>
    <dc:creator>Owen, R.L.</dc:creator>
    <dc:creator>Grininger, M.</dc:creator>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:creator>Garman, E.F.</dc:creator>
    <dc:date>2005-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049505003262</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The program RADDOSE is used to illustrate the important parameters governing the magnitude of the dose absorbed by X-ray irradiated protein crystals, with reference to a selenomethionine-containing example and a crystal of a highly X-ray sensitive native protein, for which calculations are compared with observed lifetime.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ABSORBED DOSE; HENDERSON LIMIT; X-RAY DIFFRACTION; RADIATION DAMAGE; DODECIN</dc:subject>
    <dc:description>The lifetime of a macromolecular crystal in an X-ray beam is assumed to be limited by the absorbed dose. This dose, expressed in Gray (Gy = J kg−1), is a function of a number of parameters: the absorption coefficients of the constituent atoms of the crystal, the number of molecules per asymmetric unit, the beam energy, flux, size and profile, the crystal size, and the total irradiation time. The effects of these variables on the predicted absorbed dose, calculated using the program RADDOSE, are discussed and are illustrated with reference to the irradiation of a selenomethionine protein crystal of unknown structure. The results of RADDOSE can and will in the future be used to inform the data collection procedure as it sets a theoretical upper limit on the total exposure time at a certain X-ray source. However, as illustrated with an example for which the experimental data are compared with prediction, the actual lifetime of a crystal could become shorter in those cases where specific damage breaks down crucial crystal contacts.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Parameters affecting the X-ray dose absorbed by macromolecular crystals</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-05-01</prism:publicationDate>
    <prism:startingPage>268</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>275</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0285">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0285</link>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:date>2005-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504033783</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-01-01</prism:publicationDate>
    <prism:startingPage>115</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>115</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi0126">
    <title>Metallogenomics and biological X-ray absorption spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi0126</link>
    <description>An overview of the second special issue of the journal on biological applications of X-ray absorption spectroscopy (BioXAS) is presented. The emphasis is on the study of metalloproteins in the context of structural genomics programmes (metallo­genomics).</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ascone, I.</dc:creator>
    <dc:creator>Fourme, R.</dc:creator>
    <dc:creator>Hasnain, S.</dc:creator>
    <dc:creator>Hodgson, K.</dc:creator>
    <dc:date>2005-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504033412</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An overview of the second special issue of the journal on biological applications of X-ray absorption spectroscopy is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>BIOXAS; EXAFS; XANES; METALLOPROTEINS; METALLOGENOMICS</dc:subject>
    <dc:description>An overview of the second special issue of the journal on biological applications of X-ray absorption spectroscopy (BioXAS) is presented. The emphasis is on the study of metalloproteins in the context of structural genomics programmes (metallo­genomics).</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Metallogenomics and biological X-ray absorption spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-01-01</prism:publicationDate>
    <prism:startingPage>1</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>3</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5006">
    <title>The use of softer X-rays in the structure elucidation of microporous materials</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5006</link>
    <description>Microporous materials, such as zeolites and aluminophosphates, have many applications as molecular sieves and shape-selective catalysts. This is due to their three-dimensional frameworks, which contain regular pores and channels, to their high acidity, arising from Brønsted and Lewis acid active sites, and to the incorporation of transition metal atoms into framework sites. This review firstly provides an introduction into the nature and properties of these materials, and their important applications; the difficulties in their full characterization and possible methods of elucidating their structures are then outlined; finally, methods of characterization, utilizing `softer X-rays' are introduced. The first method is the determination of low concentrations of transition metals, incorporated into the frameworks using single crystal anomalous dispersion crystallography; synchrotron radiation is used to tune to the absorption edge of the metal atom in question, in order to change its signal relative to that of the rest of the structure, thereby allowing the pinpointing of its positions and the determination of its concentration at each site in the framework. Secondly, the use of longer wavelengths in powder diffraction studies is described, which, by stretching out the powder pattern, thereby reduces the overlapping of the diffraction peaks, thus allowing the structure to be solved by conventional direct methods. Finally, the use of X-ray absorption spectroscopy to determine the metal incorporation and the nature of coordination at the metal atom sites, in Mn silicalite-1 and FAPO-36, are described.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Helliwell, M.</dc:creator>
    <dc:creator>Jones, R.H.</dc:creator>
    <dc:creator>Kaucic, V.</dc:creator>
    <dc:creator>Logar, N.Z.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504032327</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The research effort on novel open-pore chemical structures requires site-specific position and occupancy determination of metal atoms. These involve K edges in the softer X-ray range, from 1.5 to 2.5 Å, leading to novel challenges in synchrotron radiation instrumentation and anomalous dispersion methods in single crystal and powder diffraction. For the latter, separating out of the powder pattern peaks, using softer X-rays, opens up application to ab initio structure solution of more complicated and larger structures.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MICROPOROUS MATERIALS; SOFTER X-RAYS; ANOMALOUS DISPERSION; MAD; POWDER DIFFRACTION; X-RAY ABSORPTION SPECTROSCOPY</dc:subject>
    <dc:description>Microporous materials, such as zeolites and aluminophosphates, have many applications as molecular sieves and shape-selective catalysts. This is due to their three-dimensional frameworks, which contain regular pores and channels, to their high acidity, arising from Brønsted and Lewis acid active sites, and to the incorporation of transition metal atoms into framework sites. This review firstly provides an introduction into the nature and properties of these materials, and their important applications; the difficulties in their full characterization and possible methods of elucidating their structures are then outlined; finally, methods of characterization, utilizing `softer X-rays' are introduced. The first method is the determination of low concentrations of transition metals, incorporated into the frameworks using single crystal anomalous dispersion crystallography; synchrotron radiation is used to tune to the absorption edge of the metal atom in question, in order to change its signal relative to that of the rest of the structure, thereby allowing the pinpointing of its positions and the determination of its concentration at each site in the framework. Secondly, the use of longer wavelengths in powder diffraction studies is described, which, by stretching out the powder pattern, thereby reduces the overlapping of the diffraction peaks, thus allowing the structure to be solved by conventional direct methods. Finally, the use of X-ray absorption spectroscopy to determine the metal incorporation and the nature of coordination at the metal atom sites, in Mn silicalite-1 and FAPO-36, are described.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The use of softer X-rays in the structure elucidation of microporous materials</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>420</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>430</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5007">
    <title>An internet-based synchrotron experiment for students measuring the X-ray magnetic circular dichroism of a PtFe alloy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5007</link>
    <description>A new internet-based synchrotron experiment for students is presented. A polarimeter and computer software have been developed for measuring via the internet the X-ray magnetic circular dichroism of PtFe around its Pt LII and LIII absorption edges. From the experiment, students can examine the X-ray magnetic circular dichroism of a thin PtFe foil utilizing circular-polarized synchrotron radiation emitted by the superconducting asymmetric wiggler at the synchrotron radiation source DELTA of the University of Dortmund.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Paulus, M.</dc:creator>
    <dc:creator>Fendt, R.</dc:creator>
    <dc:creator>Sternemann, C.</dc:creator>
    <dc:creator>Gutt, C.</dc:creator>
    <dc:creator>Hövel, H.</dc:creator>
    <dc:creator>Volmer, M.</dc:creator>
    <dc:creator>Tolan, M.</dc:creator>
    <dc:creator>Wille, K.</dc:creator>
    <dc:date>2005-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504030742</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A new internet-based synchrotron experiment for students is presented for measuring the X-ray magnetic circular dichroism of PtFe around its Pt LII and LIII absorption edges via the internet.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>XMCD; MONOCHROMATORS; BEAMLINES; INTERNET</dc:subject>
    <dc:description>A new internet-based synchrotron experiment for students is presented. A polarimeter and computer software have been developed for measuring via the internet the X-ray magnetic circular dichroism of PtFe around its Pt LII and LIII absorption edges. From the experiment, students can examine the X-ray magnetic circular dichroism of a thin PtFe foil utilizing circular-polarized synchrotron radiation emitted by the superconducting asymmetric wiggler at the synchrotron radiation source DELTA of the University of Dortmund.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>An internet-based synchrotron experiment for students measuring the X-ray magnetic circular dichroism of a PtFe alloy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-03-01</prism:publicationDate>
    <prism:startingPage>246</prism:startingPage>
    <prism:section>teaching and education</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>250</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?fh5356">
    <title>Specimen charging in X-ray absorption spectroscopy: correction of total electron yield data from stabilized zirconia in the energy range 250–915 eV</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?fh5356</link>
    <description>The effects of specimen charging on X-ray absorption spectroscopy using total electron yield have been investigated using powder samples of zirconia stabilized by a range of oxides. The stabilized zirconia powder was mixed with graphite to minimize the charging but significant modifications of the intensities of features in the X-ray absorption near-edge fine structure (XANES) still occurred. The time dependence of the charging was measured experimentally using a time scan, and an algorithm was developed to use this measured time dependence to correct the effects of the charging. The algorithm assumes that the system approaches the equilibrium state by an exponential decay. The corrected XANES show improved agreement with the electron energy-loss near-edge fine structure obtained from the same samples.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Vlachos, D.</dc:creator>
    <dc:creator>Craven, A.J.</dc:creator>
    <dc:creator>McComb, D.W.</dc:creator>
    <dc:date>2005-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504030146</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A procedure for correcting for the effects of specimen charging on X-ray absorption near-edge structure (XANES) recorded by total electron yield is discussed. The corrected XANES is compared with the electron energy-loss near-edge structure from the same materials and several sources of artefacts are discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY ABSORPTION NEAR-EDGE STRUCTURE; ELECTRON ENERGY-LOSS NEAR-EDGE STRUCTURE; CHARGING; CORRECTION FOR CHARGING; TOTAL ELECTRON YIELD</dc:subject>
    <dc:description>The effects of specimen charging on X-ray absorption spectroscopy using total electron yield have been investigated using powder samples of zirconia stabilized by a range of oxides. The stabilized zirconia powder was mixed with graphite to minimize the charging but significant modifications of the intensities of features in the X-ray absorption near-edge fine structure (XANES) still occurred. The time dependence of the charging was measured experimentally using a time scan, and an algorithm was developed to use this measured time dependence to correct the effects of the charging. The algorithm assumes that the system approaches the equilibrium state by an exponential decay. The corrected XANES show improved agreement with the electron energy-loss near-edge fine structure obtained from the same samples.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Specimen charging in X-ray absorption spectroscopy: correction of total electron yield data from stabilized zirconia in the energy range 250–915 eV</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-03-01</prism:publicationDate>
    <prism:startingPage>224</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>233</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi0110">
    <title>Heterologous metalloprotein biosynthesis in Escherichia coli: conditions for the overproduction of functional copper-containing nitrite reductase and azurin from Alcaligenes xylosoxidans</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi0110</link>
    <description>This paper reports on the optimization of conditions for the overproduction and isolation of two recombinant copper metalloproteins, originally encoded on the chromosome of the dentrifying soil bacterium Alcaligenes xylosoxidans, in the heterologous host Escherichia coli. The trimeric enzyme nitrite reductase (NiR) contains both type-1 and type-2 Cu centres, whilst its putative redox partner, azurin I, is monomeric and has only a type-1 Cu centre. Both proteins were processed and exported to the periplasm of E. coli, which is consistent with their periplasmic location in their native host A. xylosoxidans. NiR could be readily purified from the periplasmic fraction of E. coli but the enzyme as isolated possessed only type-1 Cu centres. The type-2 Cu centre could be fully reconstituted by incubation of the periplasmic fraction with copper sulfate prior to enzyme purification. Azurin I could only be isolated with a fully occupied type-1 centre when isolated from the crude cell extract but not after isolation from the periplasmic fraction, suggesting loss of the copper due to proteolysis. Based on a number of criteria, including spectroscopic, mass spectrometric, biochemical and structural analyses, both recombinant proteins were found to be indistinguishable from their native counterparts isolated from A. xylosoxidans. The findings of this work have important implications for the overproduction of recombinant metalloproteins in heterologous hosts.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Harris, R.L.</dc:creator>
    <dc:creator>Prudêncio, M.</dc:creator>
    <dc:creator>Hasnain, S.S.</dc:creator>
    <dc:creator>Eady, R.R.</dc:creator>
    <dc:creator>Sawers, R.G.</dc:creator>
    <dc:date>2005-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504027852</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Heterologous overproduction of the copper proteins nitrite reductase and azurin I from Alcaligenes xylosoxidans in Escherichia coli is described. Optimisation of conditions delivered recombinant proteins that were biochemically and spectroscopically indistinguishable from the native proteins.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COPPER PROTEINS; HETEROLOGOUS PROTEIN PRODUCTION; DENITRIFICATION; CRYSTAL STRUCTURE; METAL CENTRES</dc:subject>
    <dc:description>This paper reports on the optimization of conditions for the overproduction and isolation of two recombinant copper metalloproteins, originally encoded on the chromosome of the dentrifying soil bacterium Alcaligenes xylosoxidans, in the heterologous host Escherichia coli. The trimeric enzyme nitrite reductase (NiR) contains both type-1 and type-2 Cu centres, whilst its putative redox partner, azurin I, is monomeric and has only a type-1 Cu centre. Both proteins were processed and exported to the periplasm of E. coli, which is consistent with their periplasmic location in their native host A. xylosoxidans. NiR could be readily purified from the periplasmic fraction of E. coli but the enzyme as isolated possessed only type-1 Cu centres. The type-2 Cu centre could be fully reconstituted by incubation of the periplasmic fraction with copper sulfate prior to enzyme purification. Azurin I could only be isolated with a fully occupied type-1 centre when isolated from the crude cell extract but not after isolation from the periplasmic fraction, suggesting loss of the copper due to proteolysis. Based on a number of criteria, including spectroscopic, mass spectrometric, biochemical and structural analyses, both recombinant proteins were found to be indistinguishable from their native counterparts isolated from A. xylosoxidans. The findings of this work have important implications for the overproduction of recombinant metalloproteins in heterologous hosts.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Heterologous metalloprotein biosynthesis in Escherichia coli: conditions for the overproduction of functional copper-containing nitrite reductase and azurin from Alcaligenes xylosoxidans</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-01-01</prism:publicationDate>
    <prism:startingPage>13</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>18</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi0114">
    <title>Towards the high-throughput expression of metallo­proteins from the Mycobacterium tuberculosis genome</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi0114</link>
    <description>The provision of high-quality protein in adequate quantities is a prerequisite for any structural genomics programme. A number of proteins from the Mycobacterium tuberculosis genome have been expressed and the success at each stage of the process assessed. Major difficulties have been encountered in the purification and solubilization of many of these proteins, most likely as a result of mis-folding. Some improvements have been made to the protocol but the overall success rate is still limited; however, the use of a cell-free protein expression system will circumvent some of the difficulties encountered. Alternative purification systems are also required and the properties of a mutant blue copper protein are described, that may offer a combined purification and tagging system.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Hall, J.F.</dc:creator>
    <dc:creator>Ellis, M.J.</dc:creator>
    <dc:creator>Kigawa, T.</dc:creator>
    <dc:creator>Yabuki, T.</dc:creator>
    <dc:creator>Matsuda, T.</dc:creator>
    <dc:creator>Seki, E.</dc:creator>
    <dc:creator>Hasnain, S.S.</dc:creator>
    <dc:creator>Yokoyama, S.</dc:creator>
    <dc:date>2005-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504027864</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Attempts to produce high-quality protein from the MTB genome using the established pET expression system in E. coli are shown. The difficulties encountered at each stage are assessed and the need for alternative purification methodologies are suggested.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MYCOBACTERIUM TUBERCULOSIS; METALLOPROTEINS; CELL-FREE PROTEIN EXPRESSION; PURIFICATION TAGS</dc:subject>
    <dc:description>The provision of high-quality protein in adequate quantities is a prerequisite for any structural genomics programme. A number of proteins from the Mycobacterium tuberculosis genome have been expressed and the success at each stage of the process assessed. Major difficulties have been encountered in the purification and solubilization of many of these proteins, most likely as a result of mis-folding. Some improvements have been made to the protocol but the overall success rate is still limited; however, the use of a cell-free protein expression system will circumvent some of the difficulties encountered. Alternative purification systems are also required and the properties of a mutant blue copper protein are described, that may offer a combined purification and tagging system.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Towards the high-throughput expression of metallo­proteins from the Mycobacterium tuberculosis genome</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-01-01</prism:publicationDate>
    <prism:startingPage>4</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>7</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kv5005">
    <title>Softer and soft X-rays in macromolecular crystallography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kv5005</link>
    <description>The utilization and the potential of softer and soft X-rays in macromolecular crystallography as well as the challenges associated with the corresponding diffraction experiments and their possible remedies are reviewed.</description>
    <dc:rights>Copyright (c) 2005 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Djinović Carugo, K.</dc:creator>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:creator>Stuhrmann, H.</dc:creator>
    <dc:creator>Weiss, M.S.</dc:creator>
    <dc:date>2005-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504025762</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The utilization and the potential of softer and soft X-rays in macromolecular crystallography as well as the challenges associated with the corresponding diffraction experiments and their possible remedies are reviewed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY CRYSTALLOGRAPHY; LONGER WAVELENGTHS (1.5-3.0A); LONG WAVELENGTHS (&gt;3.0A); SOFTER X-RAYS (1.5-3.0A); SOFT X-RAYS (&gt;3.0A); X-RAY ABSORPTION; ANOMALOUS SCATTERING</dc:subject>
    <dc:description>The utilization and the potential of softer and soft X-rays in macromolecular crystallography as well as the challenges associated with the corresponding diffraction experiments and their possible remedies are reviewed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Softer and soft X-rays in macromolecular crystallography</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>12</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2005 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2005-07-01</prism:publicationDate>
    <prism:startingPage>410</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>419</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0277">
    <title>Current events</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0277</link>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:date>2004-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504025531</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Current events</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-11-01</prism:publicationDate>
    <prism:startingPage>510</prism:startingPage>
    <prism:section>current events</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>511</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5559">
    <title>Comments on Treatment of EXAFS data taken in the fluorescence mode in non-linear conditions by G. Ciatto et al. (2004). J. Synchrotron Rad. 11, 278–283</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5559</link>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Warburton, W.K.</dc:creator>
    <dc:date>2004-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504024665</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Correcting for fast-channel dead time is suggested as a means for further improving the accuracy of EXAFS data collected under non-linear conditions.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Comments on Treatment of EXAFS data taken in the fluorescence mode in non-linear conditions by G. Ciatto et al. (2004). J. Synchrotron Rad. 11, 278–283</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-11-01</prism:publicationDate>
    <prism:startingPage>508</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>508</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot2006">
    <title>Response to W. K. Warburton's Comments on Treatment of EXAFS data taken in the fluorescence mode in non-linear conditions by G. Ciatto et al. (2004). J. Synchrotron Rad. 11, 278–283</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot2006</link>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ciatto, G.</dc:creator>
    <dc:creator>d'Acapito, F.</dc:creator>
    <dc:creator>Boscherini, F.</dc:creator>
    <dc:creator>Mobilio, S.</dc:creator>
    <dc:date>2004-11-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504024598</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Responses are made to W. K. Warburton's comments in the previous paper concerning the treatment of EXAFS data taken in the fluorescence mode in non-linear conditions presented earlier.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Response to W. K. Warburton's Comments on Treatment of EXAFS data taken in the fluorescence mode in non-linear conditions by G. Ciatto et al. (2004). J. Synchrotron Rad. 11, 278–283</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>6</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-11-01</prism:publicationDate>
    <prism:startingPage>509</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>509</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0265">
    <title>Aberration corrected vacuum ultraviolet monochromator</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0265</link>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schoeffel, E.</dc:creator>
    <dc:date>2004-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504019740</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Aberration corrected vacuum ultraviolet monochromator</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-09-01</prism:publicationDate>
    <prism:startingPage>442</prism:startingPage>
    <prism:section>new commercial products</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>442</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ml5199">
    <title>The BioCAT undulator beamline 18ID: a facility for biological non-crystalline diffraction and X-ray absorption spectroscopy at the Advanced Photon Source</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ml5199</link>
    <description>The 18ID undulator beamline of the Biophysics Collaborative Access Team at the Advanced Photon Source, Argonne, IL, USA, is a high-performance instrument designed for, and dedicated to, the study of partially ordered and disordered biological materials using the techniques of small-angle X-ray scattering, fiber diffraction, and X-ray absorption spectroscopy. The beamline and associated instrumentation are described in detail and examples of the representative experimental results are presented.</description>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Fischetti, R.</dc:creator>
    <dc:creator>Stepanov, S.</dc:creator>
    <dc:creator>Rosenbaum, G.</dc:creator>
    <dc:creator>Barrea, R.</dc:creator>
    <dc:creator>Black, E.</dc:creator>
    <dc:creator>Gore, D.</dc:creator>
    <dc:creator>Heurich, R.</dc:creator>
    <dc:creator>Kondrashkina, E.</dc:creator>
    <dc:creator>Kropf, A.J.</dc:creator>
    <dc:creator>Wang, S.</dc:creator>
    <dc:creator>Zhang, K.</dc:creator>
    <dc:creator>Irving, T.C.</dc:creator>
    <dc:creator>Bunker, G.B.</dc:creator>
    <dc:date>2004-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504016760</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The undulator beamline of the Biophysics Collaborative Access Team (BioCAT), a national user facility designed and dedicated to the study of partially ordered and disordered biological materials, is described and examples of its capabilities are presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY BEAMLINES; NON-CRYSTALLINE DIFFRACTION; SMALL-ANGLE X-RAY SCATTERING; X-RAY ABSORPTION SPECTROSCOPY; XAFS; XANES; EXAFS</dc:subject>
    <dc:description>The 18ID undulator beamline of the Biophysics Collaborative Access Team at the Advanced Photon Source, Argonne, IL, USA, is a high-performance instrument designed for, and dedicated to, the study of partially ordered and disordered biological materials using the techniques of small-angle X-ray scattering, fiber diffraction, and X-ray absorption spectroscopy. The beamline and associated instrumentation are described in detail and examples of the representative experimental results are presented.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The BioCAT undulator beamline 18ID: a facility for biological non-crystalline diffraction and X-ray absorption spectroscopy at the Advanced Photon Source</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-09-01</prism:publicationDate>
    <prism:startingPage>399</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>405</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0262">
    <title>Carl-Ivar Brändén, 1934–2004</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0262</link>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schneider, G.</dc:creator>
    <dc:creator>Lindqvist, Y.</dc:creator>
    <dc:creator>Andersson, I.</dc:creator>
    <dc:creator>Knight, S.</dc:creator>
    <dc:date>2004-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504018175</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Carl-Ivar Brändén, 1934–2004</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-09-01</prism:publicationDate>
    <prism:startingPage>371</prism:startingPage>
    <prism:section>obituaries</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>371</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?me0260">
    <title>Cullie Sparks, 1929–2004</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?me0260</link>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Ice, G.E.</dc:creator>
    <dc:date>2004-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504014402</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Cullie Sparks, 1929–2004</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-07-01</prism:publicationDate>
    <prism:startingPage>303</prism:startingPage>
    <prism:section>obituaries</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>303</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?fd5004">
    <title>Image quality improvement in a hard X-ray projection microscope using total reflection mirror optics</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?fd5004</link>
    <description>A new figure correction method has been applied in order to fabricate an elliptical mirror to realize a one-dimensionally diverging X-ray beam having high image quality. Mutual relations between figure errors and intensity uniformities of diverging X-ray beams have also been investigated using a wave-optical simulator and indicate that figure errors in relatively short spatial wavelength ranges lead to high-contrast interference fringes. By using a microstitching interferometer and elastic emission machining, figure correction of an elliptical mirror with a lateral resolution close to 0.1 mm was carried out. A one-dimensional diverging X-ray obtained using the fabricated mirror was observed at SPring-8 and evaluated to have a sufficiently flat intensity distribution.</description>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Mimura, H.</dc:creator>
    <dc:creator>Yamauchi, K.</dc:creator>
    <dc:creator>Yamamura, K.</dc:creator>
    <dc:creator>Kubota, A.</dc:creator>
    <dc:creator>Matsuyama, S.</dc:creator>
    <dc:creator>Sano, Y.</dc:creator>
    <dc:creator>Ueno, K.</dc:creator>
    <dc:creator>Endo, K.</dc:creator>
    <dc:creator>Nishino, Y.</dc:creator>
    <dc:creator>Tamasaku, K.</dc:creator>
    <dc:creator>Yabashi, M.</dc:creator>
    <dc:creator>Ishikawa, T.</dc:creator>
    <dc:creator>Mori, Y.</dc:creator>
    <dc:date>2004-07-01</dc:date>
    <dc:identifier>doi:10.1107/S090904950401283X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Highly accurate elliptical mirrors have been fabricated and evaluated to have high image quality in one-dimensionally diverging X-ray beams.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY PROJECTION MICROSCOPES; COHERENT X-RAYS; X-RAY FOCUSING; WAVE-OPTICAL SIMULATION; EEM; MSI</dc:subject>
    <dc:description>A new figure correction method has been applied in order to fabricate an elliptical mirror to realize a one-dimensionally diverging X-ray beam having high image quality. Mutual relations between figure errors and intensity uniformities of diverging X-ray beams have also been investigated using a wave-optical simulator and indicate that figure errors in relatively short spatial wavelength ranges lead to high-contrast interference fringes. By using a microstitching interferometer and elastic emission machining, figure correction of an elliptical mirror with a lateral resolution close to 0.1 mm was carried out. A one-dimensional diverging X-ray obtained using the fabricated mirror was observed at SPring-8 and evaluated to have a sufficiently flat intensity distribution.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Image quality improvement in a hard X-ray projection microscope using total reflection mirror optics</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-07-01</prism:publicationDate>
    <prism:startingPage>343</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>346</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?he5286">
    <title>A large-area CMOS imager as an X-ray detector for synchrotron radiation experiments</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?he5286</link>
    <description>The performance of a CMOS flatpanel imager from Hamamatsu Photonics (C7942) has been tested in various synchrotron radiation experiments. This detector has a detection area of about 120 mm × 120 mm with 0.05 mm pixels, and a frame rate of 2 s−1. The commercially available product was insensitive to X-rays with an energy lower than 15 keV, but slight modifications solved this problem. Images obtained in small-angle scattering, protein crystallography and medical imaging experiments were all of high quality. The fast readout and the large area are advantageous in real-time imaging. Although its noise level is higher than the area detectors that are currently used in synchrotron radiation experiments, it is particularly useful in experiments where other bulky detectors cannot be used. Its relatively low price (about USD 30000) makes it a unique option in the choice of detectors.</description>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:creator>Yamamoto, M.</dc:creator>
    <dc:creator>Uesugi, K.</dc:creator>
    <dc:creator>Inoue, K.</dc:creator>
    <dc:date>2004-07-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504008519</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A CMOS flatpanel detector has been tested in various synchrotron radiation experiments.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CMOS DETECTOR; SMALL-ANGLE DIFFRACTION; MEDICAL IMAGING; PROTEIN CRYSTALLOGRAPHY; SPRING-8</dc:subject>
    <dc:description>The performance of a CMOS flatpanel imager from Hamamatsu Photonics (C7942) has been tested in various synchrotron radiation experiments. This detector has a detection area of about 120 mm × 120 mm with 0.05 mm pixels, and a frame rate of 2 s−1. The commercially available product was insensitive to X-rays with an energy lower than 15 keV, but slight modifications solved this problem. Images obtained in small-angle scattering, protein crystallography and medical imaging experiments were all of high quality. The fast readout and the large area are advantageous in real-time imaging. Although its noise level is higher than the area detectors that are currently used in synchrotron radiation experiments, it is particularly useful in experiments where other bulky detectors cannot be used. Its relatively low price (about USD 30000) makes it a unique option in the choice of detectors.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A large-area CMOS imager as an X-ray detector for synchrotron radiation experiments</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>4</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-07-01</prism:publicationDate>
    <prism:startingPage>347</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>352</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pm5003">
    <title>Soft X-ray resonant magnetic scattering from a Ni layer with modulated magnetic anisotropy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pm5003</link>
    <description>Soft X-ray resonant magnetic scattering studies on a magnetically modulated, but nominally chemically homogenous, 5 nm Ni layer in a Cu/Ni/Cu/Co/NiO/GaAs(110) system are reported. It was possible to estimate the main chemical structure of the sample on the basis of the results from specular reflectivity and rocking scans, probing the scattering vector components in the perpendicular and in-plane direction to the Ni wires, respectively. The magnetic scattering using polarized X-rays demonstrates the magnetic modulation of the Ni layer.</description>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Haznar, A.</dc:creator>
    <dc:creator>Laan, G. van der</dc:creator>
    <dc:creator>Collins, S.P.</dc:creator>
    <dc:creator>Vaz, C.A.F.</dc:creator>
    <dc:creator>Bland, J.A.C.</dc:creator>
    <dc:creator>Dhesi, S.S.</dc:creator>
    <dc:date>2004-05-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049504004868</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Structural and magnetic characterization of a magnetically modulated 5 nm Ni layer in a Cu/Ni/Cu system using specular reflection and rocking scans in X-ray resonant scattering with polarized soft X-rays.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY RESONANT MAGNETIC SCATTERING; NANOSTRUCTURES</dc:subject>
    <dc:description>Soft X-ray resonant magnetic scattering studies on a magnetically modulated, but nominally chemically homogenous, 5 nm Ni layer in a Cu/Ni/Cu/Co/NiO/GaAs(110) system are reported. It was possible to estimate the main chemical structure of the sample on the basis of the results from specular reflectivity and rocking scans, probing the scattering vector components in the perpendicular and in-plane direction to the Ni wires, respectively. The magnetic scattering using polarized X-rays demonstrates the magnetic modulation of the Ni layer.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Soft X-ray resonant magnetic scattering from a Ni layer with modulated magnetic anisotropy</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>3</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-05-01</prism:publicationDate>
    <prism:startingPage>254</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>260</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ot5554">
    <title>XAFS imaging of Tsukuba gabbroic rocks: area analysis of chemical composition and local structure</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ot5554</link>
    <description>Gabbroic rocks were collected at Mount Tsukuba in Japan, and their XAFS images were studied using a projection-type X-ray fluorescence (XRF) microscope, which is a powerful new tool recently developed for extremely rapid imaging. The instrument employs a grazing-incidence arrangement in order that primary X-rays illuminate the whole sample surface, as well as parallel-beam optics and an extremely close geometry in order to detect XRF by a high-performance X-ray CCD system with 1024 × 1024 pixels. The XRF image indicated that black amphibole and white feldspar, both of which are typical mineral textures of the rock, contain iron. The origin has been suggested to be several small yellowish-brown minerals contained there. The XAFS imaging has been carried out by repeating the exposure of XRF images during the energy scan of the primary X-rays. It has been found that the structure is qualitatively close to that of olivine, and the main differences found in both areas can be explained as a difference in iron and magnesium concentration, i.e. the mixed ratio of forsterite (Mg2SiO4) and fayalite (Fe2SiO4). The feasibility of the present XAFS imaging method has been demonstrated for realistic inhomogeneous minerals.</description>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Mizusawa, M.</dc:creator>
    <dc:creator>Sakurai, K.</dc:creator>
    <dc:date>2004-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049503028024</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Local structure studies on Tsukuba gabbroic rocks are presented. A novel imaging tool, a projection-type XRF microscope, has been applied.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY FLUORESCENCE; NON-SCANNING IMAGING; PROJECTION MICROSCOPE; IRON; OLIVINE; AMPHIBOLE; FELDSPAR</dc:subject>
    <dc:description>Gabbroic rocks were collected at Mount Tsukuba in Japan, and their XAFS images were studied using a projection-type X-ray fluorescence (XRF) microscope, which is a powerful new tool recently developed for extremely rapid imaging. The instrument employs a grazing-incidence arrangement in order that primary X-rays illuminate the whole sample surface, as well as parallel-beam optics and an extremely close geometry in order to detect XRF by a high-performance X-ray CCD system with 1024 × 1024 pixels. The XRF image indicated that black amphibole and white feldspar, both of which are typical mineral textures of the rock, contain iron. The origin has been suggested to be several small yellowish-brown minerals contained there. The XAFS imaging has been carried out by repeating the exposure of XRF images during the energy scan of the primary X-rays. It has been found that the structure is qualitatively close to that of olivine, and the main differences found in both areas can be explained as a difference in iron and magnesium concentration, i.e. the mixed ratio of forsterite (Mg2SiO4) and fayalite (Fe2SiO4). The feasibility of the present XAFS imaging method has been demonstrated for realistic inhomogeneous minerals.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>XAFS imaging of Tsukuba gabbroic rocks: area analysis of chemical composition and local structure</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-03-01</prism:publicationDate>
    <prism:startingPage>209</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>213</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys0029">
    <title>Recent developments in the PHENIX software for automated crystallographic structure determination</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys0029</link>
    <description>A new software system called PHENIX (Python-based Hierarchical ENvironment for Integrated Xtallography) is being developed for the automation of crystallographic structure solution. This will provide the necessary algorithms to proceed from reduced intensity data to a refined molecular model, and facilitate structure solution for both the novice and expert crystallographer. Here, the features of PHENIXare reviewed and the recent advances in infrastructure and algorithms are briefly described.</description>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Adams, P.D.</dc:creator>
    <dc:creator>Gopal, K.</dc:creator>
    <dc:creator>Grosse-Kunstleve, R.W.</dc:creator>
    <dc:creator>Hung, L.-W.</dc:creator>
    <dc:creator>Ioerger, T.R.</dc:creator>
    <dc:creator>McCoy, A.J.</dc:creator>
    <dc:creator>Moriarty, N.W.</dc:creator>
    <dc:creator>Pai, R.K.</dc:creator>
    <dc:creator>Read, R.J.</dc:creator>
    <dc:creator>Romo, T.D.</dc:creator>
    <dc:creator>Sacchettini, J.C.</dc:creator>
    <dc:creator>Sauter, N.K.</dc:creator>
    <dc:creator>Storoni, L.C.</dc:creator>
    <dc:creator>Terwilliger, T.C.</dc:creator>
    <dc:date>2004-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049503024130</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Recent developments in PHENIX, a new software system for automated crystallographic structure determination, are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PHENIX; PYTHON; OBJECT-ORIENTED PROGRAMMING; STRATEGIES</dc:subject>
    <dc:description>A new software system called PHENIX (Python-based Hierarchical ENvironment for Integrated Xtallography) is being developed for the automation of crystallographic structure solution. This will provide the necessary algorithms to proceed from reduced intensity data to a refined molecular model, and facilitate structure solution for both the novice and expert crystallographer. Here, the features of PHENIXare reviewed and the recent advances in infrastructure and algorithms are briefly described.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Recent developments in the PHENIX software for automated crystallographic structure determination</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-01-01</prism:publicationDate>
    <prism:startingPage>53</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>55</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ys0022">
    <title>SOLVE and RESOLVE: automated structure solution, density modification and model building</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ys0022</link>
    <description>The software SOLVE and RESOLVE can carry out all the steps in macromolecular structure solution, from scaling and heavy-atom location through phasing, density modification and model-building in the MAD, SAD and MIR cases. SOLVE uses scoring scheme to convert the decision-making in macromolecular structure solution to an optimization problem. RESOLVE carries out the identification of NCS, density modification and automated model-building. The procedure is fully automated and can function at resolutions as low as 3 Å.</description>
    <dc:rights>Copyright (c) 2004 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Terwilliger, T.</dc:creator>
    <dc:date>2004-01-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049503023938</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:subject>MIR/MAD; SAD; SAS; SOFTWARE</dc:subject>
    <dc:description>The software SOLVE and RESOLVE can carry out all the steps in macromolecular structure solution, from scaling and heavy-atom location through phasing, density modification and model-building in the MAD, SAD and MIR cases. SOLVE uses scoring scheme to convert the decision-making in macromolecular structure solution to an optimization problem. RESOLVE carries out the identification of NCS, density modification and automated model-building. The procedure is fully automated and can function at resolutions as low as 3 Å.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>SOLVE and RESOLVE: automated structure solution, density modification and model building</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>11</prism:volume>
    <prism:number>1</prism:number>
    <prism:copyright>Copyright (c) 2004 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2004-01-01</prism:publicationDate>
    <prism:startingPage>49</prism:startingPage>
    <prism:section>research papers</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>52</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ht5034">
    <title>Third-Generation Hard X-ray Synchrotron Radiation Sources. Edited by D. M. Mills. New York: John Wiley, 2002. Price GBP 69.95, ISBN 0-471-31433-1.</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ht5034</link>
    <dc:rights>Copyright (c) 2003 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Schneider, J.</dc:creator>
    <dc:date>2003-09-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049503016704</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Third-Generation Hard X-ray Synchrotron Radiation Sources. Edited by D. M. Mills. New York: John Wiley, 2002. Price GBP 69.95, ISBN 0-471-31433-1.</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>10</prism:volume>
    <prism:number>5</prism:number>
    <prism:copyright>Copyright (c) 2003 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2003-09-01</prism:publicationDate>
    <prism:startingPage>405</prism:startingPage>
    <prism:section>book reviews</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>405</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi2947">
    <title>XAFS studies of nitrogenase: the MoFe and VFe proteins and the use of crystallographic coordinates in three-dimensional EXAFS data analysis. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi2947</link>
    <description>One of the authors was omitted in the published version of the paper by Strange et al. [J. Synchrotron Rad. (2003), 10, 71–75]. The full author list is given above. Since the acceptance of our paper, an atomic-resolution (1.16 Å) structure of MoFe-protein has emerged [Einsle et al. (2002), Science, 297, 1696–1700]. We take this opportunity to update Table 1 of the paper, demonstrating improved agreement of the three-dimensional XAFS refinement with atomic-resolution metrical information.</description>
    <dc:rights>Copyright (c) 2003 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Strange, R.W.</dc:creator>
    <dc:creator>Smith, B.E.</dc:creator>
    <dc:creator>Eady, R.R.</dc:creator>
    <dc:creator>Lawson, D.</dc:creator>
    <dc:creator>Hasnain, S.S.</dc:creator>
    <dc:date>2003-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049503004175</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Erratum to J. Synchrotron Rad. (2003), 10, 71–75.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>EXAFS; NITROGEN FIXATION; NITROGENASE; CRYSTAL STRUCTURE; FEMOCO</dc:subject>
    <dc:description>One of the authors was omitted in the published version of the paper by Strange et al. [J. Synchrotron Rad. (2003), 10, 71–75]. The full author list is given above. Since the acceptance of our paper, an atomic-resolution (1.16 Å) structure of MoFe-protein has emerged [Einsle et al. (2002), Science, 297, 1696–1700]. We take this opportunity to update Table 1 of the paper, demonstrating improved agreement of the three-dimensional XAFS refinement with atomic-resolution metrical information.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>XAFS studies of nitrogenase: the MoFe and VFe proteins and the use of crystallographic coordinates in three-dimensional EXAFS data analysis. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>10</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2003 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2003-03-01</prism:publicationDate>
    <prism:startingPage>197</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>197</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hi9100">
    <title>Multiple-electron excitation in X-ray absorption: a simple generic model. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hi9100</link>
    <description>Two typographical errors have been observed in the paper by Roy et al. [J. Synchrotron Rad. (2001), 8, 1103–1108]. Equation (16) should read\eqalign{P(\hbar\omega)={}&amp;P(\infty)\left[{{{\pi(2n-1)!}\over{2^{2n}(n-1)!(n+1)!}}}\right]^{-1}E_B^{\,n+1/2}\cr&amp;\times\int\limits_0^{E_{\max}}{{{E^{1/2}}\over{(E_B+E)^{n+2}[1+t_{\,o}^{\,2}\,(E_B+E)^2]}}}\,\,{\rm{d}}E,}while the correct form of equation (18) is\eqalign{P(\hbar\omega)={}&amp;P(\infty)\left[{{{\pi(2n-1)!}\over{2^{2n}(n-1)!(n+1)!}}}\right]^{-1}\cr&amp;\times\int\limits_1^{E_p/E_B}{{{(X-1)^{1/2}}\over{X^{n+2}[1+{\textstyle{1\over4}}\left({n-1}\right)^2(E_B/E_p)X^2]}}}\,\,{\rm{d}}X.}These typographical errors do not affect our results or conclusions.</description>
    <dc:rights>Copyright (c) 2003 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Roy, M.</dc:creator>
    <dc:creator>Lindsay, J.D.</dc:creator>
    <dc:creator>Louch, S.</dc:creator>
    <dc:creator>Gurman, S.J.</dc:creator>
    <dc:date>2003-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049503002656</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Erratum to J. Synchrotron Rad. (2001), 8, 1103–1108.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY ABSORPTION; EXAFS; MANY-BODY THEORY</dc:subject>
    <dc:description>Two typographical errors have been observed in the paper by Roy et al. [J. Synchrotron Rad. (2001), 8, 1103–1108]. Equation (16) should read\eqalign{P(\hbar\omega)={}&amp;P(\infty)\left[{{{\pi(2n-1)!}\over{2^{2n}(n-1)!(n+1)!}}}\right]^{-1}E_B^{\,n+1/2}\cr&amp;\times\int\limits_0^{E_{\max}}{{{E^{1/2}}\over{(E_B+E)^{n+2}[1+t_{\,o}^{\,2}\,(E_B+E)^2]}}}\,\,{\rm{d}}E,}while the correct form of equation (18) is\eqalign{P(\hbar\omega)={}&amp;P(\infty)\left[{{{\pi(2n-1)!}\over{2^{2n}(n-1)!(n+1)!}}}\right]^{-1}\cr&amp;\times\int\limits_1^{E_p/E_B}{{{(X-1)^{1/2}}\over{X^{n+2}[1+{\textstyle{1\over4}}\left({n-1}\right)^2(E_B/E_p)X^2]}}}\,\,{\rm{d}}X.}These typographical errors do not affect our results or conclusions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Multiple-electron excitation in X-ray absorption: a simple generic model. Erratum</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>10</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2003 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2003-03-01</prism:publicationDate>
    <prism:startingPage>197</prism:startingPage>
    <prism:section>addenda and errata</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>197</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ml2020">
    <title>Response to P. Suortti et al.'s and K. D. Rogers et al.'s Comments on Synchrotron fibre diffraction identifies and locates foetal collagenous breast tissue associated with breast carcinoma by V. J. James (2002). J. Synchrotron Rad. 9, 71–76</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ml2020</link>
    <dc:rights>Copyright (c) 2003 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>James, V.</dc:creator>
    <dc:date>2003-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049503002103</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Responses are made to P. Suortti et al.'s and K. D. Rogers et al.'s comments in the two previous papers.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Response to P. Suortti et al.'s and K. D. Rogers et al.'s Comments on Synchrotron fibre diffraction identifies and locates foetal collagenous breast tissue associated with breast carcinoma by V. J. James (2002). J. Synchrotron Rad. 9, 71–76</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>10</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2003 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2003-03-01</prism:publicationDate>
    <prism:startingPage>200</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>201</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ml2019">
    <title>Comments on Synchrotron fibre diffraction identifies and locates foetal collagenous breast tissue associated with breast carcinoma by V. J. James (2002). J. Synchrotron Rad. 9, 71–76</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ml2019</link>
    <dc:rights>Copyright (c) 2003 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Rogers, K.D.</dc:creator>
    <dc:creator>Hall, C.J.</dc:creator>
    <dc:creator>Hufton, A.</dc:creator>
    <dc:creator>Pinder, S.E.</dc:creator>
    <dc:date>2003-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049503002097</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Concerns regarding aspects of the paper by James (2002) are given.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Comments on Synchrotron fibre diffraction identifies and locates foetal collagenous breast tissue associated with breast carcinoma by V. J. James (2002). J. Synchrotron Rad. 9, 71–76</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>10</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2003 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2003-03-01</prism:publicationDate>
    <prism:startingPage>199</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>199</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ml2018">
    <title>Comments on Synchrotron fibre diffraction identifies and locates foetal collagenous breast tissue associated with breast carcinoma by V. J. James (2002). J. Synchrotron Rad. 9, 71–76</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ml2018</link>
    <dc:rights>Copyright (c) 2003 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0909-0495</dc:source>
    <dc:creator>Suortti, P.</dc:creator>
    <dc:creator>Fernández, M.</dc:creator>
    <dc:creator>Urban, V.</dc:creator>
    <dc:date>2003-03-01</dc:date>
    <dc:identifier>doi:10.1107/S0909049502017508</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The interpretation of data in the paper by James (2002) is questioned.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:format>text/html</dc:format>
    <dc:title>Comments on Synchrotron fibre diffraction identifies and locates foetal collagenous breast tissue associated with breast carcinoma by V. J. James (2002). J. Synchrotron Rad. 9, 71–76</dc:title>
    <dc:type>text</dc:type>
    <prism:volume>10</prism:volume>
    <prism:number>2</prism:number>
    <prism:copyright>Copyright (c) 2003 International Union of Crystallography</prism:copyright>
    <prism:publicationName>Journal of Synchrotron Radiation</prism:publicationName>
    <prism:publicationDate>2003-03-01</prism:publicationDate>
    <prism:startingPage>198</prism:startingPage>
    <prism:section>letters to the editor</prism:section>
    <prism:issn>0909-0495</prism:issn>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>198</prism:endingPage>
    <prism:eissn>1600-5775</prism:eissn>
  </item>
</rdf:RDF>
