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    <title>Open access article in Journal of Applied Crystallography</title>
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    <description>Journal of Applied Crystallography covers a wide range of crystallographic topics from the viewpoints of both techniques and theory. The journal presents papers on the application of crystallographic techniques and on the related apparatus and computer software. For many years, the Journal of Applied Crystallography has been the main vehicle for the publication of small-angle scattering papers and powder diffraction techniques. The journal is the primary place where crystallographic computer program information is published. Recent additions are a Cryocrystallography Papers section and a Software Reviews section.</description>
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    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:creator>International Union of Crystallography</dc:creator>
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    <dc:identifier>urn:issn:0021-8898</dc:identifier>
    <dc:description>Journal of Applied Crystallography covers a wide range of crystallographic topics from the viewpoints of both techniques and theory. The journal presents papers on the application of crystallographic techniques and on the related apparatus and computer software. For many years, the Journal of Applied Crystallography has been the main vehicle for the publication of small-angle scattering papers and powder diffraction techniques. The journal is the primary place where crystallographic computer program information is published. Recent additions are a Cryocrystallography Papers section and a Software Reviews section.</dc:description>
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    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
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    <description>The Crystallography Open Database (COD), which is a project that aims to gather all available inorganic, metal–organic and small organic molecule structural data in one database, is described. The database adopts an open-access model. The COD currently contains ∼80 000 entries in crystallographic information file format, with nearly full coverage of the International Union of Crystallography publications, and is growing in size and quality.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Gražulis, S.</dc:creator>
    <dc:creator>Chateigner, D.</dc:creator>
    <dc:creator>Downs, R.T.</dc:creator>
    <dc:creator>Yokochi, A. T.</dc:creator>
    <dc:creator>Quirós, M.</dc:creator>
    <dc:creator>Lutterotti, L.</dc:creator>
    <dc:creator>Manakova, E.</dc:creator>
    <dc:creator>Butkus, J.</dc:creator>
    <dc:creator>Moeck, P.</dc:creator>
    <dc:creator>Le Bail, A.</dc:creator>
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    <dc:identifier>doi:10.1107/S0021889809016690</dc:identifier>
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    <dc:language>en</dc:language>
    <dc:subject>CRYSTALLOGRAPHY OPEN DATABASE; COD; STRUCTURAL DATABASES</dc:subject>
    <dc:description>The Crystallography Open Database (COD), which is a project that aims to gather all available inorganic, metal–organic and small organic molecule structural data in one database, is described. The database adopts an open-access model. The COD currently contains ∼80 000 entries in crystallographic information file format, with nearly full coverage of the International Union of Crystallography publications, and is growing in size and quality.</dc:description>
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    <dc:title>Crystallography Open Database – an open-access collection of crystal structures</dc:title>
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    <title>Re-evaluation of formulae for X-ray stress analysis in polycrystalline specimens with fibre texture. Erratum</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ko9074</link>
    <description>Errors in the paper by Yokoyama &amp; Harada [J. Appl. Cryst. (2009), 42, 185–191] are corrected.</description>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Yokoyama, R.</dc:creator>
    <dc:creator>Harada, J.</dc:creator>
    <dc:date>2009-06-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889809015660</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Errors in the paper by Yokoyama &amp; Harada [J. Appl. Cryst. (2009), 42, 185–191] are corrected.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RESIDUAL STRESS; FIBRE TEXTURE; LAUE CLASSES</dc:subject>
    <dc:description>Errors in the paper by Yokoyama &amp; Harada [J. Appl. Cryst. (2009), 42, 185–191] are corrected.</dc:description>
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    <dc:title>Re-evaluation of formulae for X-ray stress analysis in polycrystalline specimens with fibre texture. Erratum</dc:title>
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    <prism:volume>42</prism:volume>
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    <prism:issn>0021-8898</prism:issn>
    <prism:section>addenda and errata</prism:section>
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  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?db5060">
    <title>The pseudo-single-crystal method: a third approach to crystal structure determination</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?db5060</link>
    <description>A novel method that enables single-crystal diffraction data to be obtained from a powder sample is presented. A suspension of LiCoPO4 microrods was subjected to a frequency-modulated dynamic elliptical magnetic field to align the microrods; the alignment achieved was consolidated by photopolymerization of the suspending UV-curable monomer. The composite thus obtained (referred to as a pseudo single crystal) gave rise to X-ray diffraction data from which the crystal structure was solved using the standard method for single-crystal X-ray analyses. The structure determined was in good agreement with that reported using a conventional single crystal.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
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    <dc:creator>Kimura, T.</dc:creator>
    <dc:creator>Chang, C.</dc:creator>
    <dc:creator>Kimura, F.</dc:creator>
    <dc:creator>Maeyama, M.</dc:creator>
    <dc:date>2009-06-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889809013430</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A novel method that enables single-crystal diffraction data to be obtained from a powder sample is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PSEUDO SINGLE CRYSTALS; X-RAY DIFFRACTION; LICOPO4 MICRORODS</dc:subject>
    <dc:description>A novel method that enables single-crystal diffraction data to be obtained from a powder sample is presented. A suspension of LiCoPO4 microrods was subjected to a frequency-modulated dynamic elliptical magnetic field to align the microrods; the alignment achieved was consolidated by photopolymerization of the suspending UV-curable monomer. The composite thus obtained (referred to as a pseudo single crystal) gave rise to X-ray diffraction data from which the crystal structure was solved using the standard method for single-crystal X-ray analyses. The structure determined was in good agreement with that reported using a conventional single crystal.</dc:description>
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    <dc:title>The pseudo-single-crystal method: a third approach to crystal structure determination</dc:title>
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    <prism:volume>42</prism:volume>
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    <prism:section>short communications</prism:section>
    <prism:startingPage>535</prism:startingPage>
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  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks5196">
    <title>Elastic constants of fibre-textured thin films determined by X-ray diffraction</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks5196</link>
    <description>A new methodology is presented that allows the rapid determination of elastic constants of cubic fibre-textured thin films by X-ray diffraction. The theoretical concept is developed and tested on calculated examples of Cu and CrN films. The mechanical elastic constants are extrapolated from X-ray elastic constants by taking into consideration crystal and macroscopic elastic anisotropy. The derived algorithm enables the determination of a reflection and the corresponding value of the X-ray anisotropic factor Γ for which the X-ray elastic constants are equal to their mechanical counterparts in the case of fibre-textured cubic polycrystalline aggregates. The approach is independent of the crystal elastic anisotropy and depends on the fibre-texture type, the texture sharpness, the number of randomly oriented crystallites and the supposed grain-interaction model. In the experimental part, out-of-plane Young's moduli of 111 and 311 fibre-textured Cu and CrN thin films deposited on monocrystalline Si(100) substrates are determined. The moduli are extrapolated from thin-film experimental X-ray elastic constants that are determined by a combination of X-ray diffraction substrate curvature and sin2ψ methods. For the calculation, the film macroscopic elastic anisotropy (texture) is considered. The advantage of the new technique lies in the fact that experimental moduli are determined nondestructively, using a static diffraction experiment, and represent volume-averaged quantities.</description>
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    <dc:creator>Martinschitz, K.J.</dc:creator>
    <dc:creator>Daniel, R.</dc:creator>
    <dc:creator>Mitterer, C.</dc:creator>
    <dc:creator>Keckes, J.</dc:creator>
    <dc:date>2009-06-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889809011807</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Supposing the Hill grain-interaction model, it is demonstrated that X-ray elastic constants can be used to determine mechanical elastic constants of cubic fibre-textured thin films. The new approach is demonstrated by the experimental characterization of out-of-plane moduli of fibre-textured Cu and CrN thin films.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY DIFFRACTION; THIN FILMS; ELASTIC CONSTANTS; FIBRE TEXTURE</dc:subject>
    <dc:description>A new methodology is presented that allows the rapid determination of elastic constants of cubic fibre-textured thin films by X-ray diffraction. The theoretical concept is developed and tested on calculated examples of Cu and CrN films. The mechanical elastic constants are extrapolated from X-ray elastic constants by taking into consideration crystal and macroscopic elastic anisotropy. The derived algorithm enables the determination of a reflection and the corresponding value of the X-ray anisotropic factor Γ for which the X-ray elastic constants are equal to their mechanical counterparts in the case of fibre-textured cubic polycrystalline aggregates. The approach is independent of the crystal elastic anisotropy and depends on the fibre-texture type, the texture sharpness, the number of randomly oriented crystallites and the supposed grain-interaction model. In the experimental part, out-of-plane Young's moduli of 111 and 311 fibre-textured Cu and CrN thin films deposited on monocrystalline Si(100) substrates are determined. The moduli are extrapolated from thin-film experimental X-ray elastic constants that are determined by a combination of X-ray diffraction substrate curvature and sin2ψ methods. For the calculation, the film macroscopic elastic anisotropy (texture) is considered. The advantage of the new technique lies in the fact that experimental moduli are determined nondestructively, using a static diffraction experiment, and represent volume-averaged quantities.</dc:description>
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    <dc:title>Elastic constants of fibre-textured thin films determined by X-ray diffraction</dc:title>
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    <prism:number>3</prism:number>
    <prism:volume>42</prism:volume>
    <prism:publicationDate>2009-06-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>416</prism:startingPage>
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    <prism:endingPage>428</prism:endingPage>
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    <title>PDB_REDO: automated re-refinement of X-ray structure models in the PDB</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?he5437</link>
    <description>Structural biology, homology modelling and rational drug design require accurate three-dimensional macromolecular coordinates. However, the coordinates in the Protein Data Bank (PDB) have not all been obtained using the latest experimental and computational methods. In this study a method is presented for automated re-refinement of existing structure models in the PDB. A large-scale benchmark with 16 807 PDB entries showed that they can be improved in terms of fit to the deposited experimental X-ray data as well as in terms of geometric quality. The re-refinement protocol uses TLS models to describe concerted atom movement. The resulting structure models are made available through the PDB_REDO databank (http://www.cmbi.ru.nl/pdb_redo/). Grid computing techniques were used to overcome the computational requirements of this endeavour.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Joosten, R.P.</dc:creator>
    <dc:creator>Salzemann, J.</dc:creator>
    <dc:creator>Bloch, V.</dc:creator>
    <dc:creator>Stockinger, H.</dc:creator>
    <dc:creator>Berglund, A.-C.</dc:creator>
    <dc:creator>Blanchet, C.</dc:creator>
    <dc:creator>Bongcam-Rudloff, E.</dc:creator>
    <dc:creator>Combet, C.</dc:creator>
    <dc:creator>Da Costa, A.L.</dc:creator>
    <dc:creator>Deleage, G.</dc:creator>
    <dc:creator>Diarena, M.</dc:creator>
    <dc:creator>Fabbretti, R.</dc:creator>
    <dc:creator>Fettahi, G.</dc:creator>
    <dc:creator>Flegel, V.</dc:creator>
    <dc:creator>Gisel, A.</dc:creator>
    <dc:creator>Kasam, V.</dc:creator>
    <dc:creator>Kervinen, T.</dc:creator>
    <dc:creator>Korpelainen, E.</dc:creator>
    <dc:creator>Mattila, K.</dc:creator>
    <dc:creator>Pagni, M.</dc:creator>
    <dc:creator>Reichstadt, M.</dc:creator>
    <dc:creator>Breton, V.</dc:creator>
    <dc:creator>Tickle, I.J.</dc:creator>
    <dc:creator>Vriend, G.</dc:creator>
    <dc:date>2009-06-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889809008784</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The majority of previously deposited X-ray structures can be improved by applying current refinement methods.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY CRYSTALLOGRAPHY; REFINEMENT; STRUCTURE VALIDATION; PROTEIN DATA BANK; GRID COMPUTING</dc:subject>
    <dc:description>Structural biology, homology modelling and rational drug design require accurate three-dimensional macromolecular coordinates. However, the coordinates in the Protein Data Bank (PDB) have not all been obtained using the latest experimental and computational methods. In this study a method is presented for automated re-refinement of existing structure models in the PDB. A large-scale benchmark with 16 807 PDB entries showed that they can be improved in terms of fit to the deposited experimental X-ray data as well as in terms of geometric quality. The re-refinement protocol uses TLS models to describe concerted atom movement. The resulting structure models are made available through the PDB_REDO databank (http://www.cmbi.ru.nl/pdb_redo/). Grid computing techniques were used to overcome the computational requirements of this endeavour.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>PDB_REDO: automated re-refinement of X-ray structure models in the PDB</dc:title>
    <dc:type>text</dc:type>
    <prism:number>3</prism:number>
    <prism:volume>42</prism:volume>
    <prism:publicationDate>2009-06-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
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    <prism:section>research papers</prism:section>
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  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kk5041">
    <title>Lecture demonstrations in a public lecture on `X-ray crystal structure analysis: from W. L. Bragg to the present day'</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kk5041</link>
    <dc:rights>Copyright (c) 2009 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:date>2009-04-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889809002775</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:language>en</dc:language>
    <dc:subject>LECTURE DEMONSTRATIONS; CRYSTALLOGRAPHIC TEACHING</dc:subject>
    <dc:format>text/html</dc:format>
    <dc:title>Lecture demonstrations in a public lecture on `X-ray crystal structure analysis: from W. L. Bragg to the present day'</dc:title>
    <dc:type>text</dc:type>
    <prism:number>2</prism:number>
    <prism:volume>42</prism:volume>
    <prism:publicationDate>2009-04-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2009 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>notes and news</prism:section>
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    <prism:endingPage>365</prism:endingPage>
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  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kk5034">
    <title>Constraints and restraints in crystal structure analysis</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kk5034</link>
    <description>The widely used restraint-based approach to structural analysis using diffraction data is critiqued. The convenience of using rigid constraints, through the use of internal coordinates, is discussed.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Immirzi, A.</dc:creator>
    <dc:date>2009-04-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808044142</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The restraint-based procedure in least-squares refinement is critiqued and the advantages of using internal coordinates are discussed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CONSTRAINTS; RESTRAINTS; CRYSTAL STRUCTURE ANALYSIS</dc:subject>
    <dc:description>The widely used restraint-based approach to structural analysis using diffraction data is critiqued. The convenience of using rigid constraints, through the use of internal coordinates, is discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Constraints and restraints in crystal structure analysis</dc:title>
    <dc:type>text</dc:type>
    <prism:number>2</prism:number>
    <prism:volume>42</prism:volume>
    <prism:publicationDate>2009-04-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>letters to the editor</prism:section>
    <prism:startingPage>362</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>364</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?dd5042">
    <title>Synthesis and physical properties of ferrocene derivatives. XXI. Crystal structure of a liquid crystalline ferrocene derivative, 1,1'-bis[3-[4-(4-methoxyphenoxycarbonyl)phenoxy]propyloxycarbonyl]ferrocene</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?dd5042</link>
    <description>The crystal structure of the title 1,1′-disubstituted ferrocene derivative was determined by X-ray diffraction using a single crystal. This compound exhibits a nematic phase only. The X-ray structure analysis revealed that the two substituents lie in the same direction (`U' shape) and the flexible spacer adopts a gauche conformation. These conformations are strongly related to the formation of a rod-like shape, which favors liquid crystalline behavior. In the crystal structure, C—H⋯π, π–π and T-stacking interactions were observed. It is considered that these interactions play a major role in stabilizing the molecular packing arrangement and the mesomorphism.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Okabe, T.</dc:creator>
    <dc:creator>Nakazaki, K.</dc:creator>
    <dc:creator>Igaue, T.</dc:creator>
    <dc:creator>Nakamura, N.</dc:creator>
    <dc:creator>Donnio, B.</dc:creator>
    <dc:creator>Guillon, D.</dc:creator>
    <dc:creator>Gallani, J.-L.</dc:creator>
    <dc:date>2009-02-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808042039</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The title 1,1′-disubstituted ferrocene derivative exhibits a nematic phase only, and the rod-like shape of the molecule favors liquid crystalline behavior. C—H⋯π, π–π and T-stacking interactions play a major role in stabilizing the molecular packing arrangement and the mesomorphism.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FERROCENE; LIQUID CRYSTALS; 1,1'-DISUBSTITUTED FERROCENE DERIVATIVES</dc:subject>
    <dc:description>The crystal structure of the title 1,1′-disubstituted ferrocene derivative was determined by X-ray diffraction using a single crystal. This compound exhibits a nematic phase only. The X-ray structure analysis revealed that the two substituents lie in the same direction (`U' shape) and the flexible spacer adopts a gauche conformation. These conformations are strongly related to the formation of a rod-like shape, which favors liquid crystalline behavior. In the crystal structure, C—H⋯π, π–π and T-stacking interactions were observed. It is considered that these interactions play a major role in stabilizing the molecular packing arrangement and the mesomorphism.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Synthesis and physical properties of ferrocene derivatives. XXI. Crystal structure of a liquid crystalline ferrocene derivative, 1,1'-bis[3-[4-(4-methoxyphenoxycarbonyl)phenoxy]propyloxycarbonyl]ferrocene</dc:title>
    <dc:type>text</dc:type>
    <prism:number>1</prism:number>
    <prism:volume>42</prism:volume>
    <prism:publicationDate>2009-02-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>63</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>68</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?hx5080">
    <title>Odd electron diffraction patterns in silicon nanowires and silicon thin films explained by microtwins and nanotwins</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?hx5080</link>
    <description>Odd electron diffraction patterns (EDPs) have been obtained by transmission electron microscopy (TEM) on silicon nanowires grown via the vapour–liquid–solid method and on silicon thin films deposited by electron beam evaporation. Many explanations have been given in the past, without consensus among the scientific community: size artifacts, twinning artifacts or, more widely accepted, the existence of new hexagonal Si phases. In order to resolve this issue, the microstructures of Si nanowires and Si thin films have been characterized by TEM, high-resolution transmission electron microscopy (HRTEM) and high-resolution scanning transmission electron microscopy. Despite the differences in the geometries and elaboration processes, the EDPs of the materials show great similarities. The different hypotheses reported in the literature have been investigated. It was found that the positions of the diffraction spots in the EDPs could be reproduced by simulating a hexagonal structure with c/a = 12(2/3)1/2, but the intensities in many EDPs remained unexplained. Finally, it was established that all the experimental data, i.e. EDPs and HRTEM images, agree with a classical cubic silicon structure containing two microstructural defects: (i) overlapping Σ3 microtwins which induce extra spots by double diffraction, and (ii) nanotwins which induce extra spots as a result of streaking effects. It is concluded that there is no hexagonal phase in the Si nanowires and the Si thin films presented in this work.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Cayron, C.</dc:creator>
    <dc:creator>Den Hertog, M.</dc:creator>
    <dc:creator>Latu-Romain, L.</dc:creator>
    <dc:creator>Mouchet, C.</dc:creator>
    <dc:creator>Secouard, C.</dc:creator>
    <dc:creator>Rouviere, J.-L.</dc:creator>
    <dc:creator>Rouviere, E.</dc:creator>
    <dc:creator>Simonato, J.-P.</dc:creator>
    <dc:date>2009-04-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808042131</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Anomalous extra spots visible in electron diffraction patterns of silicon nanowires and silicon thin films are explained by the presence of micro- and nanotwins.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SILICON NANOWIRES; SILICON THIN FILMS; ARTIFACTS; TWINNING</dc:subject>
    <dc:description>Odd electron diffraction patterns (EDPs) have been obtained by transmission electron microscopy (TEM) on silicon nanowires grown via the vapour–liquid–solid method and on silicon thin films deposited by electron beam evaporation. Many explanations have been given in the past, without consensus among the scientific community: size artifacts, twinning artifacts or, more widely accepted, the existence of new hexagonal Si phases. In order to resolve this issue, the microstructures of Si nanowires and Si thin films have been characterized by TEM, high-resolution transmission electron microscopy (HRTEM) and high-resolution scanning transmission electron microscopy. Despite the differences in the geometries and elaboration processes, the EDPs of the materials show great similarities. The different hypotheses reported in the literature have been investigated. It was found that the positions of the diffraction spots in the EDPs could be reproduced by simulating a hexagonal structure with c/a = 12(2/3)1/2, but the intensities in many EDPs remained unexplained. Finally, it was established that all the experimental data, i.e. EDPs and HRTEM images, agree with a classical cubic silicon structure containing two microstructural defects: (i) overlapping Σ3 microtwins which induce extra spots by double diffraction, and (ii) nanotwins which induce extra spots as a result of streaking effects. It is concluded that there is no hexagonal phase in the Si nanowires and the Si thin films presented in this work.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Odd electron diffraction patterns in silicon nanowires and silicon thin films explained by microtwins and nanotwins</dc:title>
    <dc:type>text</dc:type>
    <prism:number>2</prism:number>
    <prism:volume>42</prism:volume>
    <prism:publicationDate>2009-04-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>242</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>252</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?db5049">
    <title>Combining precession electron diffraction data with X-ray powder diffraction data to facilitate structure solution</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?db5049</link>
    <description>Information derived from precession electron diffraction (PED) patterns can be used to advantage in combination with high-resolution X-ray powder diffraction data to solve crystal structures that resist solution from X-ray data alone. PED data have been exploited in two different ways for this purpose: (1) to identify weak reflections and (2) to estimate the phases of the reflections in the projection. The former is used to improve the partitioning of the reflection intensities within an overlap group and the latter to provide some starting phases for structure determination. The information was incorporated into a powder charge-flipping algorithm for structure solution. The approaches were first developed using data for the moderately complex zeolite ZSM-5, and then tested on TNU-9, one of the two most complex zeolites known. In both cases, including PED data from just a few projections facilitated structure solution significantly.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Xie, D.</dc:creator>
    <dc:creator>Baerlocher, C.</dc:creator>
    <dc:creator>McCusker, L.B.</dc:creator>
    <dc:date>2008-12-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808034377</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>By supplementing high-resolution X-ray powder diffraction data with information derived from precession electron diffraction data, increasingly complex structures of polycrystalline materials can be solved.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CHARGE-FLIPPING ALGORITHMS; PRECESSION ELECTRON DIFFRACTION; STRUCTURE DETERMINATION; X-RAY POWDER DIFFRACTION; ZEOLITES</dc:subject>
    <dc:description>Information derived from precession electron diffraction (PED) patterns can be used to advantage in combination with high-resolution X-ray powder diffraction data to solve crystal structures that resist solution from X-ray data alone. PED data have been exploited in two different ways for this purpose: (1) to identify weak reflections and (2) to estimate the phases of the reflections in the projection. The former is used to improve the partitioning of the reflection intensities within an overlap group and the latter to provide some starting phases for structure determination. The information was incorporated into a powder charge-flipping algorithm for structure solution. The approaches were first developed using data for the moderately complex zeolite ZSM-5, and then tested on TNU-9, one of the two most complex zeolites known. In both cases, including PED data from just a few projections facilitated structure solution significantly.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Combining precession electron diffraction data with X-ray powder diffraction data to facilitate structure solution</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-12-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>1115</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1121</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kk5029">
    <title>A tutorial for learning and teaching macromol­ecular crystallography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kk5029</link>
    <description>Five experiments have been designed to be used for teaching macromolecular crystallography. The three proteins used in this tutorial are all commercially available; they can be easily and reproducibly crystallized and mounted for diffraction data collection. For each of the five experiments the raw images and the processed data of a sample diffraction data set as well as the refined coordinates and phases are provided for teaching the steps of data processing and structure determination.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Faust, A.</dc:creator>
    <dc:creator>Panjikar, S.</dc:creator>
    <dc:creator>Mueller, U.</dc:creator>
    <dc:creator>Parthasarathy, V.</dc:creator>
    <dc:creator>Schmidt, A.</dc:creator>
    <dc:creator>Lamzin, V.S.</dc:creator>
    <dc:creator>Weiss, M.S.</dc:creator>
    <dc:date>2008-12-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808032494</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A tutorial consisting of five macromolecular crystallography experiments has been assembled for teaching purposes. The described work comprises the crystallization of the proteins, diffraction data collection, data processing and automated structure determination.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MACROMOLECULAR CRYSTALLOGRAPHY; PROTEIN CRYSTALLIZATION; DIFFRACTION DATA COLLECTION; DATA PROCESSING; AUTOMATED STRUCTURE DETERMINATION</dc:subject>
    <dc:description>Five experiments have been designed to be used for teaching macromolecular crystallography. The three proteins used in this tutorial are all commercially available; they can be easily and reproducibly crystallized and mounted for diffraction data collection. For each of the five experiments the raw images and the processed data of a sample diffraction data set as well as the refined coordinates and phases are provided for teaching the steps of data processing and structure determination.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A tutorial for learning and teaching macromol­ecular crystallography</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-12-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>teaching and education</prism:section>
    <prism:startingPage>1161</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1172</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj5108">
    <title>Microstrain and grain-size analysis from diffraction peak width and graphical derivation of high-pressure thermomechanics</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj5108</link>
    <description>An analytical method is presented for deriving the thermomechanical properties of polycrystalline materials under high-pressure (P) and high-temperature (T) conditions. This method deals with non-uniform stress among heterogeneous crystal grains and surface strain in nanocrystalline materials by examining peak-width variation under different P–T conditions. Because the method deals directly with lattice d spacing and local deformation caused by stress, it can be applied to process any diffraction profile, independent of detection mode. In addition, a correction routine is developed using diffraction elastic ratios to deal with severe surface strain and/or strain anisotropy effects related to nano-scale grain sizes, so that significant data scatter can be reduced in a physically meaningful way. Graphical illustration of the resultant microstrain analysis can identify micro/local yields at the grain-to-grain interactions resulting from high stress concentration, and macro/bulk yield of the plastic deformation over the entire sample. This simple and straightforward approach is capable of revealing the corresponding micro and/or macro yield stresses, grain crushing or growth, work hardening or softening, and thermal relaxation under high-P–T conditions, as well as the intrinsic residual strain and/or surface strain in the polycrystalline bulk. In addition, this approach allows the instrumental contribution to be illustrated and subtracted in a straightforward manner, thus avoiding the potential complexities and errors resulting from instrument correction. Applications of the method are demonstrated by studies of α-SiC (6H, moissanite) and of micro- and nanocrystalline nickel by synchrotron X-ray and time-of-flight neutron diffraction.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Zhao, Y.</dc:creator>
    <dc:creator>Zhang, J.</dc:creator>
    <dc:date>2008-12-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808031762</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>By analyzing diffraction peak profiles at different P–T loading stages, the thermomechanical properties of materials can be derived, with graphical delineations of micro/macro yields, plastic flow, energy dissipation, work hardening/softening, grain crushing/growth, stress relaxation and residual strain, as well as instrument baselines for all diffraction modes.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MICROSTRAIN ANALYSIS; GRAIN-SIZE ANALYSIS; PEAK-WIDTH VARIATION; HIGH PRESSURE AND TEMPERATURE</dc:subject>
    <dc:description>An analytical method is presented for deriving the thermomechanical properties of polycrystalline materials under high-pressure (P) and high-temperature (T) conditions. This method deals with non-uniform stress among heterogeneous crystal grains and surface strain in nanocrystalline materials by examining peak-width variation under different P–T conditions. Because the method deals directly with lattice d spacing and local deformation caused by stress, it can be applied to process any diffraction profile, independent of detection mode. In addition, a correction routine is developed using diffraction elastic ratios to deal with severe surface strain and/or strain anisotropy effects related to nano-scale grain sizes, so that significant data scatter can be reduced in a physically meaningful way. Graphical illustration of the resultant microstrain analysis can identify micro/local yields at the grain-to-grain interactions resulting from high stress concentration, and macro/bulk yield of the plastic deformation over the entire sample. This simple and straightforward approach is capable of revealing the corresponding micro and/or macro yield stresses, grain crushing or growth, work hardening or softening, and thermal relaxation under high-P–T conditions, as well as the intrinsic residual strain and/or surface strain in the polycrystalline bulk. In addition, this approach allows the instrumental contribution to be illustrated and subtracted in a straightforward manner, thus avoiding the potential complexities and errors resulting from instrument correction. Applications of the method are demonstrated by studies of α-SiC (6H, moissanite) and of micro- and nanocrystalline nickel by synchrotron X-ray and time-of-flight neutron diffraction.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Microstrain and grain-size analysis from diffraction peak width and graphical derivation of high-pressure thermomechanics</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-12-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>1095</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1108</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?do5035">
    <title>X-ray tomographic reconstruction of macro­molecular samples</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?do5035</link>
    <description>The anomalous scattering properties of innate sulfur for proteins and phosphorus for DNA and RNA can be used to solve the phase problem in macromolecular crystallography (MX) via the single-wavelength anomalous dispersion method (SAD). However, this method, which is carried out at longer X-ray wavelengths (1.5–2.5 Å), is still not a routine tool in MX. The increased absorption from both air and sample associated with the use of longer X-ray wavelengths presents a key difficulty. The absorption can be corrected for through empirical algorithms, provided truly redundant data are available. Unfortunately, weakly diffracting macromolecular crystals suffer from radiation damage, resulting in a dose-dependent non-isomorphism which violates the assumption upon which these empirical algorithms are based. In this report, X-ray microtomography is used to reconstruct the three-dimensional shapes of vitrified macromolecular crystals including the surrounding solvent and sample holder. The setup can be integrated within an MX beamline environment and exploits both absorption and phase contrast. The dose needed for the tomographic measurements could be low enough to allow the technique to be used for crystal integrity characterization and alignment. X-ray tomography has some major benefits compared with the optical-light-based crystal alignment protocols currently used.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Brockhauser, S.</dc:creator>
    <dc:creator>Di Michiel, M.</dc:creator>
    <dc:creator>McGeehan, J.E.</dc:creator>
    <dc:creator>McCarthy, A.A.</dc:creator>
    <dc:creator>Ravelli, R.B.G.</dc:creator>
    <dc:date>2008-12-01</dc:date>
    <dc:identifier>doi:10.1107/S002188980802935X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>High-resolution X-ray tomography is used to reconstruct three-dimensional volumes of vitrified macromolecular crystals.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY TOMOGRAPHY; ABSORPTION CORRECTION; CRYSTAL ALIGNMENT; SYNCHROTRON RADIATION; MACROMOLECULAR CRYSTALLOGRAPHY</dc:subject>
    <dc:description>The anomalous scattering properties of innate sulfur for proteins and phosphorus for DNA and RNA can be used to solve the phase problem in macromolecular crystallography (MX) via the single-wavelength anomalous dispersion method (SAD). However, this method, which is carried out at longer X-ray wavelengths (1.5–2.5 Å), is still not a routine tool in MX. The increased absorption from both air and sample associated with the use of longer X-ray wavelengths presents a key difficulty. The absorption can be corrected for through empirical algorithms, provided truly redundant data are available. Unfortunately, weakly diffracting macromolecular crystals suffer from radiation damage, resulting in a dose-dependent non-isomorphism which violates the assumption upon which these empirical algorithms are based. In this report, X-ray microtomography is used to reconstruct the three-dimensional shapes of vitrified macromolecular crystals including the surrounding solvent and sample holder. The setup can be integrated within an MX beamline environment and exploits both absorption and phase contrast. The dose needed for the tomographic measurements could be low enough to allow the technique to be used for crystal integrity characterization and alignment. X-ray tomography has some major benefits compared with the optical-light-based crystal alignment protocols currently used.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray tomographic reconstruction of macro­molecular samples</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-12-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>1057</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1066</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?he5412">
    <title>Control of the rate of evaporation in protein crystallization by the `microbatch under oil' method</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?he5412</link>
    <description>Microbatch crystallization under oil is a powerful procedure for obtaining protein crystals. Using this method, aqueous protein solutions are dispensed under liquid oil, and water evaporates through the layer of oil, with a concomitant increase in the concentrations of both protein and precipitant until the nucleation point is reached. A technique is presented for regulating the rate of water evaporation, which permits fine tuning of the crystallization conditions as well as preventing complete desiccation of the drops in the microbatch crystallization trays.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Brumshtein, B.</dc:creator>
    <dc:creator>Greenblatt, H.M.</dc:creator>
    <dc:creator>Futerman, A.H.</dc:creator>
    <dc:creator>Silman, I.</dc:creator>
    <dc:creator>Sussman, J.L.</dc:creator>
    <dc:date>2008-10-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808024667</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A procedure is presented for controlling the rate of evaporation during `microbatch under oil' protein crystallization.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MICROBATCH; CRYSTALLIZATION UNDER OIL; PROTEIN CRYSTALLOGRAPHY; EVAPORATION</dc:subject>
    <dc:description>Microbatch crystallization under oil is a powerful procedure for obtaining protein crystals. Using this method, aqueous protein solutions are dispensed under liquid oil, and water evaporates through the layer of oil, with a concomitant increase in the concentrations of both protein and precipitant until the nucleation point is reached. A technique is presented for regulating the rate of water evaporation, which permits fine tuning of the crystallization conditions as well as preventing complete desiccation of the drops in the microbatch crystallization trays.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Control of the rate of evaporation in protein crystallization by the `microbatch under oil' method</dc:title>
    <dc:type>text</dc:type>
    <prism:number>5</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-10-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>laboratory notes</prism:section>
    <prism:startingPage>969</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>971</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ko5062">
    <title>Study of the effect of nano-sized precipitates on the mechanical properties of boron-added low-carbon steels by neutron scattering techniques</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ko5062</link>
    <description>Small-angle neutron scattering (SANS) and neutron powder diffraction (ND) techniques were used to study quantitatively the effect of nano-sized precipitates and boron addition on the mechanical properties of low-carbon steels. SANS was used to evaluate nano-sized precipitates, smaller than about 600 Å in diameter, and ND was used to determine the weight fraction of the cementite precipitates. Fine core–shell structured spherical precipitates with an average radius of ~50 Å, such as MnS and/or CuS, surrounded by BN layers were observed in the boron-added (BA) low-carbon steels; fine spherical precipitates with an average radius of ~48 Å were mainly observed in the boron-free (BF) low-carbon steels. In the BA steels, the number of boron precipitates, such as BN, Fe3(C,B) and MnS, surrounded by BN layers increased drastically at higher hot-rolling temperatures. The volume fraction of the fine precipitates of the BA steels was higher than that of the BF steels; this difference is related to the rapid growth of the BN layers on the MnS and CuS precipitates. Boron addition to low-carbon steels resulted in a reduction in strength and an improvement in elongation; this behaviour is related to the reduction of the solute carbon and the nitrogen contents in the ferrite matrix caused by the precipitation of BN, as well by the increase in the volume fraction of the cementites.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Seong, B.S.</dc:creator>
    <dc:creator>Cho, Y.R.</dc:creator>
    <dc:creator>Shin, E.J.</dc:creator>
    <dc:creator>Kim, S.I.</dc:creator>
    <dc:creator>Choi, S.-H.</dc:creator>
    <dc:creator>Kim, H.R.</dc:creator>
    <dc:creator>Kim, Y.J.</dc:creator>
    <dc:date>2008-10-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808020943</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The effect of nano-sized precipitates on the mechanical properties of boron-added low-carbon steels was studied by neutron scattering techniques such as powder diffraction, small-angle scattering and particle tracking autography.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>NEUTRON DIFFRACTION; SMALL-ANGLE NEUTRON SCATTERING (SANS); BORON-ADDED LOW-CARBON STEEL; ELONGATION; CEMENTITE; PRECIPITATES; PARTICLE TRACKING AUTORADIOGRAPHY</dc:subject>
    <dc:description>Small-angle neutron scattering (SANS) and neutron powder diffraction (ND) techniques were used to study quantitatively the effect of nano-sized precipitates and boron addition on the mechanical properties of low-carbon steels. SANS was used to evaluate nano-sized precipitates, smaller than about 600 Å in diameter, and ND was used to determine the weight fraction of the cementite precipitates. Fine core–shell structured spherical precipitates with an average radius of ~50 Å, such as MnS and/or CuS, surrounded by BN layers were observed in the boron-added (BA) low-carbon steels; fine spherical precipitates with an average radius of ~48 Å were mainly observed in the boron-free (BF) low-carbon steels. In the BA steels, the number of boron precipitates, such as BN, Fe3(C,B) and MnS, surrounded by BN layers increased drastically at higher hot-rolling temperatures. The volume fraction of the fine precipitates of the BA steels was higher than that of the BF steels; this difference is related to the rapid growth of the BN layers on the MnS and CuS precipitates. Boron addition to low-carbon steels resulted in a reduction in strength and an improvement in elongation; this behaviour is related to the reduction of the solute carbon and the nitrogen contents in the ferrite matrix caused by the precipitation of BN, as well by the increase in the volume fraction of the cementites.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Study of the effect of nano-sized precipitates on the mechanical properties of boron-added low-carbon steels by neutron scattering techniques</dc:title>
    <dc:type>text</dc:type>
    <prism:number>5</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-10-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>906</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>912</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kk5026">
    <title>Finding crystal structures from few diffraction data by a combination of a random search with genetic algorithms</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kk5026</link>
    <description>A new procedure for performing structural analysis of crystalline materials from diffraction data, using internal coordinates, is described. For starting information only unit-cell content, space group, chemical formula, molecular connectivity and a limited amount of diffraction data are required. After first selecting a number of solutions using a Monte Carlo approach with severe filters, which reject the most unrealistic solutions, genetic algorithms (crossover and mutations) are applied. In fact, the initial selection step alone is, frequently, a powerful tool for discovering structures, without recourse to the genetic algorithms. The procedure, while suffering from the limitation that connectivity must be known, is effective in cases where direct methods are not applicable because the diffraction data are scarce, are limited to low diffraction angles or are missing in specific portions of the reciprocal space. The main features of the algorithm are described and examples of validation given. The routines are now available as part of the freely distributed general-purpose program TRY. The program is available on the Web at http://www.theochem.unisa.it/try.html.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Immirzi, A.</dc:creator>
    <dc:creator>Erra, L.</dc:creator>
    <dc:creator>Tedesco, C.</dc:creator>
    <dc:date>2008-08-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808020074</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A new procedure for performing structural analysis of crystalline materials from diffraction data by random search and genetic algorithms is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>STRUCTURAL ANALYSIS; SPARSE DIFFRACTION DATA; RANDOM SEARCH ALGORITHMS; GENETIC ALGORITHMS; COMPUTER PROGRAMS; TRY</dc:subject>
    <dc:description>A new procedure for performing structural analysis of crystalline materials from diffraction data, using internal coordinates, is described. For starting information only unit-cell content, space group, chemical formula, molecular connectivity and a limited amount of diffraction data are required. After first selecting a number of solutions using a Monte Carlo approach with severe filters, which reject the most unrealistic solutions, genetic algorithms (crossover and mutations) are applied. In fact, the initial selection step alone is, frequently, a powerful tool for discovering structures, without recourse to the genetic algorithms. The procedure, while suffering from the limitation that connectivity must be known, is effective in cases where direct methods are not applicable because the diffraction data are scarce, are limited to low diffraction angles or are missing in specific portions of the reciprocal space. The main features of the algorithm are described and examples of validation given. The routines are now available as part of the freely distributed general-purpose program TRY. The program is available on the Web at http://www.theochem.unisa.it/try.html.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Finding crystal structures from few diffraction data by a combination of a random search with genetic algorithms</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>784</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>790</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks5182">
    <title>Point-focusing monochromator crystal realized by hot plastic deformation of a Ge wafer</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks5182</link>
    <description>Pre-polished Ge(111) single-crystal wafers were deformed just below the melting temperature to prepare point-focusing Johansson monochromator crystals. The (111) lattice plane had curvature 2R in the focusing plane and R perpendicular to it, with a hemispherical inner surface with a radius of R = 600 mm. By using Cu Kα radiation, the diverging X-ray beam was focused onto a small spot.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Okuda, H.</dc:creator>
    <dc:creator>Nakajima, K.</dc:creator>
    <dc:creator>Fujiwara, K.</dc:creator>
    <dc:creator>Morishita, K.</dc:creator>
    <dc:creator>Ochiai, S.</dc:creator>
    <dc:date>2008-08-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808016282</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A point-focusing Johansson monochromator crystal prepared by hot-pressing a Ge single-crystal wafer is demonstrated. By using 333 diffraction, Cu Kα radiation was focused onto a small spot.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>JOHANSSON MONOCHROMATOR; GE; HOT PLASTIC DEFORMATION</dc:subject>
    <dc:description>Pre-polished Ge(111) single-crystal wafers were deformed just below the melting temperature to prepare point-focusing Johansson monochromator crystals. The (111) lattice plane had curvature 2R in the focusing plane and R perpendicular to it, with a hemispherical inner surface with a radius of R = 600 mm. By using Cu Kα radiation, the diverging X-ray beam was focused onto a small spot.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Point-focusing monochromator crystal realized by hot plastic deformation of a Ge wafer</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>798</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>799</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pf0067">
    <title>X-ray diffraction by polycrystalline materials. By René Guine­bretière. Pp. 351. London: ISTE, 2007. Price (hardcover) EUR 124.83. ISBN 978-1905209217.</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pf0067</link>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Chateigner, D.</dc:creator>
    <dc:date>2008-08-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808015987</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>X-ray diffraction by polycrystalline materials. By René Guine­bretière. Pp. 351. London: ISTE, 2007. Price (hardcover) EUR 124.83. ISBN 978-1905209217.</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>book reviews</prism:section>
    <prism:startingPage>826</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>827</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ce5042">
    <title>A toolkit for publishing enhanced figures</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ce5042</link>
    <description>An editing toolkit has been developed to allow authors to create enhanced interactive figures for publication in crystallography journals. The visualization engine is Jmol, a Java program that can be manipulated as an applet in a web browser. The toolkit provides user-friendly widgets to manipulate the graphics state of Jmol, and persistent storage of graphics state, scripts and associated data files.</description>
    <dc:rights>http://creativecommons.org/licenses/by/2.0/uk</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>McMahon, B.</dc:creator>
    <dc:creator>Hanson, R.M.</dc:creator>
    <dc:date>2008-08-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808015616</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A description is provided of a software utility for creating interactive figures derived from crystal structures using the Java program Jmol.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COMPUTER PROGRAMS; INTERACTIVE GRAPHICS; MOLECULAR VISUALIZATION</dc:subject>
    <dc:description>An editing toolkit has been developed to allow authors to create enhanced interactive figures for publication in crystallography journals. The visualization engine is Jmol, a Java program that can be manipulated as an applet in a web browser. The toolkit provides user-friendly widgets to manipulate the graphics state of Jmol, and persistent storage of graphics state, scripts and associated data files.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A toolkit for publishing enhanced figures</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>computer programs</prism:section>
    <prism:startingPage>811</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>814</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?he5407">
    <title>VCIF2: extended CIF validation software</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?he5407</link>
    <description>Recent revisions to the CIF standard, the growing number of dictionaries and the critical role played by CIF in the IUCr publication process led the IUCr to fund a two-year project to upgrade portions of the existing CIF software base to support longer lines and more rigorous validation of CIFs against multiple layered dictionaries. A database-based approach to validation to ensure compliance with data-range and enumeration specifications, to ensure compliance with parent–child relationships, and to detect missing and duplicated tags is presented here. This approach to validation is being extended to support the handling of binary synchrotron imgCIF data.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Todorov, G.</dc:creator>
    <dc:creator>Bernstein, H.J.</dc:creator>
    <dc:date>2008-08-01</dc:date>
    <dc:identifier>doi:10.1107/S002188980801385X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A database-based approach to validation of CIFs to ensure compliance with data-range and enumeration specifications, to ensure compliance with parent–child relationships, and to detect missing and duplicated tags is presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CIF VALIDATION; BINARY IMGCIF DATA; COMPLIANCE</dc:subject>
    <dc:description>Recent revisions to the CIF standard, the growing number of dictionaries and the critical role played by CIF in the IUCr publication process led the IUCr to fund a two-year project to upgrade portions of the existing CIF software base to support longer lines and more rigorous validation of CIFs against multiple layered dictionaries. A database-based approach to validation to ensure compliance with data-range and enumeration specifications, to ensure compliance with parent–child relationships, and to detect missing and duplicated tags is presented here. This approach to validation is being extended to support the handling of binary synchrotron imgCIF data.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>VCIF2: extended CIF validation software</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>CIF applications</prism:section>
    <prism:startingPage>808</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>810</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?py5004">
    <title>Of crystals, structure factors and diffraction images</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?py5004</link>
    <description>It is suggested that it would be useful if raw X-ray diffraction images could be included in data depositions with the Protein Data Bank.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Jovine, L.</dc:creator>
    <dc:creator>Morgunova, E.</dc:creator>
    <dc:creator>Ladenstein, R.</dc:creator>
    <dc:date>2008-06-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889808008832</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>It is suggested that it would be useful if raw X-ray diffraction images could be included in data depositions with the Protein Data Bank.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DATA DEPOSITION; PROTEIN DATA BANK (PDB)</dc:subject>
    <dc:description>It is suggested that it would be useful if raw X-ray diffraction images could be included in data depositions with the Protein Data Bank.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Of crystals, structure factors and diffraction images</dc:title>
    <dc:type>text</dc:type>
    <prism:number>3</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-06-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>letters to the editor</prism:section>
    <prism:startingPage>659</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>659</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks5161">
    <title>Determination of absolute structure using Bayesian statistics on Bijvoet differences</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks5161</link>
    <description>A new probabilistic approach is introduced for the determination of the absolute structure of a compound which is known to be enantiopure based on Bijvoet-pair intensity differences. The new method provides relative probabilities for different models of the chiral composition of the structure. The outcome of this type of analysis can also be cast in the form of a new value, along with associated standard uncertainty, that resembles the value of the well known Flack x parameter. The standard uncertainty we obtain is often about half of the standard uncertainty in the value of the Flack x parameter. The proposed formalism is suited in particular to absolute configuration determination from diffraction data of biologically active (pharmaceutical) compounds where the strongest resonant scattering signal often comes from oxygen. It is shown that a reliable absolute configuration assignment in such cases can be made on the basis of Cu Kα data, and in some cases even with carefully measured Mo Kα data.</description>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Hooft, R.W.W.</dc:creator>
    <dc:creator>Straver, L.H.</dc:creator>
    <dc:creator>Spek, A.L.</dc:creator>
    <dc:date>2008-02-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807059870</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A description is given of a maximum-likelihood approach to absolute structure determinations of biologically active molecules.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ABSOLUTE STRUCTURE; FLACK X PARAMETER; BAYESIAN STATISTICS; RESONANT SCATTERING</dc:subject>
    <dc:description>A new probabilistic approach is introduced for the determination of the absolute structure of a compound which is known to be enantiopure based on Bijvoet-pair intensity differences. The new method provides relative probabilities for different models of the chiral composition of the structure. The outcome of this type of analysis can also be cast in the form of a new value, along with associated standard uncertainty, that resembles the value of the well known Flack x parameter. The standard uncertainty we obtain is often about half of the standard uncertainty in the value of the Flack x parameter. The proposed formalism is suited in particular to absolute configuration determination from diffraction data of biologically active (pharmaceutical) compounds where the strongest resonant scattering signal often comes from oxygen. It is shown that a reliable absolute configuration assignment in such cases can be made on the basis of Cu Kα data, and in some cases even with carefully measured Mo Kα data.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Determination of absolute structure using Bayesian statistics on Bijvoet differences</dc:title>
    <dc:type>text</dc:type>
    <prism:number>1</prism:number>
    <prism:volume>41</prism:volume>
    <prism:publicationDate>2008-02-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>96</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>103</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cg5071">
    <title>GenOVa: a computer program to generate orientational variants</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cg5071</link>
    <description>A computer program called GenOVa, written in Python, calculates the orientational variants, the operators (special types of misorientations between variants) and the composition table associated with a groupoid structure. The variants can be represented by three-dimensional shapes or by pole figures.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Cayron, C.</dc:creator>
    <dc:date>2007-12-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807048741</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>This computer program calculates the orientational variants, the operators and the composition table of a groupoid.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>VARIANTS; ORIENTATION; GROUPOIDS; POLE FIGURES; SIMULATIONS; COMPUTER PROGRAMS; GENOVA</dc:subject>
    <dc:description>A computer program called GenOVa, written in Python, calculates the orientational variants, the operators (special types of misorientations between variants) and the composition table associated with a groupoid structure. The variants can be represented by three-dimensional shapes or by pole figures.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>GenOVa: a computer program to generate orientational variants</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-12-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>computer programs</prism:section>
    <prism:startingPage>1179</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1182</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cg5072">
    <title>ARPGE: a computer program to automatically reconstruct the parent grains from electron backscatter diffraction data</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cg5072</link>
    <description>A computer program called ARPGE written in Python uses the theoretical results generated by the computer program GenOVa to automatically reconstruct the parent grains from electron backscatter diffraction data obtained on phase transition materials with or without residual parent phase. The misorientations between daughter grains are identified with operators, the daughter grains are identified with indexed variants, the orientations of the parent grains are determined, and some statistics on the variants and operators are established. Some examples with martensitic transformations in iron and titanium alloys were treated. Variant selection phenomena were revealed.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Cayron, C.</dc:creator>
    <dc:date>2007-12-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807048777</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A computer program has been written to reconstruct the parent grains from EBSD data of phase transition materials.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ELECTRON BACKSCATTER DIFFRACTION (EBSD); RECONSTRUCTION; PHASE TRANSFORMATION; TITANIUM; STEEL; GROUPOIDS; COMPUTER PROGRAMS; ARPGE; GENOVA</dc:subject>
    <dc:description>A computer program called ARPGE written in Python uses the theoretical results generated by the computer program GenOVa to automatically reconstruct the parent grains from electron backscatter diffraction data obtained on phase transition materials with or without residual parent phase. The misorientations between daughter grains are identified with operators, the daughter grains are identified with indexed variants, the orientations of the parent grains are determined, and some statistics on the variants and operators are established. Some examples with martensitic transformations in iron and titanium alloys were treated. Variant selection phenomena were revealed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>ARPGE: a computer program to automatically reconstruct the parent grains from electron backscatter diffraction data</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-12-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>computer programs</prism:section>
    <prism:startingPage>1183</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1188</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kk5014">
    <title>Illustrated Fourier transforms for crystallography</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kk5014</link>
    <description>Concepts such as Fourier transformation, convolution and resolution that are required to understand crystallography are illustrated through visual examples. These concepts can be explained pedagogically in a very direct way using the DigitalMicrograph software from Gatan Inc. (http://www.gatan.com/imaging/downloads.php), originally intended for electron microscopy data collection and analysis, and practical exercises developed around this tool can be used in teaching crystallography.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Aubert, E.</dc:creator>
    <dc:creator>Lecomte, C.</dc:creator>
    <dc:date>2007-12-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807043622</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Concepts such as Fourier transformation, convolution and resolution that are required to understand crystallography are illustrated through visual examples. </dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TEACHING TOOLS; DIGITALMICROGRAPH SOFTWARE; FOURIER TRANSFORM</dc:subject>
    <dc:description>Concepts such as Fourier transformation, convolution and resolution that are required to understand crystallography are illustrated through visual examples. These concepts can be explained pedagogically in a very direct way using the DigitalMicrograph software from Gatan Inc. (http://www.gatan.com/imaging/downloads.php), originally intended for electron microscopy data collection and analysis, and practical exercises developed around this tool can be used in teaching crystallography.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Illustrated Fourier transforms for crystallography</dc:title>
    <dc:type>text</dc:type>
    <prism:number>6</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-12-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>teaching and education</prism:section>
    <prism:startingPage>1153</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>1165</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks5154">
    <title>Meeting report of the BCA 25th Annual Meeting held at the University of Kent in Canterbury, UK, 16–19 April 2007</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks5154</link>
    <description>A report on the BCA 25th Annual Meeting held at the University of Kent in Canterbury, UK, 16–19 April 2007.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:date>2007-08-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807029184</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A report on the BCA 25th Annual Meeting held at the University of Kent in Canterbury, UK, 16–19 April 2007.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:description>A report on the BCA 25th Annual Meeting held at the University of Kent in Canterbury, UK, 16–19 April 2007.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Meeting report of the BCA 25th Annual Meeting held at the University of Kent in Canterbury, UK, 16–19 April 2007</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>meeting reports</prism:section>
    <prism:startingPage>808</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>809</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?he5368">
    <title>Phaser crystallographic software</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?he5368</link>
    <description>Phaser is a program for phasing macromolecular crystal structures by both molecular replacement and experimental phasing methods. The novel phasing algorithms implemented in Phaser have been developed using maximum likelihood and multivariate statistics. For molecular replacement, the new algorithms have proved to be significantly better than traditional methods in discriminating correct solutions from noise, and for single-wavelength anomalous dispersion experimental phasing, the new algorithms, which account for correlations between F+ and F−, give better phases (lower mean phase error with respect to the phases given by the refined structure) than those that use mean F and anomalous differences ΔF. One of the design concepts of Phaser was that it be capable of a high degree of automation. To this end, Phaser (written in C++) can be called directly from Python, although it can also be called using traditional CCP4 keyword-style input. Phaser is a platform for future development of improved phasing methods and their release, including source code, to the crystallographic community.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>McCoy, A.J.</dc:creator>
    <dc:creator>Grosse-Kunstleve, R.W.</dc:creator>
    <dc:creator>Adams, P.D.</dc:creator>
    <dc:creator>Winn, M.D.</dc:creator>
    <dc:creator>Storoni, L.C.</dc:creator>
    <dc:creator>Read, R.J.</dc:creator>
    <dc:date>2007-08-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807021206</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A description is given of Phaser-2.1: software for phasing macromolecular crystal structures by molecular replacement and single-wavelength anomalous dispersion phasing.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COMPUTER PROGRAMS; MOLECULAR REPLACEMENT; SAD PHASING; LIKELIHOOD; STRUCTURAL GENOMICS</dc:subject>
    <dc:description>Phaser is a program for phasing macromolecular crystal structures by both molecular replacement and experimental phasing methods. The novel phasing algorithms implemented in Phaser have been developed using maximum likelihood and multivariate statistics. For molecular replacement, the new algorithms have proved to be significantly better than traditional methods in discriminating correct solutions from noise, and for single-wavelength anomalous dispersion experimental phasing, the new algorithms, which account for correlations between F+ and F−, give better phases (lower mean phase error with respect to the phases given by the refined structure) than those that use mean F and anomalous differences ΔF. One of the design concepts of Phaser was that it be capable of a high degree of automation. To this end, Phaser (written in C++) can be called directly from Python, although it can also be called using traditional CCP4 keyword-style input. Phaser is a platform for future development of improved phasing methods and their release, including source code, to the crystallographic community.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Phaser crystallographic software</dc:title>
    <dc:type>text</dc:type>
    <prism:number>4</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>658</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>674</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?pf0048">
    <title>Personal X-ray reflections. By U. W. Arndt. Pp. 177. Twickenham: Athena Press, 2006. Price GBP 6.99, USD 11.95. ISBN 1-84401-694-3.</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?pf0048</link>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Helliwell, J.R.</dc:creator>
    <dc:date>2007-06-01</dc:date>
    <dc:identifier>doi:10.1107/S002188980701936X</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>Personal X-ray reflections. By U. W. Arndt. Pp. 177. Twickenham: Athena Press, 2006. Price GBP 6.99, USD 11.95. ISBN 1-84401-694-3.</dc:title>
    <dc:type>text</dc:type>
    <prism:number>3</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-06-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>book reviews</prism:section>
    <prism:startingPage>637</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>638</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6003">
    <title>Vesicles as reactors of nanoparticles: an anomalous small-angle X-ray scattering study of the domains rich in copper ions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6003</link>
    <description>The formation of copper hydroxide and copper oxide particles in the gaps among the stacks of multilamellar vesicles is described, illustrating a new pathway in the preparation of nanometre-scale particles. The in situ structural characterization of both the solid particles and the vesicles as a reaction medium was performed in the initial and final states of the process by using anomalous small-angle X-ray scattering (ASAXS) and freeze-fracture methods. The ASAXS method provides a description of the particle-size distribution of the copper nanoparticles, in spite of the fact that they are present in low concentration. This method allows the particle formation and growth to be monitored throughout the whole time range of the synthesis.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Bóta, A.</dc:creator>
    <dc:creator>Varga, Z.</dc:creator>
    <dc:creator>Goerigk, G.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807018882</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The gaps among the stacks of multilamellar vesicles used for the synthesis of nanoparticles are shown and characterized by ASAXS and freeze-fracture methods.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FREEZE-FRACTURE METHOD; VESICLES; NANOPARTICLES; INTERDIGITATED PHASES</dc:subject>
    <dc:description>The formation of copper hydroxide and copper oxide particles in the gaps among the stacks of multilamellar vesicles is described, illustrating a new pathway in the preparation of nanometre-scale particles. The in situ structural characterization of both the solid particles and the vesicles as a reaction medium was performed in the initial and final states of the process by using anomalous small-angle X-ray scattering (ASAXS) and freeze-fracture methods. The ASAXS method provides a description of the particle-size distribution of the copper nanoparticles, in spite of the fact that they are present in low concentration. This method allows the particle formation and growth to be monitored throughout the whole time range of the synthesis.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Vesicles as reactors of nanoparticles: an anomalous small-angle X-ray scattering study of the domains rich in copper ions</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>259</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>263</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6023">
    <title>Structural formation and many-body effect of concentrated dendrimer solutions by computer simulations</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6023</link>
    <description>Coarse-grained molecular dynamics simulations have been performed in order to study charged dendrimers in an aqueous solution. The structure factor, counterion distribution and effective interaction between molecules are clarified numerically. In particular, the many-body interactions in a triplet system are investigated, which is of importance in concentrated systems. These results shed new light on the analysis of recent small-angle X-ray and neutron scattering experiments on dendrimer solutions.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Terao, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807018055</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Structural formation and effective interaction in a charged dendrimer solution are investigated by parallel stochastic molecular dynamics simulations.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DENDRIMERS; SUPERMOLECULES; POLYELECTROLYTES</dc:subject>
    <dc:description>Coarse-grained molecular dynamics simulations have been performed in order to study charged dendrimers in an aqueous solution. The structure factor, counterion distribution and effective interaction between molecules are clarified numerically. In particular, the many-body interactions in a triplet system are investigated, which is of importance in concentrated systems. These results shed new light on the analysis of recent small-angle X-ray and neutron scattering experiments on dendrimer solutions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structural formation and many-body effect of concentrated dendrimer solutions by computer simulations</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>581</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>584</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6020">
    <title>Salt-concentration dependence of the structure and form factors for the wormlike micelle made from a dual surfactant in aqueous solutions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6020</link>
    <description>Small-angle X-ray scattering (SAXS) from dual-surfactant aqueous solutions made from sodium lauryl ether sulfate and coconut fatty acid amido propyl betaine was systematically measured as a function of the net sodium cation concentration, [Na+]*, and the surfactant concentration, CD. The SAXS intensity [I(q)] was normalized to CD and the resultant I(q)/CD was extrapolated to CD = 0 to give a form factor P(q) for each [Na+]* [where q = 4πsin(θ/2)/λ is the magnitude of the scattering vector, λ is the wavelength and 2θ is the scattering angle]. The low-q behaviour of P(q) was consistent with long rigid cylinders. The middle- and high-q profiles fitted well with a core–shell cylinder model for all [Na+]*. The core and total radii (Rc and Rs) did not depend on [Na+]* at all: Rc = 1.2 ± 0.05 and Rs = 3.1 ± 0.05 nm for [Na+]* = 0.42–1.5 mol l−1, indicating that the salt concentration changes did not induce any structural changes and re-assembling of the surfactants comprising the micelles. This fact is in contrast to the rheological behaviour where the relaxation mode strongly depends on [Na+]*. The structure factor [S(q)] was obtained by dividing I(q)/CD by P(q) for each CD and the mean distance (dm) between the micelles was obtained from the first maximum of S(q) versus q plots. The dm value decreased with increasing CD and [Na+]*, which is in good agreement with the theoretical prediction and experimental results for charged wormlike micelle solutions.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Eguchi, K.</dc:creator>
    <dc:creator>Kaneda, I.</dc:creator>
    <dc:creator>Hiwatari, Y.</dc:creator>
    <dc:creator>Masunaga, H.</dc:creator>
    <dc:creator>Sakurai, K.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807017888</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The small-angle X-ray scattering from dual-surfactant aqueous solutions made from sodium lauryl ether sulfate and coconut fatty acid amido propyl betaine was systematically measured as a function of the net sodium cation concentration and the surfactant concentration. The low-q behaviour of the form factor was consistent with long rigid cylinders while the middle- and high-q profiles fitted well with a core–shell cylinder model.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SURFACTANTS; SODIUM LAURYL ETHER SULFATE; COCONUT FATTY ACID AMIDO PROPYL BETAINE; SYNCHROTRON SAXS</dc:subject>
    <dc:description>Small-angle X-ray scattering (SAXS) from dual-surfactant aqueous solutions made from sodium lauryl ether sulfate and coconut fatty acid amido propyl betaine was systematically measured as a function of the net sodium cation concentration, [Na+]*, and the surfactant concentration, CD. The SAXS intensity [I(q)] was normalized to CD and the resultant I(q)/CD was extrapolated to CD = 0 to give a form factor P(q) for each [Na+]* [where q = 4πsin(θ/2)/λ is the magnitude of the scattering vector, λ is the wavelength and 2θ is the scattering angle]. The low-q behaviour of P(q) was consistent with long rigid cylinders. The middle- and high-q profiles fitted well with a core–shell cylinder model for all [Na+]*. The core and total radii (Rc and Rs) did not depend on [Na+]* at all: Rc = 1.2 ± 0.05 and Rs = 3.1 ± 0.05 nm for [Na+]* = 0.42–1.5 mol l−1, indicating that the salt concentration changes did not induce any structural changes and re-assembling of the surfactants comprising the micelles. This fact is in contrast to the rheological behaviour where the relaxation mode strongly depends on [Na+]*. The structure factor [S(q)] was obtained by dividing I(q)/CD by P(q) for each CD and the mean distance (dm) between the micelles was obtained from the first maximum of S(q) versus q plots. The dm value decreased with increasing CD and [Na+]*, which is in good agreement with the theoretical prediction and experimental results for charged wormlike micelle solutions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Salt-concentration dependence of the structure and form factors for the wormlike micelle made from a dual surfactant in aqueous solutions</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>264</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>268</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6027">
    <title>X-ray fluorescence correlation spectroscopy – a tool to study element-specific dynamics</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6027</link>
    <description>We have explored the feasibility of X-ray fluorescence correlation spectroscopy for studying the dynamics of colloidal particles in solution. We measured suspensions of Au nanoparticles from 5 to 150 nm diameter in water/glycerol mixtures of various compositions. Time-averaged sample properties were traced via small-angle X-ray scattering. The contrast of the measured time-correlation functions scales as expected with the particle concentration in the sample. The time constants for translational diffusion and sedimentation in water/glycerol mixtures follow only qualitatively the expected behaviour.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Leupold, O.</dc:creator>
    <dc:creator>Grübel, G.</dc:creator>
    <dc:creator>Roth, S.V.</dc:creator>
    <dc:creator>Schroer, C.</dc:creator>
    <dc:creator>Roseker, W.</dc:creator>
    <dc:creator>Sikorski, M.</dc:creator>
    <dc:creator>Robert, A.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807017852</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The dynamics of Au nanoparticles suspended in mixtures of water and glycerol are investigated by X-ray fluorescence correlation spectroscopy. The contrast of the measured time-correlation functions scales as expected with the Au particle concentration. The time constants for translational diffusion and sedimentation in water/glycerol show only qualitative agreement with the expected values.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY FLUORESCENCE CORRELATION SPECTROSCOPY; COLLOIDAL SUSPENSIONS; TIME-AVERAGED PROPERTIES</dc:subject>
    <dc:description>We have explored the feasibility of X-ray fluorescence correlation spectroscopy for studying the dynamics of colloidal particles in solution. We measured suspensions of Au nanoparticles from 5 to 150 nm diameter in water/glycerol mixtures of various compositions. Time-averaged sample properties were traced via small-angle X-ray scattering. The contrast of the measured time-correlation functions scales as expected with the particle concentration in the sample. The time constants for translational diffusion and sedimentation in water/glycerol mixtures follow only qualitatively the expected behaviour.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray fluorescence correlation spectroscopy – a tool to study element-specific dynamics</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>283</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>285</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6035">
    <title>Focusing and polarized neutron small-angle scattering spectrometer (SANS-J-II). The challenge of observation over length scales from an ångström to a micrometre</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6035</link>
    <description>SANS-J (a pinhole small-angle neutron scattering spectrometer at research reactor JRR3, Tokai, Japan) was reconstructed as a focusing and polarized neutron small-angle scattering spectrometer (SANS-J-II). By employing focusing lenses of a biconcave MgF2 crystal or of a sextupole permanent magnet and a high-resolution photomultiplier, the minimum accessible magnitude of the scattering vector qmin was improved from 3 × 10−3 Å−1 to an ultra-small-angle scattering (USAS) of 3 × 10−4 Å−1. Compared with a Bonse–Hart double-crystal method, the advantages of focusing USAS are the efficient detection of anisotropic USAS with an area detector, an improvement in q resolution Δq/q at conventional magnitudes of the scattering vector q ~ 10−3 Å−1 and a gain in neutron flux in the conventional q region of q ~ 10−3 Å−1.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Koizumi, S.</dc:creator>
    <dc:creator>Iwase, H.</dc:creator>
    <dc:creator>Suzuki, J.-</dc:creator>
    <dc:creator>Oku, T.</dc:creator>
    <dc:creator>Motokawa, R.</dc:creator>
    <dc:creator>Sasao, H.</dc:creator>
    <dc:creator>Tanaka, H.</dc:creator>
    <dc:creator>Yamaguchi, D.</dc:creator>
    <dc:creator>Shimizu, H.M.</dc:creator>
    <dc:creator>Hashimoto, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807014392</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>By using a focusing lens, a pinhole small-angle neutron spectrometer was reconstructed into a focusing ultra-small-angle scattering spectrometer (SANS-J-II).</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ULTRA-SMALL-ANGLE SCATTERING SPECTROMETER; FOCUSING AND POLARIZED SPECTROMETER; NEUTRON SCATTERING SPECTROMETER; FOCUSING LENS</dc:subject>
    <dc:description>SANS-J (a pinhole small-angle neutron scattering spectrometer at research reactor JRR3, Tokai, Japan) was reconstructed as a focusing and polarized neutron small-angle scattering spectrometer (SANS-J-II). By employing focusing lenses of a biconcave MgF2 crystal or of a sextupole permanent magnet and a high-resolution photomultiplier, the minimum accessible magnitude of the scattering vector qmin was improved from 3 × 10−3 Å−1 to an ultra-small-angle scattering (USAS) of 3 × 10−4 Å−1. Compared with a Bonse–Hart double-crystal method, the advantages of focusing USAS are the efficient detection of anisotropic USAS with an area detector, an improvement in q resolution Δq/q at conventional magnitudes of the scattering vector q ~ 10−3 Å−1 and a gain in neutron flux in the conventional q region of q ~ 10−3 Å−1.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Focusing and polarized neutron small-angle scattering spectrometer (SANS-J-II). The challenge of observation over length scales from an ångström to a micrometre</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>474</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>479</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6011">
    <title>Shear-induced structural transition in the lamellar phase of the C16E7/D2O system. Time evolution of small-angle neutron scattering at a constant shear rate</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6011</link>
    <description>The time evolution of small-angle neutron scattering is measured for the lamellar phase of a nonionic surfactant C16H33(OC2H4)7OH (C16E7) in D2O at 48 wt% at 343 K under shear flow. At the shear rates of 0.3, 1 and 3 s−1, a new diffraction peak appears at higher q [where q = (4π/λ)sin θ, and λ and 2θ are the wavelength of the neutron beam and the scattering angle, respectively] about 1–2 h after applying shear flow and coexists with the initial diffraction peak. The coexistence of two peaks continues even after 5 h at 0.3 s−1 whereas at 1 and 3 s−1 the peak at lower q disappears after about 3 h. These results indicate that the repeat distance decreases discontinuously and so suggest some sort of transition. A plot of the repeat distance after 5 h versus shear rate shows a minimum at 1 s−1, which is in good agreement with our previous results obtained by increasing the shear rate stepwise.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Miyazaki, K.</dc:creator>
    <dc:creator>Kosaka, Y.</dc:creator>
    <dc:creator>Kawabata, Y.</dc:creator>
    <dc:creator>Komura, S.</dc:creator>
    <dc:creator>Kato, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807013568</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The time evolution of the small-angle scattering of the lamellar phase of a nonionic surfactant C16H33(OC2H4)7OH (C16E7) in D2O at a constant shear rate (0.3–30 s−1) is measured. The results indicate a discontinuous decrease in the repeat distance and so suggest some sort of transition.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SURFACTANTS; SANS; LAMELLAR STRUCTURES</dc:subject>
    <dc:description>The time evolution of small-angle neutron scattering is measured for the lamellar phase of a nonionic surfactant C16H33(OC2H4)7OH (C16E7) in D2O at 48 wt% at 343 K under shear flow. At the shear rates of 0.3, 1 and 3 s−1, a new diffraction peak appears at higher q [where q = (4π/λ)sin θ, and λ and 2θ are the wavelength of the neutron beam and the scattering angle, respectively] about 1–2 h after applying shear flow and coexists with the initial diffraction peak. The coexistence of two peaks continues even after 5 h at 0.3 s−1 whereas at 1 and 3 s−1 the peak at lower q disappears after about 3 h. These results indicate that the repeat distance decreases discontinuously and so suggest some sort of transition. A plot of the repeat distance after 5 h versus shear rate shows a minimum at 1 s−1, which is in good agreement with our previous results obtained by increasing the shear rate stepwise.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Shear-induced structural transition in the lamellar phase of the C16E7/D2O system. Time evolution of small-angle neutron scattering at a constant shear rate</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>332</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>334</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6001">
    <title>Effect of lithium trifluoromethanesulfonate on the phase diagram of a liquid-crystalline amphiphilic diblock copolymer</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6001</link>
    <description>Phase transitions and nanometre-scale ordered structures of a binary system of a liquid-crystalline amphiphilic diblock copolymer, poly(ethylene oxide)-b-poly{11-[4-(4-butylphenylazo)phenoxy]undecyl methacrylate} [PEOm-b-PMA(Az)n, where m and n are the degrees of polymerization of the PEO and PMA(Az) domains, respectively], and lithium trifluoromethanesulfonate (LiCF3SO3) were investigated by differential scanning calorimetry and small-angle X-ray scattering (SAXS). PEO114-b-PMA(Az)51 formed a highly ordered hexagonally packed PEO cylinder structure in the temperature range below 393 K and transformed to a body-centred-cubic structure in the isotropic state above 393 K. The PEO114-b-PMA(Az)51/LiCF3SO3 systems with various LiCF3SO3 concentrations (molar ratio 0 &lt; LiCF3SO3/EO = fLi &lt; 1) formed the hexagonally packed cylinder structure at room temperature. From the effects of LiCF3SO3 concentration on the phase transitions, the size and the order of the hexagonally packed cylinder structure, it was found that PEO114-b-PMA(Az)51 and LiCF3SO3 formed a complex efficiently at a molar equivalent of three ethylene oxide repeating units per LiCF3SO3 unit. The ordering of the hexagonally packed cylinder structure decreased with increasing LiCF3SO3 concentration and the radius of the PEO cylinder evaluated by SAXS profile fitting increased from 2.7 to 8.3 nm. For the PEO114-b-PMA(Az)51/LiCF3SO3 system with fLi = 1, the hexagonally packed cylinder structure remained even in the isotropic state because the PEO volume fraction (φPEO) increased from φPEO = 0.06 (fLi = 0) to φPEO = 0.23 (fLi = 1) on the formation of the LiCF3SO3/PEO complex.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Yamada, T.</dc:creator>
    <dc:creator>Li, J.</dc:creator>
    <dc:creator>Koyanagi, C.</dc:creator>
    <dc:creator>Iyoda, T.</dc:creator>
    <dc:creator>Yoshida, H.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807013453</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Phase transitions and nanometre-scale ordered structures of a binary system of a liquid-crystalline amphiphilic diblock copolymer containing polyethylene oxide and lithium trifluoromethanesulfonate were investigated by differential scanning calorimetry and small-angle X-ray scattering.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AMPHIPHILIC DIBLOCK COPOLYMERS; SMALL-ANGLE X-RAY SCATTERING; LITHIUM TRIFLUOROMETHANESULFONATE; NANOCOMPOSITES</dc:subject>
    <dc:description>Phase transitions and nanometre-scale ordered structures of a binary system of a liquid-crystalline amphiphilic diblock copolymer, poly(ethylene oxide)-b-poly{11-[4-(4-butylphenylazo)phenoxy]undecyl methacrylate} [PEOm-b-PMA(Az)n, where m and n are the degrees of polymerization of the PEO and PMA(Az) domains, respectively], and lithium trifluoromethanesulfonate (LiCF3SO3) were investigated by differential scanning calorimetry and small-angle X-ray scattering (SAXS). PEO114-b-PMA(Az)51 formed a highly ordered hexagonally packed PEO cylinder structure in the temperature range below 393 K and transformed to a body-centred-cubic structure in the isotropic state above 393 K. The PEO114-b-PMA(Az)51/LiCF3SO3 systems with various LiCF3SO3 concentrations (molar ratio 0 &lt; LiCF3SO3/EO = fLi &lt; 1) formed the hexagonally packed cylinder structure at room temperature. From the effects of LiCF3SO3 concentration on the phase transitions, the size and the order of the hexagonally packed cylinder structure, it was found that PEO114-b-PMA(Az)51 and LiCF3SO3 formed a complex efficiently at a molar equivalent of three ethylene oxide repeating units per LiCF3SO3 unit. The ordering of the hexagonally packed cylinder structure decreased with increasing LiCF3SO3 concentration and the radius of the PEO cylinder evaluated by SAXS profile fitting increased from 2.7 to 8.3 nm. For the PEO114-b-PMA(Az)51/LiCF3SO3 system with fLi = 1, the hexagonally packed cylinder structure remained even in the isotropic state because the PEO volume fraction (φPEO) increased from φPEO = 0.06 (fLi = 0) to φPEO = 0.23 (fLi = 1) on the formation of the LiCF3SO3/PEO complex.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Effect of lithium trifluoromethanesulfonate on the phase diagram of a liquid-crystalline amphiphilic diblock copolymer</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>585</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>589</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6025">
    <title>Evaluation of multiple small-angle neutron scattering including magnetic interactions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6025</link>
    <description>Analytical formulae describing multiple small-angle neutron scattering in ferromagnetic materials are derived from transport equations. The derivation is based on Molière's theory of multiple small-angle scattering assuming that the mean free path of the neutrons is large compared to the size of the scatterers. In addition to the formalism developed earlier for nuclear scattering, the new formulation takes into account the spin dependence of the scattering cross section and spin flips caused by subsequent scattering events. This leads to an anomalous distribution of scattering intensity and polarization, as demonstrated by examples of model calculations and Monte Carlo simulations. In particular, multiple scattering of polarized neutrons can lead to either smoothing or sharpening of the scattered beam anisotropy depending on the polarization of the primary beam and the nuclear and magnetic contrasts of the scatterers. The presented theory has been implemented in the data-fitting program SASProFit suitable for both the modelling of multiple scattering effects and the analysis of experimental data.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Šaroun, J.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807012447</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Formulae describing multiple small-angle scattering of polarized neutrons by ferromagnetic inhomogeneities are derived. The results show an anomalous distribution of scattered neutrons due to the simultaneous effect of multiple scattering and the spin dependence of the single-scattering cross section.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MULTIPLE SMALL-ANGLE SCATTERING; NEUTRONS; FERROMAGNETS</dc:subject>
    <dc:description>Analytical formulae describing multiple small-angle neutron scattering in ferromagnetic materials are derived from transport equations. The derivation is based on Molière's theory of multiple small-angle scattering assuming that the mean free path of the neutrons is large compared to the size of the scatterers. In addition to the formalism developed earlier for nuclear scattering, the new formulation takes into account the spin dependence of the scattering cross section and spin flips caused by subsequent scattering events. This leads to an anomalous distribution of scattering intensity and polarization, as demonstrated by examples of model calculations and Monte Carlo simulations. In particular, multiple scattering of polarized neutrons can lead to either smoothing or sharpening of the scattered beam anisotropy depending on the polarization of the primary beam and the nuclear and magnetic contrasts of the scatterers. The presented theory has been implemented in the data-fitting program SASProFit suitable for both the modelling of multiple scattering effects and the analysis of experimental data.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Evaluation of multiple small-angle neutron scattering including magnetic interactions</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>701</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>705</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6014">
    <title>X-ray studies of the self-organized structure formed by 1,2-bis(4'-n-alkoxybenzoyl)hydrazine (BABH-n) homologues. 1. Ia3d-gyroid structure</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6014</link>
    <description>The cubic (Cub) phase structure of a thermotropic mesogen 1,2-bis(4′-n-alkoxybenzoyl)hydrazine (BABH-n, where n is the number of C atoms in the aliphatic tail) was examined by small-angle X-ray scattering. The BABH-n system exhibits two types of Cub phases, Ia3d type and Im3m type. In the phase diagram as a function of the tail length (n) the Im3m-Cub phase region (n = 13–16) was sandwiched by two Ia3d-Cub phase regions with n &lt; 13 and n &gt; 16. On the basis of the triply periodic minimal surface (TPMS) picture, the Ia3d and Im3m structures are described by the gyroid (G) and doubled-P (PP) surfaces, respectively. In this paper we focused attention on the internal structure of the Ia3d-Cub phase at the molecular level. By examining how the relative intensity of the 220 reflection with respect to the 211 reference peak varies with n, we have successfully determined the position of the aliphatic tails, which are located on the G-TPMSs. As far as we know, this is the first approach to clarifying the internal structure of the thermotropic Ia3d-Cub phase. The usefulness of the systematic studies with respect to the tail length n has also been demonstrated.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Kutsumizu, S.</dc:creator>
    <dc:creator>Mori, H.</dc:creator>
    <dc:creator>Fukatami, M.</dc:creator>
    <dc:creator>Saito, K.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807011958</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Examination of the relative intensity of the X-ray 220 reflection with respect to the 211 reference peak as a function of the alkoxy chain length of the title compounds enables the internal structure of the thermotropic Ia3d cubic phase to be clarified.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; SELF-ORGANIZED STRUCTURES; THERMOTROPIC CUBIC MESOPHASES; IA3D-GYROID; BABH</dc:subject>
    <dc:description>The cubic (Cub) phase structure of a thermotropic mesogen 1,2-bis(4′-n-alkoxybenzoyl)hydrazine (BABH-n, where n is the number of C atoms in the aliphatic tail) was examined by small-angle X-ray scattering. The BABH-n system exhibits two types of Cub phases, Ia3d type and Im3m type. In the phase diagram as a function of the tail length (n) the Im3m-Cub phase region (n = 13–16) was sandwiched by two Ia3d-Cub phase regions with n &lt; 13 and n &gt; 16. On the basis of the triply periodic minimal surface (TPMS) picture, the Ia3d and Im3m structures are described by the gyroid (G) and doubled-P (PP) surfaces, respectively. In this paper we focused attention on the internal structure of the Ia3d-Cub phase at the molecular level. By examining how the relative intensity of the 220 reflection with respect to the 211 reference peak varies with n, we have successfully determined the position of the aliphatic tails, which are located on the G-TPMSs. As far as we know, this is the first approach to clarifying the internal structure of the thermotropic Ia3d-Cub phase. The usefulness of the systematic studies with respect to the tail length n has also been demonstrated.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray studies of the self-organized structure formed by 1,2-bis(4'-n-alkoxybenzoyl)hydrazine (BABH-n) homologues. 1. Ia3d-gyroid structure</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>279</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>282</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?kk5010">
    <title>Operator-assisted harvesting of protein crystals using a universal micromanipulation robot</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?kk5010</link>
    <description>High-throughput crystallography has reached a level of automation where complete computer-assisted robotic crystallization pipelines are capable of cocktail preparation, crystallization plate setup, and inspection and interpretation of results. While mounting of crystal pins, data collection and structure solution are highly automated, crystal harvesting and cryocooling remain formidable challenges towards full automation. To address the final frontier in achieving fully automated high-throughput crystallography, the prototype of an anthropomorphic six-axis universal micromanipulation robot (UMR) has been designed and tested; this UMR is capable of operator-assisted harvesting and cryoquenching of protein crystals as small as 10 µm from a variety of 96-well plates. The UMR is equipped with a versatile tool exchanger providing full operational flexibility. Trypsin crystals harvested and cryoquenched using the UMR have yielded a 1.5 Å structure demonstrating the feasibility of robotic protein crystal harvesting.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Viola, R.</dc:creator>
    <dc:creator>Carman, P.</dc:creator>
    <dc:creator>Walsh, J.</dc:creator>
    <dc:creator>Miller, E.</dc:creator>
    <dc:creator>Benning, M.</dc:creator>
    <dc:creator>Frankel, D.</dc:creator>
    <dc:creator>McPherson, A.</dc:creator>
    <dc:creator>Cudney, B.</dc:creator>
    <dc:creator>Rupp, B.</dc:creator>
    <dc:date>2007-06-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807012149</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The prototype of a universal micromanipulation robot for crystal harvesting is presented, and a robotically harvested trypsin crystal yields a high-resolution structure demonstrating the feasibility of robotic protein crystal harvesting.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AUTOMATED CRYSTAL HARVESTING; CRYSTAL MOUNTING; CRYOPROTECTION; TRYPSIN; PROTEASE; BENZAMIDINE COMPLEX; PROTAMINE; INTERMOLECULAR CONTACTS; CRYSTALLIZATION ADDITIVES</dc:subject>
    <dc:description>High-throughput crystallography has reached a level of automation where complete computer-assisted robotic crystallization pipelines are capable of cocktail preparation, crystallization plate setup, and inspection and interpretation of results. While mounting of crystal pins, data collection and structure solution are highly automated, crystal harvesting and cryocooling remain formidable challenges towards full automation. To address the final frontier in achieving fully automated high-throughput crystallography, the prototype of an anthropomorphic six-axis universal micromanipulation robot (UMR) has been designed and tested; this UMR is capable of operator-assisted harvesting and cryoquenching of protein crystals as small as 10 µm from a variety of 96-well plates. The UMR is equipped with a versatile tool exchanger providing full operational flexibility. Trypsin crystals harvested and cryoquenched using the UMR have yielded a 1.5 Å structure demonstrating the feasibility of robotic protein crystal harvesting.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Operator-assisted harvesting of protein crystals using a universal micromanipulation robot</dc:title>
    <dc:type>text</dc:type>
    <prism:number>3</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-06-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>research papers</prism:section>
    <prism:startingPage>539</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>545</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6011">
    <title>Hierarchical structure of niobate nanosheets in aqueous solution</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6011</link>
    <description>The hierarchical structure of an aqueous dispersion of niobate nanosheets was explored by using a combined method of ultra-small-angle and small-angle scattering of neutrons and X-rays. The concentration of the sheets studied was in the range where the dispersion exhibits a liquid-crystal phase as evidenced by observation between crossed polarizers in a previous report. The scattering data covered a wide q scale of more than four orders of magnitude [3 × 10−4 ≤ q ≤ 10 nm−1, where q = (4π/λ)sin(θ/2), λ and θ being the wavelength of the incident beam and the scattering angle, respectively], corresponding to the length scale l = 2π/q from ~1 nm to ~20 µm. The scattering analyses provided information on the hierarchical structural elements including: (i) single nanosheets as a structure element (hierarchy I), (ii) parallel stacks of the sheets (hierarchy II), and (iii) spatial arrangements of the stacks (hierarchy III), in order of increasing length scale. Hierarchy II is closely related to the liquid-crystal nature of the dispersion in which the spacing and the persistence length, normal and parallel to the stack surface, respectively, were disclosed. Hierarchy III gives rise to the low-q upturn in the scattering profile, which may be characterized by mass-fractal-like power-law scattering behavior. This finding is a surprise from the viewpoint of the liquid-crystal nature of the dispersion, a possible model of which is proposed in the text.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Yamaguchi, D.</dc:creator>
    <dc:creator>Miyamoto, N.</dc:creator>
    <dc:creator>Koizumi, S.</dc:creator>
    <dc:creator>Nakato, T.</dc:creator>
    <dc:creator>Hashimoto, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807011727</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The hierarchical structure of an aqueous dispersion of niobate nanosheets was investigated by (ultra-)small-angle scattering methods.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POTASSIUM NIOBATE; NANOSHEETS; USANS; SANS; HIERARCHICAL STRUCTURES; LIQUID CRYSTALS; FRACTALS</dc:subject>
    <dc:description>The hierarchical structure of an aqueous dispersion of niobate nanosheets was explored by using a combined method of ultra-small-angle and small-angle scattering of neutrons and X-rays. The concentration of the sheets studied was in the range where the dispersion exhibits a liquid-crystal phase as evidenced by observation between crossed polarizers in a previous report. The scattering data covered a wide q scale of more than four orders of magnitude [3 × 10−4 ≤ q ≤ 10 nm−1, where q = (4π/λ)sin(θ/2), λ and θ being the wavelength of the incident beam and the scattering angle, respectively], corresponding to the length scale l = 2π/q from ~1 nm to ~20 µm. The scattering analyses provided information on the hierarchical structural elements including: (i) single nanosheets as a structure element (hierarchy I), (ii) parallel stacks of the sheets (hierarchy II), and (iii) spatial arrangements of the stacks (hierarchy III), in order of increasing length scale. Hierarchy II is closely related to the liquid-crystal nature of the dispersion in which the spacing and the persistence length, normal and parallel to the stack surface, respectively, were disclosed. Hierarchy III gives rise to the low-q upturn in the scattering profile, which may be characterized by mass-fractal-like power-law scattering behavior. This finding is a surprise from the viewpoint of the liquid-crystal nature of the dispersion, a possible model of which is proposed in the text.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Hierarchical structure of niobate nanosheets in aqueous solution</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>101</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>105</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6016">
    <title>Characterization of two-dimensional ultra-small-angle X-ray scattering apparatus for application to rubber filled with spherical silica under elongation</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6016</link>
    <description>Two-dimensional ultra-small-angle X-ray scattering (2D-USAXS) apparatus at SPring-8 has been characterized. 2D-USAXS is a promising tool to study the structural change of the hierachical aggregate structure of fillers such as carbon black and silica particles in rubber. The aggregate structure of fillers is key to understanding the reinforcement effects which fillers show in rubber. We have applied 2D-USAXS to rubber filled with spherical silica particles and proved it to be a powerful technique.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Shinohara, Y.</dc:creator>
    <dc:creator>Kishimoto, H.</dc:creator>
    <dc:creator>Inoue, K.</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>Muraoka, K.</dc:creator>
    <dc:creator>Mizoguchi, T.</dc:creator>
    <dc:creator>Amemiya, Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807011697</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Two-dimensional ultra-small-angle X-ray scattering apparatus at SPring-8 has been characterized and applied to stretched rubber filled with spherical silica particles.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TIME-RESOLVED TWO-DIMENSIONAL USAXS; FILLED RUBBER</dc:subject>
    <dc:description>Two-dimensional ultra-small-angle X-ray scattering (2D-USAXS) apparatus at SPring-8 has been characterized. 2D-USAXS is a promising tool to study the structural change of the hierachical aggregate structure of fillers such as carbon black and silica particles in rubber. The aggregate structure of fillers is key to understanding the reinforcement effects which fillers show in rubber. We have applied 2D-USAXS to rubber filled with spherical silica particles and proved it to be a powerful technique.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Characterization of two-dimensional ultra-small-angle X-ray scattering apparatus for application to rubber filled with spherical silica under elongation</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>397</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>401</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6023">
    <title>Study on two-dimensional small-angle X-ray scattering of in situ silica filled nanocomposite elastomer during deformation</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6023</link>
    <description>Morphological change of in situ generated silica particles was investigated by a time-resolved two-dimensional small-angle X-ray scattering technique and a simultaneous tensile measurement. The in situ silica particles with diameter ca 34 nm were homogeneously dispersed in a rubbery matrix and the morphological change of the particles was followed up to the elongation ratio α = 2 during stretching and from α = 2.5 during retracting. The observed two-dimensional small-angle X-ray scattering patterns agreed with the simulation results by Rharbi et al. [Europhys. Lett. (1999), 46, 472–478] where a shear displacement model was proposed for the deformation mode of their soft nanocomposite.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Ikeda, Y.</dc:creator>
    <dc:creator>Yasuda, Y.</dc:creator>
    <dc:creator>Yamamoto, S.</dc:creator>
    <dc:creator>Morita, Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807011740</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>In situ silica filled soft nanocomposite was prepared by the sol–gel reaction of tetraethoxysilane in peroxide-crosslinked isoprene rubber. The morphological change of the in situ silica particles during the uniaxial stretching and retracting processes was investigated by SAXS.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TIME-RESOLVED SAXS; SILICA; SOFT MATTER; DEFORMATION</dc:subject>
    <dc:description>Morphological change of in situ generated silica particles was investigated by a time-resolved two-dimensional small-angle X-ray scattering technique and a simultaneous tensile measurement. The in situ silica particles with diameter ca 34 nm were homogeneously dispersed in a rubbery matrix and the morphological change of the particles was followed up to the elongation ratio α = 2 during stretching and from α = 2.5 during retracting. The observed two-dimensional small-angle X-ray scattering patterns agreed with the simulation results by Rharbi et al. [Europhys. Lett. (1999), 46, 472–478] where a shear displacement model was proposed for the deformation mode of their soft nanocomposite.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Study on two-dimensional small-angle X-ray scattering of in situ silica filled nanocomposite elastomer during deformation</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>549</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>552</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6022">
    <title>Lamellar crystal thickness transition of melt-crystallized isotactic polybutene-1 observed by small-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6022</link>
    <description>The first-order long period L1, the second-order long period L2 and lamellar crystal thickness lc of isotactic polybutene-1 have been investigated for crystallization in the melt over a wide range (313.2 to 363.2 K) of crystallization temperatures by small-angle X-ray scattering experiments and density measurements. The long period L1 shows a single linear dependence on inverse supercooling. The crystal thickness lc, however, demonstrates two linear dependences on inverse supercooling and a transition from one dependence to the other has been observed around 338.2 K, where lc becomes comparable with the radius of gyration Rg of the samples.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Yamashita, M.</dc:creator>
    <dc:creator>Kato, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807011570</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The first-order long period, the second-order long period and lamellar crystal thickness lc of isotactic polybutene-1 have been investigated for crystallization in the melt over a wide range (313.2–363.2 K) of crystallization temperatures by small-angle X-ray scattering experiments and density measurements. The crystal thickness lc demonstrates two linear dependences on inverse supercooling and a transition from one dependence to the other has been observed around 338.2 K, where lc becomes comparable with the radius of gyration Rg of the samples.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SMALL-ANGLE X-RAY SCATTERING; ISOTACTIC POLYBUTENE-1; TETRAGONAL FORM; MELT CRYSTALLIZATION; LAMELLAR CRYSTAL THICKNESS</dc:subject>
    <dc:description>The first-order long period L1, the second-order long period L2 and lamellar crystal thickness lc of isotactic polybutene-1 have been investigated for crystallization in the melt over a wide range (313.2 to 363.2 K) of crystallization temperatures by small-angle X-ray scattering experiments and density measurements. The long period L1 shows a single linear dependence on inverse supercooling. The crystal thickness lc, however, demonstrates two linear dependences on inverse supercooling and a transition from one dependence to the other has been observed around 338.2 K, where lc becomes comparable with the radius of gyration Rg of the samples.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Lamellar crystal thickness transition of melt-crystallized isotactic polybutene-1 observed by small-angle X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>650</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>655</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6020">
    <title>Surface free energies of isotactic polybutene-1 tetragonal and trigonal crystals: the role of conformational entropy of side chains</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6020</link>
    <description>Lateral and end surface free energies of melt-crystallized isotactic polybutene-1 (it-PB1) trigonal and tetragonal crystals have been determined by small-angle X-ray scattering and in situ observation of the crystal growth kinetics. The lateral surface free energy σ of the trigonal phase is about seven times as large as the value σHoff calculated according to Hoffman's equation [Hoffman (1992). Polymer, 33, 2643–2644], while that of the tetragonal phase is roughly in agreement with the estimation. The discrepancy between the values of σ and σHoff for the trigonal phase can be attributed to the loss of conformational entropy of the ethyl side chains of it-PB1.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Yamashita, M.</dc:creator>
    <dc:creator>Kato, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807011259</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Lateral surface free energies σ of isotactic polybutene-1 trigonal and tetragonal crystals grown in the melt have been determined from small-angle X-ray scattering experiments, differential scanning calorimetry and in situ observation of crystal growth kinetics. The σ value of the trigonal crystals is about seven times as large as the value theoretically estimated, while σ for the tetragonal crystals is roughly in agreement with the estimation.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SMALL-ANGLE X-RAY SCATTERING; ISOTACTIC POLYBUTENE-1; TRIGONAL FORM; TETRAGONAL FORM; MELT CRYSTALLIZATION; SIDE CHAIN; CONFORMATIONAL ENTROPY; SURFACE FREE ENERGY</dc:subject>
    <dc:description>Lateral and end surface free energies of melt-crystallized isotactic polybutene-1 (it-PB1) trigonal and tetragonal crystals have been determined by small-angle X-ray scattering and in situ observation of the crystal growth kinetics. The lateral surface free energy σ of the trigonal phase is about seven times as large as the value σHoff calculated according to Hoffman's equation [Hoffman (1992). Polymer, 33, 2643–2644], while that of the tetragonal phase is roughly in agreement with the estimation. The discrepancy between the values of σ and σHoff for the trigonal phase can be attributed to the loss of conformational entropy of the ethyl side chains of it-PB1.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Surface free energies of isotactic polybutene-1 tetragonal and trigonal crystals: the role of conformational entropy of side chains</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>558</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>563</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6016">
    <title>Phase behavior of platelet-shaped nanosilicate colloids in saline solutions – a small-angle X-ray scattering study</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6016</link>
    <description>A study of polydisperse suspensions of fluorohectorite clay in saline solutions is presented. The suspended clay colloids consist of stacks of nanosilicate sheets several tenths of a nanometre thick. They are polydisperse both with respect to the number of stacked nanolayers and with respect to their extension along the sheets. Due to this polydispersity, a spontaneous gravity-induced vertical segregation occurs in the sample tubes and results in the presence of up to four different phases on top of each other. Precise characterization of the phase diagram of the samples as a function of salt concentration and vertical position in the tubes, based on small-angle X-ray scattering data, is presented. The vertical positions of the phase boundaries were monitored by analyzing the eccentricity of elliptic fits to iso-intensity cuts of the scattering images. The intensity profiles along the two principal directions of scattering display two power-law behaviors with a smooth transition between them and show the absence of positional order in all phases.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Fonseca, D.M.</dc:creator>
    <dc:creator>Méheust, Y.</dc:creator>
    <dc:creator>Fossum, J.O.</dc:creator>
    <dc:creator>Knudsen, K.D.</dc:creator>
    <dc:creator>Måløy, K.J.</dc:creator>
    <dc:creator>Parmar, K.P.S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807010825</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Precise characterization of the phase diagram for suspensions of sodium fluorohectorite colloids in saline solutions is achieved from small-angle X-ray scattering measurements. Radial intensity profiles are also addressed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PLATELET-SHAPED COLLOIDS; NEMATIC ORDERING; PHASE DIAGRAMS; SAXS</dc:subject>
    <dc:description>A study of polydisperse suspensions of fluorohectorite clay in saline solutions is presented. The suspended clay colloids consist of stacks of nanosilicate sheets several tenths of a nanometre thick. They are polydisperse both with respect to the number of stacked nanolayers and with respect to their extension along the sheets. Due to this polydispersity, a spontaneous gravity-induced vertical segregation occurs in the sample tubes and results in the presence of up to four different phases on top of each other. Precise characterization of the phase diagram of the samples as a function of salt concentration and vertical position in the tubes, based on small-angle X-ray scattering data, is presented. The vertical positions of the phase boundaries were monitored by analyzing the eccentricity of elliptic fits to iso-intensity cuts of the scattering images. The intensity profiles along the two principal directions of scattering display two power-law behaviors with a smooth transition between them and show the absence of positional order in all phases.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Phase behavior of platelet-shaped nanosilicate colloids in saline solutions – a small-angle X-ray scattering study</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>292</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>296</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6010">
    <title>Repulsive interlamellar interaction induced by addition of colloidal particles</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6010</link>
    <description>The effects of colloidal particles confined between lamellar membrane slits on interlamellar interactions have been investigated by small-angle neutron scattering. On addition of colloidal particles to a lamellar phase composed of a non-ionic surfactant, the first lamellar peak becomes sharper and higher-order peaks appear. Thus the colloidal particles suppress undulation fluctuations of lamellar membranes by their steric hindrance, which results in a repulsive interlamellar interaction. As the interlamellar distance decreases, the position of the Bragg peak shifts towards higher q [where q is the magnitude of scattering vector, given by q = (4\pi/\lambda)\sin\theta, where 2\theta is the scattering angle and λ is the wavelength] and the peak intensity weakens. This tendency is completely opposite to the behavior of non-ionic surfactant lamellar phases, where the interlamellar interaction is governed by the Helfrich interaction. A phenomenological free-energy model is proposed based on the restriction of membrane fluctuations by colloidal particles. This model describes the experimental results well.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Suganuma, Y.</dc:creator>
    <dc:creator>Imai, M.</dc:creator>
    <dc:creator>Nakaya, K.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807010345</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The addition of colloidal particles between lamellar membrane slits induced a repulsive interlamellar interaction which showed a unique interlamellar distance dependence.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>INTERLAMELLAR INTERACTIONS; COLLOIDS; HELFRICH INTERACTION; SANS</dc:subject>
    <dc:description>The effects of colloidal particles confined between lamellar membrane slits on interlamellar interactions have been investigated by small-angle neutron scattering. On addition of colloidal particles to a lamellar phase composed of a non-ionic surfactant, the first lamellar peak becomes sharper and higher-order peaks appear. Thus the colloidal particles suppress undulation fluctuations of lamellar membranes by their steric hindrance, which results in a repulsive interlamellar interaction. As the interlamellar distance decreases, the position of the Bragg peak shifts towards higher q [where q is the magnitude of scattering vector, given by q = (4\pi/\lambda)\sin\theta, where 2\theta is the scattering angle and λ is the wavelength] and the peak intensity weakens. This tendency is completely opposite to the behavior of non-ionic surfactant lamellar phases, where the interlamellar interaction is governed by the Helfrich interaction. A phenomenological free-energy model is proposed based on the restriction of membrane fluctuations by colloidal particles. This model describes the experimental results well.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Repulsive interlamellar interaction induced by addition of colloidal particles</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>303</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>306</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6006">
    <title>Solution structure of Ca2+/calmodulin complexed with a lentivirus lytic peptide 1 reveals a novel mode of molecular recognition</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6006</link>
    <description>Small-angle X-ray scattering was used to analyze the interaction of Ca2+/calmodulin (CaM) with a lentivirus lytic peptide 1 (LLP1) derived from the cytoplasmic tail of HIV-1 transmembrane glycoprotein. The synthetic peptide homologues of LLP1 were selected from three species of the glycoprotein: ENV_HV1A2, ENV_HV1B1 and ENV_HV1H2. Ca2+/CaM binds LLP1 with the truncation of three or ten residues and adopts almost the same globular structure as that of the complex with a peptide from myosin light chain kinase (MLCK), indicating that the Ca2+/CaM-binding site locates on the shorter sequence. Moreover, Ca2+/CaM binds a peptide with the opposite sequence and adopts almost the same globular structure as that in the original sequence. Taken together, the results provide evidence that LLP1 can bind to the N- and C-terminal lobes of CaM with a polarity opposite to that observed for the CaM–MLCK complex and the binding mode of Ca2+/CaM molecular recognition is well preserved despite the sequence variation in the three species, suggesting that this region of the transmembrane glycoprotein is important to viral replication.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Izumi, Y.</dc:creator>
    <dc:creator>Amano, A.</dc:creator>
    <dc:creator>Saito, T.</dc:creator>
    <dc:creator>Jinbo, Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807010229</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The solution structure of Ca2+/calmodulin complexed with a lentivirus lytic peptide 1 reveals a novel mode of molecular recognition. The result suggests that this region of the transmembrane glycoprotein is important to viral replication.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>LLP1; CALMODULIN; SMALL-ANGLE X-RAY SCATTERING; NOVEL MOLECULAR RECOGNITION MODES</dc:subject>
    <dc:description>Small-angle X-ray scattering was used to analyze the interaction of Ca2+/calmodulin (CaM) with a lentivirus lytic peptide 1 (LLP1) derived from the cytoplasmic tail of HIV-1 transmembrane glycoprotein. The synthetic peptide homologues of LLP1 were selected from three species of the glycoprotein: ENV_HV1A2, ENV_HV1B1 and ENV_HV1H2. Ca2+/CaM binds LLP1 with the truncation of three or ten residues and adopts almost the same globular structure as that of the complex with a peptide from myosin light chain kinase (MLCK), indicating that the Ca2+/CaM-binding site locates on the shorter sequence. Moreover, Ca2+/CaM binds a peptide with the opposite sequence and adopts almost the same globular structure as that in the original sequence. Taken together, the results provide evidence that LLP1 can bind to the N- and C-terminal lobes of CaM with a polarity opposite to that observed for the CaM–MLCK complex and the binding mode of Ca2+/CaM molecular recognition is well preserved despite the sequence variation in the three species, suggesting that this region of the transmembrane glycoprotein is important to viral replication.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Solution structure of Ca2+/calmodulin complexed with a lentivirus lytic peptide 1 reveals a novel mode of molecular recognition</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>170</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>174</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6018">
    <title>Living anionic polymerization of methyl meth­acrylate controlled by metal-free phosphazene catalyst as observed by small-angle neutron scattering, gel-permeation chromatography and UV–visible spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6018</link>
    <description>Phosphazene (PZN) catalyst, PZN catalyst coexisting with a co-catalyst 1-hydroxycyclohexyl phenyl ketone (Irgacure 184; IRG) and polymethylmethacrylate (PMMA) (prepared by catalytic living anionic polymerization using the PZN catalyst and IRG) have been observed for the first time by small-angle neutron scattering (SANS) and UV–visible spectroscopy to elucidate the aggregation behavior of the PZN molecules themselves and the state of living chain ends in a living polymer solution. PZN catalyst in deuterated tetrahydrofuran (thf-d8) showed SANS curves fitted by a form factor for a sphere whose radius Rs is larger (1.4–1.6 nm) than a single PZN molecule (0.65 nm), indicating formation of PZN aggregates in thf-d8. In a nonpolar solvent, benzene-d6, Rs was even larger (3.1 nm), indicating formation of larger aggregates. By adding IRG to PZN solution, an excess scattering appeared in the SANS profile and a strong band emerged in the UV–visible spectrum. This result indicates strong interaction of IRG with PZN not only on a molecular scale but also on a mesoscopic scale. The SANS profile from the living polymer solution in thf-d8 was observed to be fitted by the sum of the profile for the aggregated PZN/IRG complex and that for Gaussian chains of PMMA. The molecular weight of the PMMA determined by SANS, 2100 g mol−1, was in agreement with that estimated from gel-permeation chromatography, indicating that the anionic living chain ends and their counter ions (PZN) are dissociated in thf-d8; thus, the chains are not associated into multiple-ion pairs.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Miyamoto, N.</dc:creator>
    <dc:creator>Inoue, Y.</dc:creator>
    <dc:creator>Koizumi, S.</dc:creator>
    <dc:creator>Hashimoto, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009673</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Phosphazene (PZN) catalyst, a mixture of PZN and a co-catalyst 1-hydroxycyclohexyl phenyl ketone (Irgacure 184; IRG), and polymethylmethacrylate prepared by catalytic living anionic polymerization using the PZN catalyst and IRG have been observed for the first time by small-angle neutron scattering and UV–visible spectroscopy to elucidate the aggregation behavior of the PZN molecules and the state of living chain ends in a living polymer solution.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AGGREGATES; LIVING ANIONIC POLYMERIZATION; PHOSPHAZENE CATALYST; METHYLMETHACRYLATE; SMALL-ANGLE NEUTRON SCATTERING; UV-VISIBLE SPECTROSCOPY</dc:subject>
    <dc:description>Phosphazene (PZN) catalyst, PZN catalyst coexisting with a co-catalyst 1-hydroxycyclohexyl phenyl ketone (Irgacure 184; IRG) and polymethylmethacrylate (PMMA) (prepared by catalytic living anionic polymerization using the PZN catalyst and IRG) have been observed for the first time by small-angle neutron scattering (SANS) and UV–visible spectroscopy to elucidate the aggregation behavior of the PZN molecules themselves and the state of living chain ends in a living polymer solution. PZN catalyst in deuterated tetrahydrofuran (thf-d8) showed SANS curves fitted by a form factor for a sphere whose radius Rs is larger (1.4–1.6 nm) than a single PZN molecule (0.65 nm), indicating formation of PZN aggregates in thf-d8. In a nonpolar solvent, benzene-d6, Rs was even larger (3.1 nm), indicating formation of larger aggregates. By adding IRG to PZN solution, an excess scattering appeared in the SANS profile and a strong band emerged in the UV–visible spectrum. This result indicates strong interaction of IRG with PZN not only on a molecular scale but also on a mesoscopic scale. The SANS profile from the living polymer solution in thf-d8 was observed to be fitted by the sum of the profile for the aggregated PZN/IRG complex and that for Gaussian chains of PMMA. The molecular weight of the PMMA determined by SANS, 2100 g mol−1, was in agreement with that estimated from gel-permeation chromatography, indicating that the anionic living chain ends and their counter ions (PZN) are dissociated in thf-d8; thus, the chains are not associated into multiple-ion pairs.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Living anionic polymerization of methyl meth­acrylate controlled by metal-free phosphazene catalyst as observed by small-angle neutron scattering, gel-permeation chromatography and UV–visible spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>568</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>572</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6019">
    <title>Study of ferrite ferrofluids by small-angle scattering of polarized neutrons</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6019</link>
    <description>Nanoparticles consisting of a magnetic core (Fe3O4, CoFe2O4 and CuFe2O4) and a hydrophobic shell were prepared by chemical co-precipitation of the inorganic cores and by subsequently modifying the surface with dodecanoic acid. The nanoparticles were then dispersed in cyclohexane to form stable ferrofluids. These dispersions were investigated by small-angle scattering of polarized neutrons and the data were interpreted according to a `pearl-necklace' model, opportunely modified to account for the core–shell structure of the particles. Results of the fitting show that the particles consist of a magnetic core with a mean radius of 40–50 Å and an organic shell with a thickness of 7–8 Å. These nanoparticles assemble in fractal aggregates when a magnetic field is applied.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Bonini, M.</dc:creator>
    <dc:creator>Wiedenmann, A.</dc:creator>
    <dc:creator>Baglioni, P.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009600</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>This work reports the synthesis and the characterization by small-angle scattering of polarized neutrons of ferrofluids consisting of ferrite nanoparticles coated by dodecanoic acid and dispersed in cyclohexane.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SANSPOL; FERROFLUIDS; MAGNETIC NANOPARTICLES; FRACTALS</dc:subject>
    <dc:description>Nanoparticles consisting of a magnetic core (Fe3O4, CoFe2O4 and CuFe2O4) and a hydrophobic shell were prepared by chemical co-precipitation of the inorganic cores and by subsequently modifying the surface with dodecanoic acid. The nanoparticles were then dispersed in cyclohexane to form stable ferrofluids. These dispersions were investigated by small-angle scattering of polarized neutrons and the data were interpreted according to a `pearl-necklace' model, opportunely modified to account for the core–shell structure of the particles. Results of the fitting show that the particles consist of a magnetic core with a mean radius of 40–50 Å and an organic shell with a thickness of 7–8 Å. These nanoparticles assemble in fractal aggregates when a magnetic field is applied.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Study of ferrite ferrofluids by small-angle scattering of polarized neutrons</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>254</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>258</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6033">
    <title>Biological small-angle X-ray scattering facility at the Stanford Synchrotron Radiation Laboratory</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6033</link>
    <description>Beamline 4-2 at the Stanford Synchrotron Radiation Laboratory is a small-angle X-ray scattering/diffraction facility dedicated to structural studies on mostly noncrystalline biological systems. The instrument consists of a pinhole camera, which covers the magnitude of the scattering vector Q in the range 0.004–1.3 Å−1 [Q = (4π/λ)sin θ, where θ and λ are one half of the scattering angle and the X-ray wavelength, respectively], and a Bonse–Hart geometry ultra-small-angle X-ray scattering setup for the Q range an order of magnitude smaller. The pinhole camera allows quick automated distance and detector selection among any combination of five distances and three position-sensitive detectors. The double-crystal monochromator can have either Si 111 crystals or a pair of synthetic multilayer diffractive elements for higher flux applications. We have adopted a suite of software originally developed for macromolecular crystallography for integrated beamline control as well as static and slow time-resolved small-angle scattering data collection. This article outlines recent technological developments and specialized instrumentation for conducting noncrystalline scattering experiments in structural biology at improved time and spatial resolutions.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Smolsky, I.L.</dc:creator>
    <dc:creator>Liu, P.</dc:creator>
    <dc:creator>Niebuhr, M.</dc:creator>
    <dc:creator>Ito, K.</dc:creator>
    <dc:creator>Weiss, T.M.</dc:creator>
    <dc:creator>Tsuruta, H.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009624</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Beamline 4-2 at the Stanford Synchrotron Radiation Laboratory is a small-angle X-ray scattering/diffraction facility dedicated to structural studies on mostly noncrystalline biological systems. This article outlines recent technological developments and specialized instrumentation for structural biology research at improved time and spatial resolutions.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SMALL-ANGLE SCATTERING; SYNCHROTRON RADIATION; SOLUTION SCATTERING; TIME-RESOLVED STUDIES</dc:subject>
    <dc:description>Beamline 4-2 at the Stanford Synchrotron Radiation Laboratory is a small-angle X-ray scattering/diffraction facility dedicated to structural studies on mostly noncrystalline biological systems. The instrument consists of a pinhole camera, which covers the magnitude of the scattering vector Q in the range 0.004–1.3 Å−1 [Q = (4π/λ)sin θ, where θ and λ are one half of the scattering angle and the X-ray wavelength, respectively], and a Bonse–Hart geometry ultra-small-angle X-ray scattering setup for the Q range an order of magnitude smaller. The pinhole camera allows quick automated distance and detector selection among any combination of five distances and three position-sensitive detectors. The double-crystal monochromator can have either Si 111 crystals or a pair of synthetic multilayer diffractive elements for higher flux applications. We have adopted a suite of software originally developed for macromolecular crystallography for integrated beamline control as well as static and slow time-resolved small-angle scattering data collection. This article outlines recent technological developments and specialized instrumentation for conducting noncrystalline scattering experiments in structural biology at improved time and spatial resolutions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Biological small-angle X-ray scattering facility at the Stanford Synchrotron Radiation Laboratory</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>453</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>458</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6013">
    <title>Small-angle light and X-ray scattering measurements of a protein–oligosaccharide complex mucin in solution</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6013</link>
    <description>The molecular assembly and the chain conformation of intact bovine submaxillary mucin (BSM) in solution over wide-ranging concentrations were characterized by using low-angle laser light scattering and small-angle X-ray scattering (SAXS) methods. The specific refractive index increment of BSM was estimated to be 0.152 ml g−1 and was used to determine the molecular weight of BSM by low-angle laser light scattering photometry combined with high-performance gel chromatography. The total molecular weight of BSM was 55 million and the molecular weight of the main fractionated components was about 2 million. Fractal analysis of the SAXS data revealed that the intact BSM molecule is a chain with excluded volume (fractal dimension 1.67) at concentrations of 1.4 and 3.6 mg ml−1 and a chain with a Gaussian chain character (fractal dimension 2) at concentrations of 7.2–15 mg ml−1. Moreover, the Kratky plots of the SAXS data showed that the chain conformation of BSM molecules is a Gaussian (unfolded) structure in solution. The estimated cross-sectional radius of gyration value lay in the range 0.65–0.76 nm, which is reasonable for a long thin shape.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Watanabe, Y.</dc:creator>
    <dc:creator>Inoko, Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009247</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The molecular assembly and chain conformation of a glycoprotein mucin are characterized by using small-angle scattering methods.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>LOW-ANGLE LASER LIGHT SCATTERING; SAXS; MUCINS; GLYCOPROTEINS; BOVINE SUBMAXILLARY MUCIN</dc:subject>
    <dc:description>The molecular assembly and the chain conformation of intact bovine submaxillary mucin (BSM) in solution over wide-ranging concentrations were characterized by using low-angle laser light scattering and small-angle X-ray scattering (SAXS) methods. The specific refractive index increment of BSM was estimated to be 0.152 ml g−1 and was used to determine the molecular weight of BSM by low-angle laser light scattering photometry combined with high-performance gel chromatography. The total molecular weight of BSM was 55 million and the molecular weight of the main fractionated components was about 2 million. Fractal analysis of the SAXS data revealed that the intact BSM molecule is a chain with excluded volume (fractal dimension 1.67) at concentrations of 1.4 and 3.6 mg ml−1 and a chain with a Gaussian chain character (fractal dimension 2) at concentrations of 7.2–15 mg ml−1. Moreover, the Kratky plots of the SAXS data showed that the chain conformation of BSM molecules is a Gaussian (unfolded) structure in solution. The estimated cross-sectional radius of gyration value lay in the range 0.65–0.76 nm, which is reasonable for a long thin shape.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle light and X-ray scattering measurements of a protein–oligosaccharide complex mucin in solution</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>209</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>212</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6030">
    <title>New two-dimensional data treatment software for small-angle scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6030</link>
    <description>A new program is presented which performs data treatment in one, two or three dimensions. While one-dimensional data treatment can be performed easily by many programs (canSAS, EMBL, ISIS, ILL, NIST), few deal efficiently with more dimensions. Indeed, specific attention has to be paid to the selection of the relevant data. Their display and models are relatively complex. This new program has been developed according to the needs of small-angle scattering users, but is not limited to these fields. Its original purpose was to model forward anisotropic scattering and diffuse scattering typically produced by large structures such as polymers, aggregates, self-assembly systems or micellar solutions. It is also suited to modelling Bragg scattering. With time, many filter configurations (rectangles or sectors, with possible symmetries and display along various coordinates) and many model functions (centred or not, possibly with cofactors, with Cartesian, polar, or three-dimensional coordinates) have been added. Models are fitted by the steepest descent model with χ2 as the minimization function. The software is written in Fortran with the PGPLOT graphics package. It runs with the Windows operating system.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Pépy, G.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009314</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A description is given of a new interactive data-treatment program which was mostly developed to analyse two-dimensional small-angle data files. The treatment process is described through specific menus. Several examples show the most useful characteristics of this software.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DATA TREATMENT; TWO-DIMENSIONAL DATA; SMALL-ANGLE SCATTERING; SOFTWARE</dc:subject>
    <dc:description>A new program is presented which performs data treatment in one, two or three dimensions. While one-dimensional data treatment can be performed easily by many programs (canSAS, EMBL, ISIS, ILL, NIST), few deal efficiently with more dimensions. Indeed, specific attention has to be paid to the selection of the relevant data. Their display and models are relatively complex. This new program has been developed according to the needs of small-angle scattering users, but is not limited to these fields. Its original purpose was to model forward anisotropic scattering and diffuse scattering typically produced by large structures such as polymers, aggregates, self-assembly systems or micellar solutions. It is also suited to modelling Bragg scattering. With time, many filter configurations (rectangles or sectors, with possible symmetries and display along various coordinates) and many model functions (centred or not, possibly with cofactors, with Cartesian, polar, or three-dimensional coordinates) have been added. Models are fitted by the steepest descent model with χ2 as the minimization function. The software is written in Fortran with the PGPLOT graphics package. It runs with the Windows operating system.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>New two-dimensional data treatment software for small-angle scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>433</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>438</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6024">
    <title>Multiple-length-scale small-angle X-ray scattering analysis on maghemite nanocomposites</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6024</link>
    <description>Small-angle X-ray scattering (SAXS) analysis has been performed on maghemite–poly(4-vinylpyridine) nanocomposites prepared by in situ precipitation from iron–polymer coordination compounds. According to electron microscopy observations, the nanocomposites contain isolated spherical particles with a narrow size distribution, uniformly distributed throughout the polymer matrix. The scattering intensity of nanocomposites has relevant contributions from both the polymer and the nanocomposites, showing features characteristic of multiscale structured systems, namely two power laws and a Guinier regime. The data have been analysed in terms of Beaucage's unified approach and it is found that the maghemite particle size increases with the iron/polymer weight ratio used in the preparation of the nanocomposites. SAXS curves also feature a bump that was analysed as arising from a second particle population or from interactions. Magnetization and transmission electron microscopy results give arguments favouring the latter interpretation. It is found that the maghemite particle sizes vary linearly with the iron weight ratio used in the preparation of the nanocomposites.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Millan, A.</dc:creator>
    <dc:creator>Urtizberea, A.</dc:creator>
    <dc:creator>Silva, N.J.O.</dc:creator>
    <dc:creator>Boesecke, P.</dc:creator>
    <dc:creator>Natividad, E.</dc:creator>
    <dc:creator>Palacio, F.</dc:creator>
    <dc:creator>Snoeck, E.</dc:creator>
    <dc:creator>Soriano, L.</dc:creator>
    <dc:creator>Gutiérrez, A.</dc:creator>
    <dc:creator>Quirós, C.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009387</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>We report small-angle X-ray scattering analysis of maghemite polymer nanocomposites containing spherical particles uniformly distributed in the polymer matrix. Scattering intensity curves show features characteristic of multiscale structured systems. Based on the Beaucage approach, we conclude that the nanoparticle size increases with the iron loading used in the preparation of the nanocomposite.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SMALL-ANGLE X-RAY SCATTERING; NANOCOMPOSITES; NANOPARTICLES; MAGHEMITE</dc:subject>
    <dc:description>Small-angle X-ray scattering (SAXS) analysis has been performed on maghemite–poly(4-vinylpyridine) nanocomposites prepared by in situ precipitation from iron–polymer coordination compounds. According to electron microscopy observations, the nanocomposites contain isolated spherical particles with a narrow size distribution, uniformly distributed throughout the polymer matrix. The scattering intensity of nanocomposites has relevant contributions from both the polymer and the nanocomposites, showing features characteristic of multiscale structured systems, namely two power laws and a Guinier regime. The data have been analysed in terms of Beaucage's unified approach and it is found that the maghemite particle size increases with the iron/polymer weight ratio used in the preparation of the nanocomposites. SAXS curves also feature a bump that was analysed as arising from a second particle population or from interactions. Magnetization and transmission electron microscopy results give arguments favouring the latter interpretation. It is found that the maghemite particle sizes vary linearly with the iron weight ratio used in the preparation of the nanocomposites.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Multiple-length-scale small-angle X-ray scattering analysis on maghemite nanocomposites</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>696</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>700</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6010">
    <title>Initial process of amyloid formation of apomyoglobin and effect of glycosphingolipid GM1</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6010</link>
    <description>Using small-angle and wide-angle X-ray scattering techniques it has been possible to clarify the helix-to-sheet (cross-β) transition and the stacking process of the cross-β sheet of apomyoglobin as a model for amyloid. The present results indicate that the cross-β formation and the pleated sheet stacking start concurrently and that the stacking continues progressively after the saturation of the cross-β formation. The effect of glycosphingolipids on the above processes has also been studied. At high molar ratio of glycosphingolipid to apomyoglobin the growth of the amyloid is suppressed.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Onai, T.</dc:creator>
    <dc:creator>Koizumi, M.</dc:creator>
    <dc:creator>Lu, H.</dc:creator>
    <dc:creator>Inoue, K.</dc:creator>
    <dc:creator>Hirai, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009211</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Using small-angle and wide-angle X-ray scattering techniques it has been possible to clarify the helix-to-sheet (cross-β) transition and the stacking process of the cross-β sheet of apomyoglobin as a model for amyloid.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>APOMYOGLOBIN; AMYLOID; GANGLIOSIDE</dc:subject>
    <dc:description>Using small-angle and wide-angle X-ray scattering techniques it has been possible to clarify the helix-to-sheet (cross-β) transition and the stacking process of the cross-β sheet of apomyoglobin as a model for amyloid. The present results indicate that the cross-β formation and the pleated sheet stacking start concurrently and that the stacking continues progressively after the saturation of the cross-β formation. The effect of glycosphingolipids on the above processes has also been studied. At high molar ratio of glycosphingolipid to apomyoglobin the growth of the amyloid is suppressed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Initial process of amyloid formation of apomyoglobin and effect of glycosphingolipid GM1</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>184</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>189</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6015">
    <title>Small-angle X-ray and small-angle neutron scattering investigations of colloidal dispersions of magnetic nanoparticles and clay nanoplatelets</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6015</link>
    <description>We investigated mixed colloidal dispersions of clay platelets and magnetic nanoparticles using small-angle X-ray and neutron scattering. Our results show that the contribution to the scattering is essentially due to the magnetic nanoparticles. The scattering intensities are proportional to the concentration of magnetic particles, indicating that from the scattering point of view the sample is a colloidal dispersion of non-interacting magnetic objects, although the laponite and magnetic particles clearly interact when the sample textures are observed in an optical microscope. The visually observed phase separation may be characterized as a liquid–gas transition.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Paula, F.L.O.</dc:creator>
    <dc:creator>Aquino, R.</dc:creator>
    <dc:creator>da Silva, G.J.</dc:creator>
    <dc:creator>Depeyrot, J.</dc:creator>
    <dc:creator>Tourinho, F.A.</dc:creator>
    <dc:creator>Fossum, J.O.</dc:creator>
    <dc:creator>Knudsen, K.D.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009181</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Mixed colloidal dispersions of clay platelets and magnetic nanoparticles were investigated using small-angle X-ray and neutron scattering. The main contribution to the scattering is due to the magnetic nanoparticles. The scattering intensities are proportional to the concentration of magnetic particles, thus from the scattering point of view the sample is a colloidal dispersion of non-interacting magnetic objects, although the laponite and magnetic particles clearly interact when the sample textures are observed in an optical microscope. The phase separation may be characterized as a liquid–gas transition.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FERROFLUIDS; CLAYS; NANOPARTICLES; COMPOSITE MATERIALS; SAXS; SANS</dc:subject>
    <dc:description>We investigated mixed colloidal dispersions of clay platelets and magnetic nanoparticles using small-angle X-ray and neutron scattering. Our results show that the contribution to the scattering is essentially due to the magnetic nanoparticles. The scattering intensities are proportional to the concentration of magnetic particles, indicating that from the scattering point of view the sample is a colloidal dispersion of non-interacting magnetic objects, although the laponite and magnetic particles clearly interact when the sample textures are observed in an optical microscope. The visually observed phase separation may be characterized as a liquid–gas transition.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle X-ray and small-angle neutron scattering investigations of colloidal dispersions of magnetic nanoparticles and clay nanoplatelets</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>269</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>273</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6012">
    <title>Measurement of self-diffusion constant with two-dimensional X-ray photon correlation spectroscopy</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6012</link>
    <description>The X-ray photon correlation spectroscopy technique probes the slow dynamics of disordered materials, overcoming the limitations of using photon correlation spectroscopy with coherent visible light. It extends the accessible range of the modulus of the scattering vector to short wavelength density fluctuations and is not sensitive to multiple scattering. We measure here experimentally the short-time self-diffusion coefficient D_{\rm S} of a charge-stabilized colloidal dispersion. It is in contradiction with theoretical models including many-body hydrodynamic interactions.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Robert, A.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009168</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Two-dimensional XPCS allows the dynamics of large wavectors in materials opaque to visible light to be probed. The self-diffusion constant of a colloidal dispersion is probed and compared with available models.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>XPCS; COLLOIDS; SELF DIFFUSION; DENSITY FLUCTUATIONS</dc:subject>
    <dc:description>The X-ray photon correlation spectroscopy technique probes the slow dynamics of disordered materials, overcoming the limitations of using photon correlation spectroscopy with coherent visible light. It extends the accessible range of the modulus of the scattering vector to short wavelength density fluctuations and is not sensitive to multiple scattering. We measure here experimentally the short-time self-diffusion coefficient D_{\rm S} of a charge-stabilized colloidal dispersion. It is in contradiction with theoretical models including many-body hydrodynamic interactions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Measurement of self-diffusion constant with two-dimensional X-ray photon correlation spectroscopy</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>34</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>37</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6004">
    <title>The dynamic behavior of magnetic colloids in suspension</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6004</link>
    <description>The dynamic behavior of magnetic colloidal particles in suspension is investigated. The particles of the core–shell colloid consist of a cobalt ferrite core embedded in a silica shell and are stabilized by surface charges. As the suspension is strongly opaque to visible light, it can not be probed by dynamic light scattering techniques as a result of strong multiple scattering as well as absorption effects. Therefore, the static and dynamic behavior is probed with small-angle X-ray scattering and X-ray photon correlation spectroscopy (XPCS), respectively. Using XPCS, we are able to study the diffusion coefficient of an opaque colloidal system as a function of the scattering vector. In this paper, we report on the behavior of the colloidal system in the absence of an external magnetic field, meaning that the magnetic moments of the particles are oriented randomly. We find no evidence for magnetic interactions in the static data, while the dynamic XPCS data deviate very significantly from the predictions of model calculations.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Autenrieth, T.</dc:creator>
    <dc:creator>Robert, A.</dc:creator>
    <dc:creator>Wagner, J.</dc:creator>
    <dc:creator>Grübel, G.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807009016</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The short-time diffusion of a magnetic charge-stabilized colloidal suspension in the absence of an external applied magnetic field has been investigated by means of X-ray photon correlation spectroscopy.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MAGNETIC CORE-SHELL COLLOIDS; HYDRODYNAMIC INTERACTIONS; X-RAY PHOTON CORRELATION SPECTROSCOPY</dc:subject>
    <dc:description>The dynamic behavior of magnetic colloidal particles in suspension is investigated. The particles of the core–shell colloid consist of a cobalt ferrite core embedded in a silica shell and are stabilized by surface charges. As the suspension is strongly opaque to visible light, it can not be probed by dynamic light scattering techniques as a result of strong multiple scattering as well as absorption effects. Therefore, the static and dynamic behavior is probed with small-angle X-ray scattering and X-ray photon correlation spectroscopy (XPCS), respectively. Using XPCS, we are able to study the diffusion coefficient of an opaque colloidal system as a function of the scattering vector. In this paper, we report on the behavior of the colloidal system in the absence of an external magnetic field, meaning that the magnetic moments of the particles are oriented randomly. We find no evidence for magnetic interactions in the static data, while the dynamic XPCS data deviate very significantly from the predictions of model calculations.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The dynamic behavior of magnetic colloids in suspension</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>250</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>253</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6009">
    <title>Structural characterization of N-lignoceroyl (C24:0) sphingomyelin bilayer membranes: a re-evaluation</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6009</link>
    <description>Sphingomyelin (SM) is a membrane lipid and plays important roles in signaling, protein trafficking, cell growth and death. The structure of the bilayer of a hydrated highly asymmetric SM, N-lignoceroyl (C24:0) SM, has been investigated with X-ray diffraction (XRD), simultaneous small-angle X-ray scattering (SAXS), wide-angle XRD and SAXS. At temperatures between two endothermic transitions of hydrated C24:0 SM bilayers, the C24:0 SM formed a ripple phase with the ripple periodicity of ~12–14 nm. At about three months incubation at 277 K, the formation of a stable phase with a short lamellar spacing of 5.62 nm was induced. Based upon the structures revealed by this study and the phase behavior, intermolecular interactions between C24:0 SM molecules in the bilayer membrane are discussed.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Takahashi, H.</dc:creator>
    <dc:creator>Hayakawa, T.</dc:creator>
    <dc:creator>Kawasaki, Y.</dc:creator>
    <dc:creator>Ito, K.</dc:creator>
    <dc:creator>Fujisawa, T.</dc:creator>
    <dc:creator>Kodama, M.</dc:creator>
    <dc:creator>Kobayashi, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S002188980700859X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Sphingomyelin is one of the major sphingolipid components of many animal plasma membranes. SAXS and XRD studies revealed that N-lignocerol (C24:0) sphingomyelin bilayers have a ripple phase and an additional low-temperature stable phase.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; XRD; LAMELLAR STRUCTURE; ELECTRON DENSITY PROFILE; RIPPLE PHASE; STABLE PHASE</dc:subject>
    <dc:description>Sphingomyelin (SM) is a membrane lipid and plays important roles in signaling, protein trafficking, cell growth and death. The structure of the bilayer of a hydrated highly asymmetric SM, N-lignoceroyl (C24:0) SM, has been investigated with X-ray diffraction (XRD), simultaneous small-angle X-ray scattering (SAXS), wide-angle XRD and SAXS. At temperatures between two endothermic transitions of hydrated C24:0 SM bilayers, the C24:0 SM formed a ripple phase with the ripple periodicity of ~12–14 nm. At about three months incubation at 277 K, the formation of a stable phase with a short lamellar spacing of 5.62 nm was induced. Based upon the structures revealed by this study and the phase behavior, intermolecular interactions between C24:0 SM molecules in the bilayer membrane are discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structural characterization of N-lignoceroyl (C24:0) sphingomyelin bilayer membranes: a re-evaluation</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>312</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>317</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6013">
    <title>Mesoscopic structure of dry-pressed clay samples from small-angle X-ray scattering measurements</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6013</link>
    <description>Weakly hydrated samples of platelet-shaped nano-particles obtained by dry-pressing suspensions of the synthetic Na fluorohectorite clay are studied. The particles consist of stacks of several tens of 1 nm-thick nanosilicate platelets. They form a compound of quasi-two-dimensional particles whose average director is aligned with the direction of the uniaxial stress applied at dehydration. Small-angle X-ray scattering images from these samples are either isotropic or anisotropic, depending on the sample orientation with respect to the X-ray beam. From anisotropic images, changes in the scattering objects' orientation distribution probability (ODP) function are investigated as the temperature is lowered, thus triggering swelling of the individual particles by water intercalation. This is done, on the one hand, by inferring the width of the ODP function from the eccentricity of quasi-elliptic iso-intensity cuts of the small-angle scattering images, and, on the other hand, by obtaining the ODP function from azimuthal profiles of the images. The decays of the scattering intensity as a function of momentum transfer along the two principal directions of the images exhibit power law behaviors. A crossover scale between two power law regimes is observed on the profiles recorded along the horizontal axis; it corresponds to the typical pore size along the direction of the initially applied load. These results are compared with a previous study of similar systems.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Méheust, Y.</dc:creator>
    <dc:creator>Dagois-Bohy, S.</dc:creator>
    <dc:creator>Knudsen, K.D.</dc:creator>
    <dc:creator>Fossum, J.O.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807008552</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Small-angle X-ray scattering is used to investigate the meso-structure of dry-pressed samples of nano-layered platelet-shaped clay particles, as water is absorbed into individual particles. The orientational order of the assembly is nematic. Orientation distributions are monitored and show a moderate decrease of this order with water uptake.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>NEMATIC ORDER; PLATELETS; SAXS; ANISOTROPY; WATER ABSORPTION</dc:subject>
    <dc:description>Weakly hydrated samples of platelet-shaped nano-particles obtained by dry-pressing suspensions of the synthetic Na fluorohectorite clay are studied. The particles consist of stacks of several tens of 1 nm-thick nanosilicate platelets. They form a compound of quasi-two-dimensional particles whose average director is aligned with the direction of the uniaxial stress applied at dehydration. Small-angle X-ray scattering images from these samples are either isotropic or anisotropic, depending on the sample orientation with respect to the X-ray beam. From anisotropic images, changes in the scattering objects' orientation distribution probability (ODP) function are investigated as the temperature is lowered, thus triggering swelling of the individual particles by water intercalation. This is done, on the one hand, by inferring the width of the ODP function from the eccentricity of quasi-elliptic iso-intensity cuts of the small-angle scattering images, and, on the other hand, by obtaining the ODP function from azimuthal profiles of the images. The decays of the scattering intensity as a function of momentum transfer along the two principal directions of the images exhibit power law behaviors. A crossover scale between two power law regimes is observed on the profiles recorded along the horizontal axis; it corresponds to the typical pore size along the direction of the initially applied load. These results are compared with a previous study of similar systems.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Mesoscopic structure of dry-pressed clay samples from small-angle X-ray scattering measurements</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>286</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>291</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6021">
    <title>Structural development of dynamically asymmetric polymer blends under uniaxial stretching</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6021</link>
    <description>The time-resolved small-angle X-ray scattering technique was used to investigate the structural change during uniaxial stretching of dynamically asymmetric polymer blends irradiated by an electron beam. The concentration fluctuations were enhanced by stretching and became large in particular along the direction of deformation. In the early stages of the stretch-induced enhancement of concentration fluctuations, the growth rate of their q-Fourier mode was found to have a maximum at a certain value of q [= (4π/λ)sin(θ/2), where θ and λ are the scattering angle and the wavelength of the X-rays, respectively]. A dominant mode in the enhancement of concentration fluctuations exists in the initial stage, like the early stage of spinodal decomposition for fluid mixtures. The viscoelastic effects of the growth rate were taken into consideration, so that for blends irradiated by an electron beam, elastic effects are found to significantly suppress the growth rate of concentration fluctuations at small wavenumbers.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Takeno, H.</dc:creator>
    <dc:creator>Uehara, H.</dc:creator>
    <dc:creator>Murakami, S.</dc:creator>
    <dc:creator>Takenaka, M.</dc:creator>
    <dc:creator>Kim, M.I.</dc:creator>
    <dc:creator>Nagasawa, N.</dc:creator>
    <dc:creator>Sasaki, S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807008497</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The structural change during uniaxial stretching was investigated by use of time-resolved small-angle X-ray scattering for dynamically asymmetric polymer blends irradiated by an electron beam. A dominant mode at the early stage of the stretch-induced enhancement of concentration fluctuations exists, similar to early stage spinodal decomposition for fluid mixtures.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLYMER BLENDS; DYNAMICAL ASYMMETRY; UNIAXIAL STRETCHING; SAXS</dc:subject>
    <dc:description>The time-resolved small-angle X-ray scattering technique was used to investigate the structural change during uniaxial stretching of dynamically asymmetric polymer blends irradiated by an electron beam. The concentration fluctuations were enhanced by stretching and became large in particular along the direction of deformation. In the early stages of the stretch-induced enhancement of concentration fluctuations, the growth rate of their q-Fourier mode was found to have a maximum at a certain value of q [= (4π/λ)sin(θ/2), where θ and λ are the scattering angle and the wavelength of the X-rays, respectively]. A dominant mode in the enhancement of concentration fluctuations exists in the initial stage, like the early stage of spinodal decomposition for fluid mixtures. The viscoelastic effects of the growth rate were taken into consideration, so that for blends irradiated by an electron beam, elastic effects are found to significantly suppress the growth rate of concentration fluctuations at small wavenumbers.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structural development of dynamically asymmetric polymer blends under uniaxial stretching</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>656</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>661</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6008">
    <title>Chloride-ion concentration dependence of molecular dimension in the acid-denatured state of equine β-lactoglobulin</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6008</link>
    <description>The chloride-ion concentration dependence of the molecular dimension in the acid-denatured state of equine β-lactoglobulin (ELG) was investigated by small-angle X-ray scattering. In the presence of chloride ion, ELG has a globular and compact conformation (the A state). The molecular dimension of ELG increases little with decreasing chloride-ion concentration. A remarkable dependence was observed for a mutant protein in which both Cys66 and Cys160 were replaced with Ala (C66A/C160A). In the presence of chloride ion, C66A/C160A has a globular and compact conformation, like the wild type. In the absence of chloride ion, however, the molecular dimension and shape was close to that in the urea-unfolded state. Previously, we have shown that the helix content in the acid-denatured state increases with decreasing chloride-ion concentration [Yamada et al. (2006). Proteins Struct. Funct. Bioinf. 63, 595–602]. These results suggest that the secondary structure in the A state is mainly determined by non-local interactions. When they are absent in an expanded conformation, the local interactions become predominant and the amount of non-native α-helix increases.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Yamada, Y.</dc:creator>
    <dc:creator>Yajima, T.</dc:creator>
    <dc:creator>Tsukamoto, S.</dc:creator>
    <dc:creator>Nakagawa, K.</dc:creator>
    <dc:creator>Fujiwara, K.</dc:creator>
    <dc:creator>Kihara, H.</dc:creator>
    <dc:creator>Ikeguchi, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807008278</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The chloride-ion concentration dependence of the molecular shape in the acid-denatured state of equine β-lactoglobulin was observed by small-angle X-ray scattering. The results indicated that the compact molten globule is transformed to an expanded conformation with decreasing chloride-ion concentration. Interestingly, this change accompanied the increase in the helix content as measured by circular dichroic spectra.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MOLTEN GLOBULE; SMALL-ANGLE X-RAY SCATTERING; DISULFIDE BOND; [BETA]-LACTOGLOBULIN</dc:subject>
    <dc:description>The chloride-ion concentration dependence of the molecular dimension in the acid-denatured state of equine β-lactoglobulin (ELG) was investigated by small-angle X-ray scattering. In the presence of chloride ion, ELG has a globular and compact conformation (the A state). The molecular dimension of ELG increases little with decreasing chloride-ion concentration. A remarkable dependence was observed for a mutant protein in which both Cys66 and Cys160 were replaced with Ala (C66A/C160A). In the presence of chloride ion, C66A/C160A has a globular and compact conformation, like the wild type. In the absence of chloride ion, however, the molecular dimension and shape was close to that in the urea-unfolded state. Previously, we have shown that the helix content in the acid-denatured state increases with decreasing chloride-ion concentration [Yamada et al. (2006). Proteins Struct. Funct. Bioinf. 63, 595–602]. These results suggest that the secondary structure in the A state is mainly determined by non-local interactions. When they are absent in an expanded conformation, the local interactions become predominant and the amount of non-native α-helix increases.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Chloride-ion concentration dependence of molecular dimension in the acid-denatured state of equine β-lactoglobulin</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>213</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>216</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6029">
    <title>Effect of cations on the structure of sodium bis(2-ethylhexyl)sulfosuccinate water-in-oil microemulsion</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6029</link>
    <description>We have characterized the structure of water/sodium bis(2-ethylhexyl)sulfosuccinate (AOT)/isooctane water-in-oil microemulsion depending on the concentrations of monovalent and divalent cations (Na+, K+, Ca2+) in the water pool. We have found that the presence of salts affects the microemulsion structures differently at low and high water contents. Increasing the salt concentration suppresses the oligomerization of the microemulsions at low water content, whereas it reduces the microemulsion radius at high water content. The present results clearly indicate that not only electrostatic repulsion between AOT headgroups but also negative or positive hydration effects by salts dominate the structure and dynamics of AOT microemulsions, as suggested by a recent molecular dynamics simulation.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Kawai-Hirai, R.</dc:creator>
    <dc:creator>Hirai, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807008151</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The structure and oligomerization of sodium bis(2-ethylhexyl)sulfosuccinate water-in-oil microemulsion under the presence of monovalent and divalent salts in the water pool are dominated not only by the electrostatic effect between polar headgroups but also by the hydration effect by salts.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MICROEMULSIONS; AOT; CATIONS; SALTS; SODIUM BIS(2-ETHYLHEXYL)SULFOSUCCINATE</dc:subject>
    <dc:description>We have characterized the structure of water/sodium bis(2-ethylhexyl)sulfosuccinate (AOT)/isooctane water-in-oil microemulsion depending on the concentrations of monovalent and divalent cations (Na+, K+, Ca2+) in the water pool. We have found that the presence of salts affects the microemulsion structures differently at low and high water contents. Increasing the salt concentration suppresses the oligomerization of the microemulsions at low water content, whereas it reduces the microemulsion radius at high water content. The present results clearly indicate that not only electrostatic repulsion between AOT headgroups but also negative or positive hydration effects by salts dominate the structure and dynamics of AOT microemulsions, as suggested by a recent molecular dynamics simulation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Effect of cations on the structure of sodium bis(2-ethylhexyl)sulfosuccinate water-in-oil microemulsion</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>274</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>278</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6026">
    <title>Time-resolved grazing-incidence small-angle X-ray scattering studies of lipid multibilayers with the insertion of amyloid peptide during the swelling process</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6026</link>
    <description>The β-amyloid peptide (Aβ) (1–40) is one of the major components that form Alzheimer's amyloid deposits. Studies of the membrane insertion of amyloid showed that amyloid is surface active and can insert into lipid monolayers [Ji et al. (2002). Biochemistry (Moscow), 67, 1283–1288; Ege &amp; Lee (2004). Biophys. J. 87, 1732–1740]. The interaction between the peptide and a lipid monolayer or bilayer is critical to the understanding of the formation of amyloid peptide deposits on the membrane. In this paper, we have studied the structural transition of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) multibilayers with the insertion of amyloid peptide 1–40 by grazing-incidence small-angle X-ray scattering at different bilayer hydration levels (changing the relatively humidity). We mixed the DPPC and amyloid peptide in an organic solvent at a 10 to 1 weight ratio, then cast it onto a silicon wafer to form the mixed lipid multibilayer film. In this study of the pure DPPC multibilayer film and the DPPC multibilayer film inserted with amyloid peptide, it was found that the hydration process was bimodal with a better-hydrated top layer and a less-hydrated bottom layer. The gel-to-ripple phase transition suffers a strong confinement effect due to the presence of the solid substrate. With the insertion of the amyloid peptide, the ripple phase of the membrane bilayers was suppressed at high humidity and the whole film can be swollen more uniformly at lower incubation time than the pure DPPC film supported on a silicon wafer. This means water vapor can penetrate more easily into the DPPC bilayers inserted with Aβ than into the pure DPPC bilayers. Amyloid peptides were found to form clusters in the bilayer and possess in-plane correlation. From analyzing the diffuse scattering around the Bragg peak in the lateral direction, the amyloid peptides are found to form clusters in the bilayer with a radius of about 9 nm. It is also estimated that the number of Aβ molecules in one cluster is about 12 and on average each Aβ molecule occupies an interface area of about 22 nm2. As the relative humidity exceeds about 94%, the Aβ clusters seem to develop an ordered structure with a spacing of about 300 Å.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Lin, J.-M.</dc:creator>
    <dc:creator>Lin, T.-L.</dc:creator>
    <dc:creator>Jeng, U.-S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807008199</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The structural transition of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) multibilayers with the insertion of amyloid peptide 1–40 was studied by grazing-incidence small-angle X-ray scattering at different bilayer hydration levels. With the insertion of the amyloid peptide, the ripple phase of the membrane bilayers was suppressed at high humidity and the whole film can be swollen more uniformly at lower incubation time than the pure DPPC film supported on a silicon wafer.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>GISAXS; DPPC MULTIBILAYER FILMS; AMYLOID PEPTIDE; MEMBRANE SWELLING</dc:subject>
    <dc:description>The β-amyloid peptide (Aβ) (1–40) is one of the major components that form Alzheimer's amyloid deposits. Studies of the membrane insertion of amyloid showed that amyloid is surface active and can insert into lipid monolayers [Ji et al. (2002). Biochemistry (Moscow), 67, 1283–1288; Ege &amp; Lee (2004). Biophys. J. 87, 1732–1740]. The interaction between the peptide and a lipid monolayer or bilayer is critical to the understanding of the formation of amyloid peptide deposits on the membrane. In this paper, we have studied the structural transition of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) multibilayers with the insertion of amyloid peptide 1–40 by grazing-incidence small-angle X-ray scattering at different bilayer hydration levels (changing the relatively humidity). We mixed the DPPC and amyloid peptide in an organic solvent at a 10 to 1 weight ratio, then cast it onto a silicon wafer to form the mixed lipid multibilayer film. In this study of the pure DPPC multibilayer film and the DPPC multibilayer film inserted with amyloid peptide, it was found that the hydration process was bimodal with a better-hydrated top layer and a less-hydrated bottom layer. The gel-to-ripple phase transition suffers a strong confinement effect due to the presence of the solid substrate. With the insertion of the amyloid peptide, the ripple phase of the membrane bilayers was suppressed at high humidity and the whole film can be swollen more uniformly at lower incubation time than the pure DPPC film supported on a silicon wafer. This means water vapor can penetrate more easily into the DPPC bilayers inserted with Aβ than into the pure DPPC bilayers. Amyloid peptides were found to form clusters in the bilayer and possess in-plane correlation. From analyzing the diffuse scattering around the Bragg peak in the lateral direction, the amyloid peptides are found to form clusters in the bilayer with a radius of about 9 nm. It is also estimated that the number of Aβ molecules in one cluster is about 12 and on average each Aβ molecule occupies an interface area of about 22 nm2. As the relative humidity exceeds about 94%, the Aβ clusters seem to develop an ordered structure with a spacing of about 300 Å.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Time-resolved grazing-incidence small-angle X-ray scattering studies of lipid multibilayers with the insertion of amyloid peptide during the swelling process</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>367</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>372</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6005">
    <title>Small-angle X-ray scattering investigation of water droplets in mist</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6005</link>
    <description>Small-angle X-ray scattering measurements of water droplets in a mist were carried out using the BL15XU beamline at SPring-8. The diameter of the water droplets generated by ultrasonic atomization was found to be ≥ 50 nm and had no distribution in the range under 50 nm, as predicted. The study also showed how difficult it is to measure the small-angle scattering of low-density materials, such as liquid droplets in a mist.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Yano, Y.F.</dc:creator>
    <dc:creator>Matsuura, K.</dc:creator>
    <dc:creator>Fukazu, T.</dc:creator>
    <dc:creator>Abe, F.</dc:creator>
    <dc:creator>Wakisaka, A.</dc:creator>
    <dc:creator>Kobara, H.</dc:creator>
    <dc:creator>Kaneko, K.</dc:creator>
    <dc:creator>Kumagai, A.</dc:creator>
    <dc:creator>Katsuya, Y.</dc:creator>
    <dc:creator>Okui, M.</dc:creator>
    <dc:creator>Tanaka, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807008138</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Small-angle X-ray scattering measurements of water droplets in a mist were carried out using the BL15XU beamline at SPring-8.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; LIQUID DROPLETS; MIST; FLOW CELL; ULTRASONIC ATOMIZATION</dc:subject>
    <dc:description>Small-angle X-ray scattering measurements of water droplets in a mist were carried out using the BL15XU beamline at SPring-8. The diameter of the water droplets generated by ultrasonic atomization was found to be ≥ 50 nm and had no distribution in the range under 50 nm, as predicted. The study also showed how difficult it is to measure the small-angle scattering of low-density materials, such as liquid droplets in a mist.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle X-ray scattering investigation of water droplets in mist</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>318</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>320</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6025">
    <title>Small-angle scattering investigations of magnesium hydride used as a hydrogen storage material</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6025</link>
    <description>In this work, high-energy ball-milled magnesium hydride samples used for hydrogen storage are investigated using small- and ultra-small-angle neutron scattering (SANS) as well as small-angle X-ray scattering (SAXS). Size distributions of inhomogeneities with dimensions from 10 Å up to more than 10 µm, corresponding to crystallite and particle sizes obtained by X-ray diffraction and electron microscopy, are determined as a function of milling time, milling tool material and added metal oxide catalysts in order to study the influence of the microstructure on the sorption kinetics. Significant changes of the volume fraction distributions are found for samples containing the catalyst chromium oxide, particularly when the catalyst particles are nanometre-sized. Cr2O3 is an effective agent for breaking up particles during the milling process. The comparison of SANS and SAXS curves give some of the first information about the distribution of hydrogen-containing structures. Using anomalous small-angle X-ray scattering, an energy-dependent scattering is found for an MgHx sample with 1 mol% Fe2O3. From the separated scattering curve a size distribution of hard spheres is obtained with a size range which is expected for crystallite and particle sizes of the Fe2O3 catalyst. Chemical shifts in the absorption spectra give information about the stability of the metal oxide catalysts during the milling process.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Pranzas, P.K.</dc:creator>
    <dc:creator>Dornheim, M.</dc:creator>
    <dc:creator>Boesenberg, U.</dc:creator>
    <dc:creator>Ares Fernandez, J.R.</dc:creator>
    <dc:creator>Goerigk, G.</dc:creator>
    <dc:creator>Roth, S.V.</dc:creator>
    <dc:creator>Gehrke, R.</dc:creator>
    <dc:creator>Schreyer, A.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807008023</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Structural changes in magnesium hydride with and without metal oxide catalysts are characterized using small- and ultra-small-angle neutron scattering, small-angle X-ray scattering, X-ray diffraction and electron microscopy in order to analyse the relation between structure and hydrogen sorption kinetics.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>METAL HYDRIDES; MGH2; HYDROGEN STORAGE; SANS; USANS; SAXS; ASAXS</dc:subject>
    <dc:description>In this work, high-energy ball-milled magnesium hydride samples used for hydrogen storage are investigated using small- and ultra-small-angle neutron scattering (SANS) as well as small-angle X-ray scattering (SAXS). Size distributions of inhomogeneities with dimensions from 10 Å up to more than 10 µm, corresponding to crystallite and particle sizes obtained by X-ray diffraction and electron microscopy, are determined as a function of milling time, milling tool material and added metal oxide catalysts in order to study the influence of the microstructure on the sorption kinetics. Significant changes of the volume fraction distributions are found for samples containing the catalyst chromium oxide, particularly when the catalyst particles are nanometre-sized. Cr2O3 is an effective agent for breaking up particles during the milling process. The comparison of SANS and SAXS curves give some of the first information about the distribution of hydrogen-containing structures. Using anomalous small-angle X-ray scattering, an energy-dependent scattering is found for an MgHx sample with 1 mol% Fe2O3. From the separated scattering curve a size distribution of hard spheres is obtained with a size range which is expected for crystallite and particle sizes of the Fe2O3 catalyst. Chemical shifts in the absorption spectra give information about the stability of the metal oxide catalysts during the milling process.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle scattering investigations of magnesium hydride used as a hydrogen storage material</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>383</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>387</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6028">
    <title>Structure and dynamics of thin polymer films using synchrotron X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6028</link>
    <description>Recent measurements of the scattering function and of the dynamics of surface and interfacial fluctuations in thin supported molten films and bilayers using synchrotron X-ray diffuse scattering and photon correlation spectroscopy in reflection geometry are reported. The results for monolayer films thicker than four times of the radius of gyration of polystyrene show behavior of normal over-damped capillary waves expected for the surface fluctuations of a viscous liquid. However, thinner films show deviations indicating the need to account for viscoelasticity. The theory has been extended to the surface and interfacial modes in a bilayer film system. The results are discussed in terms of surface tension, viscosity and shear modulus. Also recent experiments to measure the isothermal compressibility of supported polystyrene films by studying `bulk' scattering from the interior of the films is discussed.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Jiang, Z.</dc:creator>
    <dc:creator>Kim, H.</dc:creator>
    <dc:creator>Lee, H.</dc:creator>
    <dc:creator>Lee, Y.J.</dc:creator>
    <dc:creator>Jiao, X.</dc:creator>
    <dc:creator>Li, C.</dc:creator>
    <dc:creator>Lurio, L.B.</dc:creator>
    <dc:creator>Hu, X.</dc:creator>
    <dc:creator>Lal, J.</dc:creator>
    <dc:creator>Narayanan, S.</dc:creator>
    <dc:creator>Sandy, A.</dc:creator>
    <dc:creator>Rafailovich, M.</dc:creator>
    <dc:creator>Sinha, S.K.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807007996</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Synchrotron X-ray diffuse scattering and photon correlation spectroscopy in reflection geometry were used to measure the structure and dynamic properties at the surface, interface and in the interior of supported polymer films.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY DIFFUSE SCATTERING; X-RAY PHOTON CORRELATION SPECTROSCOPY; POLYMER FILMS</dc:subject>
    <dc:description>Recent measurements of the scattering function and of the dynamics of surface and interfacial fluctuations in thin supported molten films and bilayers using synchrotron X-ray diffuse scattering and photon correlation spectroscopy in reflection geometry are reported. The results for monolayer films thicker than four times of the radius of gyration of polystyrene show behavior of normal over-damped capillary waves expected for the surface fluctuations of a viscous liquid. However, thinner films show deviations indicating the need to account for viscoelasticity. The theory has been extended to the surface and interfacial modes in a bilayer film system. The results are discussed in terms of surface tension, viscosity and shear modulus. Also recent experiments to measure the isothermal compressibility of supported polystyrene films by studying `bulk' scattering from the interior of the films is discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structure and dynamics of thin polymer films using synchrotron X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>18</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>22</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6021">
    <title>Structural changes in gradient colloidal thin gold films deposited from aqueous solution</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6021</link>
    <description>Pattern formation is investigated in a one-dimensional gradient prepared from an aqueous colloidal gold nanoparticle solution. The hydrodynamic process can be reconstructed by determining the prominent length scales and surface roughness in the dried gradient. The structural information is obtained using a combination of grazing-incidence small-angle X-ray scattering, which is a method of high-statistical relevance, and a moderate microfocused beam. This allows for scanning the gradient and to locally reveal the structure of the thin film. Our results, based on a simplified hydrodynamic model, indicate a system oscillating between depleted regions, nanoparticle domains and complete nanoparticle layers.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Roth, S.V.</dc:creator>
    <dc:creator>Müller-Buschbaum, P.</dc:creator>
    <dc:creator>Timmann, A.</dc:creator>
    <dc:creator>Perlich, J.</dc:creator>
    <dc:creator>Gehrke, R.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807007716</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A gradient in a colloidal thin film prepared from solution is investigated using microbeam grazing-incidence small-angle X-ray scattering. A cross-over and oscillation between a complete layer and depleted regions are detected.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MICROBEAMS; GRAZING-INCIDENCE SMALL-ANGLE X-RAY SCATTERING; COLLOIDS; COMBINATORIAL TECHNIQUES</dc:subject>
    <dc:description>Pattern formation is investigated in a one-dimensional gradient prepared from an aqueous colloidal gold nanoparticle solution. The hydrodynamic process can be reconstructed by determining the prominent length scales and surface roughness in the dried gradient. The structural information is obtained using a combination of grazing-incidence small-angle X-ray scattering, which is a method of high-statistical relevance, and a moderate microfocused beam. This allows for scanning the gradient and to locally reveal the structure of the thin film. Our results, based on a simplified hydrodynamic model, indicate a system oscillating between depleted regions, nanoparticle domains and complete nanoparticle layers.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structural changes in gradient colloidal thin gold films deposited from aqueous solution</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>346</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>349</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6015">
    <title>Scanning X-ray imaging with small-angle scattering contrast</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6015</link>
    <description>An X-ray scanning imaging technique using the integrated intensity of the small-angle X-ray scattering (SAXS) signal is presented. The technique is based on two-dimensional scanning of a thin sample section with an X-ray microbeam, collecting SAXS patterns at every scanning step using a two-dimensional detector. The integrated intensity within pre-defined regions of interest of the SAXS patterns is used to image bulk nanostructural features in the specimen with micrometre resolution which are usually not accessible by other methods such as light microscopy or scanning electron microscopy. The possibilities and limitations of the method are discussed with particular emphasis on the sources of contrast in the SAXS region for three biological specimens: cortical bone, eggshell and hair. Two main sources of image contrast are identified in the form of orientation effects for strongly anisotropic systems like cortical bone and differences in the local volume fraction of the scattering entities in eggshell. Moreover, other parameters than the integrated intensity can be quantitatively deduced from the SAXS patterns, for instance, the mean thickness of mineral platelets in bone or the strain distributions in a hair deformed plastically by microindentation.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Gourrier, A.</dc:creator>
    <dc:creator>Wagermaier, W.</dc:creator>
    <dc:creator>Burghammer, M.</dc:creator>
    <dc:creator>Lammie, D.</dc:creator>
    <dc:creator>Gupta, H.S.</dc:creator>
    <dc:creator>Fratzl, P.</dc:creator>
    <dc:creator>Riekel, C.</dc:creator>
    <dc:creator>Wess, T.J.</dc:creator>
    <dc:creator>Paris, O.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807006693</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A scanning X-ray imaging technique using the integrated small-angle scattering (SAXS) intensity is presented. The origin of the SAXS contrast is discussed for three biological materials: bone, eggshell and hair.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY IMAGING; SMALL-ANGLE X-RAY SCATTERING; BONE; EGGSHELL; HAIR</dc:subject>
    <dc:description>An X-ray scanning imaging technique using the integrated intensity of the small-angle X-ray scattering (SAXS) signal is presented. The technique is based on two-dimensional scanning of a thin sample section with an X-ray microbeam, collecting SAXS patterns at every scanning step using a two-dimensional detector. The integrated intensity within pre-defined regions of interest of the SAXS patterns is used to image bulk nanostructural features in the specimen with micrometre resolution which are usually not accessible by other methods such as light microscopy or scanning electron microscopy. The possibilities and limitations of the method are discussed with particular emphasis on the sources of contrast in the SAXS region for three biological specimens: cortical bone, eggshell and hair. Two main sources of image contrast are identified in the form of orientation effects for strongly anisotropic systems like cortical bone and differences in the local volume fraction of the scattering entities in eggshell. Moreover, other parameters than the integrated intensity can be quantitatively deduced from the SAXS patterns, for instance, the mean thickness of mineral platelets in bone or the strain distributions in a hair deformed plastically by microindentation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Scanning X-ray imaging with small-angle scattering contrast</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>78</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>82</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6011">
    <title>Shape of α-crystallin analyzed by small-angle neutron scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6011</link>
    <description>The size and shape of aggregates of human recombinant αA-crystallin and αB-crystallin are investigated with small-angle neutron scattering and dynamic light scattering. At a bioactive temperature (310 K), both polypeptides form aggregates with almost the same size and shape. The αB-crystallin maintains an almost identical size and shape at 310 and 288 K, whereas the aggregate of αA-crystallin shows deformation at 288 K. This result suggests that at the lower temperature there is a difference in structural stability between the two aggregates of the polypeptides.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Sugiyama, M.</dc:creator>
    <dc:creator>Fujii, N.</dc:creator>
    <dc:creator>Morimoto, Y.</dc:creator>
    <dc:creator>Otomo, T.</dc:creator>
    <dc:creator>Takata, S.</dc:creator>
    <dc:creator>Misawa, M.</dc:creator>
    <dc:creator>Annaka, M.</dc:creator>
    <dc:creator>Itoh, K.</dc:creator>
    <dc:creator>Mori, K.</dc:creator>
    <dc:creator>Sato, T.</dc:creator>
    <dc:creator>Kurabayashi, S.</dc:creator>
    <dc:creator>Fukunaga, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807006838</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The size and shape of aggregates of human recombinant&gt; αA- and αB-crystallins are investigated with small-angle neutron scattering and dynamic light scattering at 310 K and 288 K. The aggregates of αB-crystallin are stable at both temperatures but those of αA-crystallin are deformed at the lower temperature (288 K).</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>[ALPHA]A-CRYSTALLIN; [ALPHA]B-CRYSTALLIN; SMALL-ANGLE NEUTRON SCATTERING; DYNAMIC LIGHT SCATTERING</dc:subject>
    <dc:description>The size and shape of aggregates of human recombinant αA-crystallin and αB-crystallin are investigated with small-angle neutron scattering and dynamic light scattering. At a bioactive temperature (310 K), both polypeptides form aggregates with almost the same size and shape. The αB-crystallin maintains an almost identical size and shape at 310 and 288 K, whereas the aggregate of αA-crystallin shows deformation at 288 K. This result suggests that at the lower temperature there is a difference in structural stability between the two aggregates of the polypeptides.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Shape of α-crystallin analyzed by small-angle neutron scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>200</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>204</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6005">
    <title>The two-Yukawa model and its applications: the cases of charged proteins and copolymer micellar solutions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6005</link>
    <description>Charged and uncharged colloidal systems are known from experiment to display an extremely rich phase behavior, which is ultimately determined by the effective pair potential between particles in solution. As a confirmation, the recent striking observation of an equilibrium cluster phase in charged globular protein solutions [Stradner, Sedgwick, Cardinaux, Poon, Egelhaaf &amp; Schurtenberger (2004). Nature, 432, 492–495] has been interpreted as the effect of competing short-range attractive and long-range repulsive interactions. The `two-Yukawa (2Y) fluid' model assumes an interparticle potential consisting of a hard core plus an attractive and a repulsive Yukawa tail. We show that this rather simple model can indeed explain satisfactorily the structural properties of diverse colloidal materials, measured in small-angle neutron scattering (SANS) experiments, including the cases of equilibrium cluster formation and soft-core repulsion. We apply this model to the analysis of SANS data from horse-heart cytochrome c protein solutions (whose effective potential can be modeled as a hard-sphere part plus a short-range attraction and a weaker screened electrostatic repulsion) and micellar solutions of a triblock copolymer (whose effective potential can be modeled as a hard-sphere part plus a repulsive shoulder and a short-range attraction). The accuracy of the 2Y model predictions is successfully tested against Monte Carlo simulations in both cases.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Chen, S.-H.</dc:creator>
    <dc:creator>Broccio, M.</dc:creator>
    <dc:creator>Liu, Y.</dc:creator>
    <dc:creator>Fratini, E.</dc:creator>
    <dc:creator>Baglioni, P.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807006723</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An analytical model for the structure factor, based on an effective interaction potential made of an attractive Yukawa term plus a repulsive Yukawa term, has been applied to charged proteins and copolymer micellar solutions.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CHARGED PROTEINS; MICELLAR SOLUTIONS; TWO-YUKAWA FLUID MODEL</dc:subject>
    <dc:description>Charged and uncharged colloidal systems are known from experiment to display an extremely rich phase behavior, which is ultimately determined by the effective pair potential between particles in solution. As a confirmation, the recent striking observation of an equilibrium cluster phase in charged globular protein solutions [Stradner, Sedgwick, Cardinaux, Poon, Egelhaaf &amp; Schurtenberger (2004). Nature, 432, 492–495] has been interpreted as the effect of competing short-range attractive and long-range repulsive interactions. The `two-Yukawa (2Y) fluid' model assumes an interparticle potential consisting of a hard core plus an attractive and a repulsive Yukawa tail. We show that this rather simple model can indeed explain satisfactorily the structural properties of diverse colloidal materials, measured in small-angle neutron scattering (SANS) experiments, including the cases of equilibrium cluster formation and soft-core repulsion. We apply this model to the analysis of SANS data from horse-heart cytochrome c protein solutions (whose effective potential can be modeled as a hard-sphere part plus a short-range attraction and a weaker screened electrostatic repulsion) and micellar solutions of a triblock copolymer (whose effective potential can be modeled as a hard-sphere part plus a repulsive shoulder and a short-range attraction). The accuracy of the 2Y model predictions is successfully tested against Monte Carlo simulations in both cases.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The two-Yukawa model and its applications: the cases of charged proteins and copolymer micellar solutions</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>321</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>326</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6031">
    <title>Performance of the 36 m small-angle neutron scattering spectrometer at BATAN, Serpong, Indonesia</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6031</link>
    <description>A 36 m small-angle neutron scattering (SANS) spectrometer (SMARTer) has been installed at the end of a 49 m long neutron guide tube and located in the neutron guide hall at the Neutron Scattering Laboratory (NSL), Serpong, Indonesia. At present, this is the largest SANS spectrometer in the Asia–Pacific region and consists of an 18 m long tube collimation system and another 18 m long tube to accommodate a 128 × 128 3He two-dimensional position-sensitive detector. The detector can be moved continuously from 1.5 to 18 m and can be shifted laterally by 0.1 m to cover a large range of Q, where Q is the magnitude of the scattering vector given by Q = (4\pi /\lambda) \sin (\theta /2), θ is the scattering angle and λ is the wavelength. By selecting the rotational speed of the velocity selector, the incident thermal neutron beam will have a wavelength λ in the range 3–6 Å and a Q range of 0.002–0.6 Å−1. The maximum neutron flux at the sample position is 4 × 106 neutrons cm−2 s−1. Measurements of some standard samples using SMARTer are reported for inter-laboratory comparisons that show, for the first time, how SMARTer's capabilities compare with those of other prominent SANS instruments.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Putra, E.G.R.</dc:creator>
    <dc:creator>Ikram, A.</dc:creator>
    <dc:creator>Santoso, E.</dc:creator>
    <dc:creator>Bharoto, B.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S002188980700605X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>An inter-laboratory comparison of the 36 m small-angle neutron scattering (SANS) spectrometer at BATAN with those of other prominent SANS spectrometers is reported.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SANS; BLOCK COPOLYMERS; SOFT CONDENSED MATTER; SMARTER</dc:subject>
    <dc:description>A 36 m small-angle neutron scattering (SANS) spectrometer (SMARTer) has been installed at the end of a 49 m long neutron guide tube and located in the neutron guide hall at the Neutron Scattering Laboratory (NSL), Serpong, Indonesia. At present, this is the largest SANS spectrometer in the Asia–Pacific region and consists of an 18 m long tube collimation system and another 18 m long tube to accommodate a 128 × 128 3He two-dimensional position-sensitive detector. The detector can be moved continuously from 1.5 to 18 m and can be shifted laterally by 0.1 m to cover a large range of Q, where Q is the magnitude of the scattering vector given by Q = (4\pi /\lambda) \sin (\theta /2), θ is the scattering angle and λ is the wavelength. By selecting the rotational speed of the velocity selector, the incident thermal neutron beam will have a wavelength λ in the range 3–6 Å and a Q range of 0.002–0.6 Å−1. The maximum neutron flux at the sample position is 4 × 106 neutrons cm−2 s−1. Measurements of some standard samples using SMARTer are reported for inter-laboratory comparisons that show, for the first time, how SMARTer's capabilities compare with those of other prominent SANS instruments.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Performance of the 36 m small-angle neutron scattering spectrometer at BATAN, Serpong, Indonesia</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>447</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>452</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6036">
    <title>Wide-q observation from 10−4 to 2.0 Å−1 using a focusing and polarized neutron small-angle scattering spectrometer, SANS-J-II</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6036</link>
    <description>In order to extend an upper q-limit [q is the magnitude of the scattering vector q, defined by q = (4π/λ)sinθ, where λ and 2θ are the wavelength and the scattering angle, respectively], high-angle 3He sub-detectors were installed on a focusing and polarized neutron small-angle scattering spectrometer (SANS-J-II) at JRR-3, Tokai, Japan. Consequently, the upper q-limit was improved from 0.2 to 2.0 Å−1. To quantitatively discriminate spin incoherent scattering from hydrogen or to perform nuclear spin polarization contrast variation, a remanent supermirror analyser is also available on the high-angle sub-detector. By combining a focusing ultra-small-angle scattering, realised by compound and/or magnetic lens and high-resolution area detector, SANS-J-II is able to cover from 3 × 10−4 to 2.0 Å−1 (four orders of magnitude of q), which benefits investigation of hierarchically ordered systems, found widely in hard, soft and bio-materials.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Iwase, H.</dc:creator>
    <dc:creator>Koizumi, S.</dc:creator>
    <dc:creator>Suzuki, J.</dc:creator>
    <dc:creator>Oku, T.</dc:creator>
    <dc:creator>Sasao, H.</dc:creator>
    <dc:creator>Tanaka, H.</dc:creator>
    <dc:creator>Shimizu, H.M.</dc:creator>
    <dc:creator>Hashimoto, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807006280</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A conventional pinhole-type small-angle neutron scattering spectrometer (SANS-J) was successfully reconstructed to be a focusing and polarized neutron small-angle scattering (SANS-J-II) instrument, with a wide q-region from ultra-small-angle scattering of 10−4 Å−1 to high-q of 2.0 Å−1.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ULTRA-SMALL-ANGLE NEUTRON SCATTERING; FOCUSING LENS; POLARIZED NEUTRON SCATTERING</dc:subject>
    <dc:description>In order to extend an upper q-limit [q is the magnitude of the scattering vector q, defined by q = (4π/λ)sinθ, where λ and 2θ are the wavelength and the scattering angle, respectively], high-angle 3He sub-detectors were installed on a focusing and polarized neutron small-angle scattering spectrometer (SANS-J-II) at JRR-3, Tokai, Japan. Consequently, the upper q-limit was improved from 0.2 to 2.0 Å−1. To quantitatively discriminate spin incoherent scattering from hydrogen or to perform nuclear spin polarization contrast variation, a remanent supermirror analyser is also available on the high-angle sub-detector. By combining a focusing ultra-small-angle scattering, realised by compound and/or magnetic lens and high-resolution area detector, SANS-J-II is able to cover from 3 × 10−4 to 2.0 Å−1 (four orders of magnitude of q), which benefits investigation of hierarchically ordered systems, found widely in hard, soft and bio-materials.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Wide-q observation from 10−4 to 2.0 Å−1 using a focusing and polarized neutron small-angle scattering spectrometer, SANS-J-II</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>414</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>417</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6004">
    <title>Monte Carlo simulations of the new small-angle neutron scattering instrument SANS-1 at the Heinz Maier-Leibnitz Forschungsneutronenquelle</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6004</link>
    <description>A new small-angle scattering instrument SANS-1 will be installed on beamline NL 4a at the Heinz Maier-Leibnitz Forschungsneutronenquelle (FRM II). It is a joint venture between the Technische Universität München and the Geesthacht Neutron Facility (GENF). SANS-1 has been optimized to be one of the most intense and versatile small-angle scattering instruments within the boundaries of available space and interaction with neighbouring instruments. Using the program McStas, the dimensions and the features of the different optical components were investigated and compared for the final selection. A vertical S-shaped neutron guide, a tower with two possible selectors, one for medium resolution at high intensity and one for high resolution, and two optimized transmission polarizers are the main advantages of SANS-1 compared with traditional instruments at other facilities.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Gilles, R.</dc:creator>
    <dc:creator>Ostermann, A.</dc:creator>
    <dc:creator>Petry, W.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807006310</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The optimization by Monte Carlo simulation of the components of the new small-angle scattering instrument SANS-1 at the Heinz Maier-Leibnitz Forschungsneutronenquelle (FRM II) is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SANS; NEUTRON GUIDES; SELECTORS; MCSTAS SIMULATION</dc:subject>
    <dc:description>A new small-angle scattering instrument SANS-1 will be installed on beamline NL 4a at the Heinz Maier-Leibnitz Forschungsneutronenquelle (FRM II). It is a joint venture between the Technische Universität München and the Geesthacht Neutron Facility (GENF). SANS-1 has been optimized to be one of the most intense and versatile small-angle scattering instruments within the boundaries of available space and interaction with neighbouring instruments. Using the program McStas, the dimensions and the features of the different optical components were investigated and compared for the final selection. A vertical S-shaped neutron guide, a tower with two possible selectors, one for medium resolution at high intensity and one for high resolution, and two optimized transmission polarizers are the main advantages of SANS-1 compared with traditional instruments at other facilities.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Monte Carlo simulations of the new small-angle neutron scattering instrument SANS-1 at the Heinz Maier-Leibnitz Forschungsneutronenquelle</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>428</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>432</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6012">
    <title>Small-angle X-ray scattering study on conformation of poly(sodium l-glutamate) in NaCl and NaF aqueous solutions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6012</link>
    <description>The effect of anions F− and Cl− on the conformation of poly(sodium l-glutamate) (PNaGA) in added-salt aqueous solution was studied using potentiometric titration, high-resolution proton nuclear magnetic resonance (NMR), circular dichroism (CD) and small-angle X-ray scattering (SAXS) techniques. In the titration curve for PNaGA in NaCl aqueous solution, four conformation regions, i.e. aggregation-, helical-, helix-to-coil transition- and random-coiled, were clearly observed but these regions were gradually obscured when the concentration of F− was increased. Both CD and NMR spectra have clarified that the local conformation of PNaGA in NaF aqueous solution is a random-coiled state, independent of the degree of neutralization (DN). SAXS studies show that the conformation of a larger dimension for PNaGA having DN = 0.25 in 0.2 NaF aqueous solution is roughly mimicked by a worm-like chain having persistence length of ca 5.9 Å, but the conformation at DN = 0.80 is far from an isolated worm-like chain.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Shimizu, S.</dc:creator>
    <dc:creator>Muroga, Y.</dc:creator>
    <dc:creator>Hyono, T.</dc:creator>
    <dc:creator>Kurita, K.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807006255</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Local conformations of poly(sodium l-glutamate) in NaCl and NaF aqueous solutions are analyzed with small-angle X-ray scattering, circular dichroism and nuclear magnetic resonance techniques.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLY(SODIUM L-GLUTAMIC ACID); LOCAL CONFORMATION; SMALL-ANGLE X-RAY SCATTERING; WORM-LIKE CHAIN</dc:subject>
    <dc:description>The effect of anions F− and Cl− on the conformation of poly(sodium l-glutamate) (PNaGA) in added-salt aqueous solution was studied using potentiometric titration, high-resolution proton nuclear magnetic resonance (NMR), circular dichroism (CD) and small-angle X-ray scattering (SAXS) techniques. In the titration curve for PNaGA in NaCl aqueous solution, four conformation regions, i.e. aggregation-, helical-, helix-to-coil transition- and random-coiled, were clearly observed but these regions were gradually obscured when the concentration of F− was increased. Both CD and NMR spectra have clarified that the local conformation of PNaGA in NaF aqueous solution is a random-coiled state, independent of the degree of neutralization (DN). SAXS studies show that the conformation of a larger dimension for PNaGA having DN = 0.25 in 0.2 NaF aqueous solution is roughly mimicked by a worm-like chain having persistence length of ca 5.9 Å, but the conformation at DN = 0.80 is far from an isolated worm-like chain.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle X-ray scattering study on conformation of poly(sodium l-glutamate) in NaCl and NaF aqueous solutions</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>553</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>557</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6017">
    <title>Microstructure of ternary system di-lauroyl-phosphatidyl-adenosine/water/cyclohexane</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6017</link>
    <description>1,2-Dilauroyl-sn-glycero-3-phosphatidyl-adenosine in 0.1 M phosphate buffer (pH = 7.5) forms worm-like micelles that with ageing of the solution, self-assemble into helical superstructures. Small-angle neutron scattering has shown that dissolution of even small amounts of oil in the hydrophobic cores induces a dramatic structural transition to form spherical micelles. A variation of the interfacial film curvature promotes a strong change in base–base interaction pattern as shown in circular dichroism experiments.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Betti, F.</dc:creator>
    <dc:creator>Baldelli Bombelli, F.</dc:creator>
    <dc:creator>Berti, D.</dc:creator>
    <dc:creator>Bonini, M.</dc:creator>
    <dc:creator>Brandt, A.</dc:creator>
    <dc:creator>Baglioni, P.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807006218</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Microstructural characterization of 1,2-dilauroyl-sn-glycero-3-phosphatidyl-adenosine micellar solutions upon cyclohexane addition by SANS experiments with internal contrast variation.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SELF-ASSEMBLY; PHOSPHATIDYLNUCLEOSIDES; SANS; MICROEMULSION; INTERFACIAL CURVATURE</dc:subject>
    <dc:description>1,2-Dilauroyl-sn-glycero-3-phosphatidyl-adenosine in 0.1 M phosphate buffer (pH = 7.5) forms worm-like micelles that with ageing of the solution, self-assemble into helical superstructures. Small-angle neutron scattering has shown that dissolution of even small amounts of oil in the hydrophobic cores induces a dramatic structural transition to form spherical micelles. A variation of the interfacial film curvature promotes a strong change in base–base interaction pattern as shown in circular dichroism experiments.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Microstructure of ternary system di-lauroyl-phosphatidyl-adenosine/water/cyclohexane</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>240</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>244</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6021">
    <title>Modelling of bacteriophage capsids and free nucleic acids</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6021</link>
    <description>The reconstruction of sphere shells as realized in bacteriophage capsids can be achieved by ab initio modelling approaches based on a genetic algorithm or simulated annealing. The application of tight constraints such as icosahedral symmetry makes the DAMMIN procedure the method of choice. The ab initio models obtained may be compared with three-dimensional models derived from crystal data. This information, in conjunction with surface calculations and application of specific hydration algorithms, allows the generation of biophysically relevant hydrated three-dimensional models. Modelling free RNA of viruses represents another challenge to advanced modelling intentions. While application of the DAMMIN procedure provides the generation of appropriate models for the overall structure of nucleic acids, inclusion of further constraints improves the biological relevance of the resultant models. This may be achieved by our in-house program SUBSTRUCT, which allows involvement of secondary structure details.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Zipper, P.</dc:creator>
    <dc:creator>Durchschlag, H.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005936</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>SAXS-based ab initio modelling of the capsids of isometric bacteriophages allows the solution structure of the constituent hollow spheres to be reconstructed reliably. For the shape of their free nucleic acid, however, other advanced modelling approaches are to be preferred.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SMALL-ANGLE X-RAY SCATTERING; BACTERIOPHAGES; CAPSIDS; NUCLEIC ACIDS; MODELLING APPROACHES</dc:subject>
    <dc:description>The reconstruction of sphere shells as realized in bacteriophage capsids can be achieved by ab initio modelling approaches based on a genetic algorithm or simulated annealing. The application of tight constraints such as icosahedral symmetry makes the DAMMIN procedure the method of choice. The ab initio models obtained may be compared with three-dimensional models derived from crystal data. This information, in conjunction with surface calculations and application of specific hydration algorithms, allows the generation of biophysically relevant hydrated three-dimensional models. Modelling free RNA of viruses represents another challenge to advanced modelling intentions. While application of the DAMMIN procedure provides the generation of appropriate models for the overall structure of nucleic acids, inclusion of further constraints improves the biological relevance of the resultant models. This may be achieved by our in-house program SUBSTRUCT, which allows involvement of secondary structure details.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Modelling of bacteriophage capsids and free nucleic acids</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>153</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>158</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6007">
    <title>Biological solution scattering: recent achievements and future challenges</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6007</link>
    <description>In the post-genomic age it is apparent that as structures of larger macromolecules and their complexes are investigated, structure–function investigations are often confronted with the necessity to apply a portfolio of tools for biochemical and biophysical characterization. A survey of the published literature over the last decade reveals that publications in the area of structural biology employing neutron or X-ray scattering as one of their techniques tripled since 1995. Yet, taken as a whole, the contribution from small-angle scattering (SAS) to research papers dealing with structural analyses is still only of the order of 1% in 2005 (for comparison, less than 0.5% in 1995). Nevertheless, the last few years saw stimulating biological applications and analysis procedures which emphasize the growing potential of SAS applications for the structural studies of macromolecules in solution. The usage of SAS largely consists of low-resolution reconstructions of molecules with partial or without presumption of structural details, consistency analysis of high-resolution crystallographic structures and their corresponding low-resolution models determined in the solution state, and rigid-body refinement of multi-subunit assemblies including complexes and full-length multidomain proteins. Complementary structural information obtained from SAS in conjunction with data acquired by protein crystallography, NMR, molecular dynamics or computational docking provides a means to link low- and high-resolution models essential for the elucidation of biomolecular organization, interactions and function. The capabilities as well as limitations of determining low-resolution structures of multidomain proteins, macromolecular complexes and assemblies are highlighted in three examples. The first example is the characterization of the conformation of the PDZ region of SAP97, a multidomain protein involved in the regulation and localization of membrane receptor molecules. The second example is the characterization of the structural features of the TIM10 complex, an escort molecule for mitochondrial inner-membrane proteins, and the third example is the description of the shape and pH-induced conformational transition of a full-length bacterial potassium channel. The latter two in particular benefited from neutron scattering with contrast variation by using H–D labelling of the macromolecular complex or the solvent, respectively.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Grossmann, J.G.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005821</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Solution X-ray and neutron scattering methods are briefly reviewed in view of their appeal and recent progress in data-analysis procedures. Specific examples are discussed highlighting the potential of the techniques and their future developments and applications to structural investigations in the post-genomics era.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY SCATTERING; NEUTRON SCATTERING; LOW-RESOLUTION STRUCTURES; MACROMOLECULES; MULTIDOMAIN PROTEINS; PROTEIN COMPLEXES; RIGID-BODY MODELLING; COMPUTER SIMULATION; PDZ DOMAIN; TIM10; KCSA</dc:subject>
    <dc:description>In the post-genomic age it is apparent that as structures of larger macromolecules and their complexes are investigated, structure–function investigations are often confronted with the necessity to apply a portfolio of tools for biochemical and biophysical characterization. A survey of the published literature over the last decade reveals that publications in the area of structural biology employing neutron or X-ray scattering as one of their techniques tripled since 1995. Yet, taken as a whole, the contribution from small-angle scattering (SAS) to research papers dealing with structural analyses is still only of the order of 1% in 2005 (for comparison, less than 0.5% in 1995). Nevertheless, the last few years saw stimulating biological applications and analysis procedures which emphasize the growing potential of SAS applications for the structural studies of macromolecules in solution. The usage of SAS largely consists of low-resolution reconstructions of molecules with partial or without presumption of structural details, consistency analysis of high-resolution crystallographic structures and their corresponding low-resolution models determined in the solution state, and rigid-body refinement of multi-subunit assemblies including complexes and full-length multidomain proteins. Complementary structural information obtained from SAS in conjunction with data acquired by protein crystallography, NMR, molecular dynamics or computational docking provides a means to link low- and high-resolution models essential for the elucidation of biomolecular organization, interactions and function. The capabilities as well as limitations of determining low-resolution structures of multidomain proteins, macromolecular complexes and assemblies are highlighted in three examples. The first example is the characterization of the conformation of the PDZ region of SAP97, a multidomain protein involved in the regulation and localization of membrane receptor molecules. The second example is the characterization of the structural features of the TIM10 complex, an escort molecule for mitochondrial inner-membrane proteins, and the third example is the description of the shape and pH-induced conformational transition of a full-length bacterial potassium channel. The latter two in particular benefited from neutron scattering with contrast variation by using H–D labelling of the macromolecular complex or the solvent, respectively.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Biological solution scattering: recent achievements and future challenges</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>217</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>222</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6015">
    <title>Analysis of small-angle X-ray scattering data of protein–detergent complexes by singular value decomposition</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6015</link>
    <description>Small-angle X-ray scattering can be a valuable tool in the structural characterization of membrane protein–detergent complexes (PDCs). However, a major challenge is to separate the PDC scattering signal from that of the `empty' detergent micelle in a protein–detergent mixture. We briefly review an approach that allows approximate determination of the PDC scattering signal at low momentum transfer and present a novel approach that employs a singular value decomposition (SVD) and fitting of scattering data collected at different protein–detergent stoichiometries. The SVD approach allows the scattering profile for the PDC over the entire measured momentum transfer range to be obtained, it is applicable to strongly scattering detergents and can take into account interparticle interference. The two approaches are contrasted and an application to the membrane protein TM0026 from Thermotoga maritima is presented.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Lipfert, J.</dc:creator>
    <dc:creator>Columbus, L.</dc:creator>
    <dc:creator>Chu, V.B.</dc:creator>
    <dc:creator>Doniach, S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005791</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>We present a method to separate the protein–detergent complex scattering signal from that of `empty' detergent micelles in small-angle X-ray scattering data of protein–detergent mixtures. The approach relies on singular value decomposition and fitting to data collected at different protein–detergent stoichiometries.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>PROTEIN-DETERGENT COMPLEXES; SINGULAR VALUE DECOMPOSITION; MEMBRANE PROTEINS; SAXS</dc:subject>
    <dc:description>Small-angle X-ray scattering can be a valuable tool in the structural characterization of membrane protein–detergent complexes (PDCs). However, a major challenge is to separate the PDC scattering signal from that of the `empty' detergent micelle in a protein–detergent mixture. We briefly review an approach that allows approximate determination of the PDC scattering signal at low momentum transfer and present a novel approach that employs a singular value decomposition (SVD) and fitting of scattering data collected at different protein–detergent stoichiometries. The SVD approach allows the scattering profile for the PDC over the entire measured momentum transfer range to be obtained, it is applicable to strongly scattering detergents and can take into account interparticle interference. The two approaches are contrasted and an application to the membrane protein TM0026 from Thermotoga maritima is presented.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Analysis of small-angle X-ray scattering data of protein–detergent complexes by singular value decomposition</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>235</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>239</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6029">
    <title>In situ investigation of annealing effect on lamellar stacking structure of polyethylene thin films by synchrotron grazing-incidence small-angle and wide-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6029</link>
    <description>We have investigated lamellar stacking structure of melt-crystallized and annealed high-density polyethylene (HDPE) thin films, with a thickness of ca 400 nm prepared on silicon wafers, using synchrotron grazing-incidence small-angle and wide-angle X-ray scattering (GISWAXS) measurements at the BL40B2 beamline in SPring-8. In-situ measurements of GISWAXS were carried out for the films in a stepwise annealing process under vacuum. Scattering peaks relating to the long period, the average distance between stacked crystalline lamellae, were measured only in the in-plane direction near the Yoneda peak of the grazing-incidence small-angle X-ray scattering patterns. On the other hand, the orthorhombic (110) and (200) reflections of oriented HDPE crystals were measured in the out-of-plane direction of the grazing-incidence wide-angle X-ray scattering patterns. It was revealed that crystalline lamellae were stacked in a parallel direction to the film surface and the long period increased from ca 25 nm to ca 32 nm in a stepwise annealing process. Within a lamella, molecular chains were found to be packed regularly and the chain axis (the c axis) was relatively oriented parallel to the film surface.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Sasaki, S.</dc:creator>
    <dc:creator>Masunaga, H.</dc:creator>
    <dc:creator>Tajiri, H.</dc:creator>
    <dc:creator>Inoue, K.</dc:creator>
    <dc:creator>Okuda, H.</dc:creator>
    <dc:creator>Noma, H.</dc:creator>
    <dc:creator>Honda, K.</dc:creator>
    <dc:creator>Takahara, A.</dc:creator>
    <dc:creator>Takata, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S002188980700578X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The annealing effect on lamellar stacking structure of polyethylene thin films prepared on silicon wafers has been investigated in terms of molecular- and meso -scale regularity by in-situ synchrotron grazing-incidence small-angle and wide-angle X-ray scattering measurements.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLYETHYLENE THIN FILM; LAMELLAR STACKING STRUCTURE; IN-SITU SYNCHROTRON GISAXS; IN-SITU SYNCHROTRON GIWAXS; ANNEALING EFFECT</dc:subject>
    <dc:description>We have investigated lamellar stacking structure of melt-crystallized and annealed high-density polyethylene (HDPE) thin films, with a thickness of ca 400 nm prepared on silicon wafers, using synchrotron grazing-incidence small-angle and wide-angle X-ray scattering (GISWAXS) measurements at the BL40B2 beamline in SPring-8. In-situ measurements of GISWAXS were carried out for the films in a stepwise annealing process under vacuum. Scattering peaks relating to the long period, the average distance between stacked crystalline lamellae, were measured only in the in-plane direction near the Yoneda peak of the grazing-incidence small-angle X-ray scattering patterns. On the other hand, the orthorhombic (110) and (200) reflections of oriented HDPE crystals were measured in the out-of-plane direction of the grazing-incidence wide-angle X-ray scattering patterns. It was revealed that crystalline lamellae were stacked in a parallel direction to the film surface and the long period increased from ca 25 nm to ca 32 nm in a stepwise annealing process. Within a lamella, molecular chains were found to be packed regularly and the chain axis (the c axis) was relatively oriented parallel to the film surface.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>In situ investigation of annealing effect on lamellar stacking structure of polyethylene thin films by synchrotron grazing-incidence small-angle and wide-angle X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>642</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>644</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6003">
    <title>Contribution of small-angle X-ray scattering to microstructural investigation of newly developed Mg–rare earth alloys for structural applications</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6003</link>
    <description>New Mg–Y–Gd–Mn alloys, strengthened by a dense fine scale precipitation, have been recently designed for structural applications up to 523 K. The qualitative small-angle X-ray scattering study presented here enlightens the mechanical properties at high temperature of these alloys. Small Guinier–Preston zones have been evidenced in alloys maintained at room temperature after quenching. The metastable phases, studied in parallel using high-resolution transmission electron microscopy and responsible for the good mechanical properties, are difficult to quantify completely owing to their complex microstructure of interconnected globular and faceted precipitates.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Antion, C.</dc:creator>
    <dc:creator>Bley, F.</dc:creator>
    <dc:creator>Donnadieu, P.</dc:creator>
    <dc:creator>Deschamps, A.</dc:creator>
    <dc:creator>Pisch, A.</dc:creator>
    <dc:creator>Blandin, J.-J.</dc:creator>
    <dc:creator>Tassin-Arques, C.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005493</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>New magnesium–rare earth alloys, strengthened by a dense fine scale precipitation, have been designed for structural applications up to 523 K. A complementary study using small-angle X-ray scattering is presented here.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MG-RARE EARTH ALLOYS; AGE-HARDENING; SAXS</dc:subject>
    <dc:description>New Mg–Y–Gd–Mn alloys, strengthened by a dense fine scale precipitation, have been recently designed for structural applications up to 523 K. The qualitative small-angle X-ray scattering study presented here enlightens the mechanical properties at high temperature of these alloys. Small Guinier–Preston zones have been evidenced in alloys maintained at room temperature after quenching. The metastable phases, studied in parallel using high-resolution transmission electron microscopy and responsible for the good mechanical properties, are difficult to quantify completely owing to their complex microstructure of interconnected globular and faceted precipitates.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Contribution of small-angle X-ray scattering to microstructural investigation of newly developed Mg–rare earth alloys for structural applications</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>126</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>131</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6001">
    <title>Small-angle fibre diffraction studies of corneal matrix structure: a depth-profiled investigation of the human eye-bank cornea</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6001</link>
    <description>In the cornea of the eye light transmission is facilitated by the regular arrangement and uniform diameter of collagen fibrils that constitute the bulk of the extracellular corneal matrix. Matrix architecture, in turn, is believed to be governed by interactions between collagen fibrils and proteoglycan molecules modified with sulfated glycosaminoglycan side chains. Here, we outline the contribution made by small-angle X-ray scattering studies of the cornea in understanding the role of sulfated glycosaminoglycans in the control of collagen architecture in cornea, and present new depth-profiled microbeam data from swollen human eye-bank corneas that indicate no significant change in collagen fibril diameter throughout the tissue, but a lower collagen interfibrillar spacing in the anterior-most stromal regions compared with the ultrastructure of the deeper cornea.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Quantock, A.J.</dc:creator>
    <dc:creator>Boote, C.</dc:creator>
    <dc:creator>Young, R.D.</dc:creator>
    <dc:creator>Hayes, S.</dc:creator>
    <dc:creator>Tanioka, H.</dc:creator>
    <dc:creator>Kawasaki, S.</dc:creator>
    <dc:creator>Ohta, N.</dc:creator>
    <dc:creator>Iida, T.</dc:creator>
    <dc:creator>Yagi, N.</dc:creator>
    <dc:creator>Kinoshita, S.</dc:creator>
    <dc:creator>Meek, K.M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005523</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The depth-profiled ultrastructure of the collagen fibrillar matrix in the swollen human eye-bank cornea was studied by microbeam small-angle X-ray scattering at a spatial resolution of 25 µm to provide information about collagen fibril diameter, spacing and orientation.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FIBRE DIFFRACTION; HUMAN EYE-BANK CORNEA; CORNEAL MATRIX STRUCTURE; SAXS</dc:subject>
    <dc:description>In the cornea of the eye light transmission is facilitated by the regular arrangement and uniform diameter of collagen fibrils that constitute the bulk of the extracellular corneal matrix. Matrix architecture, in turn, is believed to be governed by interactions between collagen fibrils and proteoglycan molecules modified with sulfated glycosaminoglycan side chains. Here, we outline the contribution made by small-angle X-ray scattering studies of the cornea in understanding the role of sulfated glycosaminoglycans in the control of collagen architecture in cornea, and present new depth-profiled microbeam data from swollen human eye-bank corneas that indicate no significant change in collagen fibril diameter throughout the tissue, but a lower collagen interfibrillar spacing in the anterior-most stromal regions compared with the ultrastructure of the deeper cornea.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle fibre diffraction studies of corneal matrix structure: a depth-profiled investigation of the human eye-bank cornea</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>335</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>340</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6012">
    <title>Anomalous grazing-incidence small-angle X-ray scattering investigation on the surface morphology of an FePt magnetic nanoparticle monolayer on functional modulated substrates</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6012</link>
    <description>The structural stability and coalescence of self-assembled FePt monolayer nanoparticles on functional substrates with/without an Au overlayer during annealing were studied. From X-ray diffraction and the anomalous grazing-incidence small-angle X-ray scattering techniques, the nanoparticles were found to be intact under the annealing process when a 5–10 nm overlayer of Au was deposited on top of FePt monolayer nanoparticles. From the simulation result, the particle size 4.5 ± 0.5 nm is typically unchanged, but the distance between particles is reduced from 7.5 ± 1.5 nm to 5.5 ± 1.1 nm after annealing. The results suggest that the 5 nm Au coverlayer is an effective diffusing barrier layer to prevent the FePt nanoparticles from sintering during the annealing process.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Huang, T.-W.</dc:creator>
    <dc:creator>Yu, K.-L.</dc:creator>
    <dc:creator>Liao, Y.-F.</dc:creator>
    <dc:creator>Lee, C.-H.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005390</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Anomalous grazing-incidence small-angle X-ray scattering was used to verify that FePt nanoparticles remain intact under an Au overlayer during annealing at 1073 K.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SELF-ASSEMBLED NANOPARTICLES; FEPT; X-RAY SCATTERING; ANOMALOUS GISAXS</dc:subject>
    <dc:description>The structural stability and coalescence of self-assembled FePt monolayer nanoparticles on functional substrates with/without an Au overlayer during annealing were studied. From X-ray diffraction and the anomalous grazing-incidence small-angle X-ray scattering techniques, the nanoparticles were found to be intact under the annealing process when a 5–10 nm overlayer of Au was deposited on top of FePt monolayer nanoparticles. From the simulation result, the particle size 4.5 ± 0.5 nm is typically unchanged, but the distance between particles is reduced from 7.5 ± 1.5 nm to 5.5 ± 1.1 nm after annealing. The results suggest that the 5 nm Au coverlayer is an effective diffusing barrier layer to prevent the FePt nanoparticles from sintering during the annealing process.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Anomalous grazing-incidence small-angle X-ray scattering investigation on the surface morphology of an FePt magnetic nanoparticle monolayer on functional modulated substrates</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>480</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>484</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6026">
    <title>Polarized small-angle neutron scattering study of two-dimensional spatially ordered systems of nickel nanowires</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6026</link>
    <description>The magnetic and structural properties of two-dimensional spatially ordered systems of ferromagnetic nickel nanowires embedded into an Al2O3 matrix have been studied using polarized small-angle neutron scattering (polarized SANS). We measured the total (nuclear and magnetic) scattering I(q) as a polarization-independent scattering, the field-dependent scattering as IH(q) = I(q, H) − I(q, 0), where H is the magnetic field, and the nuclear-magnetic interference as a polarization-dependent (P) scattering ΔI(q, P). A typical scattering pattern is composed of the diffuse small-angle scattering and the Bragg peak. It is shown that the introduction of Ni into the matrix does not change the position of the Bragg peak but results in an increase of the scattering intensity both in the small-angle region and at the Bragg positions. An external magnetic field was applied perpendicular or parallel to the long dimension of the nanowires in order to reveal the anisotropic properties of the magnetic system. It is shown that, firstly, the magnetic-field-dependent scattering IH(q) provides new and principally different information as compared with the interference term ΔI(q). Secondly, two contributions to the interference term ΔI(q) (ascribed to the diffuse scattering and to the diffraction peaks) have different signs indicating different origins of the scattering objects. Thirdly, polarized SANS gives a detailed picture of the magnetization process, which could not be obtained by methods of standard magnetometry.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Grigoryeva, N.A.</dc:creator>
    <dc:creator>Grigoriev, S.V.</dc:creator>
    <dc:creator>Eckerlebe, H.</dc:creator>
    <dc:creator>Eliseev, A.A.</dc:creator>
    <dc:creator>Lukashin, A.V.</dc:creator>
    <dc:creator>Napolskii, K.S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005559</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Polarized small-angle neutron scattering is used for the characterization of the structure and magnetic properties of two-dimensional spatially ordered systems of ferromagnetic nickel nanowires. These systems are promising for high-density data storage devices.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLARIZED SANS; NUCLEAR MAGNETIC INTERFERENCE; MAGNETIC NANOCOMPOSITES; DATA STORAGE DEVICES</dc:subject>
    <dc:description>The magnetic and structural properties of two-dimensional spatially ordered systems of ferromagnetic nickel nanowires embedded into an Al2O3 matrix have been studied using polarized small-angle neutron scattering (polarized SANS). We measured the total (nuclear and magnetic) scattering I(q) as a polarization-independent scattering, the field-dependent scattering as IH(q) = I(q, H) − I(q, 0), where H is the magnetic field, and the nuclear-magnetic interference as a polarization-dependent (P) scattering ΔI(q, P). A typical scattering pattern is composed of the diffuse small-angle scattering and the Bragg peak. It is shown that the introduction of Ni into the matrix does not change the position of the Bragg peak but results in an increase of the scattering intensity both in the small-angle region and at the Bragg positions. An external magnetic field was applied perpendicular or parallel to the long dimension of the nanowires in order to reveal the anisotropic properties of the magnetic system. It is shown that, firstly, the magnetic-field-dependent scattering IH(q) provides new and principally different information as compared with the interference term ΔI(q). Secondly, two contributions to the interference term ΔI(q) (ascribed to the diffuse scattering and to the diffraction peaks) have different signs indicating different origins of the scattering objects. Thirdly, polarized SANS gives a detailed picture of the magnetization process, which could not be obtained by methods of standard magnetometry.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Polarized small-angle neutron scattering study of two-dimensional spatially ordered systems of nickel nanowires</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>532</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>536</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6025">
    <title>Spin-echo small-angle neutron scattering study of the domain structure of an Ni layer on a Cu substrate</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6025</link>
    <description>Spin-echo small-angle neutron scattering (SESANS) is used to study the magnetic domain structure of an Ni layer electrodeposited onto a Cu substrate. The domain structure of the sample corresponds to the hard-plane model, where the magnetization in the domains is directed perpendicular to the layer; the domain length coincides with the thickness of the layer of the order of 10 µm and its width is of the order of 1 µm. The pair correlation function of the magnetization has been directly measured. It is established that the width of the domain depends linearly on its thickness. The domain structure does not depend on heating at temperatures below T_{\rm C} of nickel. Annealing at T\, \gt\, T_{\rm C} results in a reconstruction of the domain structure with a tendency to the easy-plane model, i.e. with domain magnetization in the plane. The multiple scattering effect is studied and may be taken into account. This experiment demonstrates the possibilities of magnetic SESANS. Some aspects of this novel technique are pointed out.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Grigoriev, S.V.</dc:creator>
    <dc:creator>Chetverikov, Y.O.</dc:creator>
    <dc:creator>Zabenkin, V.N.</dc:creator>
    <dc:creator>Kraan, W.H.</dc:creator>
    <dc:creator>Rekveldt, M.T.</dc:creator>
    <dc:creator>van Dijk, N.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005249</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Spin-echo small-angle neutron scattering is used to study the magnetic domain structure of an Ni layer on a Cu substrate. The experiments demonstrate the possibilities of this novel technique.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SPIN-ECHO SMALL-ANGLE NEUTRON SCATTERING; SESANS; MAGNETIC DOMAINS; HARD-PLANE MODEL</dc:subject>
    <dc:description>Spin-echo small-angle neutron scattering (SESANS) is used to study the magnetic domain structure of an Ni layer electrodeposited onto a Cu substrate. The domain structure of the sample corresponds to the hard-plane model, where the magnetization in the domains is directed perpendicular to the layer; the domain length coincides with the thickness of the layer of the order of 10 µm and its width is of the order of 1 µm. The pair correlation function of the magnetization has been directly measured. It is established that the width of the domain depends linearly on its thickness. The domain structure does not depend on heating at temperatures below T_{\rm C} of nickel. Annealing at T\, \gt\, T_{\rm C} results in a reconstruction of the domain structure with a tendency to the easy-plane model, i.e. with domain magnetization in the plane. The multiple scattering effect is studied and may be taken into account. This experiment demonstrates the possibilities of magnetic SESANS. Some aspects of this novel technique are pointed out.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Spin-echo small-angle neutron scattering study of the domain structure of an Ni layer on a Cu substrate</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>111</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>115</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6021">
    <title>Microstructural investigation of low-dose neutron irradiation effects in martensitic steels for nuclear application by means of small-angle neutron scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6021</link>
    <description>The microstructural effect of low-dose neutron irradiation and subsequent high-temperature tempering in the reduced activation ferritic/martensitic steel F82H-mod. (7.73 Cr, 0.09 C, 0.08 Mn, 0.19 V, 2.06 W, 0.02 Ta, wt%, bal. Fe) has been studied using small-angle neutron scattering (SANS). The investigated samples were irradiated with thermal neutrons at 523 K, to dose levels of 2.4 displacements per atom then tempered for 2 h at 1043 K. The SANS measurements were carried out at the D22 instrument of the High Flux Reactor at the Institut Max von Laue–Paul Langevin, Grenoble, France. The differences observed in nuclear and magnetic small-angle neutron scattering cross-sections after subtraction of the reference sample from the irradiated one suggest that the irradiation and the subsequent post-irradiation tempering produce the growth of non-magnetic precipitates; the results are also compared with those obtained on other ferritic/martensitic steels, with different chemical composition, irradiated under the same conditions.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Coppola, R.</dc:creator>
    <dc:creator>Lindau, R.</dc:creator>
    <dc:creator>May, R.P.</dc:creator>
    <dc:creator>Möslang, A.</dc:creator>
    <dc:creator>Valli, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005110</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The microstructural effect of low-dose neutron irradiation in ferritic/martensitic steels has been investigated by means of small-angle neutron scattering: depending on the initial steel composition different microstructural evolutions are observed during post-irradiation tempering.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SMALL-ANGLE NEUTRON SCATTERING; RADIATION DAMAGE; MARTENSITIC STEELS</dc:subject>
    <dc:description>The microstructural effect of low-dose neutron irradiation and subsequent high-temperature tempering in the reduced activation ferritic/martensitic steel F82H-mod. (7.73 Cr, 0.09 C, 0.08 Mn, 0.19 V, 2.06 W, 0.02 Ta, wt%, bal. Fe) has been studied using small-angle neutron scattering (SANS). The investigated samples were irradiated with thermal neutrons at 523 K, to dose levels of 2.4 displacements per atom then tempered for 2 h at 1043 K. The SANS measurements were carried out at the D22 instrument of the High Flux Reactor at the Institut Max von Laue–Paul Langevin, Grenoble, France. The differences observed in nuclear and magnetic small-angle neutron scattering cross-sections after subtraction of the reference sample from the irradiated one suggest that the irradiation and the subsequent post-irradiation tempering produce the growth of non-magnetic precipitates; the results are also compared with those obtained on other ferritic/martensitic steels, with different chemical composition, irradiated under the same conditions.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Microstructural investigation of low-dose neutron irradiation effects in martensitic steels for nuclear application by means of small-angle neutron scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>142</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>146</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6006">
    <title>Unraveling the equilibrium chain exchange kinetics of polymeric micelles using small-angle neutron scattering – architectural and topological effects</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6006</link>
    <description>In this paper, we present a study of micellar structures formed by poly(styrene)-poly(butadiene) (PS10-PB10; the numbers indicate the molecular weight in kg mol−1) diblock copolymers and PB10-PS20-PB10 triblock copolymers in different n-alkane solvents. Particular emphasis is placed on the dynamic properties of these micelles under equilibrium which are studied using a novel time-resolved small-angle neutron scattering technique. The results show that the structures of the micelles are very similar for both the diblock and triblock copolymers, which allows a direct comparison of the dynamic properties. A novel logarithmic relaxation is found for both the triblock and the diblock micelles which is not consistent with theoretical expectations. However, for the diblock micelles, the relaxation kinetics seem to approach the rate and the single exponential decay predicted by Halperin &amp; Alexander [Macromolecules, (1989), 22, 2403–2412] when the micellar cores are strongly swollen with solvent. For the triblock micelles a logarithmic relaxation is found for all cases as an effect of additional topological knots present even in highly swollen micellar cores. This behavior is assigned to an increased coupling of chain motion within the dense confined core – an effect which seems to vanish in diblock micelles when the core is sufficiently swollen.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Lund, R.</dc:creator>
    <dc:creator>Willner, L.</dc:creator>
    <dc:creator>Richter, D.</dc:creator>
    <dc:creator>Iatrou, H.</dc:creator>
    <dc:creator>Hadjichristidis, N.</dc:creator>
    <dc:creator>Lindner, P.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005201</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Using time-resolved small-angle neutron scattering it is possible to extract the equilibrium exchange kinetics of polymeric micelles. This paper provides insight into the effect of topological constraints on the expulsion time by comparing results from A-B diblock and A-B-A triblock copolymer micelles.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TIME-RESOLVED SMALL-ANGLE NEUTRON SCATTERING; MICELLES; EXCHANGE KINETICS; POLYMERS</dc:subject>
    <dc:description>In this paper, we present a study of micellar structures formed by poly(styrene)-poly(butadiene) (PS10-PB10; the numbers indicate the molecular weight in kg mol−1) diblock copolymers and PB10-PS20-PB10 triblock copolymers in different n-alkane solvents. Particular emphasis is placed on the dynamic properties of these micelles under equilibrium which are studied using a novel time-resolved small-angle neutron scattering technique. The results show that the structures of the micelles are very similar for both the diblock and triblock copolymers, which allows a direct comparison of the dynamic properties. A novel logarithmic relaxation is found for both the triblock and the diblock micelles which is not consistent with theoretical expectations. However, for the diblock micelles, the relaxation kinetics seem to approach the rate and the single exponential decay predicted by Halperin &amp; Alexander [Macromolecules, (1989), 22, 2403–2412] when the micellar cores are strongly swollen with solvent. For the triblock micelles a logarithmic relaxation is found for all cases as an effect of additional topological knots present even in highly swollen micellar cores. This behavior is assigned to an increased coupling of chain motion within the dense confined core – an effect which seems to vanish in diblock micelles when the core is sufficiently swollen.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Unraveling the equilibrium chain exchange kinetics of polymeric micelles using small-angle neutron scattering – architectural and topological effects</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>327</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>331</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6015">
    <title>Residual orientation in micro-injection molded parts</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6015</link>
    <description>The residual orientation following micro-injection molding of small rectangular plates with linear polyethylene has been examined using small-angle neutron scattering, and small- and wide-angle X-ray scattering. The effect of changing the molding conditions has been examined, and the residual chain orientation has been compared to the residual orientation of the crystallites as a function of position in the sample. This study has found that, for micromoldings, the orientation of the crystallites decreases with increasing injection speed and increasing mold thickness. The combined data suggest that the majority of the orientation present comes from oriented crystal growth rather than residual chain orientation.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Healy, J.</dc:creator>
    <dc:creator>Edward, G.H.</dc:creator>
    <dc:creator>Knott, R.B.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807005080</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The residual orientation in micro-injection molded polyethylene parts was examined using small-angle neutron scattering, and small- and wide-angle X-ray scattering. The primary cause of residual orientation was found to be oriented crystal growth rather than chain orientation resulting from the injection molding process.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; WAXS; SANS; INJECTION MOLDING; POLYETHYLENE</dc:subject>
    <dc:description>The residual orientation following micro-injection molding of small rectangular plates with linear polyethylene has been examined using small-angle neutron scattering, and small- and wide-angle X-ray scattering. The effect of changing the molding conditions has been examined, and the residual chain orientation has been compared to the residual orientation of the crystallites as a function of position in the sample. This study has found that, for micromoldings, the orientation of the crystallites decreases with increasing injection speed and increasing mold thickness. The combined data suggest that the majority of the orientation present comes from oriented crystal growth rather than residual chain orientation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Residual orientation in micro-injection molded parts</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>393</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>396</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6005">
    <title>On the heterogeneous character of water's amorphous polymorphism</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6005</link>
    <description>In this paper we report in situ small-angle neutron scattering results on the high-density amorphous (HDA) and low-density amorphous (LDA) ice structures and on intermediate structures as found during the temperature-induced transformation of HDA into LDA. We show that the small-angle signal is characterized by two Q regimes featuring different properties [Q is the modulus of the scattering vector defined as Q = (4\pi/\lambda_{\rm i})\sin(\theta) with \theta being half the scattering angle and \lambda_{\rm i} the incident neutron wavelength]. The very low Q regime (\lt\, \sim \!5\times 10^{-2} Å−1) is dominated by a Porod-limit scattering. Its intensity reduces during the course of the HDA-to-LDA transformation following kinetics reminiscent of those observed in wide-angle diffraction experiments. The small-angle neutron scattering form factor in the intermediate regime of 5 \times 10^{-2} \,\lt\, Q \,\lt\, 0.5 Å−1 for HDA and LDA features a rather flat plateau. However, the HDA signal shows an ascending intensity towards smaller Q marking this amorphous structure as heterogeneous. When following the HDA-to-LDA transition, the form factor shows a pronounced transient excess in intensity marking all intermediate structures as strongly heterogeneous on a length scale of some nanometres.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Koza, M.M.</dc:creator>
    <dc:creator>May, R.P.</dc:creator>
    <dc:creator>Schober, H.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807004992</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Two spatial regimes of structural heterogeneity have been identified in amorphous ice structures by small-angle neutron scattering experiments. These are a transient contrast change on a nanometre scale being equally reflected by changes in diffraction data, and a Porod-limit scattering on a micrometre scale demonstrating the presence of interfaces in the amorphous samples.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AMORPHOUS POLYMORPHISM; WATER; SANS; ICE</dc:subject>
    <dc:description>In this paper we report in situ small-angle neutron scattering results on the high-density amorphous (HDA) and low-density amorphous (LDA) ice structures and on intermediate structures as found during the temperature-induced transformation of HDA into LDA. We show that the small-angle signal is characterized by two Q regimes featuring different properties [Q is the modulus of the scattering vector defined as Q = (4\pi/\lambda_{\rm i})\sin(\theta) with \theta being half the scattering angle and \lambda_{\rm i} the incident neutron wavelength]. The very low Q regime (\lt\, \sim \!5\times 10^{-2} Å−1) is dominated by a Porod-limit scattering. Its intensity reduces during the course of the HDA-to-LDA transformation following kinetics reminiscent of those observed in wide-angle diffraction experiments. The small-angle neutron scattering form factor in the intermediate regime of 5 \times 10^{-2} \,\lt\, Q \,\lt\, 0.5 Å−1 for HDA and LDA features a rather flat plateau. However, the HDA signal shows an ascending intensity towards smaller Q marking this amorphous structure as heterogeneous. When following the HDA-to-LDA transition, the form factor shows a pronounced transient excess in intensity marking all intermediate structures as strongly heterogeneous on a length scale of some nanometres.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>On the heterogeneous character of water's amorphous polymorphism</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>517</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>521</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6009">
    <title>Structural study of nanocrystalline nickel thin films</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6009</link>
    <description>Nickel thin films (400 nm) were deposited by magnetron sputtering onto fused silica substrates. The effects of argon pressure and substrate temperature (from room temperature to 973 K) upon the film structure were investigated. The film structure was studied using grazing-incidence small-angle X-ray scattering (GISAXS) and X-ray diffraction (XRD) analysis. It was found that the prepared nanocrystalline Ni films contain two kinds of inhomogeneities observable by GISAXS, namely isotropic and platelet-like. Up to about 373 K the isotropic or spherical `particles' prevail, while above that temperature the platelet-like `particles' predominate. These inhomogeneities are ascribed to intergranular matter or grain boundaries, since the grain size (as determined from the XRD patterns) was found to increase from 7 nm in samples deposited at room temperature to about 90 nm in samples deposited at 423 K or higher temperature.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Radic, N.</dc:creator>
    <dc:creator>Dubcek, P.</dc:creator>
    <dc:creator>Bernstorff, S.</dc:creator>
    <dc:creator>Djerdj, I.</dc:creator>
    <dc:creator>Tonejc, A.M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807004682</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Nanocrystalline nickel thin films have been prepared by magnetron sputtering, and have been studied by X-ray diffraction, grazing-incidence small-angle X-ray scattering and atomic force microscopy. Results are given for nanocrystalline Ni (average grain size, unit-cell parameter), intercrystalline matter (size and shape of inhomogeneities) and surface topography of the prepared samples.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>NANOCRYSTALLINE NICKEL; THIN FILMS; GISAXS; XRD; SURFACE TOPOGRAPHY; ATOMIC FORCE MICROSCOPY</dc:subject>
    <dc:description>Nickel thin films (400 nm) were deposited by magnetron sputtering onto fused silica substrates. The effects of argon pressure and substrate temperature (from room temperature to 973 K) upon the film structure were investigated. The film structure was studied using grazing-incidence small-angle X-ray scattering (GISAXS) and X-ray diffraction (XRD) analysis. It was found that the prepared nanocrystalline Ni films contain two kinds of inhomogeneities observable by GISAXS, namely isotropic and platelet-like. Up to about 373 K the isotropic or spherical `particles' prevail, while above that temperature the platelet-like `particles' predominate. These inhomogeneities are ascribed to intergranular matter or grain boundaries, since the grain size (as determined from the XRD patterns) was found to increase from 7 nm in samples deposited at room temperature to about 90 nm in samples deposited at 423 K or higher temperature.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Structural study of nanocrystalline nickel thin films</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>377</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>382</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6044">
    <title>Melting behavior of polymorphic crystals of poly(trimethylene 2,6-naphthalate) studied by simultaneous synchrotron X-ray scattering and thermal analysis</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6044</link>
    <description>The polymorphic crystallization and melting behavior of poly(trimethylene 2,6-naphthalate) (PTN) have been investigated using small-angle X-ray scattering and simultaneous wide-angle X-ray scattering (WAXS) and differential scanning calorimetry (DSC). The α-crystal, the β-crystal and the coexistence of both crystal forms of PTN develop at an isothermal temperature below 393 K, above 453 K and between these two temperatures, respectively. The simultaneous WAXS/DSC measurement provides a good way to identify the origin of multiple melting peaks and to get equilibrium melting temperatures. During the PTN melting process, the thermal evolutions of crystallinities, Bragg diffraction intensities and DSC thermograms reveal that the \alpha \rightarrow \beta phase transformation and primary and secondary crystallizations arise to generate the multiple melting peaks. The β-crystal with high equilibrium melting temperature (T^{0}_{{\rm m},\beta}} = 510 K) is a structurally stable phase while the α-crystal with low equilibrium melting temperature (T^{0}_{{\rm m},\alpha}} = 488 K) is a metastable phase. The temperature-dependent structural parameters such as the long period, lamellar thickness and amorphous thickness were extracted from the interface distribution function. Two-step changes in the lamellar thickness and the invariant during the subsequent melting of PTN crystallized at 383 K are consistent with the \alpha \rightarrow \beta transformation obtained by WAXS/DSC. The \alpha \rightarrow \beta transformation, a typical melting–recrystallization, proceeds firstly via surface melting of α-lamellae, and then the PTN chains near the boundaries of surviving α-lamellae modify their conformation to form the β-crystal resulting in thickening lamellae.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Chuang, W.-T.</dc:creator>
    <dc:creator>Hong, P.-D.</dc:creator>
    <dc:creator>Chen, C.-H.</dc:creator>
    <dc:creator>Sheu, H.-S.</dc:creator>
    <dc:creator>Jeng, U.-S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S002188980700461X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The polymorphic crystallization and melting behavior of poly(trimethylene 2,6-naphthalate) have been investigated using small-angle X-ray scattering and simultaneous wide-angle X-ray scattering and differential scanning calorimetry.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLY(TRIMETHYLENE 2,6-NAPHTHALATE); SYNCHROTRON X-RAY SCATTERING; POLYMORPHISM; MULTIPLE MELTING BEHAVIOR</dc:subject>
    <dc:description>The polymorphic crystallization and melting behavior of poly(trimethylene 2,6-naphthalate) (PTN) have been investigated using small-angle X-ray scattering and simultaneous wide-angle X-ray scattering (WAXS) and differential scanning calorimetry (DSC). The α-crystal, the β-crystal and the coexistence of both crystal forms of PTN develop at an isothermal temperature below 393 K, above 453 K and between these two temperatures, respectively. The simultaneous WAXS/DSC measurement provides a good way to identify the origin of multiple melting peaks and to get equilibrium melting temperatures. During the PTN melting process, the thermal evolutions of crystallinities, Bragg diffraction intensities and DSC thermograms reveal that the \alpha \rightarrow \beta phase transformation and primary and secondary crystallizations arise to generate the multiple melting peaks. The β-crystal with high equilibrium melting temperature (T^{0}_{{\rm m},\beta}} = 510 K) is a structurally stable phase while the α-crystal with low equilibrium melting temperature (T^{0}_{{\rm m},\alpha}} = 488 K) is a metastable phase. The temperature-dependent structural parameters such as the long period, lamellar thickness and amorphous thickness were extracted from the interface distribution function. Two-step changes in the lamellar thickness and the invariant during the subsequent melting of PTN crystallized at 383 K are consistent with the \alpha \rightarrow \beta transformation obtained by WAXS/DSC. The \alpha \rightarrow \beta transformation, a typical melting–recrystallization, proceeds firstly via surface melting of α-lamellae, and then the PTN chains near the boundaries of surviving α-lamellae modify their conformation to form the β-crystal resulting in thickening lamellae.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Melting behavior of polymorphic crystals of poly(trimethylene 2,6-naphthalate) studied by simultaneous synchrotron X-ray scattering and thermal analysis</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>637</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>641</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6018">
    <title>Fractal aggregates of the Pt nanoparticles synthesized by the polyol process and poly(N-vinyl-2-pyrrolidone) reduction</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6018</link>
    <description>Small-angle X-ray scattering was used to characterize the size and aggregation behavior of the Pt nanoparticles synthesized by the polyol process and the unusual poly(N-vinyl-2-pyrrolidone) (PVP) reduction. With formaldehyde (HCHO) as the reduction agent, the Pt nanoparticles synthesized in aqueous solutions with a high PVP/PtCl4 weight ratio were characterized by short rods with a 70% polydispersity in rod length. The size and size distribution of the rod-like Pt nanoparticles (3 nm in rod length and 2 nm in rod diameter) are consistent with the corresponding transmission electron microscopy image. With a comparable PVP/PtCl4 weight ratio in the aqueous solution containing HCHO, the high number density of reduced Pt nanoparticles led to a fractal-like aggregation with a fractal dimension of 2.1 and a correlation length of ~30 nm. We also demonstrated that Pt nanoparticles can be synthesized by PVP reduction at 323 K without HCHO. The particle size and the clustering behavior of the Pt nanoparticles reduced by PVP are closely related to the PVP concentration in the solution. Both the Pt nanoparticles synthesized in the commonly used polyol process and the unusual PVP reduction form fractal-like clusters via the PVP–metal nanoparticle association when the number density of the Pt nanoparticles in the solutions is high.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Lin, J.-M.</dc:creator>
    <dc:creator>Lin, T.-L.</dc:creator>
    <dc:creator>Jeng, U.-S.</dc:creator>
    <dc:creator>Zhong, Y.-J.</dc:creator>
    <dc:creator>Yeh, C.-T.</dc:creator>
    <dc:creator>Chen, T.-Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807004426</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Small-angle X-ray scattering was used to characterize the size and aggregation behavior of the Pt nanoparticles synthesized in the polyol process and the unusual poly(N-vinyl-2-pyrrolidone) reduction.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLYOL PROCESS; PLATINUM NANOPARTICLES; FRACTAL AGGREGATION; SAXS</dc:subject>
    <dc:description>Small-angle X-ray scattering was used to characterize the size and aggregation behavior of the Pt nanoparticles synthesized by the polyol process and the unusual poly(N-vinyl-2-pyrrolidone) (PVP) reduction. With formaldehyde (HCHO) as the reduction agent, the Pt nanoparticles synthesized in aqueous solutions with a high PVP/PtCl4 weight ratio were characterized by short rods with a 70% polydispersity in rod length. The size and size distribution of the rod-like Pt nanoparticles (3 nm in rod length and 2 nm in rod diameter) are consistent with the corresponding transmission electron microscopy image. With a comparable PVP/PtCl4 weight ratio in the aqueous solution containing HCHO, the high number density of reduced Pt nanoparticles led to a fractal-like aggregation with a fractal dimension of 2.1 and a correlation length of ~30 nm. We also demonstrated that Pt nanoparticles can be synthesized by PVP reduction at 323 K without HCHO. The particle size and the clustering behavior of the Pt nanoparticles reduced by PVP are closely related to the PVP concentration in the solution. Both the Pt nanoparticles synthesized in the commonly used polyol process and the unusual PVP reduction form fractal-like clusters via the PVP–metal nanoparticle association when the number density of the Pt nanoparticles in the solutions is high.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Fractal aggregates of the Pt nanoparticles synthesized by the polyol process and poly(N-vinyl-2-pyrrolidone) reduction</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>540</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>543</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6017">
    <title>Simplified tube form factor for analysis of small-angle scattering data from carbon nanotube filled systems</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6017</link>
    <description>This work presents an analysis method for small-angle scattering data utilizing a simplified tube (hollow cylinder) form factor. The simplified form factor captures the rod-like character of a tube at long length scales (one-dimensional), the sheet-like character of the tube wall at intermediate length scales (two-dimensional), and the surface characteristics of a tube at small length scales while suppressing the deep minima seen in the exact form factor. Ultra-small-angle X-ray scattering data from composites made with multi-walled carbon nanotubes and a bismaleimide resin are analyzed using the simplified form factor and compared with scanning electron micrographs. Although a hollow core is not evident via microscopy, a solid rod form factor does not fit the data. However, a tube form factor does fit the data and generates reasonable geometric parameters. At higher concentrations, evidence for aggregation is seen in the data. Aggregation is accommodated by including a fractal structure factor within the simplified approach, allowing facile analysis of data from aggregated (poorly dispersed) fillers.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Justice, R.S.</dc:creator>
    <dc:creator>Wang, D.H.</dc:creator>
    <dc:creator>Tan, L.-S.</dc:creator>
    <dc:creator>Schaefer, D.W.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807004153</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A simplified tube (hollow cylinder) form factor is developed and utilized to analyze ultra-small-angle X-ray scattering data obtained from multi-walled carbon nanotube/bismaleimide composite samples. The form factor is useful for distinguishing between hollow and solid cylinders as well for detecting the presence of aggregation of one-dimensional colloidal fillers in polymers.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CARBON NANOTUBES; DISPERSION; SMALL-ANGLE SCATTERING; CYLINDERS; HOLLOW CYLINDER; FORM FACTOR</dc:subject>
    <dc:description>This work presents an analysis method for small-angle scattering data utilizing a simplified tube (hollow cylinder) form factor. The simplified form factor captures the rod-like character of a tube at long length scales (one-dimensional), the sheet-like character of the tube wall at intermediate length scales (two-dimensional), and the surface characteristics of a tube at small length scales while suppressing the deep minima seen in the exact form factor. Ultra-small-angle X-ray scattering data from composites made with multi-walled carbon nanotubes and a bismaleimide resin are analyzed using the simplified form factor and compared with scanning electron micrographs. Although a hollow core is not evident via microscopy, a solid rod form factor does not fit the data. However, a tube form factor does fit the data and generates reasonable geometric parameters. At higher concentrations, evidence for aggregation is seen in the data. Aggregation is accommodated by including a fractal structure factor within the simplified approach, allowing facile analysis of data from aggregated (poorly dispersed) fillers.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Simplified tube form factor for analysis of small-angle scattering data from carbon nanotube filled systems</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>88</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>92</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6028">
    <title>In situ and time-resolved ultra small-angle neutron scattering observation on growing poly(methyl methacrylate)-block-polystyrene via reversible addition–fragmentation chain transfer living radical polymerization</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6028</link>
    <description>Reversible addition–fragmentation chain transfer (RAFT) living radical polymerization of poly(methyl methacrylate)-block-polystyrene (PMMA-b-PS) was investigated by a combined method of gel permeation chromatography (GPC) and in situ and time-resolved ultra small-angle neutron scattering (tr-USANS) measurements. GPC enables us to examine a growing single molecule as a function of polymerization time, with respect to monomer conversion, molecular weight (Mn) and polydispersity index (Mw/Mn) of PMMA-b-PS. On the other hand, tr-USANS, observing in meso-length scales from nm to µm, reveals polymerization-induced molecular self-assembly, such as microphase separation by PMMA-b-PS or macrophase separation between PMMA-b-PS and homo-polystyrene (by-product). By combining these two experimental methods, we elucidated that RAFT living polymerization was retarded by micro- and macrophase separations.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Motokawa, R.</dc:creator>
    <dc:creator>Koizumi, S.</dc:creator>
    <dc:creator>Zhao, Y.</dc:creator>
    <dc:creator>Hashimoto, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807004062</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>We investigated the time evolution of polymerization-induced molecular self-assembly, appearing in a reaction solution of living radical polymerization of poly(methyl methacrylate)-block-polystyrene by employing in situ and time-resolved ultra small-angle neutron scattering and time-resolved gel permeation chromatography methods.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLYMERIZATION-INDUCED MOLECULAR SELF-ASSEMBLY; REVERSIBLE ADDITION-FRAGMENTATION CHAIN TRANSFER POLYMERIZATION; LIVING RADICAL POLYMERIZATION; ULTRA SMALL-ANGLE NEUTRON SCATTERING; POLY(METHYL METHACRYLATE)-BLOCK-POLYSTYRENE</dc:subject>
    <dc:description>Reversible addition–fragmentation chain transfer (RAFT) living radical polymerization of poly(methyl methacrylate)-block-polystyrene (PMMA-b-PS) was investigated by a combined method of gel permeation chromatography (GPC) and in situ and time-resolved ultra small-angle neutron scattering (tr-USANS) measurements. GPC enables us to examine a growing single molecule as a function of polymerization time, with respect to monomer conversion, molecular weight (Mn) and polydispersity index (Mw/Mn) of PMMA-b-PS. On the other hand, tr-USANS, observing in meso-length scales from nm to µm, reveals polymerization-induced molecular self-assembly, such as microphase separation by PMMA-b-PS or macrophase separation between PMMA-b-PS and homo-polystyrene (by-product). By combining these two experimental methods, we elucidated that RAFT living polymerization was retarded by micro- and macrophase separations.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>In situ and time-resolved ultra small-angle neutron scattering observation on growing poly(methyl methacrylate)-block-polystyrene via reversible addition–fragmentation chain transfer living radical polymerization</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>645</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>649</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cg5057">
    <title>From CIF to virtual morphology using the WinXMorph program</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cg5057</link>
    <description>Crystal morphologies are predicted from data stored in files in the CIF format (crystallographic information file standard of the International Union of Crystallography) on the basis of the Bravais–Friedel, Donnay–Harker model. Several simple improvements to the calculation are introduced with Win­XMorph, version 1.4.9, in conjunction with illustrations of the morphologies of quartz, sucrose, lactose, pyrite and lysozyme. The morphologies of the recently discovered pentamorphs of 1,8-dihydroxyanthraquinone are predicted. Win­XMorph is available free-of-charge for educational use.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Kaminsky, W.</dc:creator>
    <dc:date>2007-04-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003986</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Crystal morphologies are predicted from data stored in files in CIF format on the basis of the Bravais–Friedel, Donnay–Harker model.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>GROWTH MODELS; CRYSTAL MORPHOLOGY; OPTICAL MICROSCOPY; SINGLE-CRYSTAL GROWTH; NATURAL CRYSTAL GROWTH; LYSOZYME</dc:subject>
    <dc:description>Crystal morphologies are predicted from data stored in files in the CIF format (crystallographic information file standard of the International Union of Crystallography) on the basis of the Bravais–Friedel, Donnay–Harker model. Several simple improvements to the calculation are introduced with Win­XMorph, version 1.4.9, in conjunction with illustrations of the morphologies of quartz, sucrose, lactose, pyrite and lysozyme. The morphologies of the recently discovered pentamorphs of 1,8-dihydroxyanthraquinone are predicted. Win­XMorph is available free-of-charge for educational use.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>From CIF to virtual morphology using the WinXMorph program</dc:title>
    <dc:type>text</dc:type>
    <prism:number>2</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>CIF applications</prism:section>
    <prism:startingPage>382</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>385</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6037">
    <title>A focusing-geometry small-angle neutron scattering instrument with a magnetic neutron lens</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6037</link>
    <description>We have constructed a focusing-geometry small-angle neutron scattering (FSANS) instrument, SANS-J-II, with two kinds of neutron focusing device: a series of compound refractive lenses made of MgF2 and a magnetic neutron lens based on an extended Halbach-type sextupole magnet. In this study, we investigated the performance of the FSANS instrument with the magnetic neutron lens. The intensity distribution of a direct neutron beam focused on the detector plane by the magnetic neutron lens had a ratio of the peak height to the background level of \sim\!6\times 10^4 for a polarized neutron beam with a polarization degree of \sim \!0.99. It is found that a minimum value of the measurable q range [where q is the modulus of the scattering vector and is defined as q = (4\pi/\lambda)\sin(\theta/2), where \theta is the scattering angle and \lambda is the neutron wavelength], q_{\rm min}, of 6.5 \times 10^{-4} Å−1 can be achieved by the FSANS instrument with the magnetic neutron lens using neutrons with \lambda = 6.6 Å and \Delta \lambda/\lambda = 0.13 for the full width at half maximum.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Oku, T.</dc:creator>
    <dc:creator>Iwase, H.</dc:creator>
    <dc:creator>Shinohara, T.</dc:creator>
    <dc:creator>Yamada, S.</dc:creator>
    <dc:creator>Hirota, K.</dc:creator>
    <dc:creator>Koizumi, S.</dc:creator>
    <dc:creator>Suzuki, J.-</dc:creator>
    <dc:creator>Hashimoto, T.</dc:creator>
    <dc:creator>Shimizu, H.M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003822</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A focusing-geometry small-angle neutron scattering (FSANS) instrument with a magnetic neutron lens based on an extended Halbach-type sextupole magnet has been constructed and tested. A minimum value of the measurable q range, q_{\rm min}, of 6.5 \times 10^{-4} Å−1 could be achieved by the FSANS instrument using a neutron wavelength \lambda = 6.6 Å with \Delta \lambda/\lambda = 0.13 for the full width at half maximum.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>FOCUSING-GEOMETRY SANS; MAGNETIC NEUTRON LENS; INSTRUMENTATION; SANS-J-II</dc:subject>
    <dc:description>We have constructed a focusing-geometry small-angle neutron scattering (FSANS) instrument, SANS-J-II, with two kinds of neutron focusing device: a series of compound refractive lenses made of MgF2 and a magnetic neutron lens based on an extended Halbach-type sextupole magnet. In this study, we investigated the performance of the FSANS instrument with the magnetic neutron lens. The intensity distribution of a direct neutron beam focused on the detector plane by the magnetic neutron lens had a ratio of the peak height to the background level of \sim\!6\times 10^4 for a polarized neutron beam with a polarization degree of \sim \!0.99. It is found that a minimum value of the measurable q range [where q is the modulus of the scattering vector and is defined as q = (4\pi/\lambda)\sin(\theta/2), where \theta is the scattering angle and \lambda is the neutron wavelength], q_{\rm min}, of 6.5 \times 10^{-4} Å−1 can be achieved by the FSANS instrument with the magnetic neutron lens using neutrons with \lambda = 6.6 Å and \Delta \lambda/\lambda = 0.13 for the full width at half maximum.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A focusing-geometry small-angle neutron scattering instrument with a magnetic neutron lens</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>408</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>413</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6029">
    <title>Contrast variation in X-ray and neutron scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6029</link>
    <description>This contribution is meant to highlight some progress in those areas of contrast variation which are known to be technically more difficult but which promise interesting applications. These concern the use of the anomalous dispersion of light elements, like sulfur and phosphorus in structural studies and experiments of polarized neutron scattering from nuclear spin polarized samples.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Stuhrmann, H.B.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003718</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Methods of contrast variation in X-ray and neutron scattering are reviewed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>RESONANT CONTRAST; PHOSPHORUS; NUCLEAR SPIN CONTRAST; HYDROGEN</dc:subject>
    <dc:description>This contribution is meant to highlight some progress in those areas of contrast variation which are known to be technically more difficult but which promise interesting applications. These concern the use of the anomalous dispersion of light elements, like sulfur and phosphorus in structural studies and experiments of polarized neutron scattering from nuclear spin polarized samples.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Contrast variation in X-ray and neutron scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>23</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>27</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6022">
    <title>Homodyne and heterodyne X-ray photon correlation spectroscopy: latex particles and elastomers</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6022</link>
    <description>In a coherent X-ray small-angle experiment, heterodyning between the scattering amplitudes of two samples is obtained by stacking a static reference and a fluctuating sample. Results of homodyne and heterodyne measurements are compared in the case of 98 nm diameter latex particles in glycerol. The method is also used for the study of the slow relaxation process of carbon-black-filled ethylene–propylene elastomers corresponding to the relaxation of the carbon black skeleton after a 100% elongation. On the scale of the 10 µm coherent beam, heterodyning is used to separate fluctuations from long-term flowing of the sample. We show that this flow can be observed for about 10 h, with velocities of the order of nanometres per second. Random fluctuations are dominant in the speckle changes only for large q values (q &gt; 2 × 10−2 Å−1) and after a long relaxation time.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Livet, F.</dc:creator>
    <dc:creator>Bley, F.</dc:creator>
    <dc:creator>Ehrburger-Dolle, F.</dc:creator>
    <dc:creator>Morfin, I.</dc:creator>
    <dc:creator>Geissler, E.</dc:creator>
    <dc:creator>Sutton, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003561</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Interferences are observed in coherent X-ray small-angle scattering between a static reference and a fluctuating sample. Heterodyning makes possible the observation of Doppler shifts with sample drift velocities in the nanometres per second range.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>COHERENT X-RAY BEAMS; DYNAMICS OF RUBBERS; HETERODYNING; SMALL-ANGLE X-RAY SCATTERING; LATEX</dc:subject>
    <dc:description>In a coherent X-ray small-angle experiment, heterodyning between the scattering amplitudes of two samples is obtained by stacking a static reference and a fluctuating sample. Results of homodyne and heterodyne measurements are compared in the case of 98 nm diameter latex particles in glycerol. The method is also used for the study of the slow relaxation process of carbon-black-filled ethylene–propylene elastomers corresponding to the relaxation of the carbon black skeleton after a 100% elongation. On the scale of the 10 µm coherent beam, heterodyning is used to separate fluctuations from long-term flowing of the sample. We show that this flow can be observed for about 10 h, with velocities of the order of nanometres per second. Random fluctuations are dominant in the speckle changes only for large q values (q &gt; 2 × 10−2 Å−1) and after a long relaxation time.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Homodyne and heterodyne X-ray photon correlation spectroscopy: latex particles and elastomers</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>38</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>42</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6011">
    <title>Precursory microstructures in Zr–Cu–Al–Ni bulk metallic glasses examined by anomalous small-angle scattering at the Zr K edge</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6011</link>
    <description>Anomalous small-angle X-ray scattering measurements of Zr–Cu–Al–Ni quaternary alloys have been made at the Zr K absorption edge. In melt-quenched samples, small cluster components without crystallization were found. The contrast change at the edge suggested that compositional fluctuation of Al is incorporated.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Okuda, H.</dc:creator>
    <dc:creator>Murase, I.</dc:creator>
    <dc:creator>Ochiai, S.</dc:creator>
    <dc:creator>Saida, J.</dc:creator>
    <dc:creator>Yokoyama, Y.</dc:creator>
    <dc:creator>Inoue, K.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003524</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Microstructures in Zr–Cu–Al–Ni bulk metallic glasses consisting only of metallic elements have been examined by anomalous small-angle scattering at the Zr K edge. The cluster-like scattering was analysed in terms of composition fluctuation.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ANOMALOUS SMALL-ANGLE SCATTERING; BULK METALLIC GLASSES; ZR-CU-AL-NI ALLOYS; PRECURSORY STRUCTURES</dc:subject>
    <dc:description>Anomalous small-angle X-ray scattering measurements of Zr–Cu–Al–Ni quaternary alloys have been made at the Zr K absorption edge. In melt-quenched samples, small cluster components without crystallization were found. The contrast change at the edge suggested that compositional fluctuation of Al is incorporated.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Precursory microstructures in Zr–Cu–Al–Ni bulk metallic glasses examined by anomalous small-angle scattering at the Zr K edge</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>138</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>141</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6012">
    <title>A modified Ising model for the thermodynamic properties of local and global protein folding–unfolding observed by circular dichroism and small-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6012</link>
    <description>Based on the mean-field approximation, we have applied a modified Ising model to describe general protein unfolding behavior at thermodynamic equilibrium with the free energy contributed by the subgroup units (amino acids or peptide bonds) of the protein. With the thermodynamic properties of the protein, this model can associate the stepwise change of an unfolding fraction ratio profile with the local and global conformation unfolding. Taking cytochrome c (cyt c) as a model protein, we have observed, using small-angle X-ray scattering and circular dichroism (CD), the global and local structure changes for the protein in three kinds of denaturant environments: acid, urea and guanidine hydrochloride. The small-angle X-ray scattering and CD results are mapped to the unfolding fractions as a function of the pH value or denaturant concentration, from which we have extracted local and global unfolding free energies of cyt c in different denaturant environments using a modified Ising model. Based on the characteristics of the thermodynamic properties deduced from the local and global protein folding–unfolding, we discuss the thermodynamic stabilities of the protein in the three denaturant environments, and the possible correlation between the global conformation change of the protein and the local unfolding activities of the S—Fe bond in the Met80-heme and the α-helices.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Shiu, Y.-J.</dc:creator>
    <dc:creator>Jeng, U.-S.</dc:creator>
    <dc:creator>Su, C.</dc:creator>
    <dc:creator>Huang, Y.-S.</dc:creator>
    <dc:creator>Hayashi, M.</dc:creator>
    <dc:creator>Liang, K.-K.</dc:creator>
    <dc:creator>Yeh, Y.-L.</dc:creator>
    <dc:creator>Lin, S.-H.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003597</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The application of a modified Ising model for the thermodynamic properties of local and global protein folding–unfolding is described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>THERMODYNAMICS; ISING MODEL; GLOBAL AND LOCAL PROTEIN FOLDING-UNFOLDING; SMALL-ANGLE X-RAY SCATTERING</dc:subject>
    <dc:description>Based on the mean-field approximation, we have applied a modified Ising model to describe general protein unfolding behavior at thermodynamic equilibrium with the free energy contributed by the subgroup units (amino acids or peptide bonds) of the protein. With the thermodynamic properties of the protein, this model can associate the stepwise change of an unfolding fraction ratio profile with the local and global conformation unfolding. Taking cytochrome c (cyt c) as a model protein, we have observed, using small-angle X-ray scattering and circular dichroism (CD), the global and local structure changes for the protein in three kinds of denaturant environments: acid, urea and guanidine hydrochloride. The small-angle X-ray scattering and CD results are mapped to the unfolding fractions as a function of the pH value or denaturant concentration, from which we have extracted local and global unfolding free energies of cyt c in different denaturant environments using a modified Ising model. Based on the characteristics of the thermodynamic properties deduced from the local and global protein folding–unfolding, we discuss the thermodynamic stabilities of the protein in the three denaturant environments, and the possible correlation between the global conformation change of the protein and the local unfolding activities of the S—Fe bond in the Met80-heme and the α-helices.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A modified Ising model for the thermodynamic properties of local and global protein folding–unfolding observed by circular dichroism and small-angle X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>195</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>199</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6023">
    <title>A combined small-angle scattering study of a chemical reaction at specific sites and reaction-induced self-assembly as a problem in open non-equilibrium phenomena</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6023</link>
    <description>As a problem in open non-equilibrium phenomena, small-angle scattering (SAS) studies of chemical reactions at specific sites and reaction-induced self-assembly of a system which is obtained by mixing two stable solutions of palladium acetate [Pd(OAc)2] in N,N-dimethylformamide and the second-generation polyamidoamine dendrimer in methanol are presented. The self-assembly was studied using a combination of neutron and X-ray SAS. The results revealed that the self-assembly involves the initial formation of aggregates of an average radius of 20 nm composed of the dendrimers and Pd(OAc)2 followed by formation of palladium nanoparticles of a radius of 2.0 nm inside the aggregates. The aggregates were found to provide a special field for a chemical reaction for reduction of Pd(II) ions with methanol and for the self-assembly of the reduction products of Pd(0) atoms into nanoparticles. The nanoparticles are found to be trapped and stabilized in the aggregates.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Hashimoto, T.</dc:creator>
    <dc:creator>Tanaka, H.</dc:creator>
    <dc:creator>Koizumi, S.</dc:creator>
    <dc:creator>Naka, K.</dc:creator>
    <dc:creator>Chujo, Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003445</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>As a problem in open non-equilibrium phenomena, small-angle scattering studies of a chemical reaction at specific sites and reaction-induced self-assembly of the system which is induced by mixing two stable solutions of palladium(II) acetate [Pd(OAc)2] in N,N-dimethylformamide and the second-generation polyamidoamine dendrimer in methanol are presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; SANS; PAMAM; OPEN NON-EQUILIBRIUM PHENOMENA; STABLE SOLUTIONS; SELF-ASSEMBLY</dc:subject>
    <dc:description>As a problem in open non-equilibrium phenomena, small-angle scattering (SAS) studies of chemical reactions at specific sites and reaction-induced self-assembly of a system which is obtained by mixing two stable solutions of palladium acetate [Pd(OAc)2] in N,N-dimethylformamide and the second-generation polyamidoamine dendrimer in methanol are presented. The self-assembly was studied using a combination of neutron and X-ray SAS. The results revealed that the self-assembly involves the initial formation of aggregates of an average radius of 20 nm composed of the dendrimers and Pd(OAc)2 followed by formation of palladium nanoparticles of a radius of 2.0 nm inside the aggregates. The aggregates were found to provide a special field for a chemical reaction for reduction of Pd(II) ions with methanol and for the self-assembly of the reduction products of Pd(0) atoms into nanoparticles. The nanoparticles are found to be trapped and stabilized in the aggregates.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A combined small-angle scattering study of a chemical reaction at specific sites and reaction-induced self-assembly as a problem in open non-equilibrium phenomena</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>73</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>77</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6014">
    <title>Collapse of the hydration shell of a protein prior to thermal unfolding</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6014</link>
    <description>Based on high statistical quality wide-angle X-ray scattering data for the unfolding–refolding process of hen egg-white lysozyme (HEWL), we have analysed the change of the hydration shell as a function temperature using the program CRYSOL. The present results suggest that the decrease of the hydration-shell density starts from a lower temperature than the transition temperature of the collapse of the tertiary structure of HEWL. Although the use of CRYSOL for scattering data for proteins before the transition has an apparent limitation, the collapse of the hydration shell prior to the unfolding of HEWL agrees with a slight tendency of the radius of gyration to decrease during the thermal unfolding process.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Koizumi, M.</dc:creator>
    <dc:creator>Hirai, H.</dc:creator>
    <dc:creator>Onai, T.</dc:creator>
    <dc:creator>Inoue, K.</dc:creator>
    <dc:creator>Hirai, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003354</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The change of the hydration shell of hen egg-white lysozyme during the unfolding–refolding process as a function temperature has been analysed. The decrease of the hydration-shell density starts from a lower temperature than the transition temperature of the collapse of the tertiary structure.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>THERMAL UNFOLDING; HEN EGG-WHITE LYSOZYME; WAXS; PROTEIN HYDRATION SHELL</dc:subject>
    <dc:description>Based on high statistical quality wide-angle X-ray scattering data for the unfolding–refolding process of hen egg-white lysozyme (HEWL), we have analysed the change of the hydration shell as a function temperature using the program CRYSOL. The present results suggest that the decrease of the hydration-shell density starts from a lower temperature than the transition temperature of the collapse of the tertiary structure of HEWL. Although the use of CRYSOL for scattering data for proteins before the transition has an apparent limitation, the collapse of the hydration shell prior to the unfolding of HEWL agrees with a slight tendency of the radius of gyration to decrease during the thermal unfolding process.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Collapse of the hydration shell of a protein prior to thermal unfolding</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>175</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>178</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6007">
    <title>A small-angle X-ray scattering study of the effect of chain architecture on the shear-induced crystallization of branched and linear poly(ethylene terephthalate)</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6007</link>
    <description>The synchrotron-based small-angle X-ray scattering (SAXS) technique was used to investigate the shear-induced crystallization kinetics of branched/unbranched poly(ethylene terephthalate) (PET). Reactive extrusion of bottle-grade PET with the branching and chain-extension agents pyromellitic dianhydride and pentaerythritol results in enhanced rheological properties, such as higher melt strength and higher viscosity. In this study, six samples of PET were investigated: linear PET [intrinsic viscosity (IV) ≃ 0.76 dm3 g−1]; four branched PETs produced from linear PET by a reactive extrusion technique (IV ≃ 0.86–1.06 dm3 g−1); and a control PET (IV ≃ 0.73 dm3 g−1) extruded under the same conditions without reactive agents. SAXS data were recorded for the PET at the melt temperature and time-resolved SAXS data were recorded following the application of a step shear (53 s−1 for 2 s). As the PET IV was increased, the extent of shear-induced orientation increased, whilst the time taken for the polymer to initiate and complete crystallization decreased.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Hanley, T.</dc:creator>
    <dc:creator>Sutton, D.</dc:creator>
    <dc:creator>Heeley, E.</dc:creator>
    <dc:creator>Moad, G.</dc:creator>
    <dc:creator>Knott, R.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807003512</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Reactive extrusion of PET with branching and chain-extension agents results in enhanced rheological properties. Small-angle X-ray scattering was used to establish the crystallization kinetics and the molecular architecture following a step shear in the melt. Linear PET exhibited isotropic crystallization that was slower with increasing molecular weight, while long-chain-branched PET showed the opposite trend.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLY(ETHYLENE TEREPHTHALATE); BRANCHED PETS; POLYESTERS; CRYSTALLIZATION; SAXS</dc:subject>
    <dc:description>The synchrotron-based small-angle X-ray scattering (SAXS) technique was used to investigate the shear-induced crystallization kinetics of branched/unbranched poly(ethylene terephthalate) (PET). Reactive extrusion of bottle-grade PET with the branching and chain-extension agents pyromellitic dianhydride and pentaerythritol results in enhanced rheological properties, such as higher melt strength and higher viscosity. In this study, six samples of PET were investigated: linear PET [intrinsic viscosity (IV) ≃ 0.76 dm3 g−1]; four branched PETs produced from linear PET by a reactive extrusion technique (IV ≃ 0.86–1.06 dm3 g−1); and a control PET (IV ≃ 0.73 dm3 g−1) extruded under the same conditions without reactive agents. SAXS data were recorded for the PET at the melt temperature and time-resolved SAXS data were recorded following the application of a step shear (53 s−1 for 2 s). As the PET IV was increased, the extent of shear-induced orientation increased, whilst the time taken for the polymer to initiate and complete crystallization decreased.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A small-angle X-ray scattering study of the effect of chain architecture on the shear-induced crystallization of branched and linear poly(ethylene terephthalate)</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>599</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>604</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6013">
    <title>Concentration fluctuations induced by orientation fluctuations in polybutadiene–4-cyano-4'-n-octylbiphenyl mixtures</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6013</link>
    <description>The changes in concentration fluctuations of polymer–liquid crystal (LC) binary mixtures with temperature were investigated by small-angle X-ray scattering in their one-phase region and in the isotropic state of the LC. The concentration fluctuations consist of two modes: an OZD mode expressed by the Ornstein–Zernike–Debye equation with a correlation length ξ and a DB mode expressed by the Debye–Buche equation with a correlation length l. The temperature dependence of the OZD mode exhibits critical phenomena similar to common binary mixtures. Under the condition where the LC molecules are oriented by an electric field, the OZD mode is insensitive to the orientation while the DB mode is enhanced perpendicular to the orientation direction. These results indicate that the DB mode is induced by the orientation of the LC molecules.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Shimizu, H.</dc:creator>
    <dc:creator>Takenaka, M.</dc:creator>
    <dc:creator>Nishitsuji, S.</dc:creator>
    <dc:creator>Hasegawa, H.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807002981</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The changes in concentration fluctuations of polymer–liquid crystal binary mixtures with temperature were investigated by small-angle X-ray scattering in their one-phase region and in the isotropic state of the liquid crystal. The concentration fluctuations consist of two modes: an OZD mode expressed by the Ornstein–Zernike–Debye equation with a correlation length ξ and a DB mode expressed by the Debye–Buche equation with a correlation length l.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>POLYMER-LIQUID CRYSTAL MIXTURES; SAXS; POLYBUTADIENE; 4-CYANO-4'-N-OCTYLBIPHENYL</dc:subject>
    <dc:description>The changes in concentration fluctuations of polymer–liquid crystal (LC) binary mixtures with temperature were investigated by small-angle X-ray scattering in their one-phase region and in the isotropic state of the LC. The concentration fluctuations consist of two modes: an OZD mode expressed by the Ornstein–Zernike–Debye equation with a correlation length ξ and a DB mode expressed by the Debye–Buche equation with a correlation length l. The temperature dependence of the OZD mode exhibits critical phenomena similar to common binary mixtures. Under the condition where the LC molecules are oriented by an electric field, the OZD mode is insensitive to the orientation while the DB mode is enhanced perpendicular to the orientation direction. These results indicate that the DB mode is induced by the orientation of the LC molecules.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Concentration fluctuations induced by orientation fluctuations in polybutadiene–4-cyano-4'-n-octylbiphenyl mixtures</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>662</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>665</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6018">
    <title>ATSAS 2.1 – towards automated and web-supported small-angle scattering data analysis</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6018</link>
    <description>Small-angle scattering (SAS) is frequently employed for screening large numbers of samples and for studying these samples under different conditions, including space- and time-resolved analysis. These measurements produce immense amounts of data, especially on modern high-flux and high-brilliance sources (e.g. third-generation synchrotrons). In biological SAS, like high-throughput macromolecular crystallography, large-scale analysis of proteins and macromolecular complexes is also emerging. Automation of data analysis becomes an indispensable prerequisite for adequate evaluation of high-throughput SAS experiments. Here a prototype of an automated data-analysis system for isotropic solution scattering based on the further development of the programs belonging to the package ATSAS 2.1 is reported. This system allows the major analysis tasks starting from the raw data processing and, for monodisperse systems, finishing with a three-dimensional model, to be performed automatically. Convenient web interfaces for the online use of individual ATSAS programs are also provided.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Petoukhov, M.V.</dc:creator>
    <dc:creator>Konarev, P.V.</dc:creator>
    <dc:creator>Kikhney, A.G.</dc:creator>
    <dc:creator>Svergun, D.I.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807002853</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>New features of the small-angle scattering data analysis package ATSAS 2.1 that allow automated data processing and web-based access are described.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAS DATA ANALYSIS; AUTOMATED DATA PROCESSING; HIGH-THROUGHPUT SAS; SHAPE DETERMINATION; WEB ACCESS</dc:subject>
    <dc:description>Small-angle scattering (SAS) is frequently employed for screening large numbers of samples and for studying these samples under different conditions, including space- and time-resolved analysis. These measurements produce immense amounts of data, especially on modern high-flux and high-brilliance sources (e.g. third-generation synchrotrons). In biological SAS, like high-throughput macromolecular crystallography, large-scale analysis of proteins and macromolecular complexes is also emerging. Automation of data analysis becomes an indispensable prerequisite for adequate evaluation of high-throughput SAS experiments. Here a prototype of an automated data-analysis system for isotropic solution scattering based on the further development of the programs belonging to the package ATSAS 2.1 is reported. This system allows the major analysis tasks starting from the raw data processing and, for monodisperse systems, finishing with a three-dimensional model, to be performed automatically. Convenient web interfaces for the online use of individual ATSAS programs are also provided.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>ATSAS 2.1 – towards automated and web-supported small-angle scattering data analysis</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>223</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>228</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6028">
    <title>Reverse Monte Carlo analysis for small-angle scattering of expanded fluid Hg: connection to the wide-angle structure factor</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6028</link>
    <description>A preliminary result of reverse Monte Carlo (RMC) analysis of small-angle X-ray scattering data for expanded fluid Hg with the help of wide-angle X-ray diffraction data in the same thermodynamic state is presented. In RMC analysis, three-dimensional configurations of 100000 Hg atoms were modeled to see the large density fluctuation associated with liquid–vapor critical phenomena. It was found that interpolation of measured structure factors is necessary for RMC analysis.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Hagita, K.</dc:creator>
    <dc:creator>Arai, T.</dc:creator>
    <dc:creator>Inui, M.</dc:creator>
    <dc:creator>Matsuda, K.</dc:creator>
    <dc:creator>Tamura, K.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807002713</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A preliminary result of reverse Monte Carlo analysis of small-angle X-ray scattering data for expanded fluid Hg with the help of wide-angle X-ray diffraction data in the same thermodynamic state is presented. To see the large density fluctuation associated with liquid–vapor critical phenomena, a three-dimensional configuration of 100000 Hg atoms is modeled.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>REVERSE MONTE CARLO ANALYSIS; SAXS; EXPANDED FLUID HG; STRUCTURE FACTORS; LIQUID-VAPOR CRITICAL PHENOMENA</dc:subject>
    <dc:description>A preliminary result of reverse Monte Carlo (RMC) analysis of small-angle X-ray scattering data for expanded fluid Hg with the help of wide-angle X-ray diffraction data in the same thermodynamic state is presented. In RMC analysis, three-dimensional configurations of 100000 Hg atoms were modeled to see the large density fluctuation associated with liquid–vapor critical phenomena. It was found that interpolation of measured structure factors is necessary for RMC analysis.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Reverse Monte Carlo analysis for small-angle scattering of expanded fluid Hg: connection to the wide-angle structure factor</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>544</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>548</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6002">
    <title>Two-dimensional small-angle X-ray scattering from as-grown and heat-treated synthetic quartz</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6002</link>
    <description>The small-angle X-ray scattering (SAXS) in as-grown and heat-treated quartz crystals was investigated as a function of the azimuth angle around the primary beam. For this, samples parallel to (10\bar 10) were extracted from Z- and −X-growth sectors of a synthetic quartz bar which had the OH content evaluated by infrared spectroscopy (IRS). In addition, SAXS and IRS were independently recorded as a function of heating temperature. As a result, the two-dimensional SAXS images revealed an anisotropic pattern randomly decorated by low-intensity Kossel lines. The intensities were projected along specific directions or were axially integrated around the primary beam. It was observed that the Porod invariant (Q) increased and the Kossel lines moved slightly to higher q values with increasing temperature. The effect of the sample orientation on the Q value and the lack of a clear relationship between Q and OH content suggested that the diffuse scattering due to the periodicity of the crystal lattice played an important role in the small-angle scattering of quartz. The net scattering intensities produced by heat-treatment at 873 K were attributed to molecular water aggregates created by the diffusion of as-grown OH defects.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Guzzo, P.L.</dc:creator>
    <dc:creator>Shinohara, A.H.</dc:creator>
    <dc:creator>Santos, A.E.F.</dc:creator>
    <dc:creator>Funari, S.S.</dc:creator>
    <dc:creator>Daito, S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807002609</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The contribution of molecular water aggregates in the small-angle X-ray scattering of quartz crystals was investigated as a function of the azimuth angle around the primary beam. The presence of Kossel lines randomly decorating the anisotropic two-dimensional pattern and the lack of a clear relationship between Porod invariant and OH content revealed that diffuse scattering plays an important role in the scattering of quartz crystal.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>WATER AGGREGATES; DIFFUSE SCATTERING; ANISOTROPY; KOSSEL LINES; INFRARED SPECTROSCOPY</dc:subject>
    <dc:description>The small-angle X-ray scattering (SAXS) in as-grown and heat-treated quartz crystals was investigated as a function of the azimuth angle around the primary beam. For this, samples parallel to (10\bar 10) were extracted from Z- and −X-growth sectors of a synthetic quartz bar which had the OH content evaluated by infrared spectroscopy (IRS). In addition, SAXS and IRS were independently recorded as a function of heating temperature. As a result, the two-dimensional SAXS images revealed an anisotropic pattern randomly decorated by low-intensity Kossel lines. The intensities were projected along specific directions or were axially integrated around the primary beam. It was observed that the Porod invariant (Q) increased and the Kossel lines moved slightly to higher q values with increasing temperature. The effect of the sample orientation on the Q value and the lack of a clear relationship between Q and OH content suggested that the diffuse scattering due to the periodicity of the crystal lattice played an important role in the small-angle scattering of quartz. The net scattering intensities produced by heat-treatment at 873 K were attributed to molecular water aggregates created by the diffusion of as-grown OH defects.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Two-dimensional small-angle X-ray scattering from as-grown and heat-treated synthetic quartz</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>132</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>137</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6016">
    <title>Accuracy of molecular mass determination of proteins in solution by small-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6016</link>
    <description>One of the most important overall parameters, which can be derived from small-angle X-ray scattering (SAXS) experiments on macromolecular solutions is the molecular mass (MM) of the solute. In particular, for a monodisperse protein solution, MM of the solute is calculated from the extrapolated scattering intensity at zero angle I(0). Assessing MM by SAXS provides valuable information about the oligomeric state and absence of unspecific aggregation in solution. The value of MM can either be estimated by comparison with a protein standard with a known MM or by determining the absolute scattering intensity using, e.g., water scattering. In both cases, knowledge about the solute concentration and about the partial specific volume of the protein is required. By measuring 13 well characterized globular proteins with MMs ranging from 13.7 to 669 kDa we analyze the sources of possible systematic deviations and assess the accuracy of MM determination using SAXS. The data indicate that all these proteins have approximately the same `effective' value of the partial specific volume of about 0.7425 cm3 g−1. It is shown that both inter-protein and water calibration can be used for molecular mass determination by SAXS and in most cases the errors do not exceed 10%.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Mylonas, E.</dc:creator>
    <dc:creator>Svergun, D.I.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S002188980700252X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A systematic evaluation of the accuracy of molecular mass determination of proteins using small-angle X-ray scattering.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; ABSOLUTE CALIBRATION; MOLECULAR MASS; PARTIAL SPECIFIC VOLUME; WATER SCATTERING</dc:subject>
    <dc:description>One of the most important overall parameters, which can be derived from small-angle X-ray scattering (SAXS) experiments on macromolecular solutions is the molecular mass (MM) of the solute. In particular, for a monodisperse protein solution, MM of the solute is calculated from the extrapolated scattering intensity at zero angle I(0). Assessing MM by SAXS provides valuable information about the oligomeric state and absence of unspecific aggregation in solution. The value of MM can either be estimated by comparison with a protein standard with a known MM or by determining the absolute scattering intensity using, e.g., water scattering. In both cases, knowledge about the solute concentration and about the partial specific volume of the protein is required. By measuring 13 well characterized globular proteins with MMs ranging from 13.7 to 669 kDa we analyze the sources of possible systematic deviations and assess the accuracy of MM determination using SAXS. The data indicate that all these proteins have approximately the same `effective' value of the partial specific volume of about 0.7425 cm3 g−1. It is shown that both inter-protein and water calibration can be used for molecular mass determination by SAXS and in most cases the errors do not exceed 10%.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Accuracy of molecular mass determination of proteins in solution by small-angle X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>245</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>249</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6042">
    <title>X-ray reflectivity studies on the deoxyribonucleic acid adsorption by 3-β-[N-(N',N'-dimethylamino­ethane)carbamoyl]cholesterol monolayer with divalent ions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6042</link>
    <description>The effect of adding divalent ions on the deoxyribonucleic acid (DNA) adsorption by a cationic lipid monolayer at the air–water interface was investigated by X-ray reflectivity on Langmuir–Blodgett films supported on silicon wafers. The films were prepared from a DC-Chol {3-β-[N-(N′,N′-dimethylaminoethane)carbamoyl]cholesterol} monolayer with 1 µM DNA in the subphase with different amounts of calcium ions added. It is found in this study that adding divalent ions, such as calcium ions, can enhance the DNA adsorption to interfaces. The adsorbed DNA layer thickness as determined by X-ray reflectivity is found to vary linearly with the square root of the ion concentration. This indicates that charge-screening effects and ion-mediated condensation play an important role in the DNA–cationic lipid monolayer interaction.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Lin, T.-L.</dc:creator>
    <dc:creator>Wu, J.-C.</dc:creator>
    <dc:creator>Jeng, U.-S.</dc:creator>
    <dc:creator>Lee, H.-Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807002452</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The effect of adding divalent ions on the deoxyribonucleic acid adsorption by a cationic lipid monolayer at the air–water interface was investigated by X-ray reflectivity.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY REFLECTIVITY; LANGMUIR-BLODGETT FILMS; LIPID MONOLAYERS; DNA ADSORPTION; DIVALENT IONS</dc:subject>
    <dc:description>The effect of adding divalent ions on the deoxyribonucleic acid (DNA) adsorption by a cationic lipid monolayer at the air–water interface was investigated by X-ray reflectivity on Langmuir–Blodgett films supported on silicon wafers. The films were prepared from a DC-Chol {3-β-[N-(N′,N′-dimethylaminoethane)carbamoyl]cholesterol} monolayer with 1 µM DNA in the subphase with different amounts of calcium ions added. It is found in this study that adding divalent ions, such as calcium ions, can enhance the DNA adsorption to interfaces. The adsorbed DNA layer thickness as determined by X-ray reflectivity is found to vary linearly with the square root of the ion concentration. This indicates that charge-screening effects and ion-mediated condensation play an important role in the DNA–cationic lipid monolayer interaction.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>X-ray reflectivity studies on the deoxyribonucleic acid adsorption by 3-β-[N-(N',N'-dimethylamino­ethane)carbamoyl]cholesterol monolayer with divalent ions</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>680</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>683</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6003">
    <title>Binding of trifluoperazine to apocalmodulin revealed by a combination of small-angle X-ray scattering and nuclear magnetic resonance</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6003</link>
    <description>Small-angle X-ray scattering (SAXS) and nuclear magnetic resonance (NMR) studies were performed to investigate the binding of trifluoperazine (TFP) to Ca2+-free calmodulin (apoCaM) with N- and C-terminal globular domains connected by a linker. The SAXS and NMR measurements were taken throughout the titration of TFP. The SAXS analyses indicate that the binding of TFP induces structural changes from a dumbbell shape to a compact globular shape in solution. The formation of the complete globular structure requires 5.0 added equivalents of TFP. An analysis of NMR chemical-shift changes indicates that the C-terminal domain of apoCaM is involved in the binding of TFP. The SAXS and NMR data reflect the high structural flexibility of apoCaM.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Matsushima, N.</dc:creator>
    <dc:creator>Hayashi, N.</dc:creator>
    <dc:creator>Watanabe, N.</dc:creator>
    <dc:creator>Jinbo, Y.</dc:creator>
    <dc:creator>Izumi, Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807002117</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Small-angle X-ray scattering and nuclear magnetic resonance studies were performed to investigate the binding of trifluoperazine to Ca2+-free calmodulin with N- and C-terminal globular domains connected by a linker.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>TRIFLUOPERAZINE; SAXS; NMR; CALMODULIN</dc:subject>
    <dc:description>Small-angle X-ray scattering (SAXS) and nuclear magnetic resonance (NMR) studies were performed to investigate the binding of trifluoperazine (TFP) to Ca2+-free calmodulin (apoCaM) with N- and C-terminal globular domains connected by a linker. The SAXS and NMR measurements were taken throughout the titration of TFP. The SAXS analyses indicate that the binding of TFP induces structural changes from a dumbbell shape to a compact globular shape in solution. The formation of the complete globular structure requires 5.0 added equivalents of TFP. An analysis of NMR chemical-shift changes indicates that the C-terminal domain of apoCaM is involved in the binding of TFP. The SAXS and NMR data reflect the high structural flexibility of apoCaM.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Binding of trifluoperazine to apocalmodulin revealed by a combination of small-angle X-ray scattering and nuclear magnetic resonance</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>179</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>183</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6016">
    <title>Small-angle neutron scattering from extended defects in diamonds</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6016</link>
    <description>The results of a small-angle neutron scattering investigation of natural and synthetic diamonds with variable concentrations and types of point defects and different degrees of deformation are reported. It is shown that deformation and/or annealing of diamonds lead to the formation of planar and three-dimensional defects, giving rise to small-angle scattering.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Shiryaev, A.A.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001859</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>It is shown that natural and synthetic diamonds contain planar and three-dimensional defects, observable by small-angle neutron scattering. These defects appear after annealing and/or deformation of the diamonds.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DIAMOND; EXTENDED DEFECTS; SMALL-ANGLE SCATTERING</dc:subject>
    <dc:description>The results of a small-angle neutron scattering investigation of natural and synthetic diamonds with variable concentrations and types of point defects and different degrees of deformation are reported. It is shown that deformation and/or annealing of diamonds lead to the formation of planar and three-dimensional defects, giving rise to small-angle scattering.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle neutron scattering from extended defects in diamonds</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>116</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>120</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6020">
    <title>Charge interaction and temperature effects on the solution structure of lysozyme as revealed by small-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6020</link>
    <description>We have studied the structure of lysozyme as influenced by solution environment using small-angle X-ray scattering (SAXS). With an ellipsoid form factor and a structure factor derived using the mean spherical approximation to account for the electrostatic repulsion of lysozyme, we have extracted detailed structural information about the protein in aqueous solutions, including the size, shape, and net charge number. The SAXS data analysis shows that lysozyme in pure water, expressing an averaged net charge number of ~6, folds to an ellipsoid-like shape with a radius of gyration Rg = 16.6 Å. Temperature-dependent SAXS for lysozyme in a buffer solution in which charge repulsion has been eliminated suggests that the protein may thermally unfold gradually along a preferred direction from the ellipsoidal shape with an aspect ratio of p ≃ 2 at 303 K to an elongated shape with p ≃ 3 at 343 K. The structural parameters of the unfolded lysozyme obtained using model fitting are compared with the envelope morphology simulated using a dummy-residues model. From the evolution of the volume of lysozyme during the thermal unfolding process, we deduce a free-energy profile for the protein thermally unfolded in water using a modified Ising model on the basis of a mean field approximation.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Huang, Y.-S.</dc:creator>
    <dc:creator>Jeng, U.-S.</dc:creator>
    <dc:creator>Shiu, Y.-J.</dc:creator>
    <dc:creator>Lai, Y.-H.</dc:creator>
    <dc:creator>Sun, Y.-S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001835</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Charge interaction and temperature effects on the solution structure of lysozyme are studied by small-angle X-ray scattering.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; ELECTROSTATIC REPULSION; DUMMY-RESIDUES MODEL; PROTEIN UNFOLDING; LYSOZYME</dc:subject>
    <dc:description>We have studied the structure of lysozyme as influenced by solution environment using small-angle X-ray scattering (SAXS). With an ellipsoid form factor and a structure factor derived using the mean spherical approximation to account for the electrostatic repulsion of lysozyme, we have extracted detailed structural information about the protein in aqueous solutions, including the size, shape, and net charge number. The SAXS data analysis shows that lysozyme in pure water, expressing an averaged net charge number of ~6, folds to an ellipsoid-like shape with a radius of gyration Rg = 16.6 Å. Temperature-dependent SAXS for lysozyme in a buffer solution in which charge repulsion has been eliminated suggests that the protein may thermally unfold gradually along a preferred direction from the ellipsoidal shape with an aspect ratio of p ≃ 2 at 303 K to an elongated shape with p ≃ 3 at 343 K. The structural parameters of the unfolded lysozyme obtained using model fitting are compared with the envelope morphology simulated using a dummy-residues model. From the evolution of the volume of lysozyme during the thermal unfolding process, we deduce a free-energy profile for the protein thermally unfolded in water using a modified Ising model on the basis of a mean field approximation.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Charge interaction and temperature effects on the solution structure of lysozyme as revealed by small-angle X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>165</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>169</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6002">
    <title>Localization of dihalogenated phenols in vesicle systems determined by contrast variation X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6002</link>
    <description>Localization of 2,4-dichloro- and 2,4-dibromophenol in multilamellar vesicles in a 1/1 dihalogenated phenol/lipid molar ratio was investigated by classical contrast variation X-ray scattering using the isomorphous replacement method. The results were compared with those obtained by anomalous small-angle X-ray scattering from a vesicle system doped with 2,4-dibromophenol. Dissimilarities in the results of the two methods are discussed, taking into account the advantages and disadvantages of both techniques in studying multilamellar systems.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Varga, Z.</dc:creator>
    <dc:creator>Bóta, A.</dc:creator>
    <dc:creator>Goerigk, G.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001987</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Using contrast variation by means of isomorphous replacement, the localization of dihalogenated phenols in multilamellar vesicles was determined, and was compared with the results of anomalous small-angle scattering.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CONTRAST VARIATION; ISOMORPHOUS REPLACEMENT; ANOMALOUS SMALL-ANGLE X-RAY SCATTERING; VESICLES; DIHALOGENATED PHENOLS; INTERDIGITATED PHASE</dc:subject>
    <dc:description>Localization of 2,4-dichloro- and 2,4-dibromophenol in multilamellar vesicles in a 1/1 dihalogenated phenol/lipid molar ratio was investigated by classical contrast variation X-ray scattering using the isomorphous replacement method. The results were compared with those obtained by anomalous small-angle X-ray scattering from a vesicle system doped with 2,4-dibromophenol. Dissimilarities in the results of the two methods are discussed, taking into account the advantages and disadvantages of both techniques in studying multilamellar systems.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Localization of dihalogenated phenols in vesicle systems determined by contrast variation X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>205</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>208</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6022">
    <title>Study of amorphous nanocrystalline thin silicon films by grazing-incidence small-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6022</link>
    <description>Thin Si films, with thicknesses between 100 and 400 nm, were deposited by radio frequency plasma enhanced chemical vapour deposition in silane gas (SiH4) highly diluted by hydrogen. The growing conditions were varied to obtain different degrees of crystal fractions and a variety in individual crystal sizes. The crystalline to amorphous volume fraction, as estimated by Raman spectroscopy, varied from 5 to 45% while the individual crystal sizes varied from 2 to 8 nm. The average density of the samples was estimated by using near infrared spectroscopy and the effective medium approximation. All samples were porous and contained void volume fraction between 15 and 25%. Grazing-incidence small-angle X-ray scattering has been performed at the ELETTRA synchrotron radiation source (Trieste, Italy). The scattering patterns of all examined samples indicate the presence of `particles' in the `bulk' of the thin films with gyration radii in the range of 2 to 5 nm. The higher values were found for the samples with a higher crystalline fraction. The size and the size distribution of `particles' depend upon the deposition conditions. The samples which had been deposited with a higher discharge power and a lower silane fraction had larger particles and the roughness of their surface was higher.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Gracin, D.</dc:creator>
    <dc:creator>Bernstorff, S.</dc:creator>
    <dc:creator>Dubcek, P.</dc:creator>
    <dc:creator>Gajovic, A.</dc:creator>
    <dc:creator>Juraic, K.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807002075</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The nanostructure of thin silicon films composed of amorphous and crystalline phases was analysed by Raman spectroscopy and grazing-incidence small-angle X-ray scattering. By Raman spectroscopy the crystalline fraction and the average individual crystal sizes were estimated while grazing-incidence small-angle X-ray scattering detected nano sized `objects', presumably voids that are non-spherical in shape, non-uniformly distributed across the depth of the samples.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>AMORPHOUS SILICON; NANOCRYSTALLINE SILICON; GISAXS; RAMAN SPECTROSCOPY</dc:subject>
    <dc:description>Thin Si films, with thicknesses between 100 and 400 nm, were deposited by radio frequency plasma enhanced chemical vapour deposition in silane gas (SiH4) highly diluted by hydrogen. The growing conditions were varied to obtain different degrees of crystal fractions and a variety in individual crystal sizes. The crystalline to amorphous volume fraction, as estimated by Raman spectroscopy, varied from 5 to 45% while the individual crystal sizes varied from 2 to 8 nm. The average density of the samples was estimated by using near infrared spectroscopy and the effective medium approximation. All samples were porous and contained void volume fraction between 15 and 25%. Grazing-incidence small-angle X-ray scattering has been performed at the ELETTRA synchrotron radiation source (Trieste, Italy). The scattering patterns of all examined samples indicate the presence of `particles' in the `bulk' of the thin films with gyration radii in the range of 2 to 5 nm. The higher values were found for the samples with a higher crystalline fraction. The size and the size distribution of `particles' depend upon the deposition conditions. The samples which had been deposited with a higher discharge power and a lower silane fraction had larger particles and the roughness of their surface was higher.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Study of amorphous nanocrystalline thin silicon films by grazing-incidence small-angle X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>373</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>376</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6004">
    <title>Low-resolution models for nucleic acids from small-angle X-ray scattering with applications to electrostatic modeling</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6004</link>
    <description>Several algorithms are available to reconstruct low-resolution electron density maps of biological macromolecules from small-angle solution scattering data. These algorithms have been extensively applied to proteins and protein complexes. Here, we demonstrate their applicability to nucleic acids by reconstructing a set of RNA and DNA molecules of known three-dimensional structure from their small-angle X-ray scattering profiles. The overall size and shape of the molecules get reproduced well in all tested cases. Furthermore, we show that the generated bead models can be used as inputs for electrostatic calculations. The number of ions bound under different solution conditions computed from numerical solutions of the Poisson–Boltzmann equation for bead models agrees very well with results of calculations on all atom models derived from crystallography. The predictions from Poisson–Boltzmann theory also agree generally well with experimentally determined ion binding numbers.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Lipfert, J.</dc:creator>
    <dc:creator>Chu, V.B.</dc:creator>
    <dc:creator>Bai, Y.</dc:creator>
    <dc:creator>Herschlag, D.</dc:creator>
    <dc:creator>Doniach, S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001707</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>It is shown that bead reconstruction algorithms can be used to obtain low-resolution three-dimensional density maps for nucleic acids from SAXS data. In addition, it is shown that the reconstructed bead models can be used to define the molecular geometry in Poisson–Boltzmann calculations to accurately determine the excess number of ions bound under different solution conditions.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; LOW-RESOLUTION MODELS; ELECTROSTATIC MODELING; NUCLEIC ACIDS</dc:subject>
    <dc:description>Several algorithms are available to reconstruct low-resolution electron density maps of biological macromolecules from small-angle solution scattering data. These algorithms have been extensively applied to proteins and protein complexes. Here, we demonstrate their applicability to nucleic acids by reconstructing a set of RNA and DNA molecules of known three-dimensional structure from their small-angle X-ray scattering profiles. The overall size and shape of the molecules get reproduced well in all tested cases. Furthermore, we show that the generated bead models can be used as inputs for electrostatic calculations. The number of ions bound under different solution conditions computed from numerical solutions of the Poisson–Boltzmann equation for bead models agrees very well with results of calculations on all atom models derived from crystallography. The predictions from Poisson–Boltzmann theory also agree generally well with experimentally determined ion binding numbers.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Low-resolution models for nucleic acids from small-angle X-ray scattering with applications to electrostatic modeling</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>229</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>234</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6006">
    <title>A visualized analysis of small-angle neutron scattering intensity: concentration fluctuation in alcohol–water mixtures</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6006</link>
    <description>Small-angle neutron scattering measurements have been performed on tert-butyl alcohol–water mixtures with alcohol concentrations from 0.05 to 0.30 mole fractions at 298, 313 and 328 K. Concentration fluctuations of the mixtures are analysed in terms of fractals. The structure of the concentration fluctuation is visualized by means of a large-scale reverse Monte Carlo technique. Percolation analysis of the visualized structure shows that the concentration fluctuation is characterized by polydisperse mass fractals, as found for 1-propanol–water mixtures. It seems that polydisperse mass fractals are a common structural characteristic in various alcohol–water mixtures.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Misawa, M.</dc:creator>
    <dc:creator>Sato, T.</dc:creator>
    <dc:creator>Onozuka, A.</dc:creator>
    <dc:creator>Maruyama, K.</dc:creator>
    <dc:creator>Mori, K.</dc:creator>
    <dc:creator>Suzuki, S.</dc:creator>
    <dc:creator>Otomo, T.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001549</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Visualized analysis of SANS from a tert-butyl alcohol–water mixture has revealed that the concentration fluctuation is characterized by polydisperse mass fractals.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>CONCENTRATION FLUCTUATIONS; VISUALIZATION; FRACTALS; ALCOHOL-WATER MIXTURES</dc:subject>
    <dc:description>Small-angle neutron scattering measurements have been performed on tert-butyl alcohol–water mixtures with alcohol concentrations from 0.05 to 0.30 mole fractions at 298, 313 and 328 K. Concentration fluctuations of the mixtures are analysed in terms of fractals. The structure of the concentration fluctuation is visualized by means of a large-scale reverse Monte Carlo technique. Percolation analysis of the visualized structure shows that the concentration fluctuation is characterized by polydisperse mass fractals, as found for 1-propanol–water mixtures. It seems that polydisperse mass fractals are a common structural characteristic in various alcohol–water mixtures.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A visualized analysis of small-angle neutron scattering intensity: concentration fluctuation in alcohol–water mixtures</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>93</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>96</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6013">
    <title>Mixed magnetic phase in 6H-type BaFeO3−δ</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6013</link>
    <description>The magnetic state in 6H-type BaFeO3−δ at low temperature was studied using small-angle neutron scattering, positive-muon spin relaxation and magnetization measurements. These experiments demonstrate the appearance of two different types of magnetic states: an antiferromagnetic ordering with a long-range correlation and magnetic domains with a short-range correlation. The antiferromagnetic Fe spin arrangement occurs below 130 K. In contrast, the magnetic domains are formed below 170 K and the average size of the magnetic domains was estimated as ~124 Å. These results explain the discrepancy of the Néel temperatures between three measurement techniques: magnetization, neutron powder diffraction and Mössbauer measurements. Furthermore, it was found that the magnetic domains coexist with the long-range antiferromagnetic ordering below 130 K.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Mori, K.</dc:creator>
    <dc:creator>Kamiyama, T.</dc:creator>
    <dc:creator>Kobayashi, H.</dc:creator>
    <dc:creator>Otomo, T.</dc:creator>
    <dc:creator>Nishiyama, K.</dc:creator>
    <dc:creator>Sugiyama, M.</dc:creator>
    <dc:creator>Itoh, K.</dc:creator>
    <dc:creator>Fukunaga, T.</dc:creator>
    <dc:creator>Ikeda, S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001653</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The magnetic properties of 6H-type BaFeO3−δ were studied using small-angle neutron scattering, positive-muon spin relaxation and magnetization measurements.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>BAFEO3-[DELTA]; MAGNETIZATION; SANS; POSITIVE-MUON SPIN RELAXATION; ANTIFERROMAGNETIC ORDERING; MAGNETIC DOMAINS</dc:subject>
    <dc:description>The magnetic state in 6H-type BaFeO3−δ at low temperature was studied using small-angle neutron scattering, positive-muon spin relaxation and magnetization measurements. These experiments demonstrate the appearance of two different types of magnetic states: an antiferromagnetic ordering with a long-range correlation and magnetic domains with a short-range correlation. The antiferromagnetic Fe spin arrangement occurs below 130 K. In contrast, the magnetic domains are formed below 170 K and the average size of the magnetic domains was estimated as ~124 Å. These results explain the discrepancy of the Néel temperatures between three measurement techniques: magnetization, neutron powder diffraction and Mössbauer measurements. Furthermore, it was found that the magnetic domains coexist with the long-range antiferromagnetic ordering below 130 K.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Mixed magnetic phase in 6H-type BaFeO3−δ</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>501</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>505</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6029">
    <title>The application of distance distribution functions to structural analysis of core–shell particles</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6029</link>
    <description>The structure of core–shell latex particles of polymethylmethacrylate (the core) and polyurethane (the shell) have been investigated by methods of small-angle X-ray scattering (SAXS) and atom-force microscopy. A set of SAXS patterns has been obtained using contrast variation method. Indirect methods have been used to follow the evolution of distance distribution functions from SAXS for lattices in various sucrose solutions over a range of solution density, yielding structural parameters of the particles such as core size, shell thickness and density of the polymers including density deviations within the particle's core and shell. A model for an ensemble of core–shell particles with a normal distribution of average electron density of both the core and the shell has been developed to fit the distance distribution functions using a random search algorithm. The effects of nanophase separation in the polyurethane is estimated using Monte Carlo simulations of the distance distribution functions where the phase-separated polyurethane is represented by spherical truncated cones in a shell simulating the location of hard and soft polyurethane blocks, respectively.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Mykhaylyk, O.O.</dc:creator>
    <dc:creator>Ryan, A.J.</dc:creator>
    <dc:creator>Tzokova, N.</dc:creator>
    <dc:creator>Williams, N.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001616</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The internal structure of core–shell particles has been studied by small-angle X-ray scattering using the method of contrast variation. The indirect Fourier transform yielded distance distribution functions that were compared with three models of increasing sophistication: simple core–shell, core shell with spherical disks and core–shell with stochastic electron density variations.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; CORE-SHELL PARTICLES; CONTRAST VARIATION METHOD; DISTANCE DISTRIBUTION FUNCTION; INDIRECT FOURIER TRANSFORMATION METHODS; PHASE SEPARATION; POLYURETHANE; POLYMETHYLMETHACRYLATE</dc:subject>
    <dc:description>The structure of core–shell latex particles of polymethylmethacrylate (the core) and polyurethane (the shell) have been investigated by methods of small-angle X-ray scattering (SAXS) and atom-force microscopy. A set of SAXS patterns has been obtained using contrast variation method. Indirect methods have been used to follow the evolution of distance distribution functions from SAXS for lattices in various sucrose solutions over a range of solution density, yielding structural parameters of the particles such as core size, shell thickness and density of the polymers including density deviations within the particle's core and shell. A model for an ensemble of core–shell particles with a normal distribution of average electron density of both the core and the shell has been developed to fit the distance distribution functions using a random search algorithm. The effects of nanophase separation in the polyurethane is estimated using Monte Carlo simulations of the distance distribution functions where the phase-separated polyurethane is represented by spherical truncated cones in a shell simulating the location of hard and soft polyurethane blocks, respectively.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>The application of distance distribution functions to structural analysis of core–shell particles</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>506</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>511</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sm6023">
    <title>Small-angle scattering studies of macromolecular solutions</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sm6023</link>
    <description>In recent years, major progress has been achieved in developing novel approaches to interpret small-angle scattering data from solutions of biological macromolecules in terms of three-dimensional models. These advanced methods include: ab initio low-resolution shape and domain structure determination; modelling of quaternary structure by rigid-body refinement; simultaneous analysis of multiple scattering patterns, e.g. from contrast variation in neutron scattering to study multicomponent complexes; validation of high-resolution models; and addition of missing loops and domains. The new techniques will be presented and practical applications of the methods are illustrated by recent examples. The use of additional information from other methods, joint applications of X-ray and neutron scattering, and the possibilities for assessing and validating the models constructed based on small-angle scattering data will be discussed.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Svergun, D.I.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001409</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Advanced methods for the analysis of small-angle scattering data from solutions of biological macromolecules are reviewed.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAS DATA ANALYSIS; AB INITIO METHODS; RIGID-BODY MODELLING; MACROMOLECULAR COMPLEXES; QUATERNARY STRUCTURE</dc:subject>
    <dc:description>In recent years, major progress has been achieved in developing novel approaches to interpret small-angle scattering data from solutions of biological macromolecules in terms of three-dimensional models. These advanced methods include: ab initio low-resolution shape and domain structure determination; modelling of quaternary structure by rigid-body refinement; simultaneous analysis of multiple scattering patterns, e.g. from contrast variation in neutron scattering to study multicomponent complexes; validation of high-resolution models; and addition of missing loops and domains. The new techniques will be presented and practical applications of the methods are illustrated by recent examples. The use of additional information from other methods, joint applications of X-ray and neutron scattering, and the possibilities for assessing and validating the models constructed based on small-angle scattering data will be discussed.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle scattering studies of macromolecular solutions</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>10</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>17</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6004">
    <title>Reordering of magnetic colloid structures in external magnetic fields</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6004</link>
    <description>Field-induced local ordering within a cobalt-based magnetic colloid has been studied with polarized small-angle scattering by turning the direction of the external magnetic field. By analysing the nuclear–magnetic cross term we were able to separate the scattering contributions from dipolar chains and domains of pseudo-crystalline hexagonal arrangements. The magnetic moments were found to be aligned along the external magnetic field and to follow the change of the field direction. The observed variation of the particle moments must give rise to a rearrangement of the local hexagonal structure with respect to the new field direction to explain the scattering pattern. We confirm this by two-dimensional simultaneous least-squares fits for different Q ranges [where Q = 4\pi \sin (\theta) / \lambda, λ is the X-ray wavelength and 2θ is the scattering angle] with a model containing a core–shell particle form factor and a structure factor composed of Gaussian peaks and contributions from polydisperse cylinders.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Heinemann, A.</dc:creator>
    <dc:creator>Wiedenmann, A.</dc:creator>
    <dc:creator>Kammel, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001410</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A polarized small-angle scattering experiment with a concentrated magnetic fluid is described confirming dipolar chains and domains of hexagonal arrangements.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SMALL-ANGLE NEUTRON SCATTERING; POLARIZED NEUTRONS; MAGNETIC SCATTERING; MAGNETIC LIQUID STRUCTURE; FERROFLUIDS</dc:subject>
    <dc:description>Field-induced local ordering within a cobalt-based magnetic colloid has been studied with polarized small-angle scattering by turning the direction of the external magnetic field. By analysing the nuclear–magnetic cross term we were able to separate the scattering contributions from dipolar chains and domains of pseudo-crystalline hexagonal arrangements. The magnetic moments were found to be aligned along the external magnetic field and to follow the change of the field direction. The observed variation of the particle moments must give rise to a rearrangement of the local hexagonal structure with respect to the new field direction to explain the scattering pattern. We confirm this by two-dimensional simultaneous least-squares fits for different Q ranges [where Q = 4\pi \sin (\theta) / \lambda, λ is the X-ray wavelength and 2θ is the scattering angle] with a model containing a core–shell particle form factor and a structure factor composed of Gaussian peaks and contributions from polydisperse cylinders.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Reordering of magnetic colloid structures in external magnetic fields</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>57</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>61</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?cj6007">
    <title>Small-angle neutron scattering study of aqueous solutions of pentanediol and hexanediol</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?cj6007</link>
    <description>Aqueous solutions of 1,2-pentanediol, 1,5-pentanediol, 1,2-hexanediol and 1,6-hexanediol have been studied by small-angle neutron scattering over a wide range of concentrations and temperatures. The structure of the solutions on the mesoscopic length scale, corresponding to the intermolecular distances, was analysed with the help of the Kirkwood–Buff formalism. 1,2-Hexanediol solutions exhibited a strong attractive diol–diol interaction, a weak diol–diol attraction was found for 1,6-hexanediol and 1,2-pentanediol, and an extremely weak diol–diol attraction was found in 1,5-pentanediol solutions. The general tendencies are the following: aggregation is stronger as the length of the hydrophobic hydrocarbon chain increases and the 1,2-diols exhibit much stronger attraction then the 1,\omega-diols. The temperature dependence of the aggregation is weak for the 1,2-diols but strong for the 1,\omega-diols, indicating in the latter case the hydrophobic character of the interaction.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Székely, N.K.</dc:creator>
    <dc:creator>Almásy, L.</dc:creator>
    <dc:creator>Rădulescu, A.</dc:creator>
    <dc:creator>Rosta, L.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001483</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Aqueous solutions of 1,2-pentanediol, 1,5-pentanediol, 1,2-hexanediol and 1,6-hexanediol have been studied by small-angle neutron scattering, and the results analysed with the help of the Kirkwood–Buff formalism. The 1,2-hexanediol solutions exhibit the strongest attractive diol–diol interaction and the excess coordination numbers are in agreement with the possibility of forming micelles.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SANS; ALKANEDIOLS; KIRKWOOD-BUFF INTEGRALS</dc:subject>
    <dc:description>Aqueous solutions of 1,2-pentanediol, 1,5-pentanediol, 1,2-hexanediol and 1,6-hexanediol have been studied by small-angle neutron scattering over a wide range of concentrations and temperatures. The structure of the solutions on the mesoscopic length scale, corresponding to the intermolecular distances, was analysed with the help of the Kirkwood–Buff formalism. 1,2-Hexanediol solutions exhibited a strong attractive diol–diol interaction, a weak diol–diol attraction was found for 1,6-hexanediol and 1,2-pentanediol, and an extremely weak diol–diol attraction was found in 1,5-pentanediol solutions. The general tendencies are the following: aggregation is stronger as the length of the hydrophobic hydrocarbon chain increases and the 1,2-diols exhibit much stronger attraction then the 1,\omega-diols. The temperature dependence of the aggregation is weak for the 1,2-diols but strong for the 1,\omega-diols, indicating in the latter case the hydrophobic character of the interaction.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle neutron scattering study of aqueous solutions of pentanediol and hexanediol</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>307</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>311</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6012">
    <title>Self-assembled films of hydrophobin protein HFBIII from Trichoderma reesei</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6012</link>
    <description>Hydrophobins are a group of small amphiphilic proteins which are known to self-assemble on interfaces. They contain eight conserved cysteine residues, which make four disulfide bridges. A new hydrophobin protein, HFBIII, from the fungus Trichoderma reesei contains one extra cysteine residue, giving the protein a naturally reactive site. The self-assembly of hydrophobin protein HFBIII was studied using grazing-incidence X-ray diffraction and reflectivity. HFBIII self-assembles into a hexagonally ordered monolayer at an air/water interface and also forms crystalline coatings on a silicon substrate. The lattice constants for the hexagonal coatings are a = b = 56.5 Å, γ = 120°. The self-assembled structure in the HFBIII film is very similar to those formed by two other T. reesei hydrophobins, HFBI and HFBII.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Kisko, K.</dc:creator>
    <dc:creator>Szilvay, G.R.</dc:creator>
    <dc:creator>Vuorimaa, E.</dc:creator>
    <dc:creator>Lemmetyinen, H.</dc:creator>
    <dc:creator>Linder, M.B.</dc:creator>
    <dc:creator>Torkkeli, M.</dc:creator>
    <dc:creator>Serimaa, R.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001331</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Self-assembled films of hydrophobin HFBIII from the fungus Trichoderma reesei were studied at an air/water interface and on a solid substrate using grazing-incidence X-ray diffraction and reflectivity.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HYDROPHOBINS; GRAZING-INCIDENCE X-RAY DIFFRACTION; SELF-ASSEMBLY; REFLECTIVITY</dc:subject>
    <dc:description>Hydrophobins are a group of small amphiphilic proteins which are known to self-assemble on interfaces. They contain eight conserved cysteine residues, which make four disulfide bridges. A new hydrophobin protein, HFBIII, from the fungus Trichoderma reesei contains one extra cysteine residue, giving the protein a naturally reactive site. The self-assembly of hydrophobin protein HFBIII was studied using grazing-incidence X-ray diffraction and reflectivity. HFBIII self-assembles into a hexagonally ordered monolayer at an air/water interface and also forms crystalline coatings on a silicon substrate. The lattice constants for the hexagonal coatings are a = b = 56.5 Å, γ = 120°. The self-assembled structure in the HFBIII film is very similar to those formed by two other T. reesei hydrophobins, HFBI and HFBII.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Self-assembled films of hydrophobin protein HFBIII from Trichoderma reesei</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>355</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>360</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6001">
    <title>Anomalous small- and wide-angle X-ray scattering and X-ray absorption spectroscopy for Pt and Pt–Ru nanoparticles</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6001</link>
    <description>We have characterized the structures of two kinds of catalytic nanoparticles of Pt and Pt–Ru, using anomalous small-angle X-ray scattering (ASAXS), anomalous wide-angle X-ray scattering (AWAXS) and extended X-ray absorption fine structure (EXAFS) spectroscopy. With several X-ray energies near the Pt LIII edge, the AWAXS data reveal a face-centered cubic (f.c.c.) crystalline structure for Pt nanoparticles supported on carbon black, whereas the ASAXS data characterize the monometallic nanoparticles as polydisperse spheres with a mean size of 23 Å and a size distribution of 20%. With similar X-ray energies, ASAXS and AWAXS data for the Pt–Ru nanoparticles indicate that they have a mean size of ~29 Å and a slightly Pt-rich core that can be characterized by an f.c.c. crystalline structure similar to that of the pure Pt nanoparticles. The coordination numbers of the bimetallic nanoparticles extracted from the EXAFS data, collected at the Pt LIII edge and Ru K edge, also reveal a consistent structure of largely, but not completely, intermixed Pt and Ru atoms in the nanoparticles.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Jeng, U.-S.</dc:creator>
    <dc:creator>Lai, Y.-H.</dc:creator>
    <dc:creator>Sheu, H.-S.</dc:creator>
    <dc:creator>Lee, J.-F.</dc:creator>
    <dc:creator>Sun, Y.-S.</dc:creator>
    <dc:creator>Chuang, W.-T.</dc:creator>
    <dc:creator>Huang, Y.-S.</dc:creator>
    <dc:creator>Liu, D.-G.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001306</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Anomalous small- and wide-angle X-ray scattering and X-ray absorption spectroscopy are used to extract structural information on monometallic Pt and bimetallic Pt–Ru nanoparticles.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>ASAXS; AWAXS; EXAFS; PT-RU NANOPARTICLES</dc:subject>
    <dc:description>We have characterized the structures of two kinds of catalytic nanoparticles of Pt and Pt–Ru, using anomalous small-angle X-ray scattering (ASAXS), anomalous wide-angle X-ray scattering (AWAXS) and extended X-ray absorption fine structure (EXAFS) spectroscopy. With several X-ray energies near the Pt LIII edge, the AWAXS data reveal a face-centered cubic (f.c.c.) crystalline structure for Pt nanoparticles supported on carbon black, whereas the ASAXS data characterize the monometallic nanoparticles as polydisperse spheres with a mean size of 23 Å and a size distribution of 20%. With similar X-ray energies, ASAXS and AWAXS data for the Pt–Ru nanoparticles indicate that they have a mean size of ~29 Å and a slightly Pt-rich core that can be characterized by an f.c.c. crystalline structure similar to that of the pure Pt nanoparticles. The coordination numbers of the bimetallic nanoparticles extracted from the EXAFS data, collected at the Pt LIII edge and Ru K edge, also reveal a consistent structure of largely, but not completely, intermixed Pt and Ru atoms in the nanoparticles.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Anomalous small- and wide-angle X-ray scattering and X-ray absorption spectroscopy for Pt and Pt–Ru nanoparticles</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>418</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>422</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks5135">
    <title>Likelihood of crystallization: experimental and computational approaches</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks5135</link>
    <description>A report on the VIZIER Workshop on the `Definition of protein domains and their likelihood of crystallization', Vienna, Austria, 28–30 June 2006.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Carugo, O.</dc:creator>
    <dc:creator>Djinovic Carugo, K.</dc:creator>
    <dc:creator>Gorbalenya, A.E.</dc:creator>
    <dc:creator>Tucker, P.</dc:creator>
    <dc:date>2007-04-01</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001136</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>A report on the VIZIER Workshop on the `Definition of protein domains and their likelihood of crystallization', Vienna, Austria, 28–30 June 2006.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>STRUCTURAL GENOMICS STUDIES; BIOINFORMATICS; PROTEIN PRODUCTION</dc:subject>
    <dc:description>A report on the VIZIER Workshop on the `Definition of protein domains and their likelihood of crystallization', Vienna, Austria, 28–30 June 2006.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Likelihood of crystallization: experimental and computational approaches</dc:title>
    <dc:type>text</dc:type>
    <prism:number>2</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>meeting reports</prism:section>
    <prism:startingPage>392</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>393</prism:endingPage>
    <prism:eissn>1600-5767</prism:eissn>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6013">
    <title>Reduction of two-dimensional small- and wide-angle X-ray scattering data</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6013</link>
    <description>At the beamlines ID01 and ID02 of the European Synchrotron Radiation Facility in Grenoble, France, position-sensitive detectors for time-resolved small- and wide-angle X-ray scattering experiments are in use. The applied data reduction method has never been described comprehensively. This article outlines the parametrization of the raw data and introduces the programs developed for this purpose. Data reduction in the sense of this article means all steps between detector readout and normalization to absolute scattering intensities. This includes all corrections that can be made without any specific knowledge of the sample, e.g. detector dark-image correction, division by a flat-field and intensity normalization. Processed data are either two- or one-dimensional. Optionally, statistical errors can be propagated through the calculations.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Boesecke, P.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807001100</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The general parametrization of a small- and wide-angle X-ray scattering experiment and a program package for quantitative data reduction are presented.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SAXS; WAXS; PINHOLE CAMERA; SYNCHROTRON X-RAYS; TIME-RESOLVED EXPERIMENTS; TWO-DIMENSIONAL DATA PROCESSING; ABSOLUTE INTENSITY NORMALIZATION; STATISTICAL ERROR PROPAGATION; METADATA; DATA FORMAT; IMAGE TRANSFORMATIONS</dc:subject>
    <dc:description>At the beamlines ID01 and ID02 of the European Synchrotron Radiation Facility in Grenoble, France, position-sensitive detectors for time-resolved small- and wide-angle X-ray scattering experiments are in use. The applied data reduction method has never been described comprehensively. This article outlines the parametrization of the raw data and introduces the programs developed for this purpose. Data reduction in the sense of this article means all steps between detector readout and normalization to absolute scattering intensities. This includes all corrections that can be made without any specific knowledge of the sample, e.g. detector dark-image correction, division by a flat-field and intensity normalization. Processed data are either two- or one-dimensional. Optionally, statistical errors can be propagated through the calculations.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Reduction of two-dimensional small- and wide-angle X-ray scattering data</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>423</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>427</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6006">
    <title>A comparison of methods for the measurement of the particle-size distribution of magnetic nanoparticles</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6006</link>
    <description>Recently, interest in magnetic particles, particularly in the nanometre-size range, has increased significantly. The main driving forces behind this interest are both the development of improved synthesis techniques and an increase in the number of potential applications for suitable magnetic nanoparticles. A critical factor of interest in both the synthesis and the development of applications is the particle-size distribution. In this paper, we investigate three common techniques for determining the particle-size distribution of magnetic nanoparticles (electron microscopy, magnetic measurements and small-angle neutron scattering). We compare the distributions determined by each technique for two standard samples and discuss their advantages, disadvantages and limitations.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Woodward, R.C.</dc:creator>
    <dc:creator>Heeris, J.</dc:creator>
    <dc:creator>St.Pierre, T.G.</dc:creator>
    <dc:creator>Saunders, M.</dc:creator>
    <dc:creator>Gilbert, E.P.</dc:creator>
    <dc:creator>Rutnakornpituk, M.</dc:creator>
    <dc:creator>Zhang, Q.</dc:creator>
    <dc:creator>Riffle, J.S.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S002188980700091X</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Transmission electron microscopy, magnetic measurements and small-angle neutron scattering are compared as methods for determining the particle-size distribution of magnetic nanoparticles.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>MAGNETIC NANOPARTICLES; FERROFLUIDS; SUPERPARAMAGNETISM; MAGNETITE; SANS; LANGEVIN FITTING; TEM</dc:subject>
    <dc:description>Recently, interest in magnetic particles, particularly in the nanometre-size range, has increased significantly. The main driving forces behind this interest are both the development of improved synthesis techniques and an increase in the number of potential applications for suitable magnetic nanoparticles. A critical factor of interest in both the synthesis and the development of applications is the particle-size distribution. In this paper, we investigate three common techniques for determining the particle-size distribution of magnetic nanoparticles (electron microscopy, magnetic measurements and small-angle neutron scattering). We compare the distributions determined by each technique for two standard samples and discuss their advantages, disadvantages and limitations.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>A comparison of methods for the measurement of the particle-size distribution of magnetic nanoparticles</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>495</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>500</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6014">
    <title>Small-angle X-ray scattering measurements of expanded fluid Se in the semiconductor–metal transition region using synchrotron radiation</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6014</link>
    <description>Small-angle X-ray scattering measurements for expanded fluid Se were carried out up to the semiconductor–metal transition region at high temperature and high pressure. A broad peak appears in the small-angle X-ray scattering profiles in the temperature range 1273 to 1773 K at 60 MPa, which suggests a correlation length of 50 Å. We fitted the patterns using a model function proposed by Teubner &amp; Strey [J. Chem. Phys. (1987), 87, 3195–3200] and obtained two characteristic lengths, the domain size of the dense and rare regions, and the correlation length concerning their boundary. The present results suggest peculiar density fluctuations accompanying the SC-M transition in fluid Se consisting of polymeric molecules.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Inui, M.</dc:creator>
    <dc:creator>Matsuda, K.</dc:creator>
    <dc:creator>Tamura, K.</dc:creator>
    <dc:creator>Satoh, K.</dc:creator>
    <dc:creator>Sobajima, A.</dc:creator>
    <dc:creator>Tada, H.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807000751</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Small-angle X-ray scattering measurements for expanded fluid Se were carried out up to the semiconductor–metal transition region. A broad peak in the small-angle X-ray scattering profiles appears, suggesting a correlation length of 50 Å.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>EXPANDED FLUID SE; SMALL-ANGLE X-RAY SCATTERING; SEMICONDUCTOR-METAL TRANSITION</dc:subject>
    <dc:description>Small-angle X-ray scattering measurements for expanded fluid Se were carried out up to the semiconductor–metal transition region at high temperature and high pressure. A broad peak appears in the small-angle X-ray scattering profiles in the temperature range 1273 to 1773 K at 60 MPa, which suggests a correlation length of 50 Å. We fitted the patterns using a model function proposed by Teubner &amp; Strey [J. Chem. Phys. (1987), 87, 3195–3200] and obtained two characteristic lengths, the domain size of the dense and rare regions, and the correlation length concerning their boundary. The present results suggest peculiar density fluctuations accompanying the SC-M transition in fluid Se consisting of polymeric molecules.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Small-angle X-ray scattering measurements of expanded fluid Se in the semiconductor–metal transition region using synchrotron radiation</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>537</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>539</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?sy6041">
    <title>Synchrotron X-ray scattering studies on the structural evolution of microbial poly(3-hydroxybutyrate)</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?sy6041</link>
    <description>The crystallization behavior of microbially synthesized poly(3-hydroxybutyrate) was studied in detail using time-resolved small-angle X-ray scattering. This polyester was found to undergo primary crystallization as well as secondary crystallization. In the primary crystallization, the thicknesses of the lamellar crystals were sensitive to the crystallization temperature, but no thickening was observed throughout the entire crystallization at a given temperature. The thickness of the lamellar crystals in the polyester was always larger than that of the amorphous layers. Secondary crystallization favorably occurred during the later stage of isothermal crystallization in competition with the continuous primary crystallization, forming secondary crystals in amorphous regions, in particular in the amorphous layers between the primarily formed lamellar crystal stacks. Compared to the primarily formed lamellar crystals, the secondary crystals had short-range-ordered structures of smaller size, a broader size distribution, and a lower electron density.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Heo, K.</dc:creator>
    <dc:creator>Yoon, J.</dc:creator>
    <dc:creator>Jin, K.S.</dc:creator>
    <dc:creator> Jin, S.</dc:creator>
    <dc:creator>Kim, G.</dc:creator>
    <dc:creator>Sato, H.</dc:creator>
    <dc:creator>Ozaki, Y.</dc:creator>
    <dc:creator>Satkowski, M.M.</dc:creator>
    <dc:creator>Noda, I.</dc:creator>
    <dc:creator>Ree, M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807000878</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The primary and secondary crystallization behaviors of microbially synthesized poly(3-hydroxybutyrate) were studied in detail by time-resolved small-angle X-ray scattering with a synchrotron-radiation source.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>X-RAY SCATTERING; MICROBIAL POLYESTER; ISOTHERMAL CRYSTALLIZATION; PRIMARY CRYSTAL; SECONDARY CRYSTAL; LAMELLAR CRYSTAL; AMORPHOUS LAYER; LONG PERIOD</dc:subject>
    <dc:description>The crystallization behavior of microbially synthesized poly(3-hydroxybutyrate) was studied in detail using time-resolved small-angle X-ray scattering. This polyester was found to undergo primary crystallization as well as secondary crystallization. In the primary crystallization, the thicknesses of the lamellar crystals were sensitive to the crystallization temperature, but no thickening was observed throughout the entire crystallization at a given temperature. The thickness of the lamellar crystals in the polyester was always larger than that of the amorphous layers. Secondary crystallization favorably occurred during the later stage of isothermal crystallization in competition with the continuous primary crystallization, forming secondary crystals in amorphous regions, in particular in the amorphous layers between the primarily formed lamellar crystal stacks. Compared to the primarily formed lamellar crystals, the secondary crystals had short-range-ordered structures of smaller size, a broader size distribution, and a lower electron density.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Synchrotron X-ray scattering studies on the structural evolution of microbial poly(3-hydroxybutyrate)</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>594</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>598</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6022">
    <title>Effects of side-chain length on the magnetic response of discotic metallomesogens</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6022</link>
    <description>The magnetic responses of columnar superstructures of discotic metallomesogens with different alkyl side-chain lengths, cobalt octa(n-alkylthio)porphyrazine (CoSx, where x is the peripheral n-alkyl chain length, x = 10, 12, 14), have been investigated by small-angle neutron scattering (SANS). CoSx (x = 10, 12, 14) were heated to their isotropic phases and cooled down to their columnar mesophases under various external magnetic fields (0.2–1.1 T) and the orientational orderings of the columnar mesophases were measured by SANS. The SANS patterns showed clear anisotropies indicating the alignment of columnar domains with their columnar directors perpendicular to the applied magnetic field. The annularly averaged SANS data, I(Φ), of CoSx (x = 10, 12, 14) under various magnetic field strengths were fitted with Lorentzian functions. The full width at half maximum (FWHM) of the I(Φ) of CoS10 and CoS12 rapidly decreases with increasing applied magnetic field and then saturates to about 42° at ~0.5 T and 50° at ~0.6 T, respectively. In the case of CoS14, however, the diffraction anisotropy was very weak even at field strengths as high as 1.13 T and the FWHM was very broad, ca. 120°. The dramatic decrease of magnetic field sensitivity of CoS14 may be attributed to the entropy increase with the side-chain length.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Lee, J.-H.</dc:creator>
    <dc:creator>Kim, H.-S.</dc:creator>
    <dc:creator>Pate, B.D.</dc:creator>
    <dc:creator>Choi, S.-M.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807000441</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>The magnetic responses of columnar discotic metallomesogens, cobalt octa(n-alkylthio)porphyrazine with different side-chain lengths (CoSx, where x is the peripheral n-alkyl chain length, x = 10, 12, 14), have been investigated by small-angle neutron scattering. The magnetic field strength required for the alignment of the columnar phase increased with the side-chain length x.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>DISCOTIC METALLOMESOGEN; COLUMNAR SUPERSTRUCTURE; MAGNETIC ALIGNMENT; SMALL-ANGLE NEUTRON SCATTERING; CHAIN LENGTH</dc:subject>
    <dc:description>The magnetic responses of columnar superstructures of discotic metallomesogens with different alkyl side-chain lengths, cobalt octa(n-alkylthio)porphyrazine (CoSx, where x is the peripheral n-alkyl chain length, x = 10, 12, 14), have been investigated by small-angle neutron scattering (SANS). CoSx (x = 10, 12, 14) were heated to their isotropic phases and cooled down to their columnar mesophases under various external magnetic fields (0.2–1.1 T) and the orientational orderings of the columnar mesophases were measured by SANS. The SANS patterns showed clear anisotropies indicating the alignment of columnar domains with their columnar directors perpendicular to the applied magnetic field. The annularly averaged SANS data, I(Φ), of CoSx (x = 10, 12, 14) under various magnetic field strengths were fitted with Lorentzian functions. The full width at half maximum (FWHM) of the I(Φ) of CoS10 and CoS12 rapidly decreases with increasing applied magnetic field and then saturates to about 42° at ~0.5 T and 50° at ~0.6 T, respectively. In the case of CoS14, however, the diffraction anisotropy was very weak even at field strengths as high as 1.13 T and the FWHM was very broad, ca. 120°. The dramatic decrease of magnetic field sensitivity of CoS14 may be attributed to the entropy increase with the side-chain length.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Effects of side-chain length on the magnetic response of discotic metallomesogens</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>68</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>72</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6031">
    <title>Density fluctuations in oxide glasses investigated by small-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6031</link>
    <description>The structure of glasses is characterized by the existence of density and composition fluctuations on the nanometre scale. We present three examples of the use of small-angle X-ray scattering to get information about these density fluctuations. The thermal history and OH content were observed to have a huge influence. The static compressibility decreases when the OH content or fictive temperature increase. We showed that temperature scanning small-angle X-ray scattering can provide an accurate description of the position, width and shape of the glass transition.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Levelut, C.</dc:creator>
    <dc:creator>Le Parc, R.</dc:creator>
    <dc:creator>Faivre, A.</dc:creator>
    <dc:creator>Brüning, R.</dc:creator>
    <dc:creator>Champagnon, B.</dc:creator>
    <dc:creator>Martinez, V.</dc:creator>
    <dc:creator>Simon, J.-P.</dc:creator>
    <dc:creator>Bley, F.</dc:creator>
    <dc:creator>Hazemann, J.-L.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807000507</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Three examples of the use of small-angle X-ray scattering in the determination of density fluctuations on the nanometre scale in silica glasses are given: the influence of thermal history and OH content; the determination of static compressibility; and temperature scanning small-angle X-ray scattering as an alternative to temperature scanning calorimetry.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>SMALL-ANGLE X-RAY SCATTERING; DENSITY FLUCTUATIONS; OXIDE GLASSES; TEMPERATURE SCANNING SMALL-ANGLE X-RAY SCATTERING</dc:subject>
    <dc:description>The structure of glasses is characterized by the existence of density and composition fluctuations on the nanometre scale. We present three examples of the use of small-angle X-ray scattering to get information about these density fluctuations. The thermal history and OH content were observed to have a huge influence. The static compressibility decreases when the OH content or fictive temperature increase. We showed that temperature scanning small-angle X-ray scattering can provide an accurate description of the position, width and shape of the glass transition.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Density fluctuations in oxide glasses investigated by small-angle X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>512</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>516</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?ks6009">
    <title>Core structure of latent heavy-ion tracks in {100} LiF derived by small-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?ks6009</link>
    <description>Radial electron densities within 27–111 µm-long ion damage trails, `latent ion tracks', created in {100} LiF by irradiation with GeV Pb and U projectiles, have been derived by means of small-angle X-ray scattering. The tracks exhibit continuous electron density decreases of 49–74% along the centers of their 2.3–3.4 nm-diameter cores. Structural alteration under the intense ion-deposited electronic excitation has been attributed to two successive processes: (a) local breakdown of the LiF lattice into fluorine molecules and Li atoms, and (b) release of the fluorine gas and of at least a portion of the voluminous Li atoms through the low-density tracks.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Abu Saleh, S.</dc:creator>
    <dc:creator>Eyal, Y.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807000064</dc:identifier>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:teaser>Small-angle X-ray scattering analyses on {100} LiF platelets following irradiation with swift Pb and U ions have revealed continuous highly depleted electron densities close to the ion trajectories, suggesting local ion-induced decomposition of the crystal followed by release of mobile alteration products.</dc:teaser>
    <dc:language>en</dc:language>
    <dc:subject>HEAVY-ION TRACKS; LATENT ION TRACKS; TRACK STRUCTURE; SAXS; LIF</dc:subject>
    <dc:description>Radial electron densities within 27–111 µm-long ion damage trails, `latent ion tracks', created in {100} LiF by irradiation with GeV Pb and U projectiles, have been derived by means of small-angle X-ray scattering. The tracks exhibit continuous electron density decreases of 49–74% along the centers of their 2.3–3.4 nm-diameter cores. Structural alteration under the intense ion-deposited electronic excitation has been attributed to two successive processes: (a) local breakdown of the LiF lattice into fluorine molecules and Li atoms, and (b) release of the fluorine gas and of at least a portion of the voluminous Li atoms through the low-density tracks.</dc:description>
    <dc:format>text/html</dc:format>
    <dc:title>Core structure of latent heavy-ion tracks in {100} LiF derived by small-angle X-ray scattering</dc:title>
    <dc:type>text</dc:type>
    <prism:number>s1</prism:number>
    <prism:volume>40</prism:volume>
    <prism:publicationDate>2007-04-21</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2007 International Union of Crystallography</prism:copyright>
    <prism:issn>0021-8898</prism:issn>
    <prism:section>short communications</prism:section>
    <prism:startingPage>121</prism:startingPage>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:endingPage>125</prism:endingPage>
    <prism:eissn/>
  </item>
  <item rdf:about="http://scripts.iucr.org/cgi-bin/paper?aj6016">
    <title>Cylindrical nanochannels in ion-track polycarbonate membranes studied by small-angle X-ray scattering</title>
    <link>http://scripts.iucr.org/cgi-bin/paper?aj6016</link>
    <description>Different types of polycarbonate foils were irradiated with 1.4 GeV Xe ions, ultra-violet (UV) treated and subsequently etched, creating cylindrical pores of high aspect ratio. The pores are perfectly well aligned and represent excellent objects for small-angle X-ray scattering. Two-dimensional scattering spectra exhibit highly anisotropic patterns with clear presentation of numerous oscillations of the Bessel function, the radial part of the scattering function. Modelling the pores as parallel cylinders allows us to deduce the pore radius and the radius dispersion as a function of UV treatment, etching time and fluence. It is demonstrated that the UV treatment has a beneficial influence on the pore-size distribution, in particular for small pores.</description>
    <dc:rights>Copyright (c) 2007 International Union of Crystallography</dc:rights>
    <dc:source>urn:issn:0021-8898</dc:source>
    <dc:creator>Pépy, G.</dc:creator>
    <dc:creator>Boesecke, P.</dc:creator>
    <dc:creator>Kuklin, A.</dc:creator>
    <dc:creator>Manceau, E.</dc:creator>
    <dc:creator>Schiedt, B.</dc:creator>
    <dc:creator>Siwy, Z.</dc:creator>
    <dc:creator>Toulemonde, M.</dc:creator>
    <dc:creator>Trautmann, C.</dc:creator>
    <dc:date>2007-04-21</dc:date>
    <dc:identifier>doi:10.1107/S0021889807000088</dc:identifier>
    <dc:publisher>Internation