<?xml version="1.0"?>
<?xml-stylesheet href="/style/rdf2html.xsl"  type="text/xsl"?><rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns="http://purl.org/rss/1.0/" xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/" xmlns:taxo="http://purl.org/rss/1.0/modules/taxonomy/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:syn="http://purl.org/rss/1.0/modules/syndication/" xmlns:admin="http://webns.net/mvcb/">
  <channel rdf:about="http://journals.iucr.org/j/journalhomepage.html">
    <title>Open access article in Journal of Applied Crystallography</title>
    <link>http://journals.iucr.org/j/journalhomepage.html</link>
    <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>
    <dc:language>en-gb</dc:language>
    <dc:rights>Copyright (c) 2008 International Union of Crystallography</dc:rights>
    <dc:publisher>International Union of Crystallography</dc:publisher>
    <dc:creator>International Union of Crystallography</dc:creator>
    <dc:source>http://journals.iucr.org</dc:source>
    <dc:identifier>urn:issn: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>
    <dc:format>text/html</dc:format>
    <dc:title>Open access article in Journal of Applied Crystallography</dc:title>
    <dc:type>text</dc:type>
    <syn:updatePeriod>yearly</syn:updatePeriod>
    <syn:updateFrequency>6</syn:updateFrequency>
    <syn:updateBase>2002-02-01T00:00+00:00</syn:updateBase>
    <prism:rightsAgent>med@iucr.org</prism:rightsAgent>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:copyright>Copyright (c) 2008 International Union of Crystallography</prism:copyright>
    <prism:issn>urn:issn:0021-8898</prism:issn>
    <items>
      <rdf:Seq>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?kk5026"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5182"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?pf0067"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ce5042"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5407"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?py5004"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5161"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cg5071"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cg5072"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?kk5014"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5154"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5368"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?pf0048"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6003"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6023"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6020"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6027"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6035"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6001"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6025"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6014"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?kk5010"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6016"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6023"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6022"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6020"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6016"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6010"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6006"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6018"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6019"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6033"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6013"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6030"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6024"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6010"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6015"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6012"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6004"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6009"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6013"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6021"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6008"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6029"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6026"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6005"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6025"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6028"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6021"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6015"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6005"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6031"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6036"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6004"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6012"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6017"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6021"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6007"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6015"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6029"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6003"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6001"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6012"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6026"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6025"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6021"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6006"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6015"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6005"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6009"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6044"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6018"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6017"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6028"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cg5057"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6037"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6029"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6022"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6012"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6023"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6014"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6007"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6013"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6018"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6028"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6002"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6016"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6042"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6003"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6016"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6020"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6002"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6022"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6004"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6006"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6013"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6029"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6023"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6004"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6007"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6012"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6001"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5135"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6013"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6006"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6014"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6041"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6022"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6031"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6009"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6016"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6040"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6001"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6019"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6008"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6003"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6004"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6039"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6033"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6007"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6017"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6034"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6032"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6008"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6002"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6002"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6024"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6024"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cj6021"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6002"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6026"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6034"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6010"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6005"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6023"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6030"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6038"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6027"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6014"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6041"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6007"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6018"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6037"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj5076"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6018"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6036"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5355"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6033"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks6027"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sy6032"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6010"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?sm6009"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6032"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6014"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6006"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?wf5024"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj6003"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?db5010"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5105"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?db5008"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?wf5025"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?dd5032"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?pf0037"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?pf0036"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?db5005"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj5065"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5102"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5345"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?wf5020"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5071"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5087"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5099"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?me0319"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?hx5036"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?wf5014"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?dd5030"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5082"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?pf0027"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?dd5018"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5074"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5337"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?zm5036"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ko5017"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?pf0021"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?hi5568"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5333"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ea5040"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?dd5017"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cg5023"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj5041"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?os5023"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5330"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?dd5015"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?os5020"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?pd5033"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?cg5019"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?hx5022"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?hx5023"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?zm5022"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks0217"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ko5011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?do5008"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj5028"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?me0275"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?me0274"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?hx5010"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks0213"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5027"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?mm0046"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?os5011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5026"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5035"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?mm0043"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5008"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks5009"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?mm0044"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?mm0045"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?dd5004"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?os5009"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ea5014"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?os5010"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?wf5005"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?wf5004"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?wf5003"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5280"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he0323"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj5016"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?es0337"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5290"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?zm5015"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?es0335"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj5011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?mm0036"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?mm0042"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?he5276"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj0008"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj0009"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?aj0011"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?ks7100"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?es0329"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?es0336"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?es0323"/>
        <rdf:li rdf:resource="http://scripts.iucr.org/cgi-bin/paper?os0104"/>
      </rdf:Seq>
    </items>
    <image rdf:resource="http://journals.iucr.org/logos/rss10j.gif"/>
  </channel>
  <image rdf:about="http://journals.iucr.org/logos/rss10j.gif">
    <title>Open access article in Journal of Applied Crystallography</title>
    <url>http://journals.iucr.org/logos/rss10j.gif</url>
    <link>http://journals.iucr.org/j/journalhomepage.html</link>
    <dc:type>Still image</dc:type>
  </image>
  <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:endingPage>790</prism:endingPage>
    <prism:publicationDate>2008-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:section>research papers</prism:section>
    <prism:startingPage>784</prism:startingPage>
  </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:endingPage>799</prism:endingPage>
    <prism:publicationDate>2008-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:section>short communications</prism:section>
    <prism:startingPage>798</prism:startingPage>
  </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:section>book reviews</prism:section>
    <prism:startingPage>826</prism:startingPage>
    <prism:endingPage>827</prism:endingPage>
  </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:endingPage>814</prism:endingPage>
    <prism:publicationDate>2008-08-01</prism:publicationDate>
    <prism:publicationName>Journal of Applied Crystallography</prism:publicationName>
    <prism:section>computer programs</prism:section>
    <prism:startingPage>811</prism:startingPage>
  </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:section>CIF applications</prism:section>
    <prism:startingPage>808</prism:startingPage>
    <prism:endingPage>810</prism:endingPage>
  </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:section>letters to the editor</prism:section>
    <prism:startingPage>659</prism:startingPage>
    <prism:endingPage>659</prism:endingPage>
  </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:section>research papers</prism:section>
    <prism:startingPage>96</prism:startingPage>
    <prism:endingPage>103</prism:endingPage>
  </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:section>computer programs</prism:section>
    <prism:startingPage>1179</prism:startingPage>
    <prism:endingPage>1182</prism:endingPage>
  </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:section>computer programs</prism:section>
    <prism:startingPage>1183</prism:startingPage>
    <prism:endingPage>1188</prism:endingPage>
  </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:section>teaching and education</prism:section>
    <prism:startingPage>1153</prism:startingPage>
    <prism:endingPage>1165</prism:endingPage>
  </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:section>meeting reports</prism:section>
    <prism:startingPage>808</prism:startingPage>
    <prism:endingPage>809</prism:endingPage>
  </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:section>research papers</prism:section>
    <prism:startingPage>658</prism:startingPage>
    <prism:endingPage>674</prism:endingPage>
  </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:section>book reviews</prism:section>
    <prism:startingPage>637</prism:startingPage>
    <prism:endingPage>638</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>259</prism:startingPage>
    <prism:endingPage>263</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>581</prism:startingPage>
    <prism:endingPage>584</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>264</prism:startingPage>
    <prism:endingPage>268</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>283</prism:startingPage>
    <prism:endingPage>285</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>474</prism:startingPage>
    <prism:endingPage>479</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>332</prism:startingPage>
    <prism:endingPage>334</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>585</prism:startingPage>
    <prism:endingPage>589</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>701</prism:startingPage>
    <prism:endingPage>705</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>279</prism:startingPage>
    <prism:endingPage>282</prism:endingPage>
  </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:section>research papers</prism:section>
    <prism:startingPage>539</prism:startingPage>
    <prism:endingPage>545</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>101</prism:startingPage>
    <prism:endingPage>105</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>397</prism:startingPage>
    <prism:endingPage>401</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>549</prism:startingPage>
    <prism:endingPage>552</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>650</prism:startingPage>
    <prism:endingPage>655</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>558</prism:startingPage>
    <prism:endingPage>563</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>292</prism:startingPage>
    <prism:endingPage>296</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>303</prism:startingPage>
    <prism:endingPage>306</prism:endingPage>
  </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:section>short communications</prism:section>
    <prism:startingPage>170</prism:startingPage>
    <prism:endingPage>174</prism:endingPage>
  </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 solu