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  <Article>
    <Journal>
      <PublisherName/>
      <JournalTitle>Acta Medica Okayama</JournalTitle>
      <Issn/>
      <Volume>61</Volume>
      <Issue>2</Issue>
      <PubDate PubStatus="ppublish">
        <Year>2000</Year>
        <Month/>
      </PubDate>
    </Journal>
    <ArticleTitle>Annealing effects on the magnetic and structural properties of single-crystal TDAE-C-60</ArticleTitle>
    <FirstPage LZero="delete"/>
    <LastPage/>
    <Language>EN</Language>
    <AuthorList>
      <Author>
        <FirstName EmptyYN="N">Takashi</FirstName>
        <LastName>Kambe</LastName>
        <Affiliation/>
      </Author>
      <Author>
        <FirstName EmptyYN="N">Yoshio</FirstName>
        <LastName>Nogami</LastName>
        <Affiliation/>
      </Author>
      <Author>
        <FirstName EmptyYN="N">Kokichi</FirstName>
        <LastName>Oshima</LastName>
        <Affiliation/>
      </Author>
    </AuthorList>
    <PublicationType/>
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    <Abstract>&lt;p&gt;Annealing effects on the magnetic and structural properties of single-crystal TDAE-C-60 are investigated. When a crystal is well-annealed at 350 K, ferromagnetic ordering takes place below 16 K, though no magnetic phase transition is shown in as-grown crystal. The saturated magnetization was obtained to be 0.9+/-0.1 mu(B) per C-60. It was first found that the well-annealed crystal shows a structural phase transition around 180 K, probably associated with the orientational ordering of C-60 molecules. On the other hand, the as-grown crystal undergoes no structural phase transition at least down to 30 K while the motion of C-60 molecules is restricted below around 150 K. The possible relation between the low-temperature structure and the magnetic ordering is discussed.&lt;/p&gt;
</Abstract>
    <CoiStatement>No potential conflict of interest relevant to this article was reported.</CoiStatement>
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  </Article>
  <Article>
    <Journal>
      <PublisherName/>
      <JournalTitle>Acta Medica Okayama</JournalTitle>
      <Issn/>
      <Volume>329-333</Volume>
      <Issue/>
      <PubDate PubStatus="ppublish">
        <Year>2003</Year>
        <Month/>
      </PubDate>
    </Journal>
    <ArticleTitle>X-ray study of modulated structures of beta-Cu&lt;sub&gt;x&lt;/sub&gt;V&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt;</ArticleTitle>
    <FirstPage LZero="delete">713</FirstPage>
    <LastPage>714</LastPage>
    <Language>EN</Language>
    <AuthorList>
      <Author>
        <FirstName EmptyYN="N">Nobuaki</FirstName>
        <LastName>Nagao</LastName>
        <Affiliation/>
      </Author>
      <Author>
        <FirstName EmptyYN="N">Yoshio</FirstName>
        <LastName>Nogami</LastName>
        <Affiliation/>
      </Author>
      <Author>
        <FirstName EmptyYN="N">Kokichi</FirstName>
        <LastName>Oshima</LastName>
        <Affiliation/>
      </Author>
      <Author>
        <FirstName EmptyYN="N">Hiroyuki</FirstName>
        <LastName>Yamada</LastName>
        <Affiliation/>
      </Author>
      <Author>
        <FirstName EmptyYN="N">Yutaka</FirstName>
        <LastName>Ueda</LastName>
        <Affiliation/>
      </Author>
    </AuthorList>
    <PublicationType/>
    <ArticleIdList>
      <ArticleId IdType="doi"/>
    </ArticleIdList>
    <Abstract>&lt;p&gt;High resolution X-ray study reveals the wave vector change in the modulated structure of the quasi-one dimensional compound beta'-Cu vanadium bronze. Structural modulation of the reduced wave vector q&lt;sub&gt;0&lt;/sub&gt; = (0, 0.305, 0) emerges below 220 K in beta'-Cu&lt;sub&gt;0.29&lt;/sub&gt;V&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt; . For beta'-Cu&lt;sub&gt;0.39&lt;/sub&gt;V&lt;sub&gt;2&lt;/sub&gt;O&lt;sub&gt;5&lt;/sub&gt;, not the single q modulation but two kinds of modulations were observed. A three-fold superlattice structure with q1 = (0, 0.333, 0) appears below 210 K. An incommensurate modulated structure with q2 = (0, 0.26 ? 0.29, 0) coexists below 175 K, whose satellite intensity and b* component Qb have temperature and passing-time dependencies between 140 K and 175 K. The competition between q&lt;sub&gt;1&lt;/sub&gt; and q&lt;sub&gt;2&lt;/sub&gt; modulations was also observed. It seems that the q&lt;sub&gt;2&lt;/sub&gt; is deeply related to the physical property change between 140 K and 180 K confirmed by the decrease in the magnetic susceptibility and the increase in the resistivity.&lt;/p&gt;
</Abstract>
    <CoiStatement>No potential conflict of interest relevant to this article was reported.</CoiStatement>
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      <Object Type="keyword">
        <Param Name="value">x-ray</Param>
      </Object>
      <Object Type="keyword">
        <Param Name="value">modulated structures</Param>
      </Object>
      <Object Type="keyword">
        <Param Name="value">low dimensional conductor</Param>
      </Object>
      <Object Type="keyword">
        <Param Name="value">vanadium bronze</Param>
      </Object>
      <Object Type="keyword">
        <Param Name="value">b-cuxv2o5</Param>
      </Object>
    </ObjectList>
    <ReferenceList/>
  </Article>
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