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    <titleInfo>
      <title>Insights into the high-pressure behavior of kaolinite from infrared spectroscopy and quantum-mechanical calculations</title>
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      <namePart type="family">Welch</namePart>
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    <abstract>The high-pressure behavior of Keokuk kaolinite has been studied to 9.5 GPa by infrared spectroscopy using synchrotron radiation. The kaolinite-I -&gt; kaolinite-II and kaolinite-II -&gt; kaolinite-III transformations have clear spectroscopic expression, with discontinuities coinciding with the transformation pressures bracketed by X-ray diffraction (Welch and Crichton in Am Mineral 95: 651654, 2010). The experimental spectra have been interpreted from band assignments derived from density functional theory for the structures of kaolinite-II and kaolinite-III, using as starting models the ab initio structures reported by Mercier and Le Page (Acta Crystallogr A B64:131-143, 2008, Mater Sci Technol 25:437-442, 2009) and unit-cell parameters from Welch and Crichton (Am Mineral 95: 651654, 2010). The relaxed theoretical structures are very similar to those reported by Mercier and Le Page (Acta Crystallogr A B64: 131-143, 2008, Mater Sci Technol 25: 437-442, 2009) in their theoretical investigation of kaolinite polytypes at high pressure. The vibrational spectra calculated from the quantum-mechanical analysis allow band assignments of the IR spectra to be made and provide insights into the behavior of different OH environments in the two high-pressure polytypes. The single perpendicular-interlayer OH group of kaolinite-III has a distinctive spectroscopic signature that is diagnostic of this polytype (v = 3,595 cm(-1) at 9.5 GPa) and is sensitive to the compression/expansion of the interlayer space. This OH group also has a distinctive signature in the calculated spectra. The spectra collected on decompression are those of kaolinite-III and persist largely unchanged to 4.6 GPa, except for a continuous blue shift of the 3,595 cm(-1) band to 3,613 cm(-1). Finally, kaolinite-I is recovered at 0.6 GPa, confirming the kaolinite-III -&gt; kaolinite-I transformation previously observed by X-ray diffraction, and the irreversibility of the kaolinite-II -&gt; kaolinite-III transformation. The ambient spectra collected at the start and finish of the experiment are those of kaolinite-I, and start/finish band frequencies agree to within 6 cm(-1).</abstract>
    <targetAudience authority="marctarget">specialized</targetAudience>
    <subject>
      <topic>Kaolinite</topic>
      <topic>Polytypism</topic>
      <topic>In situ high-P</topic>
      <topic>Synchrotron IR</topic>
      <topic>Phase transformations</topic>
      <topic>First-principles calculations</topic>
    </subject>
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      <titleInfo>
        <title>Physics and Chemistry of Minerals</title>
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      <part>
        <detail type="volume">
          <number>39</number>
        </detail>
        <detail type="volume">
          <number>2</number>
        </detail>
        <extent unit="pages">
          <list> 143-151</list>
        </extent>
      </part>
      <originInfo>
        <dateIssued>2012</dateIssued>
      </originInfo>
      <identifier type="issn">0342-1791</identifier>
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    <identifier type="uri">https://www.documentation.ird.fr/hor/fdi:010055654</identifier>
    <identifier type="doi">10.1007/s00269-011-0469-5</identifier>
    <identifier type="issn">0342-1791</identifier>
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      <recordCreationDate encoding="w3cdtf">2012-04-04</recordCreationDate>
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