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    <responseDate>2026-10-12T02:10:45Z</responseDate>
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    <identifier>10.57760/sciencedb.j00213.00274</identifier>
    <datestamp>2026-03-23T16:42:31Z</datestamp>
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<oai_dc:dc xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:date>2026-03-23</dc:date>
  <dc:title>Interpretation of Hugoniot Elastic Limit Experiments Based on High-Pressure Thermoelastic Simulations</dc:title>
  <dc:identifier>doi:10.57760/sciencedb.j00213.00274</dc:identifier>
  <dc:language>en</dc:language>
  <dc:description>This dataset compiles thermoelastic simulation data for diamond under extreme high-pressure and high-temperature conditions. Its primary objective is to provide a continuous sound velocity-pressure response relationship for the precise determination of the Hugoniot Elastic Limit (HEL).The theoretically simulated thermoelastic dataset was generated using the following methods: The static energy-volume relationship was obtained via first-principles calculations using the Vienna Ab initio Simulation Package (VASP) and fitted to the fourth-order Birch-Murnaghan Equation of State (EOS). Building upon this, the diamond EOS covering a wide temperature and pressure range (0&amp;ndash;1000 K, 0&amp;ndash;500 GPa) was constructed by combining the Quasi-Harmonic Approximation (QHA) with the Mean-Field Potential (MFP) method. Subsequently, elastic constants and sound velocities were derived from the EOS using the energy-strain method within the Quasi-Static Approximation (QSA) framework.The simulation dataset includes the following key physical quantities: temperature (T), pressure (P), elastic constants (C11, C12, C44), bulk moduli (BV, BR, BH) and shear moduli (GV, GR, GH) under the Voigt-Reuss-Hill approximation, Young's modulus (EH), Poisson's ratio (nuH), related moduli (kH, HH), anisotropy indices (AVR, AU), as well as longitudinal sound velocity (CL) and bulk sound velocity (CB).</dc:description>
  <dc:subject>Thermoelasticity ; Diamond; Equation of State</dc:subject>
  <dc:creator>Junlei Yin</dc:creator>
  <dc:creator>Xingyu Gao</dc:creator>
  <dc:creator>William Yi Wang</dc:creator>
  <dc:creator>Haifeng Liu</dc:creator>
  <dc:creator>Haifeng Song</dc:creator>
  <dc:creator>Jinshan Li</dc:creator>
  <dc:creator>Pingxiang Zhang</dc:creator>
  <dc:rights>EMBARGO</dc:rights>
  <dc:rights>https://creativecommons.org/licenses/by/4.0/</dc:rights>
  <dc:type>dataset</dc:type>
  <dc:relation>http://www.doi.org/10.7498/aps.75.20260047</dc:relation>
  <dc:publisher>Science Data Bank</dc:publisher>
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