March 28, 2026 Dataset Open Access

Chuna, Thomas; Boehme, Maximilian; Dornheim, Tobias

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  <identifier identifierType="DOI">10.14278/rodare.4580</identifier>
  <creators>
    <creator>
      <creatorName>Chuna, Thomas</creatorName>
      <givenName>Thomas</givenName>
      <familyName>Chuna</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0000-0001-8400-4495</nameIdentifier>
      <affiliation>Helmholtz-Zentrum Dresden-Rossendorf (HZDR)</affiliation>
    </creator>
    <creator>
      <creatorName>Boehme, Maximilian</creatorName>
      <givenName>Maximilian</givenName>
      <familyName>Boehme</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0000-0003-0290-3628</nameIdentifier>
      <affiliation>Lawrence Livermore National Laboratory</affiliation>
    </creator>
    <creator>
      <creatorName>Dornheim, Tobias</creatorName>
      <givenName>Tobias</givenName>
      <familyName>Dornheim</familyName>
      <nameIdentifier nameIdentifierScheme="ORCID" schemeURI="http://orcid.org/">0000-0001-7293-6615</nameIdentifier>
      <affiliation>Helmholtz-Zentrum Dresden-Rossendorf (HZDR)</affiliation>
    </creator>
  </creators>
  <titles>
    <title>Temperature dependence of the dynamic structure factor of the electron liquid via analytic continuation</title>
  </titles>
  <publisher>Rodare</publisher>
  <publicationYear>2026</publicationYear>
  <subjects>
    <subject>analytic conitnuation</subject>
    <subject>dynamic structure factor</subject>
    <subject>uniform electron gas</subject>
  </subjects>
  <dates>
    <date dateType="Issued">2026-03-28</date>
  </dates>
  <resourceType resourceTypeGeneral="Dataset"/>
  <alternateIdentifiers>
    <alternateIdentifier alternateIdentifierType="url">https://rodare.hzdr.de/record/4580</alternateIdentifier>
  </alternateIdentifiers>
  <relatedIdentifiers>
    <relatedIdentifier relatedIdentifierType="URL" relationType="IsIdenticalTo">https://www.hzdr.de/publications/Publ-43193</relatedIdentifier>
    <relatedIdentifier relatedIdentifierType="DOI" relationType="IsVersionOf">10.14278/rodare.4579</relatedIdentifier>
    <relatedIdentifier relatedIdentifierType="URL" relationType="IsPartOf">https://rodare.hzdr.de/communities/rodare</relatedIdentifier>
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  <rightsList>
    <rights rightsURI="https://creativecommons.org/licenses/by/4.0/legalcode">Creative Commons Attribution 4.0 International</rights>
    <rights rightsURI="info:eu-repo/semantics/openAccess">Open Access</rights>
  </rightsList>
  <descriptions>
    <description descriptionType="Abstract">&lt;p&gt;All results have been computed for the unpolarized UEG, i.e., with an equal number of spin-up and spin-down electrons $N^\uparrow=N^\downarrow=N/2$ for $N=34$. For $r_s = 20$ and at $\Theta=0.75$, there are 1000 independent MCMC seeds, at $\Theta=1, \, 2$ there are $280$ seeds, at $\Theta=4, \,8$ there are $277$ seeds. To compute the data, we conduct leave-one-out binning across the seeds and for all the data, the variance of the mean is $\delta F \approx 10^{-3}-10^{-4}$. This error estimate is computed for each leave-one-out-bin via Hatano&amp;#39;s error formula~\cite{hatano1994data} and verified using leave-one-out binning~\cite{berg_book_2004}. This is the online repository with the PIMC results for $F(\mathbf{q},\tau)$ and analytic continuation results for $S(q,\omega)$&amp;nbsp; seen &amp;quot;Temperature dependence of the dynamic structure factor of the electron liquid via analytic continuation&amp;quot;&amp;nbsp;article.&amp;nbsp;&lt;br&gt;
&lt;br&gt;
The data&amp;nbsp;contained here is (1) leave-one-binned imaginary time correlation functions F(tau) (units&amp;nbsp;dimensionless) over tau (units 1/Hartree) and there error (2)&amp;nbsp;the dynamic structure factors (units 1/Hartree) over omega (units Hartree) obtained using Bryan&amp;#39;s MEM with the static approximation as the Bayesian prior&amp;nbsp;(3)&amp;nbsp;the dynamic structure factors (units 1/Hartree) over omega (units Hartree) obtained using&amp;nbsp; PyLIT with the static approximation as the Bayesian prior&amp;nbsp;(4) The omega-&amp;gt;0 limit of the ideal gas susceptibility chi(q,0)/n/beta (units&amp;nbsp;dimensionless) over q (units 1/Bohr).&lt;/p&gt;</description>
  </descriptions>
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