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        <identifier>oai:materialscloud.org:qg2q2-hk221</identifier>
        <datestamp>2026-08-20T09:34:54Z</datestamp>
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          <dc:contributor>Vasilchenko, Vasilii</dc:contributor>
          <dc:creator>Vasilchenko, Vasilii</dc:creator>
          <dc:creator>Giantomassi, Matteo</dc:creator>
          <dc:creator>Poncé, Samuel</dc:creator>
          <dc:creator>Gonze, Xavier</dc:creator>
          <dc:date>2026-08-20</dc:date>
          <dc:description>&amp;lt;p&amp;gt;Polaron formation localizes charge carriers and drives a crossover from band-like to hopping transport in materials. Hopping dynamics can be obtained from DFT supercell calculations of transition states, but these suffer from polaron self-interaction, spurious electrostatics, and poor scaling with polaron size. We introduce a supercell-free framework for &amp;lt;em&amp;gt;ab initio&amp;lt;/em&amp;gt; polaron hopping transport based on variational polaron equations and the string method.&amp;nbsp;The approach optimizes transition states between self-trapped polaron states directly in reciprocal space and provides the polaron configurations along the path, enabling evaluation of adiabatic hopping rates and mobilities.&amp;nbsp;We apply the method to LiF and rutile TiO&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, revealing multi-step and anisotropic hopping mechanisms. In rutile TiO&amp;lt;sub&amp;gt;2&amp;lt;/sub&amp;gt;, the computed electron-polaron mobility agrees with experiment, whereas band-like Boltzmann transport substantially overestimates the mobility.&amp;nbsp;Our results establish a scalable route to first-principles polaron-hopping dynamics in materials in which charge motion is governed by self-trapping.&amp;lt;br&amp;gt;&amp;lt;br&amp;gt;This archive contains the data necessary to reproduce the results of the "&amp;lt;em&amp;gt;Optimal transition states for polaron hopping transport without supercells&amp;lt;/em&amp;gt;" article by Vasilii Vasilchenko, Matteo Giantomassi, Samuel Ponc&amp;eacute;, and Xavier Gonze.&amp;lt;/p&amp;gt;</dc:description>
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          <dc:identifier>https://doi.org/10.24435/materialscloud:q2-1c</dc:identifier>
          <dc:identifier>oai:materialscloud.org:qg2q2-hk221</dc:identifier>
          <dc:identifier>mcid:2026.164</dc:identifier>
          <dc:language>eng</dc:language>
          <dc:publisher>Materials Cloud</dc:publisher>
          <dc:relation>https://doi.org/10.48550/arXiv.2607.18096</dc:relation>
          <dc:relation>https://archive.materialscloud.org/communities/mcarchive</dc:relation>
          <dc:relation>https://doi.org/10.24435/materialscloud:4h-kn</dc:relation>
          <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
          <dc:rights>Creative Commons Attribution 4.0 International</dc:rights>
          <dc:rights>https://creativecommons.org/licenses/by/4.0/legalcode</dc:rights>
          <dc:subject>Polarons</dc:subject>
          <dc:subject>First-principles calculations</dc:subject>
          <dc:subject>electron-phonon coupling</dc:subject>
          <dc:subject>Minimum-energy paths</dc:subject>
          <dc:subject>Hopping transport</dc:subject>
          <dc:title>Optimal transition states for polaron hopping transport without supercells</dc:title>
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