{"paper":{"title":"Correlation energy of the spin-polarized uniform electron gas at high density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.other","physics.chem-ph","physics.comp-ph"],"primary_cat":"cond-mat.str-el","authors_text":"Peter M. W. Gill, Pierre-Fran\\c{c}ois Loos","submitted_at":"2011-04-04T08:49:36Z","abstract_excerpt":"The correlation energy per electron in the high-density uniform electron gas can be written as $\\Ec(r_s,\\zeta) = \\lam_0(\\zeta) \\ln r_s + \\eps_0(\\zeta) + \\lam_1(\\zeta) \\,r_s \\ln r_s + O(r_s)$, where $r_s$ is the Seitz radius and $\\zeta$ is the relative spin polarization. We derive an expression for $\\lam_1(\\zeta)$ which is exact for any $\\zeta$, including the paramagnetic and ferromagnetic limits, $\\lam_1(0)$ and $\\lam_1(1)$, and discover that the previously published $\\lam_1(1)$ value is incorrect. We trace this error to an integration and limit that do not commute. The spin-resolution of $\\la"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.0498","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}