{"paper":{"title":"Corresponding States of Structural Glass Formers. II","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.soft"],"primary_cat":"cond-mat.stat-mech","authors_text":"David Chandler, Juan P. Garrahan, Yael S. Elmatad","submitted_at":"2010-08-12T22:17:16Z","abstract_excerpt":"The earlier paper of this same title demonstrated a collapse of relaxation data of fragile supercooled glass forming liquids [\\textit{J. Phys. Chem. B} \\textbf{113}, 5563-5567 (2009)]. For temperature $T$ below that of the onset to supercooled behavior, $T_{\\mathrm{o}}$, the logarithm of structural relaxation time, $\\log \\tau$, is given by the parabolic form $\\log (\\tau/\\tau_{\\mathrm{o}}) \\, =\\, J^2(1/T - 1/T_{\\mathrm{o}})^{2}$, where $J$ and $\\tau_{\\mathrm{o}}$ are temperature independent. This paper presents further applications of this formula. In particular, it is shown that the effects of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.2225","kind":"arxiv","version":1},"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"}