{"paper":{"title":"Prediction of entropy stabilized incommensurate phases in the system MoS$_{2}$-MoTe$_{2}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Arunima K. Singh, Benjamin P. Burton","submitted_at":"2015-08-06T14:46:48Z","abstract_excerpt":"A first principles phase diagram calculation, that included van der Waals interactions, was performed for the system (1-X)$\\cdot$MoS$_{2}$-(X)$\\cdot$MoTe$_{2}$. Surprisingly, the predicted phase diagram has at least two ordered solid-solution phases, at $X \\approx 0.46$, even though all calculated formation energies are positive, in a ground-state analysis that examined all configurations with 16 or fewer anion sites. The lower-temperature {\\bf $I$}-phase is predicted to transform to a higher-temperature {\\bf $I^{\\prime}$}-phase at $T \\approx 500K$, and {\\bf $I^{\\prime}$} disorders at $T \\appr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.01423","kind":"arxiv","version":2},"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"}