{"paper":{"title":"Geometric Phase Effects in the Ultracold D + HD $\\to$ D + HD and D + HD $\\leftrightarrow$ H + D$_2$ Reactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.chem-ph","authors_text":"Brian K. Kendrick, Jisha Hazra, N. Balakrishnan","submitted_at":"2016-07-19T21:17:29Z","abstract_excerpt":"The results of accurate quantum reactive scattering calculations for the D + HD($v=4$, $j=0$) $\\to$ D + HD($v'$, $j'$), D + HD($v=4$, $j=0$) $\\to$ H + D$_2$($v'$, $j'$) and H + D$_2$($v=4$, $j=0$) $\\to$ D + HD($v'$,$j'$) reactions are presented for collision energies between $1\\,\\mu{\\rm K}$ and $100\\,{\\rm K}$. The ${\\it ab\\ initio}$ BKMP2 PES for the ground electronic state of H$_3$ is used and all values of total angular momentum between $J=0-4$ are included. The general vector potential approach is used to include the geometric phase. The rotationally resolved, vibrationally resolved, and to"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.05763","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"}