{"paper":{"title":"Rovibrationally-Resolved Photodissociaton of SH$^+$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph"],"primary_cat":"astro-ph.EP","authors_text":"B. M. McLaughlin, E. C. McMillan, G. Shen, J. F. McCann, P. C. Stancil","submitted_at":"2016-02-17T14:30:06Z","abstract_excerpt":"Photodissociation cross sections for the SH$^+$ radical are computed from all rovibrational (RV) levels of the ground electronic state X$~^3\\Sigma^-$ for wavelengths from threshold to 500~\\AA. The five electronic transitions, $2~ ^3\\Sigma^- \\leftarrow$ X$~^3\\Sigma^-$, $3~ ^3\\Sigma^- \\leftarrow$ X$~^3\\Sigma^-$, $A~ ^3\\Pi \\leftarrow$ X$~^3\\Sigma^-$, $2~ ^3\\Pi \\leftarrow$ X$~^3\\Sigma^-$, and $3~ ^3\\Pi \\leftarrow$ X$~^3\\Sigma^-$, are treated with a fully quantum-mechanical two-state model, {i.e. no non-adiabatic coupling between excited states was included in our work.}. The photodissociation calc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.05430","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"}