{"paper":{"title":"Decays of the Meson $B_c$ to a $P$-Wave Charmonium State $\\chi_c$ or $h_c$","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chao-Hsi Chang, Guo-Li Wang, Hong-shi Zong, YU-Qi Chen","submitted_at":"2001-03-03T10:45:01Z","abstract_excerpt":"The semileptonic decays, $B_{c}{\\longrightarrow}{\\chi_c}(h_c)+{\\ell}+{{\\nu}}_{\\ell}$, and the two-body nonleptonic decays, $B_{c}{\\longrightarrow}{\\chi_c}(h_c)+h$, (here $\\chi_c$ and $h_c$ denote $(c\\bar c[^3P_J])$ and $(c\\bar c[^1P_1])$ respectively, and $h$ indicates a meson) were computed. All of the form factors appearing in the relevant weak-current matrix elements with $B_c$ as its initial state and a $P$-wave charmonium state as its final state for the decays were precisely formulated in terms of two independent overlapping-integrations of the wave-functions of $B_c$ and the $P$-wave ch"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0103036","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"}