{"paper":{"title":"Charmed Baryon Weak Decays with SU(3) Flavor Symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Chia-Wei Liu, C.Q. Geng, Tien-Hsueh Tsai, Y.K. Hsiao","submitted_at":"2017-09-04T04:58:46Z","abstract_excerpt":"We study the semileptonic and non-leptonic charmed baryon decays with $SU(3)$ flavor symmetry, where the charmed baryons can be ${\\bf B}_{c}=(\\Xi_c^0,\\Xi_c^+,\\Lambda_c^+)$, ${\\bf B}'_{c}=(\\Sigma_c^{(++,+,0)},\\Xi_{c}^{\\prime(+,0)},\\Omega_c^0)$, ${\\bf B}_{cc}=(\\Xi_{cc}^{++},\\Xi_{cc}^+,\\Omega_{cc}^+)$, or ${\\bf B}_{ccc}=\\Omega^{++}_{ccc}$. With ${\\bf B}_n^{(\\prime)}$ denoted as the baryon octet (decuplet), we find that the ${\\bf B}_{c}\\to {\\bf B}'_n\\ell^+\\nu_\\ell$ decays are forbidden, while the $\\Omega_c^0\\to \\Omega^-\\ell^+\\nu_\\ell$, $\\Omega_{cc}^+\\to\\Omega_c^0\\ell^+\\nu_\\ell$, and $\\Omega_{ccc}^"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.00808","kind":"arxiv","version":3},"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"}