{"paper":{"title":"Predictions for $\\Xi_b^- \\rightarrow \\pi^- \\left(D_s^- \\right) \\ \\Xi_c^0 (2790) \\left(\\Xi_c^0 (2815) \\right)$ and $\\Xi_b^- \\rightarrow \\bar{\\nu}_l l \\ \\Xi_c^0 (2790) \\left(\\Xi_c^0 (2815) \\right)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"E. Oset, J. Nieves, R. P. Pavao, W. H. Liang","submitted_at":"2017-01-24T15:16:39Z","abstract_excerpt":"We have performed the calculations for the nonleptonic $\\Xi_b^- \\rightarrow \\pi^- \\ \\Xi_c^0 (2790) \\left(J=\\frac{1}{2}\\right)$ and $\\Xi_b^- \\rightarrow \\pi^- \\ \\Xi_c^0 (2815) \\left(J=\\frac{3}{2}\\right)$ and the same reactions replacing the $\\pi^-$ by a $D_s^-$. At the same time we evaluate the semileptonic rates for $\\Xi_b^- \\rightarrow \\bar{\\nu}_l l \\ \\Xi_c^0 (2790)$ and $\\Xi_b^- \\rightarrow \\bar{\\nu}_l l \\ \\Xi_c^0 (2815)$. We look at the reactions from the perspective that the $\\Xi_c^0 (2790)$ and $\\Xi_c^0 (2815)$ resonances are dynamically generated from the pseudoscalar-baryon and vector-b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.06914","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"}