{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:GFRPTVVHY5HEY3XBSZKJ67RD6B","short_pith_number":"pith:GFRPTVVH","schema_version":"1.0","canonical_sha256":"3162f9d6a7c74e4c6ee196549f7e23f061104f11adffdf5b301f092e7facd507","source":{"kind":"arxiv","id":"1701.06914","version":3},"attestation_state":"computed","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"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1701.06914","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-01-24T15:16:39Z","cross_cats_sorted":[],"title_canon_sha256":"8495fdfdfd029cb772da3cbcc7e661de124423d1f4efe3ca2e4df0eb6bd58992","abstract_canon_sha256":"ae6a27e5b84fa67558ea71c3571e0f02cab37117d5a42e4656ea253cafb07657"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:07.660505Z","signature_b64":"aOb2RJAp2Fpy1Fc0SHhdBNGwaF6Jyc82VY+TOvcTG545vF0BFoZovn9Ak9oiVY5UG4vueDxalSL3ZScSIw2vDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3162f9d6a7c74e4c6ee196549f7e23f061104f11adffdf5b301f092e7facd507","last_reissued_at":"2026-05-18T00:46:07.660019Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:07.660019Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1701.06914","created_at":"2026-05-18T00:46:07.660082+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.06914v3","created_at":"2026-05-18T00:46:07.660082+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.06914","created_at":"2026-05-18T00:46:07.660082+00:00"},{"alias_kind":"pith_short_12","alias_value":"GFRPTVVHY5HE","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_16","alias_value":"GFRPTVVHY5HEY3XB","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_8","alias_value":"GFRPTVVH","created_at":"2026-05-18T12:31:15.632608+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2602.12594","citing_title":"Probing the isospin structure and low-lying resonances in $\\Lambda_c^+ \\to n\\bar{K}^0 \\pi^+$ decays","ref_index":58,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B","json":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B.json","graph_json":"https://pith.science/api/pith-number/GFRPTVVHY5HEY3XBSZKJ67RD6B/graph.json","events_json":"https://pith.science/api/pith-number/GFRPTVVHY5HEY3XBSZKJ67RD6B/events.json","paper":"https://pith.science/paper/GFRPTVVH"},"agent_actions":{"view_html":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B","download_json":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B.json","view_paper":"https://pith.science/paper/GFRPTVVH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.06914&json=true","fetch_graph":"https://pith.science/api/pith-number/GFRPTVVHY5HEY3XBSZKJ67RD6B/graph.json","fetch_events":"https://pith.science/api/pith-number/GFRPTVVHY5HEY3XBSZKJ67RD6B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B/action/storage_attestation","attest_author":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B/action/author_attestation","sign_citation":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B/action/citation_signature","submit_replication":"https://pith.science/pith/GFRPTVVHY5HEY3XBSZKJ67RD6B/action/replication_record"}},"created_at":"2026-05-18T00:46:07.660082+00:00","updated_at":"2026-05-18T00:46:07.660082+00:00"}