{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:ZEWXZDZZSG62ASJP56KW6FVCCC","short_pith_number":"pith:ZEWXZDZZ","schema_version":"1.0","canonical_sha256":"c92d7c8f3991bda0492fef956f16a210a60583bf8251897390e50812bfba6197","source":{"kind":"arxiv","id":"nucl-th/0603061","version":1},"attestation_state":"computed","paper":{"title":"Semileptonic Decays of Heavy Omega Baryons in a Quark Model","license":"","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"nucl-th","authors_text":"Muslema Pervin, S. Capstick, W. Roberts","submitted_at":"2006-03-24T14:01:24Z","abstract_excerpt":"The semileptonic decays of $\\Omega_c$ and $\\Omega_b$ are treated in the framework of a constituent quark model developed in a previous paper on the semileptonic decays of heavy $\\Lambda$ baryons. Analytic results for the form factors for the decays to ground states and a number of excited states are evaluated. For $\\Omega_b$ to $\\Omega_c$ the form factors obtained are shown to satisfy the relations predicted at leading order in the heavy-quark effective theory at the non-recoil point. A modified fit of nonrelativistic and semirelativistic Hamiltonians generates configuration-mixed baryon wave "},"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":"nucl-th/0603061","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-03-24T14:01:24Z","cross_cats_sorted":["hep-ex","hep-ph"],"title_canon_sha256":"fa0e2d7c7495baf66edda59964f81134a63403d17fb69ab788106275d36722a5","abstract_canon_sha256":"2f464bcdd5ad5af4e8da51ac6765bba4214b340e59dc727e8a6ead505867ba0b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:31:50.212518Z","signature_b64":"NxRi6ZVN6LXOV0HY8CBvi7QvtakbtxwRIxeuSJUSFCI4+41gu0ISyGjfwgUcv2VCGqUspDFXJFgpbXFJeZjtDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c92d7c8f3991bda0492fef956f16a210a60583bf8251897390e50812bfba6197","last_reissued_at":"2026-07-04T15:31:50.212053Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:31:50.212053Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Semileptonic Decays of Heavy Omega Baryons in a Quark Model","license":"","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"nucl-th","authors_text":"Muslema Pervin, S. Capstick, W. Roberts","submitted_at":"2006-03-24T14:01:24Z","abstract_excerpt":"The semileptonic decays of $\\Omega_c$ and $\\Omega_b$ are treated in the framework of a constituent quark model developed in a previous paper on the semileptonic decays of heavy $\\Lambda$ baryons. Analytic results for the form factors for the decays to ground states and a number of excited states are evaluated. For $\\Omega_b$ to $\\Omega_c$ the form factors obtained are shown to satisfy the relations predicted at leading order in the heavy-quark effective theory at the non-recoil point. A modified fit of nonrelativistic and semirelativistic Hamiltonians generates configuration-mixed baryon wave "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0603061","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/nucl-th/0603061/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"nucl-th/0603061","created_at":"2026-07-04T15:31:50.212114+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0603061v1","created_at":"2026-07-04T15:31:50.212114+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0603061","created_at":"2026-07-04T15:31:50.212114+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZEWXZDZZSG62","created_at":"2026-07-04T15:31:50.212114+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZEWXZDZZSG62ASJP","created_at":"2026-07-04T15:31:50.212114+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZEWXZDZZ","created_at":"2026-07-04T15:31:50.212114+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.13648","citing_title":"Weak decays of singly heavy baryons: the $1/2\\to3/2$ case","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC","json":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC.json","graph_json":"https://pith.science/api/pith-number/ZEWXZDZZSG62ASJP56KW6FVCCC/graph.json","events_json":"https://pith.science/api/pith-number/ZEWXZDZZSG62ASJP56KW6FVCCC/events.json","paper":"https://pith.science/paper/ZEWXZDZZ"},"agent_actions":{"view_html":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC","download_json":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC.json","view_paper":"https://pith.science/paper/ZEWXZDZZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0603061&json=true","fetch_graph":"https://pith.science/api/pith-number/ZEWXZDZZSG62ASJP56KW6FVCCC/graph.json","fetch_events":"https://pith.science/api/pith-number/ZEWXZDZZSG62ASJP56KW6FVCCC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC/action/storage_attestation","attest_author":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC/action/author_attestation","sign_citation":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC/action/citation_signature","submit_replication":"https://pith.science/pith/ZEWXZDZZSG62ASJP56KW6FVCCC/action/replication_record"}},"created_at":"2026-07-04T15:31:50.212114+00:00","updated_at":"2026-07-04T15:31:50.212114+00:00"}