{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:A6ZXRIHE6WKDC3FLXCFRLEP7HI","short_pith_number":"pith:A6ZXRIHE","schema_version":"1.0","canonical_sha256":"07b378a0e4f594316cabb88b1591ff3a339ce292ddf0f7257c06f292081949c1","source":{"kind":"arxiv","id":"1806.08853","version":1},"attestation_state":"computed","paper":{"title":"Measurements of $\\Omega^-$ Branching Fractions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"A. Tomaradze, Kamal K. Seth, S. Dobbs, T. Xiao","submitted_at":"2018-06-22T21:01:14Z","abstract_excerpt":"Using $e^+e^-$ annihilation data taken at the CESR collider with the CLEO-c detector, measurements of two main $\\Omega^-$ branching fractions have been made using the reaction $\\psi(2S)\\to\\Omega^-\\overline{\\Omega}^+$, hyperon pair production at $\\sqrt{s}=3.69$~GeV, the peak of the $\\psi(2S)$ resonance. $\\Omega^-$ decay channels are identified through momentum distributions of charged particles, and systematics of the $\\Omega^-$ branching fractions have been studied. The result gives: $\\mathcal{B}(\\Omega^- \\to \\Lambda^0 K^-) = (68.9\\pm9.5\\pm4.3)\\%$, and $ \\mathcal{B}(\\Omega^- \\to \\Xi^0 \\pi^-) ="},"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":"1806.08853","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2018-06-22T21:01:14Z","cross_cats_sorted":[],"title_canon_sha256":"c0049159ce285a6a27d1ee78b4a63b9e3a73d989c84b9c28efc3d948be3ece39","abstract_canon_sha256":"07093b782aab9542cee6ca9bb768f87e9c81bcb78d8a926bd007150091261625"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:08:40.638806Z","signature_b64":"xvOewLYK4pRJOoQNsCOa7exq+brvKvXU/7ye8OCyZVkNV1nK+Dzn7sHsAXrN/xLgoiPvnvkBoA8ad9eMbVZnBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07b378a0e4f594316cabb88b1591ff3a339ce292ddf0f7257c06f292081949c1","last_reissued_at":"2026-05-18T00:08:40.638164Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:08:40.638164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurements of $\\Omega^-$ Branching Fractions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"A. Tomaradze, Kamal K. Seth, S. Dobbs, T. Xiao","submitted_at":"2018-06-22T21:01:14Z","abstract_excerpt":"Using $e^+e^-$ annihilation data taken at the CESR collider with the CLEO-c detector, measurements of two main $\\Omega^-$ branching fractions have been made using the reaction $\\psi(2S)\\to\\Omega^-\\overline{\\Omega}^+$, hyperon pair production at $\\sqrt{s}=3.69$~GeV, the peak of the $\\psi(2S)$ resonance. $\\Omega^-$ decay channels are identified through momentum distributions of charged particles, and systematics of the $\\Omega^-$ branching fractions have been studied. The result gives: $\\mathcal{B}(\\Omega^- \\to \\Lambda^0 K^-) = (68.9\\pm9.5\\pm4.3)\\%$, and $ \\mathcal{B}(\\Omega^- \\to \\Xi^0 \\pi^-) ="},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.08853","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":""},"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":"1806.08853","created_at":"2026-05-18T00:08:40.638265+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.08853v1","created_at":"2026-05-18T00:08:40.638265+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.08853","created_at":"2026-05-18T00:08:40.638265+00:00"},{"alias_kind":"pith_short_12","alias_value":"A6ZXRIHE6WKD","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_16","alias_value":"A6ZXRIHE6WKDC3FL","created_at":"2026-05-18T12:32:13.499390+00:00"},{"alias_kind":"pith_short_8","alias_value":"A6ZXRIHE","created_at":"2026-05-18T12:32:13.499390+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI","json":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI.json","graph_json":"https://pith.science/api/pith-number/A6ZXRIHE6WKDC3FLXCFRLEP7HI/graph.json","events_json":"https://pith.science/api/pith-number/A6ZXRIHE6WKDC3FLXCFRLEP7HI/events.json","paper":"https://pith.science/paper/A6ZXRIHE"},"agent_actions":{"view_html":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI","download_json":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI.json","view_paper":"https://pith.science/paper/A6ZXRIHE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.08853&json=true","fetch_graph":"https://pith.science/api/pith-number/A6ZXRIHE6WKDC3FLXCFRLEP7HI/graph.json","fetch_events":"https://pith.science/api/pith-number/A6ZXRIHE6WKDC3FLXCFRLEP7HI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI/action/storage_attestation","attest_author":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI/action/author_attestation","sign_citation":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI/action/citation_signature","submit_replication":"https://pith.science/pith/A6ZXRIHE6WKDC3FLXCFRLEP7HI/action/replication_record"}},"created_at":"2026-05-18T00:08:40.638265+00:00","updated_at":"2026-05-18T00:08:40.638265+00:00"}