{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:IYZRINC6X4YHL6JRNBUOG42OYL","short_pith_number":"pith:IYZRINC6","schema_version":"1.0","canonical_sha256":"463314345ebf3075f9316868e3734ec2e36066f90f988b253eee9731bc0b75d5","source":{"kind":"arxiv","id":"1907.09149","version":2},"attestation_state":"computed","paper":{"title":"Determination of the absolute branching fractions of X(3872) decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"Chang-Zheng Yuan, Chunhua Li","submitted_at":"2019-07-22T06:26:22Z","abstract_excerpt":"We report the first determination of the absolute branching fractions of the X(3872) decays by globally analyzing the measurements provided by the Belle, BaBar, BESIII, and LHCb experiments. The branching fractions of X(3872) to pi^+pi^- J/psi and D*0D0bar+c.c. are found to be (4.1^{+1.9}_{-1.1})% and (52.4^{+25.3}_{-14.3})%, respectively. The branching fractions of the decays X(3872) to gamma J/psi, gamma psi', omega J/psi, and pi^0 chi_{c1} are also determined. The global fit implies that the fraction of X(3872) decays which are not observed in experiments is (31.9_{-31.5}^{+18.1})%, which i"},"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":"1907.09149","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2019-07-22T06:26:22Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"471a6e2a39952e5b5bc95d95d055251055ce2867d2a011b0b412620a1d10b831","abstract_canon_sha256":"8b2faf1460cf65ca4dced484b47ccdf3764c5a24331ab35933b1c79dfe9e49b6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:18:38.456512Z","signature_b64":"UopIiYVwRwjqVYZaRF4SAsETalaUqoOzQYtCyC2El2lzKUryYjNmJwaadSf0uJwAbipvDlkaL2MKPp9e/WMjCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"463314345ebf3075f9316868e3734ec2e36066f90f988b253eee9731bc0b75d5","last_reissued_at":"2026-07-05T00:18:38.456069Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:18:38.456069Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Determination of the absolute branching fractions of X(3872) decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"Chang-Zheng Yuan, Chunhua Li","submitted_at":"2019-07-22T06:26:22Z","abstract_excerpt":"We report the first determination of the absolute branching fractions of the X(3872) decays by globally analyzing the measurements provided by the Belle, BaBar, BESIII, and LHCb experiments. The branching fractions of X(3872) to pi^+pi^- J/psi and D*0D0bar+c.c. are found to be (4.1^{+1.9}_{-1.1})% and (52.4^{+25.3}_{-14.3})%, respectively. The branching fractions of the decays X(3872) to gamma J/psi, gamma psi', omega J/psi, and pi^0 chi_{c1} are also determined. The global fit implies that the fraction of X(3872) decays which are not observed in experiments is (31.9_{-31.5}^{+18.1})%, which i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.09149","kind":"arxiv","version":2},"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/1907.09149/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":"1907.09149","created_at":"2026-07-05T00:18:38.456127+00:00"},{"alias_kind":"arxiv_version","alias_value":"1907.09149v2","created_at":"2026-07-05T00:18:38.456127+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.09149","created_at":"2026-07-05T00:18:38.456127+00:00"},{"alias_kind":"pith_short_12","alias_value":"IYZRINC6X4YH","created_at":"2026-07-05T00:18:38.456127+00:00"},{"alias_kind":"pith_short_16","alias_value":"IYZRINC6X4YHL6JR","created_at":"2026-07-05T00:18:38.456127+00:00"},{"alias_kind":"pith_short_8","alias_value":"IYZRINC6","created_at":"2026-07-05T00:18:38.456127+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/IYZRINC6X4YHL6JRNBUOG42OYL","json":"https://pith.science/pith/IYZRINC6X4YHL6JRNBUOG42OYL.json","graph_json":"https://pith.science/api/pith-number/IYZRINC6X4YHL6JRNBUOG42OYL/graph.json","events_json":"https://pith.science/api/pith-number/IYZRINC6X4YHL6JRNBUOG42OYL/events.json","paper":"https://pith.science/paper/IYZRINC6"},"agent_actions":{"view_html":"https://pith.science/pith/IYZRINC6X4YHL6JRNBUOG42OYL","download_json":"https://pith.science/pith/IYZRINC6X4YHL6JRNBUOG42OYL.json","view_paper":"https://pith.science/paper/IYZRINC6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1907.09149&json=true","fetch_graph":"https://pith.science/api/pith-number/IYZRINC6X4YHL6JRNBUOG42OYL/graph.json","fetch_events":"https://pith.science/api/pith-number/IYZRINC6X4YHL6JRNBUOG42OYL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IYZRINC6X4YHL6JRNBUOG42OYL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IYZRINC6X4YHL6JRNBUOG42OYL/action/storage_attestation","attest_author":"https://pith.science/pith/IYZRINC6X4YHL6JRNBUOG42OYL/action/author_attestation","sign_citation":"https://pith.science/pith/IYZRINC6X4YHL6JRNBUOG42OYL/action/citation_signature","submit_replication":"https://pith.science/pith/IYZRINC6X4YHL6JRNBUOG42OYL/action/replication_record"}},"created_at":"2026-07-05T00:18:38.456127+00:00","updated_at":"2026-07-05T00:18:38.456127+00:00"}