{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:NJFQRHYS4RYNA7AIRZ4Z25YVKF","short_pith_number":"pith:NJFQRHYS","schema_version":"1.0","canonical_sha256":"6a4b089f12e470d07c088e799d771551597268a3ce1184e78012fe27b2c66ca4","source":{"kind":"arxiv","id":"hep-ex/0408078","version":1},"attestation_state":"computed","paper":{"title":"Study of e+e- --> pi+ pi- pi0 process using initial state radiation with BABAR","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"B. Aubert, et al, The BABAR Collaboration","submitted_at":"2004-08-16T20:31:00Z","abstract_excerpt":"The process e+e- --> pi+ pi- pi0 gamma has been studied at a center-of-mass energy near the Y(4S) resonance using a 89.3 fb-1 data sample collected with the BaBar detector at the PEP-II collider. From the measured 3pi mass spectrum we have obtained the products of branching fractions for the omega and phi mesons, B(omega --> e+e-)B(omega --> 3pi)=(6.70 +/- 0.06 +/- 0.27)10-5 and B(phi --> e+e-)B(phi --> 3pi)=(4.30 +/- 0.08 +/- 0.21)10-5, and evaluated the e+e- --> pi+ pi- pi0 cross section for the e+e- center-of-mass energy range 1.05 to 3.00 GeV. About 900 e+e- --> J/psi gamma --> pi+ pi- pi0"},"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":"hep-ex/0408078","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2004-08-16T20:31:00Z","cross_cats_sorted":[],"title_canon_sha256":"f4f6c6c22df3aa6cff8f38df6d0bb664b055d9ff06a99dc97a0b3c44205a47b8","abstract_canon_sha256":"de8a4f2d58fe181c57539ddea8902096d5efcfa1ce663285e2e9b723c000921a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:31:29.730884Z","signature_b64":"t84LoHjrszTYAUNglX/c8hUHlAtEeI5tP+ObOD++LPDJqpsfkiiOAp/9Pn5OmZBWL843/5h6ARzl+wCtt2H4Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a4b089f12e470d07c088e799d771551597268a3ce1184e78012fe27b2c66ca4","last_reissued_at":"2026-07-04T15:31:29.730477Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:31:29.730477Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Study of e+e- --> pi+ pi- pi0 process using initial state radiation with BABAR","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"B. Aubert, et al, The BABAR Collaboration","submitted_at":"2004-08-16T20:31:00Z","abstract_excerpt":"The process e+e- --> pi+ pi- pi0 gamma has been studied at a center-of-mass energy near the Y(4S) resonance using a 89.3 fb-1 data sample collected with the BaBar detector at the PEP-II collider. From the measured 3pi mass spectrum we have obtained the products of branching fractions for the omega and phi mesons, B(omega --> e+e-)B(omega --> 3pi)=(6.70 +/- 0.06 +/- 0.27)10-5 and B(phi --> e+e-)B(phi --> 3pi)=(4.30 +/- 0.08 +/- 0.21)10-5, and evaluated the e+e- --> pi+ pi- pi0 cross section for the e+e- center-of-mass energy range 1.05 to 3.00 GeV. About 900 e+e- --> J/psi gamma --> pi+ pi- pi0"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0408078","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/hep-ex/0408078/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":"hep-ex/0408078","created_at":"2026-07-04T15:31:29.730540+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0408078v1","created_at":"2026-07-04T15:31:29.730540+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0408078","created_at":"2026-07-04T15:31:29.730540+00:00"},{"alias_kind":"pith_short_12","alias_value":"NJFQRHYS4RYN","created_at":"2026-07-04T15:31:29.730540+00:00"},{"alias_kind":"pith_short_16","alias_value":"NJFQRHYS4RYNA7AI","created_at":"2026-07-04T15:31:29.730540+00:00"},{"alias_kind":"pith_short_8","alias_value":"NJFQRHYS","created_at":"2026-07-04T15:31:29.730540+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2006.04822","citing_title":"The anomalous magnetic moment of the muon in the Standard Model","ref_index":44,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF","json":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF.json","graph_json":"https://pith.science/api/pith-number/NJFQRHYS4RYNA7AIRZ4Z25YVKF/graph.json","events_json":"https://pith.science/api/pith-number/NJFQRHYS4RYNA7AIRZ4Z25YVKF/events.json","paper":"https://pith.science/paper/NJFQRHYS"},"agent_actions":{"view_html":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF","download_json":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF.json","view_paper":"https://pith.science/paper/NJFQRHYS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0408078&json=true","fetch_graph":"https://pith.science/api/pith-number/NJFQRHYS4RYNA7AIRZ4Z25YVKF/graph.json","fetch_events":"https://pith.science/api/pith-number/NJFQRHYS4RYNA7AIRZ4Z25YVKF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF/action/storage_attestation","attest_author":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF/action/author_attestation","sign_citation":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF/action/citation_signature","submit_replication":"https://pith.science/pith/NJFQRHYS4RYNA7AIRZ4Z25YVKF/action/replication_record"}},"created_at":"2026-07-04T15:31:29.730540+00:00","updated_at":"2026-07-04T15:31:29.730540+00:00"}