{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:RR7ER2C63DUFAQVXQMIAKVNA3Y","short_pith_number":"pith:RR7ER2C6","schema_version":"1.0","canonical_sha256":"8c7e48e85ed8e85042b783100555a0de3d751a4e05a1d1e812a87a07af9e827c","source":{"kind":"arxiv","id":"hep-ex/0103021","version":3},"attestation_state":"computed","paper":{"title":"First Observation of B -> D(*) rho', rho' -> omega pi-","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CLEO Collaboration, et al, J. Alexander","submitted_at":"2001-03-15T17:00:29Z","abstract_excerpt":"We report on the observation of B-> D(*) pi+ pi- pi- pi^o decays. The branching ratios for D*+ and D*o are (1.72+/-0.14+/-0.24)% and (1.80+/-0.24+/-0.27)%, respectively. Each final state has a D* omega pi- component, with branching ratios (0.29+/-0.03+/-0.04)% and (0.45+/-0.10+/-0.07)% for the D*+ and D*o modes, respectively. We also observe B -> D omega pi- decays. The branching ratios for D+ and Do are (0.28+/-0.05+/-0.04)% and (0.41+/-0.07+/-0.06)%, respectively. A spin parity analysis of the D omega pi- final state prefers a wide 1^- resonance. A fit to the omega pi- mass spectrum finds a "},"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/0103021","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2001-03-15T17:00:29Z","cross_cats_sorted":[],"title_canon_sha256":"0359c78ff631c70984a7de91fc3d2387671758ea7c1c68b73705f947e811c5ab","abstract_canon_sha256":"7267c04e2e446be918e54993f1bb926e077470213c87c0d88958781ad924798b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:29:39.284152Z","signature_b64":"vlLuRsN3vEvVHurGdGCM4tw/mWgHvUWTX9wU4zOR+nzUG1T7cVxdNZ0DTrXIISnIq7rcQhCvVlzzHvXSxHRABQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c7e48e85ed8e85042b783100555a0de3d751a4e05a1d1e812a87a07af9e827c","last_reissued_at":"2026-07-04T17:29:39.283731Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:29:39.283731Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"First Observation of B -> D(*) rho', rho' -> omega pi-","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CLEO Collaboration, et al, J. Alexander","submitted_at":"2001-03-15T17:00:29Z","abstract_excerpt":"We report on the observation of B-> D(*) pi+ pi- pi- pi^o decays. The branching ratios for D*+ and D*o are (1.72+/-0.14+/-0.24)% and (1.80+/-0.24+/-0.27)%, respectively. Each final state has a D* omega pi- component, with branching ratios (0.29+/-0.03+/-0.04)% and (0.45+/-0.10+/-0.07)% for the D*+ and D*o modes, respectively. We also observe B -> D omega pi- decays. The branching ratios for D+ and Do are (0.28+/-0.05+/-0.04)% and (0.41+/-0.07+/-0.06)%, respectively. A spin parity analysis of the D omega pi- final state prefers a wide 1^- resonance. A fit to the omega pi- mass spectrum finds a "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0103021","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ex/0103021/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/0103021","created_at":"2026-07-04T17:29:39.283798+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0103021v3","created_at":"2026-07-04T17:29:39.283798+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0103021","created_at":"2026-07-04T17:29:39.283798+00:00"},{"alias_kind":"pith_short_12","alias_value":"RR7ER2C63DUF","created_at":"2026-07-04T17:29:39.283798+00:00"},{"alias_kind":"pith_short_16","alias_value":"RR7ER2C63DUFAQVX","created_at":"2026-07-04T17:29:39.283798+00:00"},{"alias_kind":"pith_short_8","alias_value":"RR7ER2C6","created_at":"2026-07-04T17:29:39.283798+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/RR7ER2C63DUFAQVXQMIAKVNA3Y","json":"https://pith.science/pith/RR7ER2C63DUFAQVXQMIAKVNA3Y.json","graph_json":"https://pith.science/api/pith-number/RR7ER2C63DUFAQVXQMIAKVNA3Y/graph.json","events_json":"https://pith.science/api/pith-number/RR7ER2C63DUFAQVXQMIAKVNA3Y/events.json","paper":"https://pith.science/paper/RR7ER2C6"},"agent_actions":{"view_html":"https://pith.science/pith/RR7ER2C63DUFAQVXQMIAKVNA3Y","download_json":"https://pith.science/pith/RR7ER2C63DUFAQVXQMIAKVNA3Y.json","view_paper":"https://pith.science/paper/RR7ER2C6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0103021&json=true","fetch_graph":"https://pith.science/api/pith-number/RR7ER2C63DUFAQVXQMIAKVNA3Y/graph.json","fetch_events":"https://pith.science/api/pith-number/RR7ER2C63DUFAQVXQMIAKVNA3Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RR7ER2C63DUFAQVXQMIAKVNA3Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RR7ER2C63DUFAQVXQMIAKVNA3Y/action/storage_attestation","attest_author":"https://pith.science/pith/RR7ER2C63DUFAQVXQMIAKVNA3Y/action/author_attestation","sign_citation":"https://pith.science/pith/RR7ER2C63DUFAQVXQMIAKVNA3Y/action/citation_signature","submit_replication":"https://pith.science/pith/RR7ER2C63DUFAQVXQMIAKVNA3Y/action/replication_record"}},"created_at":"2026-07-04T17:29:39.283798+00:00","updated_at":"2026-07-04T17:29:39.283798+00:00"}