{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:C7J7GPU3AUOGKK4DWIMQ62U7NW","short_pith_number":"pith:C7J7GPU3","schema_version":"1.0","canonical_sha256":"17d3f33e9b051c652b83b2190f6a9f6da64e9c48a9a28e474c389272dc7cd197","source":{"kind":"arxiv","id":"1105.5159","version":1},"attestation_state":"computed","paper":{"title":"Measurements of branching fractions and CP asymmetries and studies of angular distributions for B to phi phi K decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, J. P. Lees, The BABAR Collaboration","submitted_at":"2011-05-25T22:08:34Z","abstract_excerpt":"We present branching fraction and CP asymmetry measurements as well as angular studies of B to phi phi K decays using 464 x 10^6 BBbar events collected by the BaBar experiment. The branching fractions are measured in the phi phi invariant mass range below the eta_c resonance (m_phiphi <2.85 GeV). We find\n  B(B+ to phi phi K+) = (5.6 +/- 0.5 +/- 0.3) x 10^-6 and\n  B(B0 to phi phi K0) = (4.5 +/- 0.8 +/- 0.3) x 10^-6, where the first uncertaintiy is statistical and the second systematic. The measured direct CP asymmetries for the B+- decays are\n  A_CP = -0.10 +/- 0.08 +/- 0.02 below the eta_c thr"},"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":"1105.5159","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-05-25T22:08:34Z","cross_cats_sorted":[],"title_canon_sha256":"ec7c9b3548b85e868bd69a7e217b6822ab307fe9fd4e199a5751a48a3fd1ff28","abstract_canon_sha256":"087c0c3cf9ca32e0b9b1a79446567018260db9b7de0d5ea7b204b230cb1ad5df"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:16:22.345707Z","signature_b64":"jK/DNRbaBKbQZdBCBt5EQ+TdHyQQiW1Q+K3vdjyj1xBvW8074ZG3gCJnSwQdYuOYbKI6+3v232RS0hotJB16DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"17d3f33e9b051c652b83b2190f6a9f6da64e9c48a9a28e474c389272dc7cd197","last_reissued_at":"2026-05-18T04:16:22.345020Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:16:22.345020Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurements of branching fractions and CP asymmetries and studies of angular distributions for B to phi phi K decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"et al, J. P. Lees, The BABAR Collaboration","submitted_at":"2011-05-25T22:08:34Z","abstract_excerpt":"We present branching fraction and CP asymmetry measurements as well as angular studies of B to phi phi K decays using 464 x 10^6 BBbar events collected by the BaBar experiment. The branching fractions are measured in the phi phi invariant mass range below the eta_c resonance (m_phiphi <2.85 GeV). We find\n  B(B+ to phi phi K+) = (5.6 +/- 0.5 +/- 0.3) x 10^-6 and\n  B(B0 to phi phi K0) = (4.5 +/- 0.8 +/- 0.3) x 10^-6, where the first uncertaintiy is statistical and the second systematic. The measured direct CP asymmetries for the B+- decays are\n  A_CP = -0.10 +/- 0.08 +/- 0.02 below the eta_c thr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.5159","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":"1105.5159","created_at":"2026-05-18T04:16:22.345125+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.5159v1","created_at":"2026-05-18T04:16:22.345125+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.5159","created_at":"2026-05-18T04:16:22.345125+00:00"},{"alias_kind":"pith_short_12","alias_value":"C7J7GPU3AUOG","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_16","alias_value":"C7J7GPU3AUOGKK4D","created_at":"2026-05-18T12:26:24.575870+00:00"},{"alias_kind":"pith_short_8","alias_value":"C7J7GPU3","created_at":"2026-05-18T12:26:24.575870+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/C7J7GPU3AUOGKK4DWIMQ62U7NW","json":"https://pith.science/pith/C7J7GPU3AUOGKK4DWIMQ62U7NW.json","graph_json":"https://pith.science/api/pith-number/C7J7GPU3AUOGKK4DWIMQ62U7NW/graph.json","events_json":"https://pith.science/api/pith-number/C7J7GPU3AUOGKK4DWIMQ62U7NW/events.json","paper":"https://pith.science/paper/C7J7GPU3"},"agent_actions":{"view_html":"https://pith.science/pith/C7J7GPU3AUOGKK4DWIMQ62U7NW","download_json":"https://pith.science/pith/C7J7GPU3AUOGKK4DWIMQ62U7NW.json","view_paper":"https://pith.science/paper/C7J7GPU3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.5159&json=true","fetch_graph":"https://pith.science/api/pith-number/C7J7GPU3AUOGKK4DWIMQ62U7NW/graph.json","fetch_events":"https://pith.science/api/pith-number/C7J7GPU3AUOGKK4DWIMQ62U7NW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C7J7GPU3AUOGKK4DWIMQ62U7NW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C7J7GPU3AUOGKK4DWIMQ62U7NW/action/storage_attestation","attest_author":"https://pith.science/pith/C7J7GPU3AUOGKK4DWIMQ62U7NW/action/author_attestation","sign_citation":"https://pith.science/pith/C7J7GPU3AUOGKK4DWIMQ62U7NW/action/citation_signature","submit_replication":"https://pith.science/pith/C7J7GPU3AUOGKK4DWIMQ62U7NW/action/replication_record"}},"created_at":"2026-05-18T04:16:22.345125+00:00","updated_at":"2026-05-18T04:16:22.345125+00:00"}