{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:YKOO7BOBJ3HBT3NOPG5WFP7KNG","short_pith_number":"pith:YKOO7BOB","schema_version":"1.0","canonical_sha256":"c29cef85c14ece19edae79bb62bfea69bd8edfea20188b2520d184868ab26f49","source":{"kind":"arxiv","id":"1011.0960","version":2},"attestation_state":"computed","paper":{"title":"S-, P- and D-wave final state interactions and CP violation in B+- --> pi+- pi-+ pi+- decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A. Furman, B. Loiseau, J.-P. Dedonder, L. Lesniak, R. Kaminski","submitted_at":"2010-11-03T18:29:52Z","abstract_excerpt":"We study CP violation and the contribution of the strong pion-pion interactions in the three-body B+- --> pi+- pi-+ pi+- decays within a quasi two-body QCD factorization approach. The short distance interaction amplitude is calculated in the next-to-leading order in the strong coupling constant with vertex and penguin corrections. The meson-meson final state interactions are described by pion non-strange scalar and vector form factors for the S and P waves and by a relativistic Breit-Wigner formula for the D wave. The pion scalar form factor is calculated from a unitary relativistic coupled-ch"},"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":"1011.0960","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-11-03T18:29:52Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"9466afc4323ebe3afc0941fcd69c051e393ed57fd5a4b229f4aa545be6763375","abstract_canon_sha256":"7e0516acc0778a6b39653decbec22173a596fc2db173bd858cd316a91dd1f114"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:05.689859Z","signature_b64":"qypWW6o32Xsbtv/D12nGR5Nsxb8nJn45oxwFiukT/RAME7k2o1+L29z3DSgatc1SIxYQznXiizblGBhihF4sBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c29cef85c14ece19edae79bb62bfea69bd8edfea20188b2520d184868ab26f49","last_reissued_at":"2026-05-18T04:13:05.689432Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:05.689432Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"S-, P- and D-wave final state interactions and CP violation in B+- --> pi+- pi-+ pi+- decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"A. Furman, B. Loiseau, J.-P. Dedonder, L. Lesniak, R. Kaminski","submitted_at":"2010-11-03T18:29:52Z","abstract_excerpt":"We study CP violation and the contribution of the strong pion-pion interactions in the three-body B+- --> pi+- pi-+ pi+- decays within a quasi two-body QCD factorization approach. The short distance interaction amplitude is calculated in the next-to-leading order in the strong coupling constant with vertex and penguin corrections. The meson-meson final state interactions are described by pion non-strange scalar and vector form factors for the S and P waves and by a relativistic Breit-Wigner formula for the D wave. The pion scalar form factor is calculated from a unitary relativistic coupled-ch"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1011.0960","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":""},"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":"1011.0960","created_at":"2026-05-18T04:13:05.689488+00:00"},{"alias_kind":"arxiv_version","alias_value":"1011.0960v2","created_at":"2026-05-18T04:13:05.689488+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1011.0960","created_at":"2026-05-18T04:13:05.689488+00:00"},{"alias_kind":"pith_short_12","alias_value":"YKOO7BOBJ3HB","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_16","alias_value":"YKOO7BOBJ3HBT3NO","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_8","alias_value":"YKOO7BOB","created_at":"2026-05-18T12:26:17.028572+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.01305","citing_title":"$B_c$ meson decays into $S$-wave charmonium plus light meson pairs in the perturbative QCD approach","ref_index":70,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG","json":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG.json","graph_json":"https://pith.science/api/pith-number/YKOO7BOBJ3HBT3NOPG5WFP7KNG/graph.json","events_json":"https://pith.science/api/pith-number/YKOO7BOBJ3HBT3NOPG5WFP7KNG/events.json","paper":"https://pith.science/paper/YKOO7BOB"},"agent_actions":{"view_html":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG","download_json":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG.json","view_paper":"https://pith.science/paper/YKOO7BOB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1011.0960&json=true","fetch_graph":"https://pith.science/api/pith-number/YKOO7BOBJ3HBT3NOPG5WFP7KNG/graph.json","fetch_events":"https://pith.science/api/pith-number/YKOO7BOBJ3HBT3NOPG5WFP7KNG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG/action/storage_attestation","attest_author":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG/action/author_attestation","sign_citation":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG/action/citation_signature","submit_replication":"https://pith.science/pith/YKOO7BOBJ3HBT3NOPG5WFP7KNG/action/replication_record"}},"created_at":"2026-05-18T04:13:05.689488+00:00","updated_at":"2026-05-18T04:13:05.689488+00:00"}