{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:BAXQETIEH3ZNJS667A4ZPXUNDW","short_pith_number":"pith:BAXQETIE","schema_version":"1.0","canonical_sha256":"082f024d043ef2d4cbdef83997de8d1db8965da107a2038084a2e0f512aeecb2","source":{"kind":"arxiv","id":"1303.0846","version":3},"attestation_state":"computed","paper":{"title":"Extraction of the CP-violating phase $\\gamma$ using $B \\to K \\pi \\pi$ and $B \\to K K {\\bar K}$ decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bhubanjyoti Bhattacharya, David London, Maxime Imbeault","submitted_at":"2013-03-04T21:02:13Z","abstract_excerpt":"Using the B{\\sc a}B{\\sc ar}\\ measurements of the Dalitz plots for $B^0 \\to K^+\\pi^0\\pi^-$, $B^0 \\to K^0\\pi^+\\pi^-$, $B^+ \\to K^+\\pi^+\\pi^-$, $B^0 \\to K^+ K^0 K^-$, and $B^0 \\to K^0 K^0 {\\bar K}^0$ decays, we demonstrate that it is possible to cleanly extract the weak phase $\\gamma$. We find four possible solutions. Three of these -- $32^\\circ$, $259^\\circ$, and $315^\\circ$ -- are in disagreement with the SM, while one -- $77^\\circ$ -- is consistent with the SM. An advantage of this Dalitz-plot method is that one can obtain many independent measurements of $\\gamma$, thereby reducing its statist"},"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":"1303.0846","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-04T21:02:13Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"bd94d2439e4b7eb39de183a95d0955025c5c058d2160bb0595aa646137b96204","abstract_canon_sha256":"dd68fcfa647d7b22e16917cb915f6ec83468bcf79434184233f4729f6fd7d160"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:04:13.896471Z","signature_b64":"F+8JZuP7frs2PB5uP6fotnluA9pTY3Cxs/T3PZak9BnCfRwLoO4WXKniYy5goBUh9+b/ThQEvwstKCVD+TwXCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"082f024d043ef2d4cbdef83997de8d1db8965da107a2038084a2e0f512aeecb2","last_reissued_at":"2026-05-18T03:04:13.895934Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:04:13.895934Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Extraction of the CP-violating phase $\\gamma$ using $B \\to K \\pi \\pi$ and $B \\to K K {\\bar K}$ decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bhubanjyoti Bhattacharya, David London, Maxime Imbeault","submitted_at":"2013-03-04T21:02:13Z","abstract_excerpt":"Using the B{\\sc a}B{\\sc ar}\\ measurements of the Dalitz plots for $B^0 \\to K^+\\pi^0\\pi^-$, $B^0 \\to K^0\\pi^+\\pi^-$, $B^+ \\to K^+\\pi^+\\pi^-$, $B^0 \\to K^+ K^0 K^-$, and $B^0 \\to K^0 K^0 {\\bar K}^0$ decays, we demonstrate that it is possible to cleanly extract the weak phase $\\gamma$. We find four possible solutions. Three of these -- $32^\\circ$, $259^\\circ$, and $315^\\circ$ -- are in disagreement with the SM, while one -- $77^\\circ$ -- is consistent with the SM. An advantage of this Dalitz-plot method is that one can obtain many independent measurements of $\\gamma$, thereby reducing its statist"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.0846","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":""},"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":"1303.0846","created_at":"2026-05-18T03:04:13.896012+00:00"},{"alias_kind":"arxiv_version","alias_value":"1303.0846v3","created_at":"2026-05-18T03:04:13.896012+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.0846","created_at":"2026-05-18T03:04:13.896012+00:00"},{"alias_kind":"pith_short_12","alias_value":"BAXQETIEH3ZN","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"BAXQETIEH3ZNJS66","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"BAXQETIE","created_at":"2026-05-18T12:27:38.830355+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/BAXQETIEH3ZNJS667A4ZPXUNDW","json":"https://pith.science/pith/BAXQETIEH3ZNJS667A4ZPXUNDW.json","graph_json":"https://pith.science/api/pith-number/BAXQETIEH3ZNJS667A4ZPXUNDW/graph.json","events_json":"https://pith.science/api/pith-number/BAXQETIEH3ZNJS667A4ZPXUNDW/events.json","paper":"https://pith.science/paper/BAXQETIE"},"agent_actions":{"view_html":"https://pith.science/pith/BAXQETIEH3ZNJS667A4ZPXUNDW","download_json":"https://pith.science/pith/BAXQETIEH3ZNJS667A4ZPXUNDW.json","view_paper":"https://pith.science/paper/BAXQETIE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1303.0846&json=true","fetch_graph":"https://pith.science/api/pith-number/BAXQETIEH3ZNJS667A4ZPXUNDW/graph.json","fetch_events":"https://pith.science/api/pith-number/BAXQETIEH3ZNJS667A4ZPXUNDW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BAXQETIEH3ZNJS667A4ZPXUNDW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BAXQETIEH3ZNJS667A4ZPXUNDW/action/storage_attestation","attest_author":"https://pith.science/pith/BAXQETIEH3ZNJS667A4ZPXUNDW/action/author_attestation","sign_citation":"https://pith.science/pith/BAXQETIEH3ZNJS667A4ZPXUNDW/action/citation_signature","submit_replication":"https://pith.science/pith/BAXQETIEH3ZNJS667A4ZPXUNDW/action/replication_record"}},"created_at":"2026-05-18T03:04:13.896012+00:00","updated_at":"2026-05-18T03:04:13.896012+00:00"}