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Lipkin","submitted_at":"2011-07-10T19:33:09Z","abstract_excerpt":"New data analysis with Pauli blocking explains observation of CP violation in $B^o\\rightarrow K\\pi$ decays, absence in $B^{\\pm} \\rightarrow K\\pi$ decays and gives new predictions agreeing with experiment. Branching ratio data show pure I=1/2 amplitude predicted by pure penguin transitions for separate relations within charged and neutral B decays, but strong violation of penguin I=1/2 isospin relation between charged and neutral decays. $B(B^o \\rightarrow K^+ \\pi^-) - 2B(B^o\\rightarrow K^o \\pi^o) =\n  %(19.4 \\pm 0.6)- 2\\cdot (9.4 \\pm 0.6) =\n  (0.6 \\pm 1.3)\\cdot 10^-6 \\approx 0$\n  $2B(B^+ \\right"},"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":"1107.1888","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-07-10T19:33:09Z","cross_cats_sorted":[],"title_canon_sha256":"e9c01f7df45f3b954c75ccf7366d2279bff63731ef82d416fb7621d7e077095d","abstract_canon_sha256":"d821aec62943c8915c5f0f04c01b9bc3451a207e02743af035a07f8a3346f069"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:18:33.935436Z","signature_b64":"1Ha2pSuUhGcbVHS5Cc9SHMXLSTRWSMSQToZ0HtCxXvIuqA7LeIRZpbFmIAGDyHyScmzCiTBkjJ7C02e8L4ybAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d8f363e32470bf908713bc20ee35e28d59c44f61cd2aeaee9a28e446c151d21b","last_reissued_at":"2026-05-18T04:18:33.934811Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:18:33.934811Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"New Analysis of $B \\rightarrow K\\pi$ data with Pauli blocking CP violation in $B^o$ decays, not in $B^{\\pm}$ SU(3) use of $B \\rightarrow \\pi\\pi$ data invalid for $B \\rightarrow K\\pi$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Harry J. Lipkin","submitted_at":"2011-07-10T19:33:09Z","abstract_excerpt":"New data analysis with Pauli blocking explains observation of CP violation in $B^o\\rightarrow K\\pi$ decays, absence in $B^{\\pm} \\rightarrow K\\pi$ decays and gives new predictions agreeing with experiment. Branching ratio data show pure I=1/2 amplitude predicted by pure penguin transitions for separate relations within charged and neutral B decays, but strong violation of penguin I=1/2 isospin relation between charged and neutral decays. $B(B^o \\rightarrow K^+ \\pi^-) - 2B(B^o\\rightarrow K^o \\pi^o) =\n  %(19.4 \\pm 0.6)- 2\\cdot (9.4 \\pm 0.6) =\n  (0.6 \\pm 1.3)\\cdot 10^-6 \\approx 0$\n  $2B(B^+ \\right"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.1888","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":"1107.1888","created_at":"2026-05-18T04:18:33.934888+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.1888v1","created_at":"2026-05-18T04:18:33.934888+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.1888","created_at":"2026-05-18T04:18:33.934888+00:00"},{"alias_kind":"pith_short_12","alias_value":"3DZWHYZEOC7Z","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_16","alias_value":"3DZWHYZEOC7ZBBYT","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_8","alias_value":"3DZWHYZE","created_at":"2026-05-18T12:26:18.847500+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/3DZWHYZEOC7ZBBYTXQQO4NPCRV","json":"https://pith.science/pith/3DZWHYZEOC7ZBBYTXQQO4NPCRV.json","graph_json":"https://pith.science/api/pith-number/3DZWHYZEOC7ZBBYTXQQO4NPCRV/graph.json","events_json":"https://pith.science/api/pith-number/3DZWHYZEOC7ZBBYTXQQO4NPCRV/events.json","paper":"https://pith.science/paper/3DZWHYZE"},"agent_actions":{"view_html":"https://pith.science/pith/3DZWHYZEOC7ZBBYTXQQO4NPCRV","download_json":"https://pith.science/pith/3DZWHYZEOC7ZBBYTXQQO4NPCRV.json","view_paper":"https://pith.science/paper/3DZWHYZE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.1888&json=true","fetch_graph":"https://pith.science/api/pith-number/3DZWHYZEOC7ZBBYTXQQO4NPCRV/graph.json","fetch_events":"https://pith.science/api/pith-number/3DZWHYZEOC7ZBBYTXQQO4NPCRV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3DZWHYZEOC7ZBBYTXQQO4NPCRV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3DZWHYZEOC7ZBBYTXQQO4NPCRV/action/storage_attestation","attest_author":"https://pith.science/pith/3DZWHYZEOC7ZBBYTXQQO4NPCRV/action/author_attestation","sign_citation":"https://pith.science/pith/3DZWHYZEOC7ZBBYTXQQO4NPCRV/action/citation_signature","submit_replication":"https://pith.science/pith/3DZWHYZEOC7ZBBYTXQQO4NPCRV/action/replication_record"}},"created_at":"2026-05-18T04:18:33.934888+00:00","updated_at":"2026-05-18T04:18:33.934888+00:00"}