{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:HXFP4ZQKZSXN2CA4SULZPRAZR6","short_pith_number":"pith:HXFP4ZQK","schema_version":"1.0","canonical_sha256":"3dcafe660accaedd081c951797c4198fbe69a9988afcd47da670a39ceed3842e","source":{"kind":"arxiv","id":"hep-ph/9904427","version":1},"attestation_state":"computed","paper":{"title":"CP Violation and Prospects at B Factories and Hadron Colliders","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Ali (DESY, Hamburg)","submitted_at":"1999-04-22T10:27:35Z","abstract_excerpt":"We review the information on the CKM matrix elements, unitarity triangle and CP-violating phases $\\alpha, \\beta$ and $\\gamma$ in the standard model which will be measured in the forthcoming experiments at B factories, HERA-B and hadron colliders. We also discuss two-body non-leptonic decays $B \\to h_1 h_2$, with $h_i$ being light mesons, which are interesting from the point of view of CP violation and measurements of these phases. Partial rate CP asymmetries are presented in a number of decay modes using factorization for the matrix elements of the operators in the effective weak Hamiltonian. "},"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-ph/9904427","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1999-04-22T10:27:35Z","cross_cats_sorted":[],"title_canon_sha256":"692ba2cf92c8e76ed81cbf41ebbd1620bb1badc60f58c30894c6a4a2aa966418","abstract_canon_sha256":"149287c8017a388b9338df504a9a28ce3135a8d6a481c1639789aa3a3fc4cbfd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:30:58.015462Z","signature_b64":"LjMQvoY7R2sekJfgpk41pVk/FWkQ2dM6F1v6cnulmADIQf3EhqAc+s5zR70ZD8p3f4KsAWZF9l6tqrftXADfAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3dcafe660accaedd081c951797c4198fbe69a9988afcd47da670a39ceed3842e","last_reissued_at":"2026-07-04T14:30:58.014931Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:30:58.014931Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"CP Violation and Prospects at B Factories and Hadron Colliders","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Ali (DESY, Hamburg)","submitted_at":"1999-04-22T10:27:35Z","abstract_excerpt":"We review the information on the CKM matrix elements, unitarity triangle and CP-violating phases $\\alpha, \\beta$ and $\\gamma$ in the standard model which will be measured in the forthcoming experiments at B factories, HERA-B and hadron colliders. We also discuss two-body non-leptonic decays $B \\to h_1 h_2$, with $h_i$ being light mesons, which are interesting from the point of view of CP violation and measurements of these phases. Partial rate CP asymmetries are presented in a number of decay modes using factorization for the matrix elements of the operators in the effective weak Hamiltonian. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9904427","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/9904427/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-ph/9904427","created_at":"2026-07-04T14:30:58.014989+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9904427v1","created_at":"2026-07-04T14:30:58.014989+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9904427","created_at":"2026-07-04T14:30:58.014989+00:00"},{"alias_kind":"pith_short_12","alias_value":"HXFP4ZQKZSXN","created_at":"2026-07-04T14:30:58.014989+00:00"},{"alias_kind":"pith_short_16","alias_value":"HXFP4ZQKZSXN2CA4","created_at":"2026-07-04T14:30:58.014989+00:00"},{"alias_kind":"pith_short_8","alias_value":"HXFP4ZQK","created_at":"2026-07-04T14:30:58.014989+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/HXFP4ZQKZSXN2CA4SULZPRAZR6","json":"https://pith.science/pith/HXFP4ZQKZSXN2CA4SULZPRAZR6.json","graph_json":"https://pith.science/api/pith-number/HXFP4ZQKZSXN2CA4SULZPRAZR6/graph.json","events_json":"https://pith.science/api/pith-number/HXFP4ZQKZSXN2CA4SULZPRAZR6/events.json","paper":"https://pith.science/paper/HXFP4ZQK"},"agent_actions":{"view_html":"https://pith.science/pith/HXFP4ZQKZSXN2CA4SULZPRAZR6","download_json":"https://pith.science/pith/HXFP4ZQKZSXN2CA4SULZPRAZR6.json","view_paper":"https://pith.science/paper/HXFP4ZQK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9904427&json=true","fetch_graph":"https://pith.science/api/pith-number/HXFP4ZQKZSXN2CA4SULZPRAZR6/graph.json","fetch_events":"https://pith.science/api/pith-number/HXFP4ZQKZSXN2CA4SULZPRAZR6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HXFP4ZQKZSXN2CA4SULZPRAZR6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HXFP4ZQKZSXN2CA4SULZPRAZR6/action/storage_attestation","attest_author":"https://pith.science/pith/HXFP4ZQKZSXN2CA4SULZPRAZR6/action/author_attestation","sign_citation":"https://pith.science/pith/HXFP4ZQKZSXN2CA4SULZPRAZR6/action/citation_signature","submit_replication":"https://pith.science/pith/HXFP4ZQKZSXN2CA4SULZPRAZR6/action/replication_record"}},"created_at":"2026-07-04T14:30:58.014989+00:00","updated_at":"2026-07-04T14:30:58.014989+00:00"}