{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:RNWFNTNP4BHEXQJ7C3QVG2TXKW","short_pith_number":"pith:RNWFNTNP","schema_version":"1.0","canonical_sha256":"8b6c56cdafe04e4bc13f16e1536a775593a5d5ad3153a7b85418f6b1363bf201","source":{"kind":"arxiv","id":"hep-ph/9409421","version":1},"attestation_state":"computed","paper":{"title":"Sources of CP Violation in the Two-Higgs Doublet Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Lincoln Wolfenstein, Yue-Liang Wu","submitted_at":"1994-09-27T10:30:06Z","abstract_excerpt":"Assuming CP violation arises solely through the Higgs potential, we develop the most general two-Higgs doublet model. There is no discrete symmetry that distinguishes the two Higgs bosons. It is assumed that an approximate global family symmetry sufficiently suppresses flavor-changing neutral scalar interactions. In addition to a CKM phase, neutral boson mixing, and superweak effects, there can be significant CP violation due to charged Higgs boson exchange. The value of $\\epsilon'/\\epsilon$ due to this last effect could be as large as in the standard model."},"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/9409421","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-09-27T10:30:06Z","cross_cats_sorted":[],"title_canon_sha256":"a0f259880a1f373f3ea84f687e07d46964f994542683c343518e31acbd591290","abstract_canon_sha256":"ed588a42b6fbe3d96b7f77623610f019a8a31975309642f2de3beb52a1997022"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:37:44.763775Z","signature_b64":"kGYuJA/1uPUemw3Y12NaeOYa5uPgErzPRjxn4uE8H4R3HSEiqjceRKz4C9TcRjkE0xDrGNeiZ4yohYh/AMZbAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8b6c56cdafe04e4bc13f16e1536a775593a5d5ad3153a7b85418f6b1363bf201","last_reissued_at":"2026-05-18T04:37:44.763133Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:37:44.763133Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Sources of CP Violation in the Two-Higgs Doublet Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Lincoln Wolfenstein, Yue-Liang Wu","submitted_at":"1994-09-27T10:30:06Z","abstract_excerpt":"Assuming CP violation arises solely through the Higgs potential, we develop the most general two-Higgs doublet model. There is no discrete symmetry that distinguishes the two Higgs bosons. It is assumed that an approximate global family symmetry sufficiently suppresses flavor-changing neutral scalar interactions. In addition to a CKM phase, neutral boson mixing, and superweak effects, there can be significant CP violation due to charged Higgs boson exchange. The value of $\\epsilon'/\\epsilon$ due to this last effect could be as large as in the standard model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9409421","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":"hep-ph/9409421","created_at":"2026-05-18T04:37:44.763221+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9409421v1","created_at":"2026-05-18T04:37:44.763221+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9409421","created_at":"2026-05-18T04:37:44.763221+00:00"},{"alias_kind":"pith_short_12","alias_value":"RNWFNTNP4BHE","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"RNWFNTNP4BHEXQJ7","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"RNWFNTNP","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.23348","citing_title":"Complex $\\tau$ Electric Dipole Moment from GeV-Scale New Physics","ref_index":31,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW","json":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW.json","graph_json":"https://pith.science/api/pith-number/RNWFNTNP4BHEXQJ7C3QVG2TXKW/graph.json","events_json":"https://pith.science/api/pith-number/RNWFNTNP4BHEXQJ7C3QVG2TXKW/events.json","paper":"https://pith.science/paper/RNWFNTNP"},"agent_actions":{"view_html":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW","download_json":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW.json","view_paper":"https://pith.science/paper/RNWFNTNP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9409421&json=true","fetch_graph":"https://pith.science/api/pith-number/RNWFNTNP4BHEXQJ7C3QVG2TXKW/graph.json","fetch_events":"https://pith.science/api/pith-number/RNWFNTNP4BHEXQJ7C3QVG2TXKW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW/action/storage_attestation","attest_author":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW/action/author_attestation","sign_citation":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW/action/citation_signature","submit_replication":"https://pith.science/pith/RNWFNTNP4BHEXQJ7C3QVG2TXKW/action/replication_record"}},"created_at":"2026-05-18T04:37:44.763221+00:00","updated_at":"2026-05-18T04:37:44.763221+00:00"}