{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1994:FVBIJH5LWGQZACVH5OPZIKDRG4","short_pith_number":"pith:FVBIJH5L","schema_version":"1.0","canonical_sha256":"2d42849fabb1a1900aa7eb9f942871373cc7b547968c3a9c6872f5aaf844c98d","source":{"kind":"arxiv","id":"hep-ph/9401311","version":1},"attestation_state":"computed","paper":{"title":"Phenomenology of models with more than two Higgs doublets","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Yuval Grossman","submitted_at":"1994-01-23T07:59:01Z","abstract_excerpt":"We study the most general Multi-Higgs-Doublet Model (MHDM) with Natural Flavor Conservation (NFC). The couplings of a charged scalar $H_i^{\\pm}$ to up quarks, down quarks and charged leptons depend on three new complex parameters, $X_i$, $Y_i$ and $Z_i$, respectively. We prove relations among these parameters. We carry out a comprehensive analysis of phenomenological constraints on the couplings of the lightest charged scalar: $X$, $Y$ and $Z$. We find that the general MHDM may differ significantly from its minimal version, the Two-Higgs-Doublet Model (2HDM)."},"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/9401311","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1994-01-23T07:59:01Z","cross_cats_sorted":[],"title_canon_sha256":"0f99b18a47acb71a3f806fa322bae0a75d3aedbdf78eeac8fb894e49e9b57924","abstract_canon_sha256":"61dcbedc26d35442186ae135bd6c45dffc34380d129d48ace14a9dea4a12bb31"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:37:45.900823Z","signature_b64":"ccT1uVnwCQeNztegW3SOAskghFFpYhhjfXSvygxaQ4UQICIjTC5IaSOtnKLuBx2b3Aixloe/0DXkhygtc4MdCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2d42849fabb1a1900aa7eb9f942871373cc7b547968c3a9c6872f5aaf844c98d","last_reissued_at":"2026-05-18T04:37:45.900078Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:37:45.900078Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phenomenology of models with more than two Higgs doublets","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Yuval Grossman","submitted_at":"1994-01-23T07:59:01Z","abstract_excerpt":"We study the most general Multi-Higgs-Doublet Model (MHDM) with Natural Flavor Conservation (NFC). The couplings of a charged scalar $H_i^{\\pm}$ to up quarks, down quarks and charged leptons depend on three new complex parameters, $X_i$, $Y_i$ and $Z_i$, respectively. We prove relations among these parameters. We carry out a comprehensive analysis of phenomenological constraints on the couplings of the lightest charged scalar: $X$, $Y$ and $Z$. We find that the general MHDM may differ significantly from its minimal version, the Two-Higgs-Doublet Model (2HDM)."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9401311","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/9401311","created_at":"2026-05-18T04:37:45.900185+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9401311v1","created_at":"2026-05-18T04:37:45.900185+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9401311","created_at":"2026-05-18T04:37:45.900185+00:00"},{"alias_kind":"pith_short_12","alias_value":"FVBIJH5LWGQZ","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"FVBIJH5LWGQZACVH","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"FVBIJH5L","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.15425","citing_title":"The $Z_3$ soft breaking in the I(2+1)HDM and its cosmological probes","ref_index":9,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4","json":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4.json","graph_json":"https://pith.science/api/pith-number/FVBIJH5LWGQZACVH5OPZIKDRG4/graph.json","events_json":"https://pith.science/api/pith-number/FVBIJH5LWGQZACVH5OPZIKDRG4/events.json","paper":"https://pith.science/paper/FVBIJH5L"},"agent_actions":{"view_html":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4","download_json":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4.json","view_paper":"https://pith.science/paper/FVBIJH5L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9401311&json=true","fetch_graph":"https://pith.science/api/pith-number/FVBIJH5LWGQZACVH5OPZIKDRG4/graph.json","fetch_events":"https://pith.science/api/pith-number/FVBIJH5LWGQZACVH5OPZIKDRG4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4/action/storage_attestation","attest_author":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4/action/author_attestation","sign_citation":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4/action/citation_signature","submit_replication":"https://pith.science/pith/FVBIJH5LWGQZACVH5OPZIKDRG4/action/replication_record"}},"created_at":"2026-05-18T04:37:45.900185+00:00","updated_at":"2026-05-18T04:37:45.900185+00:00"}