{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:IZ7I464X4TBG3ILIOPM42MCU46","short_pith_number":"pith:IZ7I464X","schema_version":"1.0","canonical_sha256":"467e8e7b97e4c26da16873d9cd3054e7b12f03d5a4f3a8bcf42c9619983348df","source":{"kind":"arxiv","id":"1203.5769","version":2},"attestation_state":"computed","paper":{"title":"Light charged Higgs bosons decaying to charm and bottom quarks in models with two or more Higgs doublets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. G. Akeroyd, J. Hernandez-Sanchez, S. Moretti","submitted_at":"2012-03-26T19:37:05Z","abstract_excerpt":"Searches for light charged Higgs bosons (H^\\pm) in the decay of top quarks, t -> H^\\pm b, are being carried out at the LHC and at the Tevatron. It is assumed that the dominant decay channels for such an H^\\pm state are either H^\\pm -> \\tau\\nu or H^\\pm -> cs, and separate searches are performed with comparable sensitivity to the parameters m_{H^\\pm} and tanbeta of the scalar potential. The branching ratio for the decay H^\\pm -> cb can be as large as 80% in the Aligned Two Higgs Doublet Model and in models with three or more Higgs doublets with natural flavour conservation, while satisfying the "},"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":"1203.5769","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-03-26T19:37:05Z","cross_cats_sorted":[],"title_canon_sha256":"8581626670444c229b2b01ff30114b93522ac6e000e10b91652a634f263dc1e2","abstract_canon_sha256":"322eed28e861ffe50402972a77b3ba0519bc12a3a8e7e2bdcf7392a11005ec19"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:22:42.844815Z","signature_b64":"FYAknto7ulOZW53aTBkG90c0hYIfOHYMJ8F83pfDOIIVzlDFRFg7A2EN/WXqFaK2+TzB0Opv0S2umIg+PBTTAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"467e8e7b97e4c26da16873d9cd3054e7b12f03d5a4f3a8bcf42c9619983348df","last_reissued_at":"2026-05-18T03:22:42.844002Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:22:42.844002Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Light charged Higgs bosons decaying to charm and bottom quarks in models with two or more Higgs doublets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. G. Akeroyd, J. Hernandez-Sanchez, S. Moretti","submitted_at":"2012-03-26T19:37:05Z","abstract_excerpt":"Searches for light charged Higgs bosons (H^\\pm) in the decay of top quarks, t -> H^\\pm b, are being carried out at the LHC and at the Tevatron. It is assumed that the dominant decay channels for such an H^\\pm state are either H^\\pm -> \\tau\\nu or H^\\pm -> cs, and separate searches are performed with comparable sensitivity to the parameters m_{H^\\pm} and tanbeta of the scalar potential. The branching ratio for the decay H^\\pm -> cb can be as large as 80% in the Aligned Two Higgs Doublet Model and in models with three or more Higgs doublets with natural flavour conservation, while satisfying the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.5769","kind":"arxiv","version":2},"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":"1203.5769","created_at":"2026-05-18T03:22:42.844139+00:00"},{"alias_kind":"arxiv_version","alias_value":"1203.5769v2","created_at":"2026-05-18T03:22:42.844139+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.5769","created_at":"2026-05-18T03:22:42.844139+00:00"},{"alias_kind":"pith_short_12","alias_value":"IZ7I464X4TBG","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"IZ7I464X4TBG3ILI","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"IZ7I464X","created_at":"2026-05-18T12:27:09.501522+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/IZ7I464X4TBG3ILIOPM42MCU46","json":"https://pith.science/pith/IZ7I464X4TBG3ILIOPM42MCU46.json","graph_json":"https://pith.science/api/pith-number/IZ7I464X4TBG3ILIOPM42MCU46/graph.json","events_json":"https://pith.science/api/pith-number/IZ7I464X4TBG3ILIOPM42MCU46/events.json","paper":"https://pith.science/paper/IZ7I464X"},"agent_actions":{"view_html":"https://pith.science/pith/IZ7I464X4TBG3ILIOPM42MCU46","download_json":"https://pith.science/pith/IZ7I464X4TBG3ILIOPM42MCU46.json","view_paper":"https://pith.science/paper/IZ7I464X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1203.5769&json=true","fetch_graph":"https://pith.science/api/pith-number/IZ7I464X4TBG3ILIOPM42MCU46/graph.json","fetch_events":"https://pith.science/api/pith-number/IZ7I464X4TBG3ILIOPM42MCU46/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IZ7I464X4TBG3ILIOPM42MCU46/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IZ7I464X4TBG3ILIOPM42MCU46/action/storage_attestation","attest_author":"https://pith.science/pith/IZ7I464X4TBG3ILIOPM42MCU46/action/author_attestation","sign_citation":"https://pith.science/pith/IZ7I464X4TBG3ILIOPM42MCU46/action/citation_signature","submit_replication":"https://pith.science/pith/IZ7I464X4TBG3ILIOPM42MCU46/action/replication_record"}},"created_at":"2026-05-18T03:22:42.844139+00:00","updated_at":"2026-05-18T03:22:42.844139+00:00"}