{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:5374CF36XTDFAXJ43IF3TGW3NH","short_pith_number":"pith:5374CF36","schema_version":"1.0","canonical_sha256":"eeffc1177ebcc6505d3cda0bb99adb69cf961a297c46b6e57612394b74c0cc99","source":{"kind":"arxiv","id":"1801.09506","version":1},"attestation_state":"computed","paper":{"title":"HDECAY: Twenty++ Years After","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Abdelhak Djouadi, Jan Kalinowski, Margarete Muehlleitner, Michael Spira","submitted_at":"2018-01-29T13:57:13Z","abstract_excerpt":"The program HDECAY determines the partial decay widths and branching ratios of the Higgs bosons within the Standard Model with three and four generations of fermions, including the case when the Higgs couplings are rescaled, a general two--Higgs doublet model where the Higgs sector is extended and incorporates five physical states and its most studied incarnation, the minimal supersymmetric Standard Model (MSSM). The program addresses all decay channels including the dominant higher-order effects such as radiative corrections and multi-body channels. Since the first launch of the program, more"},"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":"1801.09506","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2018-01-29T13:57:13Z","cross_cats_sorted":[],"title_canon_sha256":"92984fd5c5e3204c6a3a9074cb8374691c2d0fa0b9fb579d6cd1fc00931f57f4","abstract_canon_sha256":"99b1381617701c1d8d40f8a11d4787069ec4ae8068a704d7e1e9f5fbca828b70"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:28.555186Z","signature_b64":"r0lcBel2yC6KbyBNIgueByehQWuHOC4xbLyXQU/TAetuaFG9fNU0z+5ZY6CaBodne4cr79B0A8gFJqk0bAZ/Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eeffc1177ebcc6505d3cda0bb99adb69cf961a297c46b6e57612394b74c0cc99","last_reissued_at":"2026-05-17T23:50:28.554594Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:28.554594Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"HDECAY: Twenty++ Years After","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Abdelhak Djouadi, Jan Kalinowski, Margarete Muehlleitner, Michael Spira","submitted_at":"2018-01-29T13:57:13Z","abstract_excerpt":"The program HDECAY determines the partial decay widths and branching ratios of the Higgs bosons within the Standard Model with three and four generations of fermions, including the case when the Higgs couplings are rescaled, a general two--Higgs doublet model where the Higgs sector is extended and incorporates five physical states and its most studied incarnation, the minimal supersymmetric Standard Model (MSSM). The program addresses all decay channels including the dominant higher-order effects such as radiative corrections and multi-body channels. Since the first launch of the program, more"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.09506","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":"1801.09506","created_at":"2026-05-17T23:50:28.554687+00:00"},{"alias_kind":"arxiv_version","alias_value":"1801.09506v1","created_at":"2026-05-17T23:50:28.554687+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.09506","created_at":"2026-05-17T23:50:28.554687+00:00"},{"alias_kind":"pith_short_12","alias_value":"5374CF36XTDF","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_16","alias_value":"5374CF36XTDFAXJ4","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_8","alias_value":"5374CF36","created_at":"2026-05-18T12:32:05.422762+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.20186","citing_title":"WIMP-like Dark Matter Without Thermalization At Freeze-Out","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"2509.01682","citing_title":"Towards a Unified Framework for Pseudo-Nambu-Goldstone Dark Matter and Electroweak Baryogenesis","ref_index":37,"is_internal_anchor":true},{"citing_arxiv_id":"2604.24152","citing_title":"Probing the electron Yukawa coupling via resonant Higgs boson production at FCC-ee via $e^+e^- \\to H \\to WW^*$ in lepton-plus-jets final states","ref_index":57,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH","json":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH.json","graph_json":"https://pith.science/api/pith-number/5374CF36XTDFAXJ43IF3TGW3NH/graph.json","events_json":"https://pith.science/api/pith-number/5374CF36XTDFAXJ43IF3TGW3NH/events.json","paper":"https://pith.science/paper/5374CF36"},"agent_actions":{"view_html":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH","download_json":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH.json","view_paper":"https://pith.science/paper/5374CF36","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1801.09506&json=true","fetch_graph":"https://pith.science/api/pith-number/5374CF36XTDFAXJ43IF3TGW3NH/graph.json","fetch_events":"https://pith.science/api/pith-number/5374CF36XTDFAXJ43IF3TGW3NH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH/action/storage_attestation","attest_author":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH/action/author_attestation","sign_citation":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH/action/citation_signature","submit_replication":"https://pith.science/pith/5374CF36XTDFAXJ43IF3TGW3NH/action/replication_record"}},"created_at":"2026-05-17T23:50:28.554687+00:00","updated_at":"2026-05-17T23:50:28.554687+00:00"}