{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:XRJJCP462ZWYYDW7VFXQTFPP3Y","short_pith_number":"pith:XRJJCP46","schema_version":"1.0","canonical_sha256":"bc52913f9ed66d8c0edfa96f0995efde28831833f5d7fd63c6e25f5c117fb8a1","source":{"kind":"arxiv","id":"1912.02010","version":1},"attestation_state":"computed","paper":{"title":"PROPHECY4F 3.0: A Monte Carlo program for Higgs-boson decays into four-fermion final states in and beyond the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexander M\\\"uck, Ansgar Denner, Stefan Dittmaier","submitted_at":"2019-12-04T14:22:09Z","abstract_excerpt":"The Monte Carlo generator PPROPHECY4F provides a PROPer description of the Higgs dECaY into 4 Fermions within the Standard Model, the Standard Model with a fourth fermion generation, a simple Higgs-singlet extension of the Standard Model, and the Two-Higgs-Doublet Model. The fully differential predictions include the full QCD and electroweak next-to-leading-order corrections, all interference contributions between different WW/ZZ channels, and all off-shell effects of intermediate W/Z bosons. PPROPHECY4F computes the inclusive partial decay widths and allows for the computation of binned diffe"},"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":"1912.02010","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-12-04T14:22:09Z","cross_cats_sorted":[],"title_canon_sha256":"87e2e9f697743f5987bd948c83d3012e7cdcaf694c2ff5ba059732e1108d18b4","abstract_canon_sha256":"0688c1d098269c7bbe8fd6868b62752d38c922876a19596bd8ac4f7a455d3c20"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:12:29.600972Z","signature_b64":"LZ6lIp4q0UyGFJx2lVRhbiZKOT9eX6PIgp5OBqx8tUPZhHYdvJ8m1iIFUXm+hsRh5q5mrTiVa2P16OfNPpf+DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bc52913f9ed66d8c0edfa96f0995efde28831833f5d7fd63c6e25f5c117fb8a1","last_reissued_at":"2026-07-05T01:12:29.600571Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:12:29.600571Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"PROPHECY4F 3.0: A Monte Carlo program for Higgs-boson decays into four-fermion final states in and beyond the Standard Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexander M\\\"uck, Ansgar Denner, Stefan Dittmaier","submitted_at":"2019-12-04T14:22:09Z","abstract_excerpt":"The Monte Carlo generator PPROPHECY4F provides a PROPer description of the Higgs dECaY into 4 Fermions within the Standard Model, the Standard Model with a fourth fermion generation, a simple Higgs-singlet extension of the Standard Model, and the Two-Higgs-Doublet Model. The fully differential predictions include the full QCD and electroweak next-to-leading-order corrections, all interference contributions between different WW/ZZ channels, and all off-shell effects of intermediate W/Z bosons. PPROPHECY4F computes the inclusive partial decay widths and allows for the computation of binned diffe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1912.02010","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/1912.02010/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":"1912.02010","created_at":"2026-07-05T01:12:29.600629+00:00"},{"alias_kind":"arxiv_version","alias_value":"1912.02010v1","created_at":"2026-07-05T01:12:29.600629+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1912.02010","created_at":"2026-07-05T01:12:29.600629+00:00"},{"alias_kind":"pith_short_12","alias_value":"XRJJCP462ZWY","created_at":"2026-07-05T01:12:29.600629+00:00"},{"alias_kind":"pith_short_16","alias_value":"XRJJCP462ZWYYDW7","created_at":"2026-07-05T01:12:29.600629+00:00"},{"alias_kind":"pith_short_8","alias_value":"XRJJCP46","created_at":"2026-07-05T01:12:29.600629+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2601.15983","citing_title":"Radiative corrections to decays of the 125 GeV Higgs boson in the complex Higgs triplet model","ref_index":72,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y","json":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y.json","graph_json":"https://pith.science/api/pith-number/XRJJCP462ZWYYDW7VFXQTFPP3Y/graph.json","events_json":"https://pith.science/api/pith-number/XRJJCP462ZWYYDW7VFXQTFPP3Y/events.json","paper":"https://pith.science/paper/XRJJCP46"},"agent_actions":{"view_html":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y","download_json":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y.json","view_paper":"https://pith.science/paper/XRJJCP46","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1912.02010&json=true","fetch_graph":"https://pith.science/api/pith-number/XRJJCP462ZWYYDW7VFXQTFPP3Y/graph.json","fetch_events":"https://pith.science/api/pith-number/XRJJCP462ZWYYDW7VFXQTFPP3Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y/action/storage_attestation","attest_author":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y/action/author_attestation","sign_citation":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y/action/citation_signature","submit_replication":"https://pith.science/pith/XRJJCP462ZWYYDW7VFXQTFPP3Y/action/replication_record"}},"created_at":"2026-07-05T01:12:29.600629+00:00","updated_at":"2026-07-05T01:12:29.600629+00:00"}