{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:FQKE6OES6RHEVDAIFO66K5KXXV","short_pith_number":"pith:FQKE6OES","schema_version":"1.0","canonical_sha256":"2c144f3892f44e4a8c082bbde57557bd5b9481ace78e075ed383ffbc97e6b99a","source":{"kind":"arxiv","id":"1402.1178","version":2},"attestation_state":"computed","paper":{"title":"Computing decay rates for new physics theories with FeynRules and MadGraph5/aMC@NLO","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Benjamin Fuks, Chia-Hsien Shen, Claude Duhr, Deniz Gizem Ozturk, Johan Alwall, Olivier Mattelaer","submitted_at":"2014-02-05T21:02:01Z","abstract_excerpt":"We present new features of the FeynRules and MadGraph5/aMC@NLO programs for the automatic computation of decay widths that consistently include channels of arbitrary final-state multiplicity. The implementations are generic enough so that they can be used in the framework of any quantum field theory, possibly including higher-dimensional operators. We extend at the same time the conventions of the Universal FeynRules Output (or UFO) format to include decay tables and information on the total widths. We finally provide a set of representative examples of the usage of the new functions of the di"},"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":"1402.1178","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-05T21:02:01Z","cross_cats_sorted":[],"title_canon_sha256":"5dc7a023b375f093434cb750e2b3d0861863a663024840b2603dd4a444b13baa","abstract_canon_sha256":"0ee3bf05ce5996877cefe7955d7200fc791d18e3a62cba159b82e7e6f5996ec5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:25.664693Z","signature_b64":"ggC6hKLBC6ICwCJibXwwyLqP263O+rrLOhxXXxci8gW5383Iq1aG91ZzSeqkYSzggVaAG2WF5vxceO2cvl0YBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2c144f3892f44e4a8c082bbde57557bd5b9481ace78e075ed383ffbc97e6b99a","last_reissued_at":"2026-05-18T01:26:25.664086Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:25.664086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Computing decay rates for new physics theories with FeynRules and MadGraph5/aMC@NLO","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Benjamin Fuks, Chia-Hsien Shen, Claude Duhr, Deniz Gizem Ozturk, Johan Alwall, Olivier Mattelaer","submitted_at":"2014-02-05T21:02:01Z","abstract_excerpt":"We present new features of the FeynRules and MadGraph5/aMC@NLO programs for the automatic computation of decay widths that consistently include channels of arbitrary final-state multiplicity. The implementations are generic enough so that they can be used in the framework of any quantum field theory, possibly including higher-dimensional operators. We extend at the same time the conventions of the Universal FeynRules Output (or UFO) format to include decay tables and information on the total widths. We finally provide a set of representative examples of the usage of the new functions of the di"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.1178","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":"1402.1178","created_at":"2026-05-18T01:26:25.664171+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.1178v2","created_at":"2026-05-18T01:26:25.664171+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.1178","created_at":"2026-05-18T01:26:25.664171+00:00"},{"alias_kind":"pith_short_12","alias_value":"FQKE6OES6RHE","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_16","alias_value":"FQKE6OES6RHEVDAI","created_at":"2026-05-18T12:28:28.263976+00:00"},{"alias_kind":"pith_short_8","alias_value":"FQKE6OES","created_at":"2026-05-18T12:28:28.263976+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.01966","citing_title":"Reinterpreting the ATLAS HHH$\\to 6b$ Search with CheckMATE and Rivet: Validation, TRSM Benchmarks, and HL-LHC Prospects","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2412.07651","citing_title":"An EWPD SMEFT likelihood for the LHC -- and how to improve it with measurements of W and Z boson properties","ref_index":58,"is_internal_anchor":true},{"citing_arxiv_id":"2604.23038","citing_title":"Mono-Z' Signatures in the B-L Supersymmetric Standard Model at the LHC","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"1405.0301","citing_title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","ref_index":106,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV","json":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV.json","graph_json":"https://pith.science/api/pith-number/FQKE6OES6RHEVDAIFO66K5KXXV/graph.json","events_json":"https://pith.science/api/pith-number/FQKE6OES6RHEVDAIFO66K5KXXV/events.json","paper":"https://pith.science/paper/FQKE6OES"},"agent_actions":{"view_html":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV","download_json":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV.json","view_paper":"https://pith.science/paper/FQKE6OES","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.1178&json=true","fetch_graph":"https://pith.science/api/pith-number/FQKE6OES6RHEVDAIFO66K5KXXV/graph.json","fetch_events":"https://pith.science/api/pith-number/FQKE6OES6RHEVDAIFO66K5KXXV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV/action/storage_attestation","attest_author":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV/action/author_attestation","sign_citation":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV/action/citation_signature","submit_replication":"https://pith.science/pith/FQKE6OES6RHEVDAIFO66K5KXXV/action/replication_record"}},"created_at":"2026-05-18T01:26:25.664171+00:00","updated_at":"2026-05-18T01:26:25.664171+00:00"}