{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:MYKRVROFOYAMQVFEPQ5JIAC7CC","short_pith_number":"pith:MYKRVROF","schema_version":"1.0","canonical_sha256":"66151ac5c57600c854a47c3a94005f10aac96cf20bd855b02d29ec2a8fcc6815","source":{"kind":"arxiv","id":"1501.07226","version":2},"attestation_state":"computed","paper":{"title":"Higgs boson decay into b-quarks at NNLO accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Claude Duhr, Francesco Tramontano, Gabor Somogyi, Vittorio Del Duca, Zoltan Trocsanyi","submitted_at":"2015-01-28T18:29:07Z","abstract_excerpt":"We compute the fully differential decay rate of the Standard Model Higgs boson into b-quarks at next-to-next-to-leading order (NNLO) accuracy in alpha_S. We employ a general subtraction scheme developed for the calculation of higher order perturbative corrections to QCD jet cross sections, which is based on the universal infrared factorization properties of QCD squared matrix elements. We show that the subtractions render the various contributions to the NNLO correction finite. In particular, we demonstrate analytically that the sum of integrated subtraction terms correctly reproduces the infr"},"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":"1501.07226","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-01-28T18:29:07Z","cross_cats_sorted":[],"title_canon_sha256":"758e353bdb6b5a04b1ac3a22a237e86390425d8b2a594e01545124d8da089216","abstract_canon_sha256":"52a7b8713f77fdcbf39ea17b592ce2a8605c678c1e093cc8a8f091fa255d5224"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:49.332944Z","signature_b64":"ZP2rHhn09Wrk2XYEUkNT/zqEV9ZrGcVY/1+JTOpbSYxpndtvbadEA9wQleH8jZwJ6sy6Uo6QhQDS4oa4kekbCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"66151ac5c57600c854a47c3a94005f10aac96cf20bd855b02d29ec2a8fcc6815","last_reissued_at":"2026-05-18T01:09:49.332158Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:49.332158Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs boson decay into b-quarks at NNLO accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Claude Duhr, Francesco Tramontano, Gabor Somogyi, Vittorio Del Duca, Zoltan Trocsanyi","submitted_at":"2015-01-28T18:29:07Z","abstract_excerpt":"We compute the fully differential decay rate of the Standard Model Higgs boson into b-quarks at next-to-next-to-leading order (NNLO) accuracy in alpha_S. We employ a general subtraction scheme developed for the calculation of higher order perturbative corrections to QCD jet cross sections, which is based on the universal infrared factorization properties of QCD squared matrix elements. We show that the subtractions render the various contributions to the NNLO correction finite. In particular, we demonstrate analytically that the sum of integrated subtraction terms correctly reproduces the infr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.07226","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":"1501.07226","created_at":"2026-05-18T01:09:49.332280+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.07226v2","created_at":"2026-05-18T01:09:49.332280+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.07226","created_at":"2026-05-18T01:09:49.332280+00:00"},{"alias_kind":"pith_short_12","alias_value":"MYKRVROFOYAM","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_16","alias_value":"MYKRVROFOYAMQVFE","created_at":"2026-05-18T12:29:32.376354+00:00"},{"alias_kind":"pith_short_8","alias_value":"MYKRVROF","created_at":"2026-05-18T12:29:32.376354+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.24403","citing_title":"CoLoRFulNNLO for hadron collisions: integrating the iterated single unresolved subtraction terms","ref_index":14,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC","json":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC.json","graph_json":"https://pith.science/api/pith-number/MYKRVROFOYAMQVFEPQ5JIAC7CC/graph.json","events_json":"https://pith.science/api/pith-number/MYKRVROFOYAMQVFEPQ5JIAC7CC/events.json","paper":"https://pith.science/paper/MYKRVROF"},"agent_actions":{"view_html":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC","download_json":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC.json","view_paper":"https://pith.science/paper/MYKRVROF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.07226&json=true","fetch_graph":"https://pith.science/api/pith-number/MYKRVROFOYAMQVFEPQ5JIAC7CC/graph.json","fetch_events":"https://pith.science/api/pith-number/MYKRVROFOYAMQVFEPQ5JIAC7CC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC/action/storage_attestation","attest_author":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC/action/author_attestation","sign_citation":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC/action/citation_signature","submit_replication":"https://pith.science/pith/MYKRVROFOYAMQVFEPQ5JIAC7CC/action/replication_record"}},"created_at":"2026-05-18T01:09:49.332280+00:00","updated_at":"2026-05-18T01:09:49.332280+00:00"}