{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:SUMXGKYKZKQIBRIIFNGBI32PSV","short_pith_number":"pith:SUMXGKYK","schema_version":"1.0","canonical_sha256":"9519732b0acaa080c5082b4c146f4f957a9caa006224692145508777e9e58bd5","source":{"kind":"arxiv","id":"hep-ph/0207004","version":3},"attestation_state":"computed","paper":{"title":"Higgs boson production at hadron colliders in NNLO QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Charalampos Anastasiou, Kirill Melnikov","submitted_at":"2002-06-29T02:51:20Z","abstract_excerpt":"We compute the total cross-section for direct Higgs boson production in hadron collisions at NNLO in perturbative QCD. A new technique which allows us to perform an algorithmic evaluation of inclusive phase-space integrals is introduced, based on the Cutkosky rules, integration by parts and the differential equation method for computing master integrals. Finally, we discuss the numerical impact of the O(alpha_s^2) QCD corrections to the Higgs boson production cross-section at the LHC and the Tevatron."},"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":"hep-ph/0207004","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-06-29T02:51:20Z","cross_cats_sorted":[],"title_canon_sha256":"a0ecba65b915ce11a98c464fedf30ec5f99fe87df7559f4e4b4cfc0d8e908d49","abstract_canon_sha256":"a1714ed313cf7da15d6c991ae2e309a2663f68637d9e5930a0f1cddb612657bb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:14.780960Z","signature_b64":"XmSDeBv+B19Zz3ilkT/He6n9ejdQU6sUyG+SYY62TAK3RfrGXHVo3v+pnDumJbRl6RUp01sxUpf3TU3MNjRaCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9519732b0acaa080c5082b4c146f4f957a9caa006224692145508777e9e58bd5","last_reissued_at":"2026-07-04T16:34:14.780622Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:14.780622Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs boson production at hadron colliders in NNLO QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Charalampos Anastasiou, Kirill Melnikov","submitted_at":"2002-06-29T02:51:20Z","abstract_excerpt":"We compute the total cross-section for direct Higgs boson production in hadron collisions at NNLO in perturbative QCD. A new technique which allows us to perform an algorithmic evaluation of inclusive phase-space integrals is introduced, based on the Cutkosky rules, integration by parts and the differential equation method for computing master integrals. Finally, we discuss the numerical impact of the O(alpha_s^2) QCD corrections to the Higgs boson production cross-section at the LHC and the Tevatron."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0207004","kind":"arxiv","version":3},"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/hep-ph/0207004/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":"hep-ph/0207004","created_at":"2026-07-04T16:34:14.780683+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0207004v3","created_at":"2026-07-04T16:34:14.780683+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0207004","created_at":"2026-07-04T16:34:14.780683+00:00"},{"alias_kind":"pith_short_12","alias_value":"SUMXGKYKZKQI","created_at":"2026-07-04T16:34:14.780683+00:00"},{"alias_kind":"pith_short_16","alias_value":"SUMXGKYKZKQIBRII","created_at":"2026-07-04T16:34:14.780683+00:00"},{"alias_kind":"pith_short_8","alias_value":"SUMXGKYK","created_at":"2026-07-04T16:34:14.780683+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":8,"internal_anchor_count":7,"sample":[{"citing_arxiv_id":"2606.21702","citing_title":"Analytic results for heavy-quark contributions to charged-current DIS at NNLO","ref_index":57,"is_internal_anchor":true},{"citing_arxiv_id":"2606.28239","citing_title":"Gravitational Compton scattering at the fourth post-Minkowskian order","ref_index":122,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28590","citing_title":"Two-loop QCD corrections to $ H \\rightarrow b + \\bar{b} + g $ at higher powers in the dimensional regulator","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28590","citing_title":"Two-loop QCD corrections to $ H \\rightarrow b + \\bar{b} + g $ at higher powers in the dimensional regulator","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2606.03510","citing_title":"Analysis of the $C\\!P$ structure of the Yukawa coupling between the Higgs boson and tau leptons in proton-proton collisions at $\\sqrt{s}$ = 13.6 TeV","ref_index":103,"is_internal_anchor":true},{"citing_arxiv_id":"2606.05309","citing_title":"Interference effects in gluon-fusion Higgs boson production","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2512.24403","citing_title":"CoLoRFulNNLO for hadron collisions: integrating the iterated single unresolved subtraction terms","ref_index":20,"is_internal_anchor":true},{"citing_arxiv_id":"2604.12613","citing_title":"Next-to-next-to-next-to-leading order QCD corrections to photon-pair production","ref_index":29,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV","json":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV.json","graph_json":"https://pith.science/api/pith-number/SUMXGKYKZKQIBRIIFNGBI32PSV/graph.json","events_json":"https://pith.science/api/pith-number/SUMXGKYKZKQIBRIIFNGBI32PSV/events.json","paper":"https://pith.science/paper/SUMXGKYK"},"agent_actions":{"view_html":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV","download_json":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV.json","view_paper":"https://pith.science/paper/SUMXGKYK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0207004&json=true","fetch_graph":"https://pith.science/api/pith-number/SUMXGKYKZKQIBRIIFNGBI32PSV/graph.json","fetch_events":"https://pith.science/api/pith-number/SUMXGKYKZKQIBRIIFNGBI32PSV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV/action/storage_attestation","attest_author":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV/action/author_attestation","sign_citation":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV/action/citation_signature","submit_replication":"https://pith.science/pith/SUMXGKYKZKQIBRIIFNGBI32PSV/action/replication_record"}},"created_at":"2026-07-04T16:34:14.780683+00:00","updated_at":"2026-07-04T16:34:14.780683+00:00"}