{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:J7FHKEQ4ZZAF54A5GRX5HJNAFS","short_pith_number":"pith:J7FHKEQ4","schema_version":"1.0","canonical_sha256":"4fca75121cce405ef01d346fd3a5a02ca30b4ee48d1145bfb64f7eb190c0e807","source":{"kind":"arxiv","id":"0912.2104","version":1},"attestation_state":"computed","paper":{"title":"Higgs production in gluon fusion at next-to-next-to-leading order QCD for finite top mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hendrik Mantler, Kemal J. Ozeren, Robert V. Harlander, Simone Marzani","submitted_at":"2009-12-10T21:02:34Z","abstract_excerpt":"The inclusive Higgs production cross section from gluon fusion is calculated through NNLO QCD, including its top quark mass dependence. This is achieved through a matching of the 1/mtop expansion of the partonic cross sections to the exact large s-hat limits which are derived from k_T-factorization. The accuracy of this procedure is estimated to be better than 1% for the hadronic cross section. The final result is shown to be within 1% of the commonly used effective theory approach, thus confirming earlier findings."},"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":"0912.2104","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2009-12-10T21:02:34Z","cross_cats_sorted":[],"title_canon_sha256":"c57c18061bf839f10d39d4854e153dd9c920c0f80965f52d901e8ca2eb0d7e66","abstract_canon_sha256":"acbd117e3bc53b5cb63fca1b650c8d78e8df44735662ea8a0d57519a5a30f0d2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:29:29.140852Z","signature_b64":"SV4mQ5iYQReLNcKPjCGt8snhBGj1QeVRKjdU8dA626PU7FIJBBCovapcLYUfqXYhi353aVeFf9Jws9pOMJznDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4fca75121cce405ef01d346fd3a5a02ca30b4ee48d1145bfb64f7eb190c0e807","last_reissued_at":"2026-07-04T17:29:29.140467Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:29:29.140467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs production in gluon fusion at next-to-next-to-leading order QCD for finite top mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Hendrik Mantler, Kemal J. Ozeren, Robert V. Harlander, Simone Marzani","submitted_at":"2009-12-10T21:02:34Z","abstract_excerpt":"The inclusive Higgs production cross section from gluon fusion is calculated through NNLO QCD, including its top quark mass dependence. This is achieved through a matching of the 1/mtop expansion of the partonic cross sections to the exact large s-hat limits which are derived from k_T-factorization. The accuracy of this procedure is estimated to be better than 1% for the hadronic cross section. The final result is shown to be within 1% of the commonly used effective theory approach, thus confirming earlier findings."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0912.2104","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/0912.2104/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":"0912.2104","created_at":"2026-07-04T17:29:29.140529+00:00"},{"alias_kind":"arxiv_version","alias_value":"0912.2104v1","created_at":"2026-07-04T17:29:29.140529+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0912.2104","created_at":"2026-07-04T17:29:29.140529+00:00"},{"alias_kind":"pith_short_12","alias_value":"J7FHKEQ4ZZAF","created_at":"2026-07-04T17:29:29.140529+00:00"},{"alias_kind":"pith_short_16","alias_value":"J7FHKEQ4ZZAF54A5","created_at":"2026-07-04T17:29:29.140529+00:00"},{"alias_kind":"pith_short_8","alias_value":"J7FHKEQ4","created_at":"2026-07-04T17:29:29.140529+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2605.19016","citing_title":"Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13.6 TeV with the ATLAS dete","ref_index":61,"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":113,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19016","citing_title":"Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13.6 TeV with the ATLAS dete","ref_index":61,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS","json":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS.json","graph_json":"https://pith.science/api/pith-number/J7FHKEQ4ZZAF54A5GRX5HJNAFS/graph.json","events_json":"https://pith.science/api/pith-number/J7FHKEQ4ZZAF54A5GRX5HJNAFS/events.json","paper":"https://pith.science/paper/J7FHKEQ4"},"agent_actions":{"view_html":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS","download_json":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS.json","view_paper":"https://pith.science/paper/J7FHKEQ4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0912.2104&json=true","fetch_graph":"https://pith.science/api/pith-number/J7FHKEQ4ZZAF54A5GRX5HJNAFS/graph.json","fetch_events":"https://pith.science/api/pith-number/J7FHKEQ4ZZAF54A5GRX5HJNAFS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS/action/storage_attestation","attest_author":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS/action/author_attestation","sign_citation":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS/action/citation_signature","submit_replication":"https://pith.science/pith/J7FHKEQ4ZZAF54A5GRX5HJNAFS/action/replication_record"}},"created_at":"2026-07-04T17:29:29.140529+00:00","updated_at":"2026-07-04T17:29:29.140529+00:00"}