{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:G66FHCFADP73LF23YSGIAH6IWD","short_pith_number":"pith:G66FHCFA","schema_version":"1.0","canonical_sha256":"37bc5388a01bffb5975bc48c801fc8b0f0d2cbddd150407abc22f29e5d8747d2","source":{"kind":"arxiv","id":"1003.4451","version":2},"attestation_state":"computed","paper":{"title":"Higgs production via vector-boson fusion at NNLO in QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fabio Maltoni, Marco Zaro, Paolo Bolzoni, Sven-Olaf Moch","submitted_at":"2010-03-23T16:13:16Z","abstract_excerpt":"We present the total cross sections at next-to-next-to-leading order (NNLO) in the strong coupling for Higgs production via weak boson fusion. Our results are obtained via the structure function approach, which builds upon the approximate, though very accurate, factorization of the QCD corrections between the two quark lines. The theoretical uncertainty on the total cross sections at the LHC from higher order corrections and the parton distribution uncertainties are estimated at the 2% level each for a wide range of Higgs boson masses."},"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":"1003.4451","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-03-23T16:13:16Z","cross_cats_sorted":[],"title_canon_sha256":"2a14bfa029980872bee3652e7466266a2b6095e3ac5ae7bab9c7095f20074f6f","abstract_canon_sha256":"a7511fc209e233c0be001b42990e029c79006209ef3becc91c73abab76584103"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:40.580024Z","signature_b64":"4mkXY1tbPbOhwOQrE01ZOavJDNR7PV92Sc0NX4g4rM26zUb6w/nhFgzTxCadiishbssxwUbFrIXJx5TRnQnmCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"37bc5388a01bffb5975bc48c801fc8b0f0d2cbddd150407abc22f29e5d8747d2","last_reissued_at":"2026-05-18T02:33:40.579490Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:40.579490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs production via vector-boson fusion at NNLO in QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fabio Maltoni, Marco Zaro, Paolo Bolzoni, Sven-Olaf Moch","submitted_at":"2010-03-23T16:13:16Z","abstract_excerpt":"We present the total cross sections at next-to-next-to-leading order (NNLO) in the strong coupling for Higgs production via weak boson fusion. Our results are obtained via the structure function approach, which builds upon the approximate, though very accurate, factorization of the QCD corrections between the two quark lines. The theoretical uncertainty on the total cross sections at the LHC from higher order corrections and the parton distribution uncertainties are estimated at the 2% level each for a wide range of Higgs boson masses."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.4451","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":"1003.4451","created_at":"2026-05-18T02:33:40.579564+00:00"},{"alias_kind":"arxiv_version","alias_value":"1003.4451v2","created_at":"2026-05-18T02:33:40.579564+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.4451","created_at":"2026-05-18T02:33:40.579564+00:00"},{"alias_kind":"pith_short_12","alias_value":"G66FHCFADP73","created_at":"2026-05-18T12:26:07.630475+00:00"},{"alias_kind":"pith_short_16","alias_value":"G66FHCFADP73LF23","created_at":"2026-05-18T12:26:07.630475+00:00"},{"alias_kind":"pith_short_8","alias_value":"G66FHCFA","created_at":"2026-05-18T12:26:07.630475+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"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":68,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD","json":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD.json","graph_json":"https://pith.science/api/pith-number/G66FHCFADP73LF23YSGIAH6IWD/graph.json","events_json":"https://pith.science/api/pith-number/G66FHCFADP73LF23YSGIAH6IWD/events.json","paper":"https://pith.science/paper/G66FHCFA"},"agent_actions":{"view_html":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD","download_json":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD.json","view_paper":"https://pith.science/paper/G66FHCFA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1003.4451&json=true","fetch_graph":"https://pith.science/api/pith-number/G66FHCFADP73LF23YSGIAH6IWD/graph.json","fetch_events":"https://pith.science/api/pith-number/G66FHCFADP73LF23YSGIAH6IWD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD/action/storage_attestation","attest_author":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD/action/author_attestation","sign_citation":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD/action/citation_signature","submit_replication":"https://pith.science/pith/G66FHCFADP73LF23YSGIAH6IWD/action/replication_record"}},"created_at":"2026-05-18T02:33:40.579564+00:00","updated_at":"2026-05-18T02:33:40.579564+00:00"}