{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:45CRWR3YK2FXWGHSX6GIOQJB6Q","short_pith_number":"pith:45CRWR3Y","schema_version":"1.0","canonical_sha256":"e7451b4778568b7b18f2bf8c874121f407bbe33506e89c74f7eb3ca067db5c93","source":{"kind":"arxiv","id":"1802.02445","version":1},"attestation_state":"computed","paper":{"title":"Second-order QCD effects in Higgs boson production through vector boson fusion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Huss, E.W.N. Glover, J. Cruz-Martinez, T. Gehrmann","submitted_at":"2018-02-07T14:44:16Z","abstract_excerpt":"We compute the factorising second-order QCD corrections to the electroweak production of a Higgs boson through vector boson fusion. Our calculation is fully differential in the kinematics of the Higgs boson and of the final state jets, and uses the antenna subtraction method to handle infrared singular configurations in the different parton-level contributions. Our results allow us to reassess the impact of the next-to-leading order (NLO) QCD corrections to electroweak Higgs-plus-three-jet production and of the next-to-next-to-leading order (NNLO) QCD corrections to electroweak Higgs-plus-two-"},"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":"1802.02445","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-02-07T14:44:16Z","cross_cats_sorted":[],"title_canon_sha256":"9ab2cd8d747efe93dc48797dc9c3ef7db7418b0b7a8d5aea022cce73d25ae9da","abstract_canon_sha256":"b04854683f5ce0f188e3d71d0bb755c932632125bfdcbda20484a991ed4ad73c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:17:05.022068Z","signature_b64":"i1IYhnUIqcJEwgmzl/Jv0TMrRBelgEYlTopGcIJpvOaN8i+v12soVI52GGwjzgMEmqeV1gvS5qEPMjonkDckAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e7451b4778568b7b18f2bf8c874121f407bbe33506e89c74f7eb3ca067db5c93","last_reissued_at":"2026-05-18T00:17:05.021430Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:17:05.021430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Second-order QCD effects in Higgs boson production through vector boson fusion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Huss, E.W.N. Glover, J. Cruz-Martinez, T. Gehrmann","submitted_at":"2018-02-07T14:44:16Z","abstract_excerpt":"We compute the factorising second-order QCD corrections to the electroweak production of a Higgs boson through vector boson fusion. Our calculation is fully differential in the kinematics of the Higgs boson and of the final state jets, and uses the antenna subtraction method to handle infrared singular configurations in the different parton-level contributions. Our results allow us to reassess the impact of the next-to-leading order (NLO) QCD corrections to electroweak Higgs-plus-three-jet production and of the next-to-next-to-leading order (NNLO) QCD corrections to electroweak Higgs-plus-two-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.02445","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":""},"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":"1802.02445","created_at":"2026-05-18T00:17:05.021539+00:00"},{"alias_kind":"arxiv_version","alias_value":"1802.02445v1","created_at":"2026-05-18T00:17:05.021539+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.02445","created_at":"2026-05-18T00:17:05.021539+00:00"},{"alias_kind":"pith_short_12","alias_value":"45CRWR3YK2FX","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_16","alias_value":"45CRWR3YK2FXWGHS","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_8","alias_value":"45CRWR3Y","created_at":"2026-05-18T12:32:05.422762+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.06689","citing_title":"Les Houches 2023 -- Physics at TeV Colliders: Report on the Standard Model Precision Wishlist","ref_index":153,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04009","citing_title":"Two-loop leading-color QCD corrections for Higgs plus two-jet production in the heavy-top limit","ref_index":8,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q","json":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q.json","graph_json":"https://pith.science/api/pith-number/45CRWR3YK2FXWGHSX6GIOQJB6Q/graph.json","events_json":"https://pith.science/api/pith-number/45CRWR3YK2FXWGHSX6GIOQJB6Q/events.json","paper":"https://pith.science/paper/45CRWR3Y"},"agent_actions":{"view_html":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q","download_json":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q.json","view_paper":"https://pith.science/paper/45CRWR3Y","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1802.02445&json=true","fetch_graph":"https://pith.science/api/pith-number/45CRWR3YK2FXWGHSX6GIOQJB6Q/graph.json","fetch_events":"https://pith.science/api/pith-number/45CRWR3YK2FXWGHSX6GIOQJB6Q/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q/action/timestamp_anchor","attest_storage":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q/action/storage_attestation","attest_author":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q/action/author_attestation","sign_citation":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q/action/citation_signature","submit_replication":"https://pith.science/pith/45CRWR3YK2FXWGHSX6GIOQJB6Q/action/replication_record"}},"created_at":"2026-05-18T00:17:05.021539+00:00","updated_at":"2026-05-18T00:17:05.021539+00:00"}