{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:2CTJHBNBJX6JWN2SHUF2DSYXOU","short_pith_number":"pith:2CTJHBNB","schema_version":"1.0","canonical_sha256":"d0a69385a14dfc9b37523d0ba1cb17750f4e528b6bd79bc24c88d79ee0adce49","source":{"kind":"arxiv","id":"2305.08016","version":1},"attestation_state":"computed","paper":{"title":"On the non-factorizable corrections to Higgs boson production in weak boson fusion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christian Br{\\o}nnum-Hansen, Kirill Melnikov, Konstantin Asteriadis","submitted_at":"2023-05-13T22:03:01Z","abstract_excerpt":"We discuss the non-factorizable corrections to Higgs boson production in weak boson fusion at the Large Hadron Collider. Such corrections depend on the finite part of the two-loop virtual amplitude $q \\, Q \\rightarrow q^\\prime \\, Q^\\prime + H$ which, up to now, has only been computed in the eikonal approximation. We combine this contribution with real-virtual and double-real non-factorizable QCD corrections and study their impact on the various observables in weak boson fusion. We find that the non-factorizable corrections are strongly dominated by the two-loop virtual contributions, while all"},"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":"2305.08016","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2023-05-13T22:03:01Z","cross_cats_sorted":[],"title_canon_sha256":"40779619380a5986c50710b448c66fd2699716524bde14ff8326863c02611e58","abstract_canon_sha256":"1d29bf0eee654b28cf8bbe7719a5ab1d46c673b40c9cc7f2134dbd8448640d2a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:09:56.994673Z","signature_b64":"J0w3Nm6C/txPnePQQ/eJ+N9BO2+2Sce4l8jBQFV2ehrh1Oh5U4Hii7NSfiBCzo98O9hNRd2Id6IspS7LPGGlCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d0a69385a14dfc9b37523d0ba1cb17750f4e528b6bd79bc24c88d79ee0adce49","last_reissued_at":"2026-07-05T06:09:56.994269Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:09:56.994269Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the non-factorizable corrections to Higgs boson production in weak boson fusion","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Christian Br{\\o}nnum-Hansen, Kirill Melnikov, Konstantin Asteriadis","submitted_at":"2023-05-13T22:03:01Z","abstract_excerpt":"We discuss the non-factorizable corrections to Higgs boson production in weak boson fusion at the Large Hadron Collider. Such corrections depend on the finite part of the two-loop virtual amplitude $q \\, Q \\rightarrow q^\\prime \\, Q^\\prime + H$ which, up to now, has only been computed in the eikonal approximation. We combine this contribution with real-virtual and double-real non-factorizable QCD corrections and study their impact on the various observables in weak boson fusion. We find that the non-factorizable corrections are strongly dominated by the two-loop virtual contributions, while all"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.08016","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/2305.08016/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":"2305.08016","created_at":"2026-07-05T06:09:56.994323+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.08016v1","created_at":"2026-07-05T06:09:56.994323+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.08016","created_at":"2026-07-05T06:09:56.994323+00:00"},{"alias_kind":"pith_short_12","alias_value":"2CTJHBNBJX6J","created_at":"2026-07-05T06:09:56.994323+00:00"},{"alias_kind":"pith_short_16","alias_value":"2CTJHBNBJX6JWN2S","created_at":"2026-07-05T06:09:56.994323+00:00"},{"alias_kind":"pith_short_8","alias_value":"2CTJHBNB","created_at":"2026-07-05T06:09:56.994323+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.09112","citing_title":"Precision tools for the simulation of double-Higgs production via vector-boson fusion","ref_index":41,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU","json":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU.json","graph_json":"https://pith.science/api/pith-number/2CTJHBNBJX6JWN2SHUF2DSYXOU/graph.json","events_json":"https://pith.science/api/pith-number/2CTJHBNBJX6JWN2SHUF2DSYXOU/events.json","paper":"https://pith.science/paper/2CTJHBNB"},"agent_actions":{"view_html":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU","download_json":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU.json","view_paper":"https://pith.science/paper/2CTJHBNB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.08016&json=true","fetch_graph":"https://pith.science/api/pith-number/2CTJHBNBJX6JWN2SHUF2DSYXOU/graph.json","fetch_events":"https://pith.science/api/pith-number/2CTJHBNBJX6JWN2SHUF2DSYXOU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU/action/storage_attestation","attest_author":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU/action/author_attestation","sign_citation":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU/action/citation_signature","submit_replication":"https://pith.science/pith/2CTJHBNBJX6JWN2SHUF2DSYXOU/action/replication_record"}},"created_at":"2026-07-05T06:09:56.994323+00:00","updated_at":"2026-07-05T06:09:56.994323+00:00"}