{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:XE2KCWTS355WT3WN25L7J6RVUY","short_pith_number":"pith:XE2KCWTS","schema_version":"1.0","canonical_sha256":"b934a15a72df7b69eecdd757f4fa35a600079a98e4ca263e1a1d37797a5ce4fa","source":{"kind":"arxiv","id":"hep-ph/0408315","version":2},"attestation_state":"computed","paper":{"title":"Two-loop corrections to Higgs boson production","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. Smith, V. Ravindran, W.L. van Neerven","submitted_at":"2004-08-27T12:41:56Z","abstract_excerpt":"In this paper we present the complete two-loop vertex corrections to scalar and pseudo-scalar Higgs boson production for general colour factors for the gauge group ${\\rm SU(N)}$ in the limit where the top quark mass gets infinite. We derive a general formula for the vertex correction which holds for conserved and non conserved operators. For the conserved operator we take the electromagnetic vertex correction as an example whereas for the non conserved operators we take the two vertex corrections above. Our observations for the structure of the pole terms $1/\\epsilon^4$, $1/\\epsilon^3$ and $1/"},"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/0408315","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2004-08-27T12:41:56Z","cross_cats_sorted":[],"title_canon_sha256":"f336d59e3f9ddcbd27eb1eca29908af23ae87ca29c93b1a2877439a5c19a23f7","abstract_canon_sha256":"3177ab7f9909b5cf273d33edae6ef5b6005b32cd4a6f05393c58658849b21294"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:24:37.983891Z","signature_b64":"nKwZSYBqe3IkKET5ZpyPySRnHkTJfaQtQsZl07+o/E7KweJRZ9b+qro4SUV6dlJ5XDTLos3+cdPFXVqStk3xBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b934a15a72df7b69eecdd757f4fa35a600079a98e4ca263e1a1d37797a5ce4fa","last_reissued_at":"2026-07-04T17:24:37.983525Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:24:37.983525Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-loop corrections to Higgs boson production","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"J. Smith, V. Ravindran, W.L. van Neerven","submitted_at":"2004-08-27T12:41:56Z","abstract_excerpt":"In this paper we present the complete two-loop vertex corrections to scalar and pseudo-scalar Higgs boson production for general colour factors for the gauge group ${\\rm SU(N)}$ in the limit where the top quark mass gets infinite. We derive a general formula for the vertex correction which holds for conserved and non conserved operators. For the conserved operator we take the electromagnetic vertex correction as an example whereas for the non conserved operators we take the two vertex corrections above. Our observations for the structure of the pole terms $1/\\epsilon^4$, $1/\\epsilon^3$ and $1/"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0408315","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0408315/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0408315","created_at":"2026-07-04T17:24:37.983586+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0408315v2","created_at":"2026-07-04T17:24:37.983586+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0408315","created_at":"2026-07-04T17:24:37.983586+00:00"},{"alias_kind":"pith_short_12","alias_value":"XE2KCWTS355W","created_at":"2026-07-04T17:24:37.983586+00:00"},{"alias_kind":"pith_short_16","alias_value":"XE2KCWTS355WT3WN","created_at":"2026-07-04T17:24:37.983586+00:00"},{"alias_kind":"pith_short_8","alias_value":"XE2KCWTS","created_at":"2026-07-04T17:24:37.983586+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.20342","citing_title":"Renormalization of axial anomaly in SU(N)$\\times$U(1)","ref_index":21,"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":22,"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":22,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY","json":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY.json","graph_json":"https://pith.science/api/pith-number/XE2KCWTS355WT3WN25L7J6RVUY/graph.json","events_json":"https://pith.science/api/pith-number/XE2KCWTS355WT3WN25L7J6RVUY/events.json","paper":"https://pith.science/paper/XE2KCWTS"},"agent_actions":{"view_html":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY","download_json":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY.json","view_paper":"https://pith.science/paper/XE2KCWTS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0408315&json=true","fetch_graph":"https://pith.science/api/pith-number/XE2KCWTS355WT3WN25L7J6RVUY/graph.json","fetch_events":"https://pith.science/api/pith-number/XE2KCWTS355WT3WN25L7J6RVUY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY/action/storage_attestation","attest_author":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY/action/author_attestation","sign_citation":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY/action/citation_signature","submit_replication":"https://pith.science/pith/XE2KCWTS355WT3WN25L7J6RVUY/action/replication_record"}},"created_at":"2026-07-04T17:24:37.983586+00:00","updated_at":"2026-07-04T17:24:37.983586+00:00"}