{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:6JVBHU3KTD6GHGRIVEX2QEDYKW","short_pith_number":"pith:6JVBHU3K","schema_version":"1.0","canonical_sha256":"f26a13d36a98fc639a28a92fa810785595598f476da94bb38f37ffe4fa006bd8","source":{"kind":"arxiv","id":"hep-ph/0107081","version":1},"attestation_state":"computed","paper":{"title":"Higgs Radiation off Top Quarks at the Tevatron and the LHC","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"B. Pl\\\"umper, M. Kr\\\"amer, M. Spira, P.M. Zerwas, S. Dittmaier, W. Beenakker","submitted_at":"2001-07-09T13:58:45Z","abstract_excerpt":"Higgs bosons can be searched for in the channels $p\\bar p/pp\\to t\\bar tH+X$ at the Tevatron and the LHC. We have calculated the QCD corrections to these processes in the Standard Model at next-to-leading order. The higher-order corrections reduce the renormalization and factorization scale dependence considerably and stabilize the theoretical predictions for the cross sections. At the central scale $\\mu=(2m_t+M_H)/2$ the properly defined $K$ factors are slightly below unity for the Tevatron ($K \\sim 0.8$) and slightly above unity for the LHC ($K \\sim 1.2$)."},"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/0107081","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-07-09T13:58:45Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"19a3c3326a43038f135963132adf4ccd44935c747c8ee9a2b655babcbcfde233","abstract_canon_sha256":"558fefe7dcaa80bf7dbd84247fcfb95e70951836fcdff2fae157f1ea9f5795bb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:24.502689Z","signature_b64":"wZkmeQtdQJgeXm7fsIWA/1P899obLiucrWlRuVOyH6WWUVDjXPgkBuBT5hB2OwXUDe1yuccmtRi0REkmTosJBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f26a13d36a98fc639a28a92fa810785595598f476da94bb38f37ffe4fa006bd8","last_reissued_at":"2026-07-04T16:27:24.502297Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:24.502297Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs Radiation off Top Quarks at the Tevatron and the LHC","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"B. Pl\\\"umper, M. Kr\\\"amer, M. Spira, P.M. Zerwas, S. Dittmaier, W. Beenakker","submitted_at":"2001-07-09T13:58:45Z","abstract_excerpt":"Higgs bosons can be searched for in the channels $p\\bar p/pp\\to t\\bar tH+X$ at the Tevatron and the LHC. We have calculated the QCD corrections to these processes in the Standard Model at next-to-leading order. The higher-order corrections reduce the renormalization and factorization scale dependence considerably and stabilize the theoretical predictions for the cross sections. At the central scale $\\mu=(2m_t+M_H)/2$ the properly defined $K$ factors are slightly below unity for the Tevatron ($K \\sim 0.8$) and slightly above unity for the LHC ($K \\sim 1.2$)."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0107081","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/hep-ph/0107081/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/0107081","created_at":"2026-07-04T16:27:24.502364+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0107081v1","created_at":"2026-07-04T16:27:24.502364+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0107081","created_at":"2026-07-04T16:27:24.502364+00:00"},{"alias_kind":"pith_short_12","alias_value":"6JVBHU3KTD6G","created_at":"2026-07-04T16:27:24.502364+00:00"},{"alias_kind":"pith_short_16","alias_value":"6JVBHU3KTD6GHGRI","created_at":"2026-07-04T16:27:24.502364+00:00"},{"alias_kind":"pith_short_8","alias_value":"6JVBHU3K","created_at":"2026-07-04T16:27:24.502364+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.05880","citing_title":"Top-associated Higgs-boson production using perturbative fragmentation functions at next-to-leading-order","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2605.05880","citing_title":"Top-associated Higgs-boson production using perturbative fragmentation functions at next-to-leading-order","ref_index":1,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW","json":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW.json","graph_json":"https://pith.science/api/pith-number/6JVBHU3KTD6GHGRIVEX2QEDYKW/graph.json","events_json":"https://pith.science/api/pith-number/6JVBHU3KTD6GHGRIVEX2QEDYKW/events.json","paper":"https://pith.science/paper/6JVBHU3K"},"agent_actions":{"view_html":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW","download_json":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW.json","view_paper":"https://pith.science/paper/6JVBHU3K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0107081&json=true","fetch_graph":"https://pith.science/api/pith-number/6JVBHU3KTD6GHGRIVEX2QEDYKW/graph.json","fetch_events":"https://pith.science/api/pith-number/6JVBHU3KTD6GHGRIVEX2QEDYKW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW/action/storage_attestation","attest_author":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW/action/author_attestation","sign_citation":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW/action/citation_signature","submit_replication":"https://pith.science/pith/6JVBHU3KTD6GHGRIVEX2QEDYKW/action/replication_record"}},"created_at":"2026-07-04T16:27:24.502364+00:00","updated_at":"2026-07-04T16:27:24.502364+00:00"}