{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:PEGMN324OZISFHNRU45N4F7JH5","short_pith_number":"pith:PEGMN324","schema_version":"1.0","canonical_sha256":"790cc6ef5c7651229db1a73ade17e93f71c71a292173b34e982d664fb21f6f8e","source":{"kind":"arxiv","id":"hep-ph/0109062","version":2},"attestation_state":"computed","paper":{"title":"Electroweak radiative corrections to W-boson production at hadron colliders","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Michael Kramer, Stefan Dittmaier","submitted_at":"2001-09-07T15:48:47Z","abstract_excerpt":"The complete set of electroweak O(alpha) corrections to the Drell--Yan-like production of W bosons is calculated and compared to an approximation provided by the leading term of an expansion about the W-resonance pole. All relevant formulae are listed explicitly, and particular attention is paid to issues of gauge invariance and the instability of the W bosons. A detailed discussion of numerical results underlines the phenomenological importance of the electroweak corrections to W-boson production at the Tevatron and at the LHC. While the pole expansion yields a good description of resonance o"},"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/0109062","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-09-07T15:48:47Z","cross_cats_sorted":[],"title_canon_sha256":"b47e6d1c241f8f822e0d8da9860bcc9c67c61d8f2f6b4dc029ba40e7287f82e5","abstract_canon_sha256":"5b9855ea1009d84ce5b6932cdc2548c9ec4f6f0f79b21e32fdb3bc2e1ed884d2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:51:24.483422Z","signature_b64":"9Slj/0QGoNwC2y0/o47UYRr2yrx607UPDe1HutqlcVa83KSqw9alHA+r5TC3f6dING8JRbhSA9r8gTwlBNnPAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"790cc6ef5c7651229db1a73ade17e93f71c71a292173b34e982d664fb21f6f8e","last_reissued_at":"2026-07-04T15:51:24.482977Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:51:24.482977Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electroweak radiative corrections to W-boson production at hadron colliders","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Michael Kramer, Stefan Dittmaier","submitted_at":"2001-09-07T15:48:47Z","abstract_excerpt":"The complete set of electroweak O(alpha) corrections to the Drell--Yan-like production of W bosons is calculated and compared to an approximation provided by the leading term of an expansion about the W-resonance pole. All relevant formulae are listed explicitly, and particular attention is paid to issues of gauge invariance and the instability of the W bosons. A detailed discussion of numerical results underlines the phenomenological importance of the electroweak corrections to W-boson production at the Tevatron and at the LHC. While the pole expansion yields a good description of resonance o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0109062","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/0109062/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/0109062","created_at":"2026-07-04T15:51:24.483043+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0109062v2","created_at":"2026-07-04T15:51:24.483043+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0109062","created_at":"2026-07-04T15:51:24.483043+00:00"},{"alias_kind":"pith_short_12","alias_value":"PEGMN324OZIS","created_at":"2026-07-04T15:51:24.483043+00:00"},{"alias_kind":"pith_short_16","alias_value":"PEGMN324OZISFHNR","created_at":"2026-07-04T15:51:24.483043+00:00"},{"alias_kind":"pith_short_8","alias_value":"PEGMN324","created_at":"2026-07-04T15:51:24.483043+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2607.01174","citing_title":"The cleanest of them all: NLO electroweak corrections to vector-boson scattering into doubly polarised ZZ pairs at the LHC","ref_index":36,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28667","citing_title":"Towards the two-loop electroweak corrections to the Drell-Yan process: the complete fermionic contributions","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2510.07397","citing_title":"Slepton pair production at next-to-leading power","ref_index":34,"is_internal_anchor":true},{"citing_arxiv_id":"2605.09444","citing_title":"Non-factorisable electroweak virtual corrections to single-resonant processes","ref_index":39,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5","json":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5.json","graph_json":"https://pith.science/api/pith-number/PEGMN324OZISFHNRU45N4F7JH5/graph.json","events_json":"https://pith.science/api/pith-number/PEGMN324OZISFHNRU45N4F7JH5/events.json","paper":"https://pith.science/paper/PEGMN324"},"agent_actions":{"view_html":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5","download_json":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5.json","view_paper":"https://pith.science/paper/PEGMN324","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0109062&json=true","fetch_graph":"https://pith.science/api/pith-number/PEGMN324OZISFHNRU45N4F7JH5/graph.json","fetch_events":"https://pith.science/api/pith-number/PEGMN324OZISFHNRU45N4F7JH5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5/action/storage_attestation","attest_author":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5/action/author_attestation","sign_citation":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5/action/citation_signature","submit_replication":"https://pith.science/pith/PEGMN324OZISFHNRU45N4F7JH5/action/replication_record"}},"created_at":"2026-07-04T15:51:24.483043+00:00","updated_at":"2026-07-04T15:51:24.483043+00:00"}