{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1996:5G227ZEWYSUIHNVHTPHABOPIXZ","short_pith_number":"pith:5G227ZEW","schema_version":"1.0","canonical_sha256":"e9b5afe496c4a883b6a79bce00b9e8be50d9a92d00d353ce32f7999f00ee6061","source":{"kind":"arxiv","id":"hep-ph/9609326","version":2},"attestation_state":"computed","paper":{"title":"The Equivalence Theorem And Its Radiative-Correction-Free Formulation For All R_xi Gauges","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H.-J. He (DESY), W.B. Kilgore (FermiLab)","submitted_at":"1996-09-11T17:54:04Z","abstract_excerpt":"The electroweak equivalence theorem quantitatively connects the physical amplitudes of longitudinal massive gauge bosons to those of the corresponding ``unphysical'' would-be Goldstone bosons. Its precise form depends on both the gauge fixing condition and the renormalization scheme. Our previous modification-free schemes have applied to a broad class of $R_\\xi$ gauges including 't Hooft-Feynman gauge but excluding Landau gauge. In this paper we construct a new renormalization scheme in which the radiative modification factor, $C_{mod}^a$, is equal to unity for all $R_\\xi$-gauges, including bo"},"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/9609326","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-09-11T17:54:04Z","cross_cats_sorted":[],"title_canon_sha256":"49735c63ff65467b46d63eddd1cbe657f76d99ef202df319b623a5c7bbbd72ad","abstract_canon_sha256":"7970433a223c5add89964ae1a96836e257610ab0a0f57e9874f47b5920c5240a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:27.030162Z","signature_b64":"099rx8XDpoNDVDEPRIekIHAyfxn/Ba59WHS4lRJVbWH0VFQ9inn1C3CGGY+ZpSYMNnvvUKn2JYGQkl1Og7//BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e9b5afe496c4a883b6a79bce00b9e8be50d9a92d00d353ce32f7999f00ee6061","last_reissued_at":"2026-05-18T04:15:27.029819Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:27.029819Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Equivalence Theorem And Its Radiative-Correction-Free Formulation For All R_xi Gauges","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"H.-J. He (DESY), W.B. Kilgore (FermiLab)","submitted_at":"1996-09-11T17:54:04Z","abstract_excerpt":"The electroweak equivalence theorem quantitatively connects the physical amplitudes of longitudinal massive gauge bosons to those of the corresponding ``unphysical'' would-be Goldstone bosons. Its precise form depends on both the gauge fixing condition and the renormalization scheme. Our previous modification-free schemes have applied to a broad class of $R_\\xi$ gauges including 't Hooft-Feynman gauge but excluding Landau gauge. In this paper we construct a new renormalization scheme in which the radiative modification factor, $C_{mod}^a$, is equal to unity for all $R_\\xi$-gauges, including bo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9609326","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":""},"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/9609326","created_at":"2026-05-18T04:15:27.029870+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9609326v2","created_at":"2026-05-18T04:15:27.029870+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9609326","created_at":"2026-05-18T04:15:27.029870+00:00"},{"alias_kind":"pith_short_12","alias_value":"5G227ZEWYSUI","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"5G227ZEWYSUIHNVH","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"5G227ZEW","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ","json":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ.json","graph_json":"https://pith.science/api/pith-number/5G227ZEWYSUIHNVHTPHABOPIXZ/graph.json","events_json":"https://pith.science/api/pith-number/5G227ZEWYSUIHNVHTPHABOPIXZ/events.json","paper":"https://pith.science/paper/5G227ZEW"},"agent_actions":{"view_html":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ","download_json":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ.json","view_paper":"https://pith.science/paper/5G227ZEW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9609326&json=true","fetch_graph":"https://pith.science/api/pith-number/5G227ZEWYSUIHNVHTPHABOPIXZ/graph.json","fetch_events":"https://pith.science/api/pith-number/5G227ZEWYSUIHNVHTPHABOPIXZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ/action/storage_attestation","attest_author":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ/action/author_attestation","sign_citation":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ/action/citation_signature","submit_replication":"https://pith.science/pith/5G227ZEWYSUIHNVHTPHABOPIXZ/action/replication_record"}},"created_at":"2026-05-18T04:15:27.029870+00:00","updated_at":"2026-05-18T04:15:27.029870+00:00"}