{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:MJYURYFFEAU4EOJAYJ4JRFKZTP","short_pith_number":"pith:MJYURYFF","schema_version":"1.0","canonical_sha256":"627148e0a52029c23920c2789895599bc9d28d23dd26d67b138a002534971c12","source":{"kind":"arxiv","id":"hep-ph/9302311","version":1},"attestation_state":"computed","paper":{"title":"Top Near Threshold: All QCD Radiative Corrections are Trivial","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"K.Melnikov, O.Yakovlev","submitted_at":"1993-02-25T13:30:00Z","abstract_excerpt":"We have calculated part of O(${\\alpha}_{S}$) QCD radiative correction to the total cross-section of top's threshold production in $ e^{+}e^{-} \\to t\\bar t \\to W^{-} b W^{+} \\bar b$ reaction. We found out a curious fact: there is no O(${\\alpha}_{S}$) correction to the total cross-section, originated from $b \\bar b , t \\bar b ,\\bar t b $ gluon exchange and corresponding gluon emission. Thus, all O(${\\alpha}_{S}$) corrections which are non-zero, can be classified as: 1) corrections to $t \\bar t$ nonrelativistic potential 2) corrections to the top's width 3) hard gluon correction to $\\gamma t \\bar"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-ph/9302311","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1993-02-25T13:30:00Z","cross_cats_sorted":[],"title_canon_sha256":"806c01431fdb2f0402271ff93319f79ee40f62618921f07e692d88b19c269306","abstract_canon_sha256":"759ecf830ca04d37e2294f7026b80e8108c48678a494b06cd492ea6e744fa244"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:35.956521Z","signature_b64":"tuHS/OY//g4C9g92JftBuvuNpq0CVkJ45mcWJoFCuBCyjfqCyl/4ERfSUi0tvZyTSRr/2roZbTipnm8LxPXDCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"627148e0a52029c23920c2789895599bc9d28d23dd26d67b138a002534971c12","last_reissued_at":"2026-05-18T01:06:35.955820Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:35.955820Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Top Near Threshold: All QCD Radiative Corrections are Trivial","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"K.Melnikov, O.Yakovlev","submitted_at":"1993-02-25T13:30:00Z","abstract_excerpt":"We have calculated part of O(${\\alpha}_{S}$) QCD radiative correction to the total cross-section of top's threshold production in $ e^{+}e^{-} \\to t\\bar t \\to W^{-} b W^{+} \\bar b$ reaction. We found out a curious fact: there is no O(${\\alpha}_{S}$) correction to the total cross-section, originated from $b \\bar b , t \\bar b ,\\bar t b $ gluon exchange and corresponding gluon emission. Thus, all O(${\\alpha}_{S}$) corrections which are non-zero, can be classified as: 1) corrections to $t \\bar t$ nonrelativistic potential 2) corrections to the top's width 3) hard gluon correction to $\\gamma t \\bar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9302311","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":""},"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/9302311","created_at":"2026-05-18T01:06:35.955929+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9302311v1","created_at":"2026-05-18T01:06:35.955929+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9302311","created_at":"2026-05-18T01:06:35.955929+00:00"},{"alias_kind":"pith_short_12","alias_value":"MJYURYFFEAU4","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_16","alias_value":"MJYURYFFEAU4EOJA","created_at":"2026-05-18T12:25:47.102015+00:00"},{"alias_kind":"pith_short_8","alias_value":"MJYURYFF","created_at":"2026-05-18T12:25:47.102015+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.09444","citing_title":"Non-factorisable electroweak virtual corrections to single-resonant processes","ref_index":3,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP","json":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP.json","graph_json":"https://pith.science/api/pith-number/MJYURYFFEAU4EOJAYJ4JRFKZTP/graph.json","events_json":"https://pith.science/api/pith-number/MJYURYFFEAU4EOJAYJ4JRFKZTP/events.json","paper":"https://pith.science/paper/MJYURYFF"},"agent_actions":{"view_html":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP","download_json":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP.json","view_paper":"https://pith.science/paper/MJYURYFF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9302311&json=true","fetch_graph":"https://pith.science/api/pith-number/MJYURYFFEAU4EOJAYJ4JRFKZTP/graph.json","fetch_events":"https://pith.science/api/pith-number/MJYURYFFEAU4EOJAYJ4JRFKZTP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP/action/storage_attestation","attest_author":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP/action/author_attestation","sign_citation":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP/action/citation_signature","submit_replication":"https://pith.science/pith/MJYURYFFEAU4EOJAYJ4JRFKZTP/action/replication_record"}},"created_at":"2026-05-18T01:06:35.955929+00:00","updated_at":"2026-05-18T01:06:35.955929+00:00"}