{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:BDMMFS2WP5MZ6IGCIQEJ22CTOQ","short_pith_number":"pith:BDMMFS2W","schema_version":"1.0","canonical_sha256":"08d8c2cb567f599f20c244089d685374303cbf0ccbc02349e1af3f21b0f4a1c4","source":{"kind":"arxiv","id":"hep-ph/0609287","version":3},"attestation_state":"computed","paper":{"title":"Single top quark production at the Tevatron: threshold resummation and finite-order soft gluon corrections","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Nikolaos Kidonakis","submitted_at":"2006-09-27T21:09:27Z","abstract_excerpt":"I present a calculation of threshold soft-gluon corrections to single top quark production in ppbar collisions via all partonic processes in the t and s channels and via associated top quark and W boson production. The soft-gluon corrections are formally resummed to all orders, and finite-order expansions of the resummed cross section are calculated through next-to-next-to-next-to-leading order (NNNLO) at next-to-leading logarithmic (NLL) accuracy. Numerical results for single top quark production at the Tevatron are presented, including the dependence of the cross sections on the top quark ma"},"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/0609287","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-09-27T21:09:27Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"fd38b8bdaa91ccf6609f689572b8faa60cb2451366c22dd869945956bd10f630","abstract_canon_sha256":"12773835dd4d3a45fc1622d08eb6d699b9e13b07163f6e1b146b38edbb005d28"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:34.111879Z","signature_b64":"1sFpyT3g/1hb1MNkJajudSKLbSQqisvMXR1s93lqV3f/h/frLT6v59kB8p9B2p1xpep3alU6TaNEGLDez1X8CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"08d8c2cb567f599f20c244089d685374303cbf0ccbc02349e1af3f21b0f4a1c4","last_reissued_at":"2026-07-04T15:22:34.111480Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:34.111480Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Single top quark production at the Tevatron: threshold resummation and finite-order soft gluon corrections","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Nikolaos Kidonakis","submitted_at":"2006-09-27T21:09:27Z","abstract_excerpt":"I present a calculation of threshold soft-gluon corrections to single top quark production in ppbar collisions via all partonic processes in the t and s channels and via associated top quark and W boson production. The soft-gluon corrections are formally resummed to all orders, and finite-order expansions of the resummed cross section are calculated through next-to-next-to-next-to-leading order (NNNLO) at next-to-leading logarithmic (NLL) accuracy. Numerical results for single top quark production at the Tevatron are presented, including the dependence of the cross sections on the top quark ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0609287","kind":"arxiv","version":3},"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/0609287/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/0609287","created_at":"2026-07-04T15:22:34.111536+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0609287v3","created_at":"2026-07-04T15:22:34.111536+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0609287","created_at":"2026-07-04T15:22:34.111536+00:00"},{"alias_kind":"pith_short_12","alias_value":"BDMMFS2WP5MZ","created_at":"2026-07-04T15:22:34.111536+00:00"},{"alias_kind":"pith_short_16","alias_value":"BDMMFS2WP5MZ6IGC","created_at":"2026-07-04T15:22:34.111536+00:00"},{"alias_kind":"pith_short_8","alias_value":"BDMMFS2W","created_at":"2026-07-04T15:22:34.111536+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.21040","citing_title":"Constraining dimension-6 SMEFT with higher-order predictions for $p p \\to t W$","ref_index":92,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ","json":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ.json","graph_json":"https://pith.science/api/pith-number/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/graph.json","events_json":"https://pith.science/api/pith-number/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/events.json","paper":"https://pith.science/paper/BDMMFS2W"},"agent_actions":{"view_html":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ","download_json":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ.json","view_paper":"https://pith.science/paper/BDMMFS2W","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0609287&json=true","fetch_graph":"https://pith.science/api/pith-number/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/graph.json","fetch_events":"https://pith.science/api/pith-number/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/action/storage_attestation","attest_author":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/action/author_attestation","sign_citation":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/action/citation_signature","submit_replication":"https://pith.science/pith/BDMMFS2WP5MZ6IGCIQEJ22CTOQ/action/replication_record"}},"created_at":"2026-07-04T15:22:34.111536+00:00","updated_at":"2026-07-04T15:22:34.111536+00:00"}