{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:TNU5UKNDPLMSOAF7MZ4LVQCUUP","short_pith_number":"pith:TNU5UKND","schema_version":"1.0","canonical_sha256":"9b69da29a37ad92700bf6678bac054a3de1729d14e172284bed4d79b272b5359","source":{"kind":"arxiv","id":"1405.7046","version":1},"attestation_state":"computed","paper":{"title":"NNNLO soft-gluon corrections for the top-antitop pair production cross section","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Nikolaos Kidonakis","submitted_at":"2014-05-27T20:00:16Z","abstract_excerpt":"I present a calculation of next-to-next-to-next-to-leading-order (NNNLO) soft-gluon corrections for top-antitop pair production in hadronic collisions. Approximate NNNLO (aNNNLO) results are obtained by adding the NNNLO soft-gluon corrections to the complete next-to-next-to-leading-order (NNLO) cross section. Theoretical predictions are shown for the total aNNNLO $t{\\bar t}$ cross section at LHC and Tevatron energies. The aNNNLO cross sections are larger but have smaller theoretical uncertainties than at NNLO."},"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":"1405.7046","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-05-27T20:00:16Z","cross_cats_sorted":[],"title_canon_sha256":"65480deb7d588ecfb5b468a87dee0ca1f4985c0b21d2418a30b3c07678c6539f","abstract_canon_sha256":"699846e7d02174857f6ff37ae6b63ab3287c67d759579d4c20485ad80a6b25ef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:48:09.159087Z","signature_b64":"th+TofwGwv37dkPH1U+n/N4VHkNuQ18OfsBKk17/iIjGovs9+srM4z0FOJSDqibXXKqfLql0Q5EkpSbQtH2ICw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b69da29a37ad92700bf6678bac054a3de1729d14e172284bed4d79b272b5359","last_reissued_at":"2026-05-18T02:48:09.158547Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:48:09.158547Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"NNNLO soft-gluon corrections for the top-antitop pair production cross section","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Nikolaos Kidonakis","submitted_at":"2014-05-27T20:00:16Z","abstract_excerpt":"I present a calculation of next-to-next-to-next-to-leading-order (NNNLO) soft-gluon corrections for top-antitop pair production in hadronic collisions. Approximate NNNLO (aNNNLO) results are obtained by adding the NNNLO soft-gluon corrections to the complete next-to-next-to-leading-order (NNLO) cross section. Theoretical predictions are shown for the total aNNNLO $t{\\bar t}$ cross section at LHC and Tevatron energies. The aNNNLO cross sections are larger but have smaller theoretical uncertainties than at NNLO."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1405.7046","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":"1405.7046","created_at":"2026-05-18T02:48:09.158616+00:00"},{"alias_kind":"arxiv_version","alias_value":"1405.7046v1","created_at":"2026-05-18T02:48:09.158616+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1405.7046","created_at":"2026-05-18T02:48:09.158616+00:00"},{"alias_kind":"pith_short_12","alias_value":"TNU5UKNDPLMS","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"TNU5UKNDPLMSOAF7","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"TNU5UKND","created_at":"2026-05-18T12:28:49.207871+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.11333","citing_title":"Three-loop soft anomalous dimensions for top-quark production","ref_index":26,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP","json":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP.json","graph_json":"https://pith.science/api/pith-number/TNU5UKNDPLMSOAF7MZ4LVQCUUP/graph.json","events_json":"https://pith.science/api/pith-number/TNU5UKNDPLMSOAF7MZ4LVQCUUP/events.json","paper":"https://pith.science/paper/TNU5UKND"},"agent_actions":{"view_html":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP","download_json":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP.json","view_paper":"https://pith.science/paper/TNU5UKND","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1405.7046&json=true","fetch_graph":"https://pith.science/api/pith-number/TNU5UKNDPLMSOAF7MZ4LVQCUUP/graph.json","fetch_events":"https://pith.science/api/pith-number/TNU5UKNDPLMSOAF7MZ4LVQCUUP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP/action/storage_attestation","attest_author":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP/action/author_attestation","sign_citation":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP/action/citation_signature","submit_replication":"https://pith.science/pith/TNU5UKNDPLMSOAF7MZ4LVQCUUP/action/replication_record"}},"created_at":"2026-05-18T02:48:09.158616+00:00","updated_at":"2026-05-18T02:48:09.158616+00:00"}