{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:ZMDGS24CPGNJDPHJG5EP5ZTPLZ","short_pith_number":"pith:ZMDGS24C","schema_version":"1.0","canonical_sha256":"cb06696b82799a91bce93748fee66f5e4357f65cda10d9ed2552d39b95f4b545","source":{"kind":"arxiv","id":"1111.5869","version":2},"attestation_state":"computed","paper":{"title":"Top-pair production at hadron colliders with next-to-next-to-leading logarithmic soft-gluon resummation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexander Mitov, Matteo Cacciari, Michal Czakon, Michelangelo L. Mangano, Paolo Nason","submitted_at":"2011-11-24T23:14:29Z","abstract_excerpt":"Incorporating all recent theoretical advances, we resum soft-gluon corrections to the total $t\\bar t$ cross-section at hadron colliders at the next-to-next-to-leading logarithmic (NNLL) order. We perform the resummation in the well established framework of Mellin $N$-space resummation. We exhaustively study the sources of systematic uncertainty like renormalization and factorization scale variation, power suppressed effects and missing two- and higher-loop corrections. The inclusion of soft-gluon resummation at NNLL brings only a minor decrease in the perturbative uncertainty with respect to t"},"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":"1111.5869","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-11-24T23:14:29Z","cross_cats_sorted":[],"title_canon_sha256":"4429dae8bf908353a362d11a87e5f3a5bb7c80b6101465ef7bd587ff40e3a477","abstract_canon_sha256":"a3bf988e70487a11dc16ee768efecec7c027a3fb30cd22a7131416f08da9b250"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:25.613967Z","signature_b64":"Hyuy2HL5QJsOKhdR+J5U38K37xcCVaYXVGWIsxFJ9WgSFG5ldmyGxIjZzmcDcJzaD+M9GmsE3ZfopOLO+f07Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cb06696b82799a91bce93748fee66f5e4357f65cda10d9ed2552d39b95f4b545","last_reissued_at":"2026-05-18T01:59:25.613454Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:25.613454Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Top-pair production at hadron colliders with next-to-next-to-leading logarithmic soft-gluon resummation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alexander Mitov, Matteo Cacciari, Michal Czakon, Michelangelo L. Mangano, Paolo Nason","submitted_at":"2011-11-24T23:14:29Z","abstract_excerpt":"Incorporating all recent theoretical advances, we resum soft-gluon corrections to the total $t\\bar t$ cross-section at hadron colliders at the next-to-next-to-leading logarithmic (NNLL) order. We perform the resummation in the well established framework of Mellin $N$-space resummation. We exhaustively study the sources of systematic uncertainty like renormalization and factorization scale variation, power suppressed effects and missing two- and higher-loop corrections. The inclusion of soft-gluon resummation at NNLL brings only a minor decrease in the perturbative uncertainty with respect to t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.5869","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":"1111.5869","created_at":"2026-05-18T01:59:25.613534+00:00"},{"alias_kind":"arxiv_version","alias_value":"1111.5869v2","created_at":"2026-05-18T01:59:25.613534+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.5869","created_at":"2026-05-18T01:59:25.613534+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZMDGS24CPGNJ","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZMDGS24CPGNJDPHJ","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZMDGS24C","created_at":"2026-05-18T12:26:47.523578+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":7,"sample":[{"citing_arxiv_id":"2510.00160","citing_title":"Measurement of the dineutrino system kinematic variables in dileptonic top quark pair production in proton-proton collisions at$\\sqrt{s}$ = 13 TeV","ref_index":58,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":63,"is_internal_anchor":true},{"citing_arxiv_id":"2509.13759","citing_title":"Measurement of the $W$-boson angular coefficients and transverse momentum in $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector","ref_index":66,"is_internal_anchor":true},{"citing_arxiv_id":"2511.01995","citing_title":"Inclusive and differential measurements of the $\\mathrm{t\\bar{t}}\\gamma$ cross section and the $\\mathrm{t\\bar{t}}\\gamma$ / $\\mathrm{t\\bar{t}}$ cross section ratio in proton-proton collisions at $\\sqrt","ref_index":34,"is_internal_anchor":true},{"citing_arxiv_id":"2511.23091","citing_title":"Measurement of the top-quark mass using decays with a $J/\\psi$ meson at $\\sqrt{s}=$13 TeV with the ATLAS detector","ref_index":73,"is_internal_anchor":true},{"citing_arxiv_id":"2601.11780","citing_title":"Observation of a cross-section enhancement near the $t\\bar{t}$ production threshold in $\\sqrt{s}=13$ TeV $pp$ collisions with the ATLAS detector","ref_index":63,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13819","citing_title":"Search for charginos and neutralinos with $B-L$ $R$-parity violating decays in $\\sqrt{s}=13$ TeV and $13.6$ TeV $pp$ collisions with the ATLAS detector","ref_index":53,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ","json":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ.json","graph_json":"https://pith.science/api/pith-number/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/graph.json","events_json":"https://pith.science/api/pith-number/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/events.json","paper":"https://pith.science/paper/ZMDGS24C"},"agent_actions":{"view_html":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ","download_json":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ.json","view_paper":"https://pith.science/paper/ZMDGS24C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1111.5869&json=true","fetch_graph":"https://pith.science/api/pith-number/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/graph.json","fetch_events":"https://pith.science/api/pith-number/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/action/storage_attestation","attest_author":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/action/author_attestation","sign_citation":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/action/citation_signature","submit_replication":"https://pith.science/pith/ZMDGS24CPGNJDPHJG5EP5ZTPLZ/action/replication_record"}},"created_at":"2026-05-18T01:59:25.613534+00:00","updated_at":"2026-05-18T01:59:25.613534+00:00"}