{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:LUWBRSH3VPTJ2ZDXNC5R3TEO4U","short_pith_number":"pith:LUWBRSH3","schema_version":"1.0","canonical_sha256":"5d2c18c8fbabe69d647768bb1dcc8ee506087a6712a655e950d7b16edd87dbc6","source":{"kind":"arxiv","id":"1303.6254","version":1},"attestation_state":"computed","paper":{"title":"The total top quark pair production cross-section at hadron colliders through O(alpha_S^4)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alexander Mitov, Michal Czakon, Paul Fiedler","submitted_at":"2013-03-25T19:12:15Z","abstract_excerpt":"We compute the next-to-next-to-leading order (NNLO) QCD correction to the total cross-section for the reaction gg \\to t\\bar t + X. Together with the partonic channels we computed previously, the result derived in this letter completes the set of NNLO QCD corrections to the total top pair production cross-section at hadron colliders. Supplementing the fixed order results with soft-gluon resummation with next-to-next-to-leading logarithmic accuracy we estimate that the theoretical uncertainty of this observable due to unknown higher order corrections is about 3% at the LHC and 2.2% at the Tevatr"},"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":"1303.6254","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-03-25T19:12:15Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"4528a79fca5a0a38778096f4f2c64a6eeb24cf0bf82e90803e87d37ce0a96c2a","abstract_canon_sha256":"242c116795cfac1ab02d230be0ea6f94da1c4e6719882722653f04e29b5f8e7f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:16:49.303590Z","signature_b64":"RqU+d4NgbHCycp2AsVWv90k+QYV5f9cQyFotM5N1Q3bV26Cjz0xz8PF5r0Si9tcVs1eU0UKkskg5wBSLw29gCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d2c18c8fbabe69d647768bb1dcc8ee506087a6712a655e950d7b16edd87dbc6","last_reissued_at":"2026-05-18T03:16:49.302991Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:16:49.302991Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The total top quark pair production cross-section at hadron colliders through O(alpha_S^4)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alexander Mitov, Michal Czakon, Paul Fiedler","submitted_at":"2013-03-25T19:12:15Z","abstract_excerpt":"We compute the next-to-next-to-leading order (NNLO) QCD correction to the total cross-section for the reaction gg \\to t\\bar t + X. Together with the partonic channels we computed previously, the result derived in this letter completes the set of NNLO QCD corrections to the total top pair production cross-section at hadron colliders. Supplementing the fixed order results with soft-gluon resummation with next-to-next-to-leading logarithmic accuracy we estimate that the theoretical uncertainty of this observable due to unknown higher order corrections is about 3% at the LHC and 2.2% at the Tevatr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.6254","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":"1303.6254","created_at":"2026-05-18T03:16:49.303092+00:00"},{"alias_kind":"arxiv_version","alias_value":"1303.6254v1","created_at":"2026-05-18T03:16:49.303092+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.6254","created_at":"2026-05-18T03:16:49.303092+00:00"},{"alias_kind":"pith_short_12","alias_value":"LUWBRSH3VPTJ","created_at":"2026-05-18T12:27:51.066281+00:00"},{"alias_kind":"pith_short_16","alias_value":"LUWBRSH3VPTJ2ZDX","created_at":"2026-05-18T12:27:51.066281+00:00"},{"alias_kind":"pith_short_8","alias_value":"LUWBRSH3","created_at":"2026-05-18T12:27:51.066281+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":15,"internal_anchor_count":15,"sample":[{"citing_arxiv_id":"1906.10534","citing_title":"On the ratio of $t\\bar{t}\\gamma$ and $t\\bar{t}$ cross sections at the LHC","ref_index":1,"is_internal_anchor":true},{"citing_arxiv_id":"2503.17461","citing_title":"Electroweak diboson production in association with a high-mass dijet system in semileptonic final states from $pp$ collisions at $\\sqrt{s} = 13$ TeV with the ATLAS detector","ref_index":68,"is_internal_anchor":true},{"citing_arxiv_id":"2504.06689","citing_title":"Les Houches 2023 -- Physics at TeV Colliders: Report on the Standard Model Precision Wishlist","ref_index":177,"is_internal_anchor":true},{"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":57,"is_internal_anchor":true},{"citing_arxiv_id":"1912.10053","citing_title":"New CTEQ global analysis of quantum chromodynamics with high-precision data from the LHC","ref_index":183,"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":67,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16019","citing_title":"Inclusive charm and bottom quark pair production cross sections at hadron colliders at next-to-next-to-leading-order accuracy","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2506.22616","citing_title":"A novel phenomenological approach to total charm cross-section measurements at the LHC","ref_index":8,"is_internal_anchor":true},{"citing_arxiv_id":"2509.03596","citing_title":"Prospects for toponium formation at the LHC in the single-lepton mode","ref_index":43,"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":70,"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":37,"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":77,"is_internal_anchor":true},{"citing_arxiv_id":"2512.18391","citing_title":"Complete NLO corrections to off-shell $\\boldsymbol{t\\bar{t}}$ production in the $\\boldsymbol{\\ell+j}$ decay channel","ref_index":14,"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":67,"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":57,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U","json":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U.json","graph_json":"https://pith.science/api/pith-number/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/graph.json","events_json":"https://pith.science/api/pith-number/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/events.json","paper":"https://pith.science/paper/LUWBRSH3"},"agent_actions":{"view_html":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U","download_json":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U.json","view_paper":"https://pith.science/paper/LUWBRSH3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1303.6254&json=true","fetch_graph":"https://pith.science/api/pith-number/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/graph.json","fetch_events":"https://pith.science/api/pith-number/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/action/storage_attestation","attest_author":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/action/author_attestation","sign_citation":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/action/citation_signature","submit_replication":"https://pith.science/pith/LUWBRSH3VPTJ2ZDXNC5R3TEO4U/action/replication_record"}},"created_at":"2026-05-18T03:16:49.303092+00:00","updated_at":"2026-05-18T03:16:49.303092+00:00"}