{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:4HFB4RLR6NT5ETXUA6O7QCWNBP","short_pith_number":"pith:4HFB4RLR","schema_version":"1.0","canonical_sha256":"e1ca1e4571f367d24ef4079df80acd0bcee1a7174076ec6a4537b167ef775984","source":{"kind":"arxiv","id":"2106.05331","version":2},"attestation_state":"computed","paper":{"title":"A first next-to-next-to-leading order study of three-jet production at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-th"],"primary_cat":"hep-ph","authors_text":"Alexander Mitov, Michal Czakon, Rene Poncelet","submitted_at":"2021-06-09T18:42:58Z","abstract_excerpt":"Multi-jet rates at hadron colliders provide a unique possibility for probing Quantum Chromodynamics (QCD), the theory of strong interactions. By comparing theory predictions with collider data, one can directly test perturbative QCD, extract fundamental parameters like the strong coupling $\\alpha_s$ and search for physics beyond the Standard Model. In this work we calculate, for the first time, the next-to-next-to-leading (NNLO) QCD corrections to typical three-jet observables and to differential three-to-two jet ratios. We demonstrate that the inclusion of the NNLO corrections significantly r"},"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":"2106.05331","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2021-06-09T18:42:58Z","cross_cats_sorted":["hep-ex","hep-th"],"title_canon_sha256":"7ac61322bd1f7914dbff51e02e99e7f2ff18f926d6743f3c5022831164594558","abstract_canon_sha256":"ae4e8ef1ff39efe0db65606ee8287d4adc3de764f078dc8e3617d2c500364d12"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:51:52.577803Z","signature_b64":"M0nQkQNL3mW/A0dPM/cs8UjdEqQ8k6Fz10AemU5UGkq4m5b4VtPeOVv654hbxWxiQVRAOWCjsAr7A2qAg6qbAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1ca1e4571f367d24ef4079df80acd0bcee1a7174076ec6a4537b167ef775984","last_reissued_at":"2026-07-05T04:51:52.577402Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:51:52.577402Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A first next-to-next-to-leading order study of three-jet production at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-th"],"primary_cat":"hep-ph","authors_text":"Alexander Mitov, Michal Czakon, Rene Poncelet","submitted_at":"2021-06-09T18:42:58Z","abstract_excerpt":"Multi-jet rates at hadron colliders provide a unique possibility for probing Quantum Chromodynamics (QCD), the theory of strong interactions. By comparing theory predictions with collider data, one can directly test perturbative QCD, extract fundamental parameters like the strong coupling $\\alpha_s$ and search for physics beyond the Standard Model. In this work we calculate, for the first time, the next-to-next-to-leading (NNLO) QCD corrections to typical three-jet observables and to differential three-to-two jet ratios. We demonstrate that the inclusion of the NNLO corrections significantly r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.05331","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2106.05331/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":"2106.05331","created_at":"2026-07-05T04:51:52.577478+00:00"},{"alias_kind":"arxiv_version","alias_value":"2106.05331v2","created_at":"2026-07-05T04:51:52.577478+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.05331","created_at":"2026-07-05T04:51:52.577478+00:00"},{"alias_kind":"pith_short_12","alias_value":"4HFB4RLR6NT5","created_at":"2026-07-05T04:51:52.577478+00:00"},{"alias_kind":"pith_short_16","alias_value":"4HFB4RLR6NT5ETXU","created_at":"2026-07-05T04:51:52.577478+00:00"},{"alias_kind":"pith_short_8","alias_value":"4HFB4RLR","created_at":"2026-07-05T04:51:52.577478+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2504.06689","citing_title":"Les Houches 2023 -- Physics at TeV Colliders: Report on the Standard Model Precision Wishlist","ref_index":190,"is_internal_anchor":false},{"citing_arxiv_id":"2511.11424","citing_title":"Double virtual QCD corrections to $t\\bar{t}+$jet production at the LHC","ref_index":59,"is_internal_anchor":false},{"citing_arxiv_id":"2511.11537","citing_title":"Two-loop all-plus helicity amplitudes for self-dual Higgs boson with gluons via unitarity cut constraints","ref_index":66,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25490","citing_title":"Les Houches study on inclusive jet production at NNLO+NNLL","ref_index":21,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12613","citing_title":"Next-to-next-to-next-to-leading order QCD corrections to photon-pair production","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP","json":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP.json","graph_json":"https://pith.science/api/pith-number/4HFB4RLR6NT5ETXUA6O7QCWNBP/graph.json","events_json":"https://pith.science/api/pith-number/4HFB4RLR6NT5ETXUA6O7QCWNBP/events.json","paper":"https://pith.science/paper/4HFB4RLR"},"agent_actions":{"view_html":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP","download_json":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP.json","view_paper":"https://pith.science/paper/4HFB4RLR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2106.05331&json=true","fetch_graph":"https://pith.science/api/pith-number/4HFB4RLR6NT5ETXUA6O7QCWNBP/graph.json","fetch_events":"https://pith.science/api/pith-number/4HFB4RLR6NT5ETXUA6O7QCWNBP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP/action/storage_attestation","attest_author":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP/action/author_attestation","sign_citation":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP/action/citation_signature","submit_replication":"https://pith.science/pith/4HFB4RLR6NT5ETXUA6O7QCWNBP/action/replication_record"}},"created_at":"2026-07-05T04:51:52.577478+00:00","updated_at":"2026-07-05T04:51:52.577478+00:00"}