{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:ZIZY6BKSXGQ37GJZVRF7C6MM2T","short_pith_number":"pith:ZIZY6BKS","schema_version":"1.0","canonical_sha256":"ca338f0552b9a1bf9939ac4bf1798cd4f04d87d356e43650e51b2bd009a96a33","source":{"kind":"arxiv","id":"hep-ph/0311311","version":2},"attestation_state":"computed","paper":{"title":"A new method for real radiation at NNLO","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Anastasiou, Frank Petriello, Kirill Melnikov","submitted_at":"2003-11-24T20:46:46Z","abstract_excerpt":"We propose a new method of computing real emission contributions to hard QCD processes. Our approach uses sector decomposition of the exclusive final-state phase space to enable extraction of all singularities of the real emission matrix elements before integration over any kinematic variable. The exact kinematics of the real emission process are preserved in all regions of phase space. Traditional approaches to extracting singularities from real emission matrix elements, such as phase space slicing and dipole subtraction, require both the determination of counterterms for double real emission"},"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/0311311","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-11-24T20:46:46Z","cross_cats_sorted":[],"title_canon_sha256":"6083b7ab287eb8985fc50581a7571841023a8b4d796af83a236a3f11b578df86","abstract_canon_sha256":"97767b0df186bdc880601f2f4ec04bf3638426b1daa86c9793b81d52fa0a00f2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:17:41.950291Z","signature_b64":"UNDOJneKeh3IvUvDplt23Q+ajuv6nK2R4QsH6ft0BYfYfZhc/uWgoLAvlyAC6jPQNmg76DUME7z9AyHk3NosDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca338f0552b9a1bf9939ac4bf1798cd4f04d87d356e43650e51b2bd009a96a33","last_reissued_at":"2026-07-04T15:17:41.949912Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:17:41.949912Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A new method for real radiation at NNLO","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Anastasiou, Frank Petriello, Kirill Melnikov","submitted_at":"2003-11-24T20:46:46Z","abstract_excerpt":"We propose a new method of computing real emission contributions to hard QCD processes. Our approach uses sector decomposition of the exclusive final-state phase space to enable extraction of all singularities of the real emission matrix elements before integration over any kinematic variable. The exact kinematics of the real emission process are preserved in all regions of phase space. Traditional approaches to extracting singularities from real emission matrix elements, such as phase space slicing and dipole subtraction, require both the determination of counterterms for double real emission"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0311311","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/hep-ph/0311311/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/0311311","created_at":"2026-07-04T15:17:41.949973+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0311311v2","created_at":"2026-07-04T15:17:41.949973+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0311311","created_at":"2026-07-04T15:17:41.949973+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZIZY6BKSXGQ3","created_at":"2026-07-04T15:17:41.949973+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZIZY6BKSXGQ37GJZ","created_at":"2026-07-04T15:17:41.949973+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZIZY6BKS","created_at":"2026-07-04T15:17:41.949973+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2606.26247","citing_title":"Double-real corrections to color singlet decay in a parton-shower inspired scheme","ref_index":19,"is_internal_anchor":true},{"citing_arxiv_id":"2606.28239","citing_title":"Gravitational Compton scattering at the fourth post-Minkowskian order","ref_index":123,"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":174,"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":205,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T","json":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T.json","graph_json":"https://pith.science/api/pith-number/ZIZY6BKSXGQ37GJZVRF7C6MM2T/graph.json","events_json":"https://pith.science/api/pith-number/ZIZY6BKSXGQ37GJZVRF7C6MM2T/events.json","paper":"https://pith.science/paper/ZIZY6BKS"},"agent_actions":{"view_html":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T","download_json":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T.json","view_paper":"https://pith.science/paper/ZIZY6BKS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0311311&json=true","fetch_graph":"https://pith.science/api/pith-number/ZIZY6BKSXGQ37GJZVRF7C6MM2T/graph.json","fetch_events":"https://pith.science/api/pith-number/ZIZY6BKSXGQ37GJZVRF7C6MM2T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T/action/storage_attestation","attest_author":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T/action/author_attestation","sign_citation":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T/action/citation_signature","submit_replication":"https://pith.science/pith/ZIZY6BKSXGQ37GJZVRF7C6MM2T/action/replication_record"}},"created_at":"2026-07-04T15:17:41.949973+00:00","updated_at":"2026-07-04T15:17:41.949973+00:00"}