{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:LRFAIXF5ELNB5YVCIEFZXJXRFV","short_pith_number":"pith:LRFAIXF5","schema_version":"1.0","canonical_sha256":"5c4a045cbd22da1ee2a2410b9ba6f12d6541c24a066f950fd65f144d009ad7e5","source":{"kind":"arxiv","id":"2406.18374","version":1},"attestation_state":"computed","paper":{"title":"Non-Planar Two-Loop Amplitudes for Five-Parton Scattering","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Giuseppe De Laurentis","submitted_at":"2024-06-26T14:18:31Z","abstract_excerpt":"We review the current status of high-multiplicity double-virtual QCD corrections to processes relevant for LHC phenomenology. In particular, we discuss the recent full-color calculation of the five-parton process, whose two-loop amplitudes are required to obtain next-to-next-to-leading order predictions for three-jet production at the LHC. We address various aspects of the computation, including color decomposition, renormalization, partial amplitudes, color identities and the construction of the finite remainder. We review the method of numerical unitarity, which is used to generate finite-fi"},"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":"2406.18374","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-06-26T14:18:31Z","cross_cats_sorted":[],"title_canon_sha256":"38faef177c0b7d892a6f6e6e8b44ab4478a62ef3ce910adae12c7e316231cff9","abstract_canon_sha256":"23ae09ed0fda50bc6e5a4248f755b17fcd9836dabf11e55125df1aa2f6b6d4c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:37:08.475539Z","signature_b64":"MuJDko9zzz9GPgyywmAZAovXWdc9K3Uiquw924oArMtT89SXLr5xmwtYjcenVA+S+vpew217nrdXDZA2FPDUDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c4a045cbd22da1ee2a2410b9ba6f12d6541c24a066f950fd65f144d009ad7e5","last_reissued_at":"2026-07-05T08:37:08.474997Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:37:08.474997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Planar Two-Loop Amplitudes for Five-Parton Scattering","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Giuseppe De Laurentis","submitted_at":"2024-06-26T14:18:31Z","abstract_excerpt":"We review the current status of high-multiplicity double-virtual QCD corrections to processes relevant for LHC phenomenology. In particular, we discuss the recent full-color calculation of the five-parton process, whose two-loop amplitudes are required to obtain next-to-next-to-leading order predictions for three-jet production at the LHC. We address various aspects of the computation, including color decomposition, renormalization, partial amplitudes, color identities and the construction of the finite remainder. We review the method of numerical unitarity, which is used to generate finite-fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2406.18374","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2406.18374/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":"2406.18374","created_at":"2026-07-05T08:37:08.475052+00:00"},{"alias_kind":"arxiv_version","alias_value":"2406.18374v1","created_at":"2026-07-05T08:37:08.475052+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2406.18374","created_at":"2026-07-05T08:37:08.475052+00:00"},{"alias_kind":"pith_short_12","alias_value":"LRFAIXF5ELNB","created_at":"2026-07-05T08:37:08.475052+00:00"},{"alias_kind":"pith_short_16","alias_value":"LRFAIXF5ELNB5YVC","created_at":"2026-07-05T08:37:08.475052+00:00"},{"alias_kind":"pith_short_8","alias_value":"LRFAIXF5","created_at":"2026-07-05T08:37:08.475052+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.20577","citing_title":"Regge poles and cuts and the Lipatov vertex","ref_index":5,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV","json":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV.json","graph_json":"https://pith.science/api/pith-number/LRFAIXF5ELNB5YVCIEFZXJXRFV/graph.json","events_json":"https://pith.science/api/pith-number/LRFAIXF5ELNB5YVCIEFZXJXRFV/events.json","paper":"https://pith.science/paper/LRFAIXF5"},"agent_actions":{"view_html":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV","download_json":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV.json","view_paper":"https://pith.science/paper/LRFAIXF5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2406.18374&json=true","fetch_graph":"https://pith.science/api/pith-number/LRFAIXF5ELNB5YVCIEFZXJXRFV/graph.json","fetch_events":"https://pith.science/api/pith-number/LRFAIXF5ELNB5YVCIEFZXJXRFV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV/action/storage_attestation","attest_author":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV/action/author_attestation","sign_citation":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV/action/citation_signature","submit_replication":"https://pith.science/pith/LRFAIXF5ELNB5YVCIEFZXJXRFV/action/replication_record"}},"created_at":"2026-07-05T08:37:08.475052+00:00","updated_at":"2026-07-05T08:37:08.475052+00:00"}