{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:LM36B34CQUDNPUCBHY4LDQ6V6G","short_pith_number":"pith:LM36B34C","schema_version":"1.0","canonical_sha256":"5b37e0ef828506d7d0413e38b1c3d5f1bfdee1712ee758301b6d632565b50f69","source":{"kind":"arxiv","id":"2312.15051","version":2},"attestation_state":"computed","paper":{"title":"One-loop five-parton amplitudes in the NMRK limit","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Emmet P. Byrne","submitted_at":"2023-12-22T20:31:34Z","abstract_excerpt":"We analyse the real part of one-loop five-parton amplitudes in the next-to-multi-Regge kinematic (NMRK) limit, to leading power, and to finite order in the dimensional regularisation parameter. To leading logarithmic (LL) accuracy, it is known that five-parton amplitudes in this limit are given to all-orders by a single factorised expression, in which the pair of partons which are not well-separated in rapidity are described by a two-parton emission vertex. In this study, we investigate the one-loop amplitudes at next-to-leading logarithmic (NLL) accuracy, and find that is has a more complex s"},"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":"2312.15051","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-12-22T20:31:34Z","cross_cats_sorted":[],"title_canon_sha256":"a40a14cada1f3b33184bb20050f1e9cbc953b5ebbf6e06dc4102bcfdd5bd6819","abstract_canon_sha256":"9cddd2edf91dfe979e5c9a748953b32deaf7c1871b8e9dd2e0205f9c4f101c2a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:18:47.405770Z","signature_b64":"O64om47xkn9JmczGY04rgsemc5PoCFU87Pam+WlBx4nbhwrjTrxh3mCcmIMd27o3qje8vfnmGeDKzyLqfahYAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5b37e0ef828506d7d0413e38b1c3d5f1bfdee1712ee758301b6d632565b50f69","last_reissued_at":"2026-07-05T08:18:47.405236Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:18:47.405236Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One-loop five-parton amplitudes in the NMRK limit","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Emmet P. Byrne","submitted_at":"2023-12-22T20:31:34Z","abstract_excerpt":"We analyse the real part of one-loop five-parton amplitudes in the next-to-multi-Regge kinematic (NMRK) limit, to leading power, and to finite order in the dimensional regularisation parameter. To leading logarithmic (LL) accuracy, it is known that five-parton amplitudes in this limit are given to all-orders by a single factorised expression, in which the pair of partons which are not well-separated in rapidity are described by a two-parton emission vertex. In this study, we investigate the one-loop amplitudes at next-to-leading logarithmic (NLL) accuracy, and find that is has a more complex s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2312.15051","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/2312.15051/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":"2312.15051","created_at":"2026-07-05T08:18:47.405298+00:00"},{"alias_kind":"arxiv_version","alias_value":"2312.15051v2","created_at":"2026-07-05T08:18:47.405298+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2312.15051","created_at":"2026-07-05T08:18:47.405298+00:00"},{"alias_kind":"pith_short_12","alias_value":"LM36B34CQUDN","created_at":"2026-07-05T08:18:47.405298+00:00"},{"alias_kind":"pith_short_16","alias_value":"LM36B34CQUDNPUCB","created_at":"2026-07-05T08:18:47.405298+00:00"},{"alias_kind":"pith_short_8","alias_value":"LM36B34C","created_at":"2026-07-05T08:18:47.405298+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.10644","citing_title":"Regge factorization of tree-level QCD amplitudes using a minimal set of lightcone variables","ref_index":35,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G","json":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G.json","graph_json":"https://pith.science/api/pith-number/LM36B34CQUDNPUCBHY4LDQ6V6G/graph.json","events_json":"https://pith.science/api/pith-number/LM36B34CQUDNPUCBHY4LDQ6V6G/events.json","paper":"https://pith.science/paper/LM36B34C"},"agent_actions":{"view_html":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G","download_json":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G.json","view_paper":"https://pith.science/paper/LM36B34C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2312.15051&json=true","fetch_graph":"https://pith.science/api/pith-number/LM36B34CQUDNPUCBHY4LDQ6V6G/graph.json","fetch_events":"https://pith.science/api/pith-number/LM36B34CQUDNPUCBHY4LDQ6V6G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G/action/storage_attestation","attest_author":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G/action/author_attestation","sign_citation":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G/action/citation_signature","submit_replication":"https://pith.science/pith/LM36B34CQUDNPUCBHY4LDQ6V6G/action/replication_record"}},"created_at":"2026-07-05T08:18:47.405298+00:00","updated_at":"2026-07-05T08:18:47.405298+00:00"}