{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:NCNUQBBYRYI6L3ZXSX3WD7BDPQ","short_pith_number":"pith:NCNUQBBY","schema_version":"1.0","canonical_sha256":"689b4804388e11e5ef3795f761fc237c36847d74b5e503b7faf885037d06799e","source":{"kind":"arxiv","id":"2401.00931","version":3},"attestation_state":"computed","paper":{"title":"A Collinear Perspective on the Regge Limit","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"AnJie Gao, Gregory Ridgway, Iain W. Stewart, Ian Moult, Sanjay Raman","submitted_at":"2024-01-01T19:00:00Z","abstract_excerpt":"The high energy (Regge) limit provides a playground for understanding all loop structures of scattering amplitudes, and plays an important role in the description of many phenomenologically relevant cross-sections. While well understood in the planar limit, the structure of non-planar corrections introduces many fascinating complexities, for which a general organizing principle is still lacking. We study the structure of multi-reggeon exchanges in the context of the effective field theory for forward scattering, and derive their factorization into collinear operators (impact factors) and soft "},"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":"2401.00931","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-01-01T19:00:00Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"199262c4975b3f5b8af90795cd22acc2c5f0aa561673a33c08595f522292a255","abstract_canon_sha256":"175bc3c5030c0da24648be2234e1bcba279c09032a81871e95cb0d889ae1ab85"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:00:56.951926Z","signature_b64":"fs0Qu3MieJAHeL5HV/rxne2nNnhPIcmcwyDbuHB1AdfVz08u9VfzuXXY2DUmxOOH95aUnFWOzeGeJ/0eX9zKAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"689b4804388e11e5ef3795f761fc237c36847d74b5e503b7faf885037d06799e","last_reissued_at":"2026-07-05T09:00:56.951442Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:00:56.951442Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Collinear Perspective on the Regge Limit","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"AnJie Gao, Gregory Ridgway, Iain W. Stewart, Ian Moult, Sanjay Raman","submitted_at":"2024-01-01T19:00:00Z","abstract_excerpt":"The high energy (Regge) limit provides a playground for understanding all loop structures of scattering amplitudes, and plays an important role in the description of many phenomenologically relevant cross-sections. While well understood in the planar limit, the structure of non-planar corrections introduces many fascinating complexities, for which a general organizing principle is still lacking. We study the structure of multi-reggeon exchanges in the context of the effective field theory for forward scattering, and derive their factorization into collinear operators (impact factors) and soft "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.00931","kind":"arxiv","version":3},"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/2401.00931/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":"2401.00931","created_at":"2026-07-05T09:00:56.951500+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.00931v3","created_at":"2026-07-05T09:00:56.951500+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.00931","created_at":"2026-07-05T09:00:56.951500+00:00"},{"alias_kind":"pith_short_12","alias_value":"NCNUQBBYRYI6","created_at":"2026-07-05T09:00:56.951500+00:00"},{"alias_kind":"pith_short_16","alias_value":"NCNUQBBYRYI6L3ZX","created_at":"2026-07-05T09:00:56.951500+00:00"},{"alias_kind":"pith_short_8","alias_value":"NCNUQBBY","created_at":"2026-07-05T09:00:56.951500+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07788","citing_title":"Factorization of elastic, single, and double diffractive $pp$ scattering","ref_index":68,"is_internal_anchor":true},{"citing_arxiv_id":"2606.25685","citing_title":"Quark Reggeization in QCD from the Wilson line formalism","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2511.11457","citing_title":"Analytic structure of the high-energy gravitational amplitude: multi-H diagrams and classical 5PM logarithms","ref_index":57,"is_internal_anchor":false},{"citing_arxiv_id":"2605.18544","citing_title":"The Classical Gravitational Impulse at High Energies","ref_index":45,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ","json":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ.json","graph_json":"https://pith.science/api/pith-number/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/graph.json","events_json":"https://pith.science/api/pith-number/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/events.json","paper":"https://pith.science/paper/NCNUQBBY"},"agent_actions":{"view_html":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ","download_json":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ.json","view_paper":"https://pith.science/paper/NCNUQBBY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.00931&json=true","fetch_graph":"https://pith.science/api/pith-number/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/graph.json","fetch_events":"https://pith.science/api/pith-number/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/action/storage_attestation","attest_author":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/action/author_attestation","sign_citation":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/action/citation_signature","submit_replication":"https://pith.science/pith/NCNUQBBYRYI6L3ZXSX3WD7BDPQ/action/replication_record"}},"created_at":"2026-07-05T09:00:56.951500+00:00","updated_at":"2026-07-05T09:00:56.951500+00:00"}