{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:FCDGDQBHRZPMKUZTUYUKJJIR6J","short_pith_number":"pith:FCDGDQBH","schema_version":"1.0","canonical_sha256":"288661c0278e5ec55333a628a4a511f24b43e55ff1e5e9b57aa358e50f934ee2","source":{"kind":"arxiv","id":"2411.09692","version":1},"attestation_state":"computed","paper":{"title":"Reggeization in Color","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":"2024-11-14T18:57:24Z","abstract_excerpt":"In the high energy limit, $s\\gg -t$, amplitudes in planar gauge theories Reggeize, with power law behavior $\\big( \\frac{s}{-t} \\big)^{\\alpha(t)}$ governed by the Regge trajectory $\\alpha(t)$. Beyond the planar limit this simplicity is violated by \"Regge cuts\", for which practical organizational principles are still being developed. We use a top-down effective field theory organization based on color projection in the $t$ channel and rapidity evolution equations for collinear impact factors, to sum large $s\\gg -t$ logarithms for Regge cut contributions. The results are matrix equations which ar"},"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":"2411.09692","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-11-14T18:57:24Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"a851f5de612f33b721391033422b2aec2269ae6a84cbc8550744d914e04a0e0f","abstract_canon_sha256":"e6928ec7d2c68d07c558dbc4244b2b99e4fab19c1a992c7d1cb5645ab732562c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:35:30.927956Z","signature_b64":"I2vPyHOcOkkmhJN0U2sN//nTO44OAptziMEHGy5HabTaBTXzh/Sb9Bq/AJhGHsin6g4mQxNvIT3VYjPaL+JxAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"288661c0278e5ec55333a628a4a511f24b43e55ff1e5e9b57aa358e50f934ee2","last_reissued_at":"2026-07-05T09:35:30.927492Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:35:30.927492Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Reggeization in Color","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":"2024-11-14T18:57:24Z","abstract_excerpt":"In the high energy limit, $s\\gg -t$, amplitudes in planar gauge theories Reggeize, with power law behavior $\\big( \\frac{s}{-t} \\big)^{\\alpha(t)}$ governed by the Regge trajectory $\\alpha(t)$. Beyond the planar limit this simplicity is violated by \"Regge cuts\", for which practical organizational principles are still being developed. We use a top-down effective field theory organization based on color projection in the $t$ channel and rapidity evolution equations for collinear impact factors, to sum large $s\\gg -t$ logarithms for Regge cut contributions. The results are matrix equations which ar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.09692","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/2411.09692/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":"2411.09692","created_at":"2026-07-05T09:35:30.927549+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.09692v1","created_at":"2026-07-05T09:35:30.927549+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.09692","created_at":"2026-07-05T09:35:30.927549+00:00"},{"alias_kind":"pith_short_12","alias_value":"FCDGDQBHRZPM","created_at":"2026-07-05T09:35:30.927549+00:00"},{"alias_kind":"pith_short_16","alias_value":"FCDGDQBHRZPMKUZT","created_at":"2026-07-05T09:35:30.927549+00:00"},{"alias_kind":"pith_short_8","alias_value":"FCDGDQBH","created_at":"2026-07-05T09:35:30.927549+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07788","citing_title":"Factorization of elastic, single, and double diffractive $pp$ scattering","ref_index":69,"is_internal_anchor":true},{"citing_arxiv_id":"2606.25685","citing_title":"Quark Reggeization in QCD from the Wilson line formalism","ref_index":49,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J","json":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J.json","graph_json":"https://pith.science/api/pith-number/FCDGDQBHRZPMKUZTUYUKJJIR6J/graph.json","events_json":"https://pith.science/api/pith-number/FCDGDQBHRZPMKUZTUYUKJJIR6J/events.json","paper":"https://pith.science/paper/FCDGDQBH"},"agent_actions":{"view_html":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J","download_json":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J.json","view_paper":"https://pith.science/paper/FCDGDQBH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.09692&json=true","fetch_graph":"https://pith.science/api/pith-number/FCDGDQBHRZPMKUZTUYUKJJIR6J/graph.json","fetch_events":"https://pith.science/api/pith-number/FCDGDQBHRZPMKUZTUYUKJJIR6J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J/action/storage_attestation","attest_author":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J/action/author_attestation","sign_citation":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J/action/citation_signature","submit_replication":"https://pith.science/pith/FCDGDQBHRZPMKUZTUYUKJJIR6J/action/replication_record"}},"created_at":"2026-07-05T09:35:30.927549+00:00","updated_at":"2026-07-05T09:35:30.927549+00:00"}