{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:EYEBZVW6I6QOZBTT54G4COLX62","short_pith_number":"pith:EYEBZVW6","schema_version":"1.0","canonical_sha256":"26081cd6de47a0ec8673ef0dc13977f69eb5d0909d102308781589c38ac22cc7","source":{"kind":"arxiv","id":"1701.05241","version":1},"attestation_state":"computed","paper":{"title":"Two-parton scattering in the high-energy limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Einan Gardi, Leonardo Vernazza, Simon Caron-Huot","submitted_at":"2017-01-18T21:48:28Z","abstract_excerpt":"Considering $2\\to 2$ gauge-theory scattering with general colour in the high-energy limit, we compute the Regge-cut contribution to three loops through next-to-next-to-leading high-energy logarithms (NNLL) in the signature-odd sector. Our formalism is based on using the non-linear Balitsky-JIMWLK rapidity evolution equation to derive an effective Hamiltonian acting on states with a fixed number of Reggeized gluons. A new effect occurring first at NNLL is mixing between states with $k$ and $k+2$ Reggeized gluons due non-diagonal terms in this Hamiltonian. Our results are consistent with a recen"},"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":"1701.05241","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-01-18T21:48:28Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"0752314150b6e9bc33a906510e2d71fe11de67f9300a644ae8727f6c8ebfc37b","abstract_canon_sha256":"fe17576bb56bfe70929f15a710a8151c03066d1550be40d2a33fb1c8904a7430"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:41:37.482569Z","signature_b64":"NhMFz0zVLs09aEeunnEqCiGd+90tsWO1EJySxY5rq/F6dmhybFBJaFy0UPMmNK9E5UWLPdIpv1pfpB9YuL4HCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"26081cd6de47a0ec8673ef0dc13977f69eb5d0909d102308781589c38ac22cc7","last_reissued_at":"2026-05-18T00:41:37.481854Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:41:37.481854Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-parton scattering in the high-energy limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Einan Gardi, Leonardo Vernazza, Simon Caron-Huot","submitted_at":"2017-01-18T21:48:28Z","abstract_excerpt":"Considering $2\\to 2$ gauge-theory scattering with general colour in the high-energy limit, we compute the Regge-cut contribution to three loops through next-to-next-to-leading high-energy logarithms (NNLL) in the signature-odd sector. Our formalism is based on using the non-linear Balitsky-JIMWLK rapidity evolution equation to derive an effective Hamiltonian acting on states with a fixed number of Reggeized gluons. A new effect occurring first at NNLL is mixing between states with $k$ and $k+2$ Reggeized gluons due non-diagonal terms in this Hamiltonian. Our results are consistent with a recen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.05241","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":""},"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":"1701.05241","created_at":"2026-05-18T00:41:37.481979+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.05241v1","created_at":"2026-05-18T00:41:37.481979+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.05241","created_at":"2026-05-18T00:41:37.481979+00:00"},{"alias_kind":"pith_short_12","alias_value":"EYEBZVW6I6QO","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_16","alias_value":"EYEBZVW6I6QOZBTT","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_8","alias_value":"EYEBZVW6","created_at":"2026-05-18T12:31:12.930513+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.11457","citing_title":"Analytic structure of the high-energy gravitational amplitude: multi-H diagrams and classical 5PM logarithms","ref_index":75,"is_internal_anchor":true},{"citing_arxiv_id":"2604.19232","citing_title":"Progress on the soft anomalous dimension in QCD","ref_index":112,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62","json":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62.json","graph_json":"https://pith.science/api/pith-number/EYEBZVW6I6QOZBTT54G4COLX62/graph.json","events_json":"https://pith.science/api/pith-number/EYEBZVW6I6QOZBTT54G4COLX62/events.json","paper":"https://pith.science/paper/EYEBZVW6"},"agent_actions":{"view_html":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62","download_json":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62.json","view_paper":"https://pith.science/paper/EYEBZVW6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.05241&json=true","fetch_graph":"https://pith.science/api/pith-number/EYEBZVW6I6QOZBTT54G4COLX62/graph.json","fetch_events":"https://pith.science/api/pith-number/EYEBZVW6I6QOZBTT54G4COLX62/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62/action/storage_attestation","attest_author":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62/action/author_attestation","sign_citation":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62/action/citation_signature","submit_replication":"https://pith.science/pith/EYEBZVW6I6QOZBTT54G4COLX62/action/replication_record"}},"created_at":"2026-05-18T00:41:37.481979+00:00","updated_at":"2026-05-18T00:41:37.481979+00:00"}