{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:QYNNQVX4B4GXTL65FYLMUMCTI5","short_pith_number":"pith:QYNNQVX4","schema_version":"1.0","canonical_sha256":"861ad856fc0f0d79afdd2e16ca3053474ad46dbd8a2a088f89e9a3fe30f2e37a","source":{"kind":"arxiv","id":"2001.00765","version":2},"attestation_state":"computed","paper":{"title":"Photoproduction of three jets in the CGC: gluon TMDs and dilute limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cyrille Marquet, Pieter Taels, Renaud Boussarie, Tolga Altinoluk","submitted_at":"2020-01-03T09:12:35Z","abstract_excerpt":"We study the process $\\gamma A \\to q \\bar{q} g+X$ in the Color Glass Condensate (CGC) effective theory. After obtaining the cross section, we consider two kinematic limits which are encompassed in our result. In the so-called correlation limit, the vector sum of the transverse momenta of the three outgoing particles is small with respect to the individual transverse momenta; the cross section then simplifies considerably and can be written in a factorized form, sensitive to both the unpolarized and linearly-polarized Weizs\\\"acker-Williams transverse momentum dependent gluon distribution functi"},"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":"2001.00765","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2020-01-03T09:12:35Z","cross_cats_sorted":[],"title_canon_sha256":"767b835ad5544c906b22bed2130756ab531e3035e8711945b4e237deb6809511","abstract_canon_sha256":"bdbb823a94f3f85d2c055f65f22bb8cc6c2a774c38b7b922e00869f81c50c312"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:41:29.694835Z","signature_b64":"a3LVf+KZckH9x60v5YziINAWVNKxfyxMhga/KvkHccyPjN5E/MHIQlegedEz81OhtJKI1oPZfGiCxEDBvrxAAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"861ad856fc0f0d79afdd2e16ca3053474ad46dbd8a2a088f89e9a3fe30f2e37a","last_reissued_at":"2026-07-05T01:41:29.694301Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:41:29.694301Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Photoproduction of three jets in the CGC: gluon TMDs and dilute limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cyrille Marquet, Pieter Taels, Renaud Boussarie, Tolga Altinoluk","submitted_at":"2020-01-03T09:12:35Z","abstract_excerpt":"We study the process $\\gamma A \\to q \\bar{q} g+X$ in the Color Glass Condensate (CGC) effective theory. After obtaining the cross section, we consider two kinematic limits which are encompassed in our result. In the so-called correlation limit, the vector sum of the transverse momenta of the three outgoing particles is small with respect to the individual transverse momenta; the cross section then simplifies considerably and can be written in a factorized form, sensitive to both the unpolarized and linearly-polarized Weizs\\\"acker-Williams transverse momentum dependent gluon distribution functi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2001.00765","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/2001.00765/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":"2001.00765","created_at":"2026-07-05T01:41:29.694377+00:00"},{"alias_kind":"arxiv_version","alias_value":"2001.00765v2","created_at":"2026-07-05T01:41:29.694377+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2001.00765","created_at":"2026-07-05T01:41:29.694377+00:00"},{"alias_kind":"pith_short_12","alias_value":"QYNNQVX4B4GX","created_at":"2026-07-05T01:41:29.694377+00:00"},{"alias_kind":"pith_short_16","alias_value":"QYNNQVX4B4GXTL65","created_at":"2026-07-05T01:41:29.694377+00:00"},{"alias_kind":"pith_short_8","alias_value":"QYNNQVX4","created_at":"2026-07-05T01:41:29.694377+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.17993","citing_title":"From target to projectile: CSS evolution of quark TMD in different light-cone gauges","ref_index":46,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5","json":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5.json","graph_json":"https://pith.science/api/pith-number/QYNNQVX4B4GXTL65FYLMUMCTI5/graph.json","events_json":"https://pith.science/api/pith-number/QYNNQVX4B4GXTL65FYLMUMCTI5/events.json","paper":"https://pith.science/paper/QYNNQVX4"},"agent_actions":{"view_html":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5","download_json":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5.json","view_paper":"https://pith.science/paper/QYNNQVX4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2001.00765&json=true","fetch_graph":"https://pith.science/api/pith-number/QYNNQVX4B4GXTL65FYLMUMCTI5/graph.json","fetch_events":"https://pith.science/api/pith-number/QYNNQVX4B4GXTL65FYLMUMCTI5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5/action/storage_attestation","attest_author":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5/action/author_attestation","sign_citation":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5/action/citation_signature","submit_replication":"https://pith.science/pith/QYNNQVX4B4GXTL65FYLMUMCTI5/action/replication_record"}},"created_at":"2026-07-05T01:41:29.694377+00:00","updated_at":"2026-07-05T01:41:29.694377+00:00"}