{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:K72Z36PSRT64HRVGZLBXG3U4GH","short_pith_number":"pith:K72Z36PS","schema_version":"1.0","canonical_sha256":"57f59df9f28cfdc3c6a6cac3736e9c31f942316e0269b126d3bd9815233776d0","source":{"kind":"arxiv","id":"2402.05465","version":1},"attestation_state":"computed","paper":{"title":"Revisiting azimuthal angular asymmetries in diffractive di-jet production","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cheng Zhang, Ding Yu Shao, Jian Zhou, Ya-Jin Zhou, Yu Shi","submitted_at":"2024-02-08T07:55:10Z","abstract_excerpt":"We explore the impact of initial state soft gluon radiations on the azimuthal angle asymmetries in photo-production of hard di-jet via coherent diffraction in ultraperipheral heavy ion collisions, as well as in electron-proton ($ep$) and electron-nucleus ($eA$) collisions. The primary production mechanism is identified as the diffractive production of two hard jets, accompanied by a collinear gluon emission along the beam direction. In contrast, the diffractive exclusive di-jet production, where the initial state radiation is absent, is suppressed due to color transparency. Our analysis shows "},"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":"2402.05465","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-08T07:55:10Z","cross_cats_sorted":[],"title_canon_sha256":"f3c9a0f920fe04f42d572cccc4785233af796f15369fe34d41d04f18cf1198ee","abstract_canon_sha256":"e2693972a4a1bcef64e405277a97cfc3c2dec2bc0f47d10a4fdc405f0e04dcea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:42:50.730217Z","signature_b64":"R96G18K6V6sfCRVvUxD6h3QSJIBTo8QLwglmQ0kfCYdNjQ/coIj7Ddr6ErL528CQqaobQ/8Jv6mwQz+JmvudBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"57f59df9f28cfdc3c6a6cac3736e9c31f942316e0269b126d3bd9815233776d0","last_reissued_at":"2026-07-05T07:42:50.729573Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:42:50.729573Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Revisiting azimuthal angular asymmetries in diffractive di-jet production","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Cheng Zhang, Ding Yu Shao, Jian Zhou, Ya-Jin Zhou, Yu Shi","submitted_at":"2024-02-08T07:55:10Z","abstract_excerpt":"We explore the impact of initial state soft gluon radiations on the azimuthal angle asymmetries in photo-production of hard di-jet via coherent diffraction in ultraperipheral heavy ion collisions, as well as in electron-proton ($ep$) and electron-nucleus ($eA$) collisions. The primary production mechanism is identified as the diffractive production of two hard jets, accompanied by a collinear gluon emission along the beam direction. In contrast, the diffractive exclusive di-jet production, where the initial state radiation is absent, is suppressed due to color transparency. Our analysis shows "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.05465","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/2402.05465/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":"2402.05465","created_at":"2026-07-05T07:42:50.729666+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.05465v1","created_at":"2026-07-05T07:42:50.729666+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.05465","created_at":"2026-07-05T07:42:50.729666+00:00"},{"alias_kind":"pith_short_12","alias_value":"K72Z36PSRT64","created_at":"2026-07-05T07:42:50.729666+00:00"},{"alias_kind":"pith_short_16","alias_value":"K72Z36PSRT64HRVG","created_at":"2026-07-05T07:42:50.729666+00:00"},{"alias_kind":"pith_short_8","alias_value":"K72Z36PS","created_at":"2026-07-05T07:42:50.729666+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.22871","citing_title":"Twisting Small-$x$ Gluon Tomography with Orbital Angular Momentum","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02230","citing_title":"Azimuthal decorrelation in diffractive dijet production","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2605.28747","citing_title":"Maximum phase-space density of linearly polarized gluon TMDs in the saturation region","ref_index":33,"is_internal_anchor":false},{"citing_arxiv_id":"2605.01527","citing_title":"Probing Saturation Effect in Heavy Meson Pair Correlation in Forward $pA$ Collisions","ref_index":81,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH","json":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH.json","graph_json":"https://pith.science/api/pith-number/K72Z36PSRT64HRVGZLBXG3U4GH/graph.json","events_json":"https://pith.science/api/pith-number/K72Z36PSRT64HRVGZLBXG3U4GH/events.json","paper":"https://pith.science/paper/K72Z36PS"},"agent_actions":{"view_html":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH","download_json":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH.json","view_paper":"https://pith.science/paper/K72Z36PS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.05465&json=true","fetch_graph":"https://pith.science/api/pith-number/K72Z36PSRT64HRVGZLBXG3U4GH/graph.json","fetch_events":"https://pith.science/api/pith-number/K72Z36PSRT64HRVGZLBXG3U4GH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH/action/storage_attestation","attest_author":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH/action/author_attestation","sign_citation":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH/action/citation_signature","submit_replication":"https://pith.science/pith/K72Z36PSRT64HRVGZLBXG3U4GH/action/replication_record"}},"created_at":"2026-07-05T07:42:50.729666+00:00","updated_at":"2026-07-05T07:42:50.729666+00:00"}