{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:767VGLKIDE2FR27QBF3VEGN2SI","short_pith_number":"pith:767VGLKI","schema_version":"1.0","canonical_sha256":"ffbf532d48193458ebf009775219ba9236d9a87eac927ac69168838508a7fc47","source":{"kind":"arxiv","id":"2505.02711","version":2},"attestation_state":"computed","paper":{"title":"Transverse single-spin asymmetries in $\\gamma$SIDIS as a direct probe of quark-gluon-quark longitudinal momentum structure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alexei Prokudin, Daniel Pitonyak, Daniel Rein, Jack Putnam, Jacob Marsh, Marc Schlegel, Michael Harris","submitted_at":"2025-05-05T15:06:39Z","abstract_excerpt":"Transverse single-spin asymmetries in the semi-inclusive deep-inelastic production of isolated photons ($\\gamma$SIDIS), $A_{UT}^{\\gamma {\\rm SIDIS}}$, provide an unprecedented opportunity to extract the quark-gluon-quark correlators $F_{FT}(x,x')$ and $G_{FT}(x,x')$ point-by-point in their full support $x,x'$. We utilize realistic models for these functions, based on input from the Sivers transverse momentum dependent parton distribution function and imposing constraints from the $d_2$ matrix element calculated in lattice QCD, in order to provide numerical estimates for $A_{UT}^{\\gamma {\\rm SI"},"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":"2505.02711","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-05T15:06:39Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"6e3c3b7aa1d44935d6e647ab815813a0bd476ebb65f7eabaf4a177bf005fe2cd","abstract_canon_sha256":"9e93d2619f4b944e4e7bce7985c26bd6d3df436cd9b101efa5342b1eadcbe4a6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:57:20.403495Z","signature_b64":"XY7qbo9PCI830sB98syZZvAYiHhYTqvHj/IJlX94LsbRmD1G9+7EyH8ruGNHjeuEQWKMA6zU50EQQfgWODmoAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ffbf532d48193458ebf009775219ba9236d9a87eac927ac69168838508a7fc47","last_reissued_at":"2026-07-05T11:57:20.402970Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:57:20.402970Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transverse single-spin asymmetries in $\\gamma$SIDIS as a direct probe of quark-gluon-quark longitudinal momentum structure","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Alexei Prokudin, Daniel Pitonyak, Daniel Rein, Jack Putnam, Jacob Marsh, Marc Schlegel, Michael Harris","submitted_at":"2025-05-05T15:06:39Z","abstract_excerpt":"Transverse single-spin asymmetries in the semi-inclusive deep-inelastic production of isolated photons ($\\gamma$SIDIS), $A_{UT}^{\\gamma {\\rm SIDIS}}$, provide an unprecedented opportunity to extract the quark-gluon-quark correlators $F_{FT}(x,x')$ and $G_{FT}(x,x')$ point-by-point in their full support $x,x'$. We utilize realistic models for these functions, based on input from the Sivers transverse momentum dependent parton distribution function and imposing constraints from the $d_2$ matrix element calculated in lattice QCD, in order to provide numerical estimates for $A_{UT}^{\\gamma {\\rm SI"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.02711","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/2505.02711/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":"2505.02711","created_at":"2026-07-05T11:57:20.403029+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.02711v2","created_at":"2026-07-05T11:57:20.403029+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.02711","created_at":"2026-07-05T11:57:20.403029+00:00"},{"alias_kind":"pith_short_12","alias_value":"767VGLKIDE2F","created_at":"2026-07-05T11:57:20.403029+00:00"},{"alias_kind":"pith_short_16","alias_value":"767VGLKIDE2FR27Q","created_at":"2026-07-05T11:57:20.403029+00:00"},{"alias_kind":"pith_short_8","alias_value":"767VGLKI","created_at":"2026-07-05T11:57:20.403029+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI","json":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI.json","graph_json":"https://pith.science/api/pith-number/767VGLKIDE2FR27QBF3VEGN2SI/graph.json","events_json":"https://pith.science/api/pith-number/767VGLKIDE2FR27QBF3VEGN2SI/events.json","paper":"https://pith.science/paper/767VGLKI"},"agent_actions":{"view_html":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI","download_json":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI.json","view_paper":"https://pith.science/paper/767VGLKI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.02711&json=true","fetch_graph":"https://pith.science/api/pith-number/767VGLKIDE2FR27QBF3VEGN2SI/graph.json","fetch_events":"https://pith.science/api/pith-number/767VGLKIDE2FR27QBF3VEGN2SI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI/action/storage_attestation","attest_author":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI/action/author_attestation","sign_citation":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI/action/citation_signature","submit_replication":"https://pith.science/pith/767VGLKIDE2FR27QBF3VEGN2SI/action/replication_record"}},"created_at":"2026-07-05T11:57:20.403029+00:00","updated_at":"2026-07-05T11:57:20.403029+00:00"}