{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:P3RJ4OTWK2BJJ7IICO25G6G6CB","short_pith_number":"pith:P3RJ4OTW","schema_version":"1.0","canonical_sha256":"7ee29e3a76568294fd0813b5d378de1059e8d357ce9d9e1c57f41fb53c07b806","source":{"kind":"arxiv","id":"1805.05290","version":2},"attestation_state":"computed","paper":{"title":"Accessing the Gluon Sivers Function at a future Electron-Ion Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bo-Wen Xiao, E.C. Aschenauer, J.H. Lee, L. Zheng, Zhong-Bao Yin","submitted_at":"2018-05-14T17:00:53Z","abstract_excerpt":"In this work, we present a systematic study on the feasibility of probing the largely unexplored transverse momentum dependent gluon Sivers function (GSF) in open charm production, high p$_T$ charged di-hadron and di-jet production at a future high energy, high luminosity Electron-Ion Collider (EIC). The Sivers function is a measure for the anisotropy of the parton distributions in momentum space inside a transversely polarized nucleon. It is proposed that it can be studied through single spin asymmetries in the photon-gluon fusion subprocess in electron proton collisions at the EIC. Using a w"},"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":"1805.05290","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-05-14T17:00:53Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"96963d047af9d9478fd3f1627b01b667796e95293709123f7dd5efba353824bd","abstract_canon_sha256":"9636577fde5fd3a77846b825ac4fa8eeedccd39ea2bdfe5b1ea773336232260c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:07:32.526906Z","signature_b64":"UY996qQA+glpu1UwoT/iMYwVsLYYIFgIKJgyyCi++DBgoNd7wIWLNH68u/m0wvUz0tRa1MIX9IVQW3/hcNI/Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7ee29e3a76568294fd0813b5d378de1059e8d357ce9d9e1c57f41fb53c07b806","last_reissued_at":"2026-05-18T00:07:32.526068Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:07:32.526068Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Accessing the Gluon Sivers Function at a future Electron-Ion Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bo-Wen Xiao, E.C. Aschenauer, J.H. Lee, L. Zheng, Zhong-Bao Yin","submitted_at":"2018-05-14T17:00:53Z","abstract_excerpt":"In this work, we present a systematic study on the feasibility of probing the largely unexplored transverse momentum dependent gluon Sivers function (GSF) in open charm production, high p$_T$ charged di-hadron and di-jet production at a future high energy, high luminosity Electron-Ion Collider (EIC). The Sivers function is a measure for the anisotropy of the parton distributions in momentum space inside a transversely polarized nucleon. It is proposed that it can be studied through single spin asymmetries in the photon-gluon fusion subprocess in electron proton collisions at the EIC. Using a w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.05290","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":""},"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":"1805.05290","created_at":"2026-05-18T00:07:32.526214+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.05290v2","created_at":"2026-05-18T00:07:32.526214+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.05290","created_at":"2026-05-18T00:07:32.526214+00:00"},{"alias_kind":"pith_short_12","alias_value":"P3RJ4OTWK2BJ","created_at":"2026-05-18T12:32:43.782077+00:00"},{"alias_kind":"pith_short_16","alias_value":"P3RJ4OTWK2BJJ7II","created_at":"2026-05-18T12:32:43.782077+00:00"},{"alias_kind":"pith_short_8","alias_value":"P3RJ4OTW","created_at":"2026-05-18T12:32:43.782077+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2512.05199","citing_title":"Jet Charge with Global Event Shapes: Probing Quark Flavor Dynamics","ref_index":35,"is_internal_anchor":true},{"citing_arxiv_id":"2103.05419","citing_title":"Science Requirements and Detector Concepts for the Electron-Ion Collider: EIC Yellow Report","ref_index":16,"is_internal_anchor":true},{"citing_arxiv_id":"2605.07516","citing_title":"Collinear matching for leading power gluon transverse momentum distributions","ref_index":23,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB","json":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB.json","graph_json":"https://pith.science/api/pith-number/P3RJ4OTWK2BJJ7IICO25G6G6CB/graph.json","events_json":"https://pith.science/api/pith-number/P3RJ4OTWK2BJJ7IICO25G6G6CB/events.json","paper":"https://pith.science/paper/P3RJ4OTW"},"agent_actions":{"view_html":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB","download_json":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB.json","view_paper":"https://pith.science/paper/P3RJ4OTW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.05290&json=true","fetch_graph":"https://pith.science/api/pith-number/P3RJ4OTWK2BJJ7IICO25G6G6CB/graph.json","fetch_events":"https://pith.science/api/pith-number/P3RJ4OTWK2BJJ7IICO25G6G6CB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB/action/storage_attestation","attest_author":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB/action/author_attestation","sign_citation":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB/action/citation_signature","submit_replication":"https://pith.science/pith/P3RJ4OTWK2BJJ7IICO25G6G6CB/action/replication_record"}},"created_at":"2026-05-18T00:07:32.526214+00:00","updated_at":"2026-05-18T00:07:32.526214+00:00"}