{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:6LMI24YGCWJEPLVXTXXZPWYMOZ","short_pith_number":"pith:6LMI24YG","schema_version":"1.0","canonical_sha256":"f2d88d7306159247aeb79def97db0c767585982bc6e745627f073b0c1bb73f8f","source":{"kind":"arxiv","id":"2505.23487","version":1},"attestation_state":"computed","paper":{"title":"Factorized QED and QCD Contribution to Deeply Inelastic Scattering","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Jian-Wei Qiu, Jia-Yue Zhang, Justin Cammarota, Kazuhiro Watanabe","submitted_at":"2025-05-29T14:35:55Z","abstract_excerpt":"We present the first calculation of next-to-leading order (NLO) factorized QED and QCD contributions to the short-distance hard coefficients of inclusive lepton-hadron deep inelastic scattering (DIS) in a joint QED and QCD factorization approach. Unlike the traditional radiative correction approach to handle the collision-induced QED contributions to DIS, QED radiation from all charged leptons and quarks are treated equally, and their collinear sensitivities are systematically factorized into corresponding universal lepton and parton distribution functions. We demonstrate that the NLO factoriz"},"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":"2505.23487","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-ph","submitted_at":"2025-05-29T14:35:55Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"3c25ac824e801fbd5f2bcfe3e290d388ce95a070ed01c63068c2b749f5a62c21","abstract_canon_sha256":"662df7be9234738bf548de09341d6f72cee59ce3e8abf2c73d04d81f17097196"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:12:02.842193Z","signature_b64":"LUYAkRrvt+FpHo0RuIbFUrNpDcprB5wokezf+fwuB4iNWktqlJKqeBP43RUMtzOYFEG9hKPcBQFgyUQdj+4rCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2d88d7306159247aeb79def97db0c767585982bc6e745627f073b0c1bb73f8f","last_reissued_at":"2026-07-05T11:12:02.841677Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:12:02.841677Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Factorized QED and QCD Contribution to Deeply Inelastic Scattering","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Jian-Wei Qiu, Jia-Yue Zhang, Justin Cammarota, Kazuhiro Watanabe","submitted_at":"2025-05-29T14:35:55Z","abstract_excerpt":"We present the first calculation of next-to-leading order (NLO) factorized QED and QCD contributions to the short-distance hard coefficients of inclusive lepton-hadron deep inelastic scattering (DIS) in a joint QED and QCD factorization approach. Unlike the traditional radiative correction approach to handle the collision-induced QED contributions to DIS, QED radiation from all charged leptons and quarks are treated equally, and their collinear sensitivities are systematically factorized into corresponding universal lepton and parton distribution functions. We demonstrate that the NLO factoriz"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.23487","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/2505.23487/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":"2505.23487","created_at":"2026-07-05T11:12:02.841738+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.23487v1","created_at":"2026-07-05T11:12:02.841738+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.23487","created_at":"2026-07-05T11:12:02.841738+00:00"},{"alias_kind":"pith_short_12","alias_value":"6LMI24YGCWJE","created_at":"2026-07-05T11:12:02.841738+00:00"},{"alias_kind":"pith_short_16","alias_value":"6LMI24YGCWJEPLVX","created_at":"2026-07-05T11:12:02.841738+00:00"},{"alias_kind":"pith_short_8","alias_value":"6LMI24YG","created_at":"2026-07-05T11:12:02.841738+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2607.07811","citing_title":"Impact of QED Radiation on SMEFT Constraints in Deep Inelastic Scattering","ref_index":45,"is_internal_anchor":true},{"citing_arxiv_id":"2607.07908","citing_title":"QCD for electroweak precision measurements: Foundations","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2607.07664","citing_title":"Single inclusive hadron and jet production in lepton-hadron scattering","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2606.26056","citing_title":"Impact of parity-violating deep-inelastic scattering on the weak mixing angle and high-$x$ parton distributions","ref_index":96,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ","json":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ.json","graph_json":"https://pith.science/api/pith-number/6LMI24YGCWJEPLVXTXXZPWYMOZ/graph.json","events_json":"https://pith.science/api/pith-number/6LMI24YGCWJEPLVXTXXZPWYMOZ/events.json","paper":"https://pith.science/paper/6LMI24YG"},"agent_actions":{"view_html":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ","download_json":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ.json","view_paper":"https://pith.science/paper/6LMI24YG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.23487&json=true","fetch_graph":"https://pith.science/api/pith-number/6LMI24YGCWJEPLVXTXXZPWYMOZ/graph.json","fetch_events":"https://pith.science/api/pith-number/6LMI24YGCWJEPLVXTXXZPWYMOZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ/action/storage_attestation","attest_author":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ/action/author_attestation","sign_citation":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ/action/citation_signature","submit_replication":"https://pith.science/pith/6LMI24YGCWJEPLVXTXXZPWYMOZ/action/replication_record"}},"created_at":"2026-07-05T11:12:02.841738+00:00","updated_at":"2026-07-05T11:12:02.841738+00:00"}