{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:UFQAF2SYP4V3WWHWAIPSCWZJDQ","short_pith_number":"pith:UFQAF2SY","schema_version":"1.0","canonical_sha256":"a16002ea587f2bbb58f6021f215b291c164e0f424070dc44c49e392b03aa4900","source":{"kind":"arxiv","id":"hep-ph/0307023","version":2},"attestation_state":"computed","paper":{"title":"Target Mass Corrections to Electro-Weak Structure Functions and Perturbative Neutrino Cross Sections","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M.H. Reno (Iowa U.), S. Kretzer (Brookhaven & RIKEN BNL)","submitted_at":"2003-07-01T18:11:05Z","abstract_excerpt":"We provide a complete and consistent framework to include subasymptotic perturbative as well as mass corrections to the leading twist (tau=2) evaluation of charged and neutral current weak structure functions and the perturbative neutrino cross sections. We revisit previous calculations in a modern language and fill in the gaps that we find missing for a complete and ready-to-use \"NLO xi-scaling\" formulary. In particular, as a new result we formulate the mixing of the partonic and hadronic structure function tensor basis in the operator approach to deep inelastic scattering. As an underlying f"},"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":"hep-ph/0307023","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-07-01T18:11:05Z","cross_cats_sorted":[],"title_canon_sha256":"d2bfb6fe4200df13a8468978f58c52a13f758ec26be2c60b2e552fe9e2c74b66","abstract_canon_sha256":"c3b9a68e20af2d41b93034353de6f61c90099e282a510ba9de9bedeb398f5823"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:40:48.089342Z","signature_b64":"mLVw8RlO/7WkpJLILV261hLpLNNH0ZN4KnmzNLOBcwbA6MV3kcYIqWongltY8jhkBR8/vy0y+FhCU2dgccPODw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a16002ea587f2bbb58f6021f215b291c164e0f424070dc44c49e392b03aa4900","last_reissued_at":"2026-07-04T16:40:48.088943Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:40:48.088943Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Target Mass Corrections to Electro-Weak Structure Functions and Perturbative Neutrino Cross Sections","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M.H. Reno (Iowa U.), S. Kretzer (Brookhaven & RIKEN BNL)","submitted_at":"2003-07-01T18:11:05Z","abstract_excerpt":"We provide a complete and consistent framework to include subasymptotic perturbative as well as mass corrections to the leading twist (tau=2) evaluation of charged and neutral current weak structure functions and the perturbative neutrino cross sections. We revisit previous calculations in a modern language and fill in the gaps that we find missing for a complete and ready-to-use \"NLO xi-scaling\" formulary. In particular, as a new result we formulate the mixing of the partonic and hadronic structure function tensor basis in the operator approach to deep inelastic scattering. As an underlying f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0307023","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/hep-ph/0307023/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":"hep-ph/0307023","created_at":"2026-07-04T16:40:48.089009+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0307023v2","created_at":"2026-07-04T16:40:48.089009+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0307023","created_at":"2026-07-04T16:40:48.089009+00:00"},{"alias_kind":"pith_short_12","alias_value":"UFQAF2SYP4V3","created_at":"2026-07-04T16:40:48.089009+00:00"},{"alias_kind":"pith_short_16","alias_value":"UFQAF2SYP4V3WWHW","created_at":"2026-07-04T16:40:48.089009+00:00"},{"alias_kind":"pith_short_8","alias_value":"UFQAF2SY","created_at":"2026-07-04T16:40:48.089009+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.26260","citing_title":"Letter of Intent: The Forward Physics Facility","ref_index":68,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ","json":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ.json","graph_json":"https://pith.science/api/pith-number/UFQAF2SYP4V3WWHWAIPSCWZJDQ/graph.json","events_json":"https://pith.science/api/pith-number/UFQAF2SYP4V3WWHWAIPSCWZJDQ/events.json","paper":"https://pith.science/paper/UFQAF2SY"},"agent_actions":{"view_html":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ","download_json":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ.json","view_paper":"https://pith.science/paper/UFQAF2SY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0307023&json=true","fetch_graph":"https://pith.science/api/pith-number/UFQAF2SYP4V3WWHWAIPSCWZJDQ/graph.json","fetch_events":"https://pith.science/api/pith-number/UFQAF2SYP4V3WWHWAIPSCWZJDQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ/action/storage_attestation","attest_author":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ/action/author_attestation","sign_citation":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ/action/citation_signature","submit_replication":"https://pith.science/pith/UFQAF2SYP4V3WWHWAIPSCWZJDQ/action/replication_record"}},"created_at":"2026-07-04T16:40:48.089009+00:00","updated_at":"2026-07-04T16:40:48.089009+00:00"}