{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:5GZ2EXO3C4VRQTXY3UA5KZZEV4","short_pith_number":"pith:5GZ2EXO3","schema_version":"1.0","canonical_sha256":"e9b3a25ddb172b184ef8dd01d56724af2819252127307be9f29adf8be671e71e","source":{"kind":"arxiv","id":"2211.10899","version":2},"attestation_state":"computed","paper":{"title":"Semi-inclusive deeply inelastic neutrino and antineutrino nucleus scattering","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"W. Yang, X. Yang","submitted_at":"2022-11-20T08:08:50Z","abstract_excerpt":"The (anti)neutrino nucleus scattering plays a very important role in probing the hadronic structure as well as the electroweak phenomenologies. To this end, we calculate the jet production semi-inclusive deeply inelastic (anti)neutrino nucleus scattering process. The initial (anti)neutrino is assumed to be scattered off by a target particle with spin 1. Due to the limitation of the factorization theorem, calculations are carried out in the quantum chromodynamics parton model framework up to tree level twist-3. We consider both the neutral current and the charged current processes and write the"},"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":"2211.10899","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"hep-ph","submitted_at":"2022-11-20T08:08:50Z","cross_cats_sorted":[],"title_canon_sha256":"c498e9fc2dd820e6f29d3f69e1165004d558959dd0dc71b654bc34032a63f8f0","abstract_canon_sha256":"d57eb005278e973c060c14eae3628b7769abbe2b1877ae518bce3f5f916f1e1b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:15:18.326785Z","signature_b64":"737gEV59eS27QrbwU8krimonDRz0EJaFGexSFf/++E6DPJ2v7HS01HdeK7G/4MDf1agSvqlP2JviiaSpFC/KBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e9b3a25ddb172b184ef8dd01d56724af2819252127307be9f29adf8be671e71e","last_reissued_at":"2026-07-05T06:15:18.326311Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:15:18.326311Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Semi-inclusive deeply inelastic neutrino and antineutrino nucleus scattering","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"W. Yang, X. Yang","submitted_at":"2022-11-20T08:08:50Z","abstract_excerpt":"The (anti)neutrino nucleus scattering plays a very important role in probing the hadronic structure as well as the electroweak phenomenologies. To this end, we calculate the jet production semi-inclusive deeply inelastic (anti)neutrino nucleus scattering process. The initial (anti)neutrino is assumed to be scattered off by a target particle with spin 1. Due to the limitation of the factorization theorem, calculations are carried out in the quantum chromodynamics parton model framework up to tree level twist-3. We consider both the neutral current and the charged current processes and write the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.10899","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/2211.10899/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":"2211.10899","created_at":"2026-07-05T06:15:18.326380+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.10899v2","created_at":"2026-07-05T06:15:18.326380+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.10899","created_at":"2026-07-05T06:15:18.326380+00:00"},{"alias_kind":"pith_short_12","alias_value":"5GZ2EXO3C4VR","created_at":"2026-07-05T06:15:18.326380+00:00"},{"alias_kind":"pith_short_16","alias_value":"5GZ2EXO3C4VRQTXY","created_at":"2026-07-05T06:15:18.326380+00:00"},{"alias_kind":"pith_short_8","alias_value":"5GZ2EXO3","created_at":"2026-07-05T06:15:18.326380+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.18080","citing_title":"Hadron production in the charged current semi-inclusive deeply inelastic scattering of $N=Z$ nuclei","ref_index":24,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4","json":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4.json","graph_json":"https://pith.science/api/pith-number/5GZ2EXO3C4VRQTXY3UA5KZZEV4/graph.json","events_json":"https://pith.science/api/pith-number/5GZ2EXO3C4VRQTXY3UA5KZZEV4/events.json","paper":"https://pith.science/paper/5GZ2EXO3"},"agent_actions":{"view_html":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4","download_json":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4.json","view_paper":"https://pith.science/paper/5GZ2EXO3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.10899&json=true","fetch_graph":"https://pith.science/api/pith-number/5GZ2EXO3C4VRQTXY3UA5KZZEV4/graph.json","fetch_events":"https://pith.science/api/pith-number/5GZ2EXO3C4VRQTXY3UA5KZZEV4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4/action/storage_attestation","attest_author":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4/action/author_attestation","sign_citation":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4/action/citation_signature","submit_replication":"https://pith.science/pith/5GZ2EXO3C4VRQTXY3UA5KZZEV4/action/replication_record"}},"created_at":"2026-07-05T06:15:18.326380+00:00","updated_at":"2026-07-05T06:15:18.326380+00:00"}