{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:ICV7MTLB7SIABORX36JC6BDXQL","short_pith_number":"pith:ICV7MTLB","schema_version":"1.0","canonical_sha256":"40abf64d61fc9000ba37df922f047782e39d2c6675f55f7ca53cc7a2d70ea626","source":{"kind":"arxiv","id":"nucl-th/0408005","version":3},"attestation_state":"computed","paper":{"title":"Inclusive Quasi-Elastic Charged-Current Neutrino-Nucleus Reactions","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"J.E. Amaro, J. Nieves, M. Valverde","submitted_at":"2004-08-01T06:34:14Z","abstract_excerpt":"The Quasi-Elastic (QE) contribution of the nuclear inclusive electron scattering model developed in Nucl. Phys. A627 (1997) 543 is extended to the study of electroweak Charged Current (CC) induced nuclear reactions, at intermediate energies of interest for future neutrino oscillation experiments. The model accounts for, among other nuclear effects, long range nuclear (RPA) correlations, Final State Interaction (FSI) and Coulomb corrections. Predictions for the inclusive muon capture in $^{12}$C and the reaction $^{12}$C $(\\nu_\\mu,\\mu^-)X$ near threshold are also given. RPA correlations are sho"},"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":"nucl-th/0408005","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2004-08-01T06:34:14Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"c0439ae73ae6db75fd205220c6ae080d4ff519b3951cfd4a99f49c3a5fd6756a","abstract_canon_sha256":"b7b79840fb1a272a352d8b8a41d192d3fd8797daf90872d7a1bc936619a55a42"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:32.016299Z","signature_b64":"IqfDaQPUs/PH4pBAab7jnadFz6AlAbueCEuQPRylLGYPhJ/9BpPdnVTrQ7201GJu2bPj/6Uktgeh/hxyAtlBAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"40abf64d61fc9000ba37df922f047782e39d2c6675f55f7ca53cc7a2d70ea626","last_reissued_at":"2026-05-18T02:35:32.015940Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:32.015940Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inclusive Quasi-Elastic Charged-Current Neutrino-Nucleus Reactions","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"J.E. Amaro, J. Nieves, M. Valverde","submitted_at":"2004-08-01T06:34:14Z","abstract_excerpt":"The Quasi-Elastic (QE) contribution of the nuclear inclusive electron scattering model developed in Nucl. Phys. A627 (1997) 543 is extended to the study of electroweak Charged Current (CC) induced nuclear reactions, at intermediate energies of interest for future neutrino oscillation experiments. The model accounts for, among other nuclear effects, long range nuclear (RPA) correlations, Final State Interaction (FSI) and Coulomb corrections. Predictions for the inclusive muon capture in $^{12}$C and the reaction $^{12}$C $(\\nu_\\mu,\\mu^-)X$ near threshold are also given. RPA correlations are sho"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0408005","kind":"arxiv","version":3},"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":"nucl-th/0408005","created_at":"2026-05-18T02:35:32.015991+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0408005v3","created_at":"2026-05-18T02:35:32.015991+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0408005","created_at":"2026-05-18T02:35:32.015991+00:00"},{"alias_kind":"pith_short_12","alias_value":"ICV7MTLB7SIA","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_16","alias_value":"ICV7MTLB7SIABORX","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_8","alias_value":"ICV7MTLB","created_at":"2026-05-18T12:25:52.687210+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"1906.10576","citing_title":"Elastic hadron-nucleus scattering in neutrino-nucleus reactions and transverse kinematics measurements","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2605.14196","citing_title":"Benchmarking State-of-the-Art Theory and Empirical Models of Pionless Neutrino-Argon Scattering in GENIE","ref_index":52,"is_internal_anchor":true},{"citing_arxiv_id":"2605.14196","citing_title":"Benchmarking State-of-the-Art Theory and Empirical Models of Pionless Neutrino-Argon Scattering in GENIE","ref_index":23,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL","json":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL.json","graph_json":"https://pith.science/api/pith-number/ICV7MTLB7SIABORX36JC6BDXQL/graph.json","events_json":"https://pith.science/api/pith-number/ICV7MTLB7SIABORX36JC6BDXQL/events.json","paper":"https://pith.science/paper/ICV7MTLB"},"agent_actions":{"view_html":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL","download_json":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL.json","view_paper":"https://pith.science/paper/ICV7MTLB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0408005&json=true","fetch_graph":"https://pith.science/api/pith-number/ICV7MTLB7SIABORX36JC6BDXQL/graph.json","fetch_events":"https://pith.science/api/pith-number/ICV7MTLB7SIABORX36JC6BDXQL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL/action/storage_attestation","attest_author":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL/action/author_attestation","sign_citation":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL/action/citation_signature","submit_replication":"https://pith.science/pith/ICV7MTLB7SIABORX36JC6BDXQL/action/replication_record"}},"created_at":"2026-05-18T02:35:32.015991+00:00","updated_at":"2026-05-18T02:35:32.015991+00:00"}