{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:JEDGUYVCLWZ74VF4X4TCVBNTR3","short_pith_number":"pith:JEDGUYVC","schema_version":"1.0","canonical_sha256":"49066a62a25db3fe54bcbf262a85b38ed15b3755ad72bf0af1dfd013e17dac9e","source":{"kind":"arxiv","id":"2512.14097","version":3},"attestation_state":"computed","paper":{"title":"The Nucleon Axial Form Factor from Elementary Target Data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"A. Klustov\\'a, A.L. Hart, A. Lozano, A.M. Gago, A. Olivier, A.S. Meyer, C.J. Solano Salinas, C. Pernas, D.A. Harris, D. Last, D. Ruterbories, D.S. Correia, E. Granados, G.A. D\\'iaz, G. Caceres, G.N. Perdue, H. Budd, H. Gallagher, H. Schellman, J. Felix, J. Kleykamp, J.K. Nelson, K.S. McFarland, L. Zazueta (The MINERvA Collaboration), M.A. Ram\\'irez, M. Betancourt, M. Kordosky, M. Moore, M.O. Wascko, M. Sajjad Athar, N.H. Vaughan, O. Moreno, P.K. Gaur, R.D. Ransome, R. Gran, R.J. Hill, S. Akhter, S. Manly, S.M. Gilligan, T. Cai, V. Paolone, W.A. Mann, Z. Ahmad Dar","submitted_at":"2025-12-16T05:12:25Z","abstract_excerpt":"Precise neutrino-nucleon amplitudes are essential ingredients for predicting neutrino event rates in current and upcoming long-baseline neutrino oscillation experiments. A common neutrino interaction with a low reaction threshold and with most of the energy carried by two final state particles is quasielastic scattering, for which the nucleon axial form factor, $F_{A}(Q^{2})$, is a dominant source of uncertainty. Improvements to the nucleon axial form factor rely on neutrino scattering data with elementary targets to reduce or eliminate the need for nuclear modeling systematics. This work exam"},"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":"2512.14097","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2025-12-16T05:12:25Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"f6438ae638bf3f1ccb859e88e7e296a8874072527910c05f93bf971948e9bcb7","abstract_canon_sha256":"b18264dc404838dd84e73d1b8db983e6a947cbdc11407eef061e328b1ea1f397"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-23T01:24:19.493875Z","signature_b64":"FbdNBuKpFlBHAJS/JdeH9Hyzset8ZAR2SCCM12FvfOWpHIKekmA24LK4e1+xScRx84AJLlRJiCrSn8/0jtRxAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49066a62a25db3fe54bcbf262a85b38ed15b3755ad72bf0af1dfd013e17dac9e","last_reissued_at":"2026-07-23T01:24:19.492954Z","signature_status":"signed_v1","first_computed_at":"2026-07-23T01:24:19.492954Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Nucleon Axial Form Factor from Elementary Target Data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"A. Klustov\\'a, A.L. Hart, A. Lozano, A.M. Gago, A. Olivier, A.S. Meyer, C.J. Solano Salinas, C. Pernas, D.A. Harris, D. Last, D. Ruterbories, D.S. Correia, E. Granados, G.A. D\\'iaz, G. Caceres, G.N. Perdue, H. Budd, H. Gallagher, H. Schellman, J. Felix, J. Kleykamp, J.K. Nelson, K.S. McFarland, L. Zazueta (The MINERvA Collaboration), M.A. Ram\\'irez, M. Betancourt, M. Kordosky, M. Moore, M.O. Wascko, M. Sajjad Athar, N.H. Vaughan, O. Moreno, P.K. Gaur, R.D. Ransome, R. Gran, R.J. Hill, S. Akhter, S. Manly, S.M. Gilligan, T. Cai, V. Paolone, W.A. Mann, Z. Ahmad Dar","submitted_at":"2025-12-16T05:12:25Z","abstract_excerpt":"Precise neutrino-nucleon amplitudes are essential ingredients for predicting neutrino event rates in current and upcoming long-baseline neutrino oscillation experiments. A common neutrino interaction with a low reaction threshold and with most of the energy carried by two final state particles is quasielastic scattering, for which the nucleon axial form factor, $F_{A}(Q^{2})$, is a dominant source of uncertainty. Improvements to the nucleon axial form factor rely on neutrino scattering data with elementary targets to reduce or eliminate the need for nuclear modeling systematics. This work exam"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2512.14097","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2512.14097/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":"2512.14097","created_at":"2026-07-23T01:24:19.493383+00:00"},{"alias_kind":"arxiv_version","alias_value":"2512.14097v3","created_at":"2026-07-23T01:24:19.493383+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2512.14097","created_at":"2026-07-23T01:24:19.493383+00:00"},{"alias_kind":"pith_short_12","alias_value":"JEDGUYVCLWZ7","created_at":"2026-07-23T01:24:19.493383+00:00"},{"alias_kind":"pith_short_16","alias_value":"JEDGUYVCLWZ74VF4","created_at":"2026-07-23T01:24:19.493383+00:00"},{"alias_kind":"pith_short_8","alias_value":"JEDGUYVC","created_at":"2026-07-23T01:24:19.493383+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":6,"sample":[{"citing_arxiv_id":"2606.30834","citing_title":"Extraction of the nucleon axial form factor from Lattice QCD using NNLO chiral perturbation theory","ref_index":12,"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":49,"is_internal_anchor":true},{"citing_arxiv_id":"2601.21155","citing_title":"Nucleon axial-vector form factor and radius from radiatively-corrected antineutrino scattering data","ref_index":24,"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":49,"is_internal_anchor":true},{"citing_arxiv_id":"2604.24925","citing_title":"Measurement of muon (anti-)neutrino charged-current quasielastic-like cross section using off-axis NuMI beam at ICARUS","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"2605.00756","citing_title":"Two-body current and axial form factor effects in charged-current quasielastic neutrino-nucleus scattering within the NEUT event generator","ref_index":18,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3","json":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3.json","graph_json":"https://pith.science/api/pith-number/JEDGUYVCLWZ74VF4X4TCVBNTR3/graph.json","events_json":"https://pith.science/api/pith-number/JEDGUYVCLWZ74VF4X4TCVBNTR3/events.json","paper":"https://pith.science/paper/JEDGUYVC"},"agent_actions":{"view_html":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3","download_json":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3.json","view_paper":"https://pith.science/paper/JEDGUYVC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2512.14097&json=true","fetch_graph":"https://pith.science/api/pith-number/JEDGUYVCLWZ74VF4X4TCVBNTR3/graph.json","fetch_events":"https://pith.science/api/pith-number/JEDGUYVCLWZ74VF4X4TCVBNTR3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3/action/storage_attestation","attest_author":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3/action/author_attestation","sign_citation":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3/action/citation_signature","submit_replication":"https://pith.science/pith/JEDGUYVCLWZ74VF4X4TCVBNTR3/action/replication_record"}},"created_at":"2026-07-23T01:24:19.493383+00:00","updated_at":"2026-07-23T01:24:19.493383+00:00"}