{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:5Q43MR5HETDLL6PCQAYWY7XFXY","short_pith_number":"pith:5Q43MR5H","schema_version":"1.0","canonical_sha256":"ec39b647a724c6b5f9e280316c7ee5be33d9edb66744520214ef61e4db38dada","source":{"kind":"arxiv","id":"2307.14920","version":2},"attestation_state":"computed","paper":{"title":"Confronting axial-vector form factor from lattice QCD with MINERvA antineutrino-proton data","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"Oleksandr Tomalak, Rajan Gupta, Tanmoy Bhattacharya","submitted_at":"2023-07-27T15:02:12Z","abstract_excerpt":"We compare recent MINERvA antineutrino-hydrogen charged-current measurements to phenomenological predictions of the axial-vector form factor based on fits to all available electron scattering and deuterium bubble-chamber data and to representative lattice-QCD (LQCD) determination by the PNDME Collaboration. While there is $1$--$2\\sigma$ agreement in the cross section with MINERvA data for each bin in $Q^2$, we identify three regions with different relevance and opportunity for LQCD predictions. For $Q^2 \\lesssim 0.2~\\mathrm{GeV}^2$, the phenomenological extractions have large number of data po"},"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":"2307.14920","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2023-07-27T15:02:12Z","cross_cats_sorted":["hep-ex","hep-ph","nucl-ex","nucl-th"],"title_canon_sha256":"ae7f5f776504aa9fa6310b3e2fd04020799f3fd36ca33087b73165dfdfb48d8d","abstract_canon_sha256":"b80b5f2854f5face109ff22c286f6957b5b6843b91abd1dac1f6cf9cb024106a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:04:18.378627Z","signature_b64":"McqjWkVkZNiPnQYW9sm5WCGQt5qmEaJak6NO1SGOfjjzgOdm7KIaFl1jc8fDWyxLV91kUoMqSQ9/TlZzQwEPAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec39b647a724c6b5f9e280316c7ee5be33d9edb66744520214ef61e4db38dada","last_reissued_at":"2026-07-05T07:04:18.378134Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:04:18.378134Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Confronting axial-vector form factor from lattice QCD with MINERvA antineutrino-proton data","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-ex","nucl-th"],"primary_cat":"hep-lat","authors_text":"Oleksandr Tomalak, Rajan Gupta, Tanmoy Bhattacharya","submitted_at":"2023-07-27T15:02:12Z","abstract_excerpt":"We compare recent MINERvA antineutrino-hydrogen charged-current measurements to phenomenological predictions of the axial-vector form factor based on fits to all available electron scattering and deuterium bubble-chamber data and to representative lattice-QCD (LQCD) determination by the PNDME Collaboration. While there is $1$--$2\\sigma$ agreement in the cross section with MINERvA data for each bin in $Q^2$, we identify three regions with different relevance and opportunity for LQCD predictions. For $Q^2 \\lesssim 0.2~\\mathrm{GeV}^2$, the phenomenological extractions have large number of data po"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.14920","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/2307.14920/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":"2307.14920","created_at":"2026-07-05T07:04:18.378191+00:00"},{"alias_kind":"arxiv_version","alias_value":"2307.14920v2","created_at":"2026-07-05T07:04:18.378191+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.14920","created_at":"2026-07-05T07:04:18.378191+00:00"},{"alias_kind":"pith_short_12","alias_value":"5Q43MR5HETDL","created_at":"2026-07-05T07:04:18.378191+00:00"},{"alias_kind":"pith_short_16","alias_value":"5Q43MR5HETDLL6PC","created_at":"2026-07-05T07:04:18.378191+00:00"},{"alias_kind":"pith_short_8","alias_value":"5Q43MR5H","created_at":"2026-07-05T07:04:18.378191+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2601.21155","citing_title":"Nucleon axial-vector form factor and radius from radiatively-corrected antineutrino scattering data","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06559","citing_title":"The strange and flavor-singlet axial form factors of the nucleon from lattice QCD","ref_index":16,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY","json":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY.json","graph_json":"https://pith.science/api/pith-number/5Q43MR5HETDLL6PCQAYWY7XFXY/graph.json","events_json":"https://pith.science/api/pith-number/5Q43MR5HETDLL6PCQAYWY7XFXY/events.json","paper":"https://pith.science/paper/5Q43MR5H"},"agent_actions":{"view_html":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY","download_json":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY.json","view_paper":"https://pith.science/paper/5Q43MR5H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2307.14920&json=true","fetch_graph":"https://pith.science/api/pith-number/5Q43MR5HETDLL6PCQAYWY7XFXY/graph.json","fetch_events":"https://pith.science/api/pith-number/5Q43MR5HETDLL6PCQAYWY7XFXY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY/action/storage_attestation","attest_author":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY/action/author_attestation","sign_citation":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY/action/citation_signature","submit_replication":"https://pith.science/pith/5Q43MR5HETDLL6PCQAYWY7XFXY/action/replication_record"}},"created_at":"2026-07-05T07:04:18.378191+00:00","updated_at":"2026-07-05T07:04:18.378191+00:00"}