{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:MRZTR5UN4ZBHAXFGPJJ3RAQEHX","short_pith_number":"pith:MRZTR5UN","schema_version":"1.0","canonical_sha256":"647338f68de642705ca67a53b882043df6483e96e3b723b22bb7808e1b4c9464","source":{"kind":"arxiv","id":"2305.11330","version":3},"attestation_state":"computed","paper":{"title":"Nucleon Isovector Axial Form Factors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-lat","authors_text":"Boram Yoon, Huey-Wen Lin, Rajan Gupta, Tanmoy Bhattacharya, Yong-Chull Jang","submitted_at":"2023-05-18T22:41:34Z","abstract_excerpt":"We present results for the isovector axial vector form factors obtained using thirteen 2+1+1-flavor highly improved staggered quark (HISQ) ensembles generated by the MILC collaboration. The calculation of nucleon two- and three-point correlation functions has been done using Wilson-clover fermions. In the analysis of these data, we quantify the sensitivity of the results to strategies used for removing excited state contamination and invoke the partially conserved axial current relation between the form factors to choose between them. Our data driven analysis includes removing contributions fr"},"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":"2305.11330","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2023-05-18T22:41:34Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"5d0fd4dc83531f029949ff5066a3b5bcf300d12ef6f57531182045924ceba66d","abstract_canon_sha256":"19c6ec2ecd350bcd344aec9dc18064261ac0c09f4246708923348bbc4a721601"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:31:03.645113Z","signature_b64":"fXJRRxuGAnq3UiEm2Rq7gCxWI1HkfSYTKFN3nmycZsMxBMLTDWDTBxXfhkyn6u66TBGxg+9EJqEjIT+gb9YxBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"647338f68de642705ca67a53b882043df6483e96e3b723b22bb7808e1b4c9464","last_reissued_at":"2026-07-05T08:31:03.644626Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:31:03.644626Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nucleon Isovector Axial Form Factors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-lat","authors_text":"Boram Yoon, Huey-Wen Lin, Rajan Gupta, Tanmoy Bhattacharya, Yong-Chull Jang","submitted_at":"2023-05-18T22:41:34Z","abstract_excerpt":"We present results for the isovector axial vector form factors obtained using thirteen 2+1+1-flavor highly improved staggered quark (HISQ) ensembles generated by the MILC collaboration. The calculation of nucleon two- and three-point correlation functions has been done using Wilson-clover fermions. In the analysis of these data, we quantify the sensitivity of the results to strategies used for removing excited state contamination and invoke the partially conserved axial current relation between the form factors to choose between them. Our data driven analysis includes removing contributions fr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.11330","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/2305.11330/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":"2305.11330","created_at":"2026-07-05T08:31:03.644685+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.11330v3","created_at":"2026-07-05T08:31:03.644685+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.11330","created_at":"2026-07-05T08:31:03.644685+00:00"},{"alias_kind":"pith_short_12","alias_value":"MRZTR5UN4ZBH","created_at":"2026-07-05T08:31:03.644685+00:00"},{"alias_kind":"pith_short_16","alias_value":"MRZTR5UN4ZBHAXFG","created_at":"2026-07-05T08:31:03.644685+00:00"},{"alias_kind":"pith_short_8","alias_value":"MRZTR5UN","created_at":"2026-07-05T08:31:03.644685+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":0,"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":43,"is_internal_anchor":false},{"citing_arxiv_id":"2601.21155","citing_title":"Nucleon axial-vector form factor and radius from radiatively-corrected antineutrino scattering data","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2411.04268","citing_title":"FLAG Review 2024","ref_index":90,"is_internal_anchor":false},{"citing_arxiv_id":"2605.02808","citing_title":"Third moments of nucleon unpolarized, polarized, and transversity parton distribution functions from physical-point lattice QCD","ref_index":15,"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":17,"is_internal_anchor":false},{"citing_arxiv_id":"2604.16025","citing_title":"Scalar and Tensor Form Factors for $\\Lambda \\rightarrow p\\ell \\bar{\\nu}_\\ell$ from Lattice QCD","ref_index":19,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX","json":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX.json","graph_json":"https://pith.science/api/pith-number/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/graph.json","events_json":"https://pith.science/api/pith-number/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/events.json","paper":"https://pith.science/paper/MRZTR5UN"},"agent_actions":{"view_html":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX","download_json":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX.json","view_paper":"https://pith.science/paper/MRZTR5UN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.11330&json=true","fetch_graph":"https://pith.science/api/pith-number/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/graph.json","fetch_events":"https://pith.science/api/pith-number/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/action/storage_attestation","attest_author":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/action/author_attestation","sign_citation":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/action/citation_signature","submit_replication":"https://pith.science/pith/MRZTR5UN4ZBHAXFGPJJ3RAQEHX/action/replication_record"}},"created_at":"2026-07-05T08:31:03.644685+00:00","updated_at":"2026-07-05T08:31:03.644685+00:00"}