{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:IL4HQTGOWVV47ZJN2MA6IXRCJ5","short_pith_number":"pith:IL4HQTGO","schema_version":"1.0","canonical_sha256":"42f8784cceb56bcfe52dd301e45e224f5f7821830f1dfe7f84661e8a0e5e1217","source":{"kind":"arxiv","id":"2402.03024","version":1},"attestation_state":"computed","paper":{"title":"Improved analysis of isovector nucleon matrix elements with $N_f=2+1$ flavors of $\\mathcal{O}(a)$ improved Wilson fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Dalibor Djukanovic, Georg von Hippel, Hartmut Wittig, Harvey B. Meyer, Konstantin Ottnad","submitted_at":"2024-02-05T14:05:48Z","abstract_excerpt":"We present an update of our determination of the isovector charges $g_A^{u-d}$, $g_S^{u-d}$ and $g_T^{u-d}$, and the isovector twist-2 forward matrix elements $\\langle x\\rangle_{u-d}$, $\\langle x\\rangle_{\\Delta u-\\Delta d}$ and $\\langle x\\rangle_{\\delta u-\\delta d}$ on the $N_\\mathrm{f}=2+1$ gauge ensembles generated by the Coordinated Lattice Simulations (CLS) effort. We have significantly extended our coverage of the parameter space by adding ensembles at the physical pion mass and fine lattice spacing, at nearly-physical pion masses and very fine lattice spacings, and at very large physical"},"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":"2402.03024","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2024-02-05T14:05:48Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"d9a4aaa6b1b0a9692c472c3a9246e0499b95d26ac7da0e2c0509d7c42a1c3e69","abstract_canon_sha256":"180e0c2450f7ae739b10c8381f2940c01c378ae4faf72605a28b68387dab730b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:41:20.548335Z","signature_b64":"WFLnyikYW/03QUpKT+cqsEXOixNI/DrDQ/opOViq3Z+w+7JMGAE6nB439GlDKdMdgVtRedGPK9Yt6IovBOd3BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"42f8784cceb56bcfe52dd301e45e224f5f7821830f1dfe7f84661e8a0e5e1217","last_reissued_at":"2026-07-05T07:41:20.547902Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:41:20.547902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Improved analysis of isovector nucleon matrix elements with $N_f=2+1$ flavors of $\\mathcal{O}(a)$ improved Wilson fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Dalibor Djukanovic, Georg von Hippel, Hartmut Wittig, Harvey B. Meyer, Konstantin Ottnad","submitted_at":"2024-02-05T14:05:48Z","abstract_excerpt":"We present an update of our determination of the isovector charges $g_A^{u-d}$, $g_S^{u-d}$ and $g_T^{u-d}$, and the isovector twist-2 forward matrix elements $\\langle x\\rangle_{u-d}$, $\\langle x\\rangle_{\\Delta u-\\Delta d}$ and $\\langle x\\rangle_{\\delta u-\\delta d}$ on the $N_\\mathrm{f}=2+1$ gauge ensembles generated by the Coordinated Lattice Simulations (CLS) effort. We have significantly extended our coverage of the parameter space by adding ensembles at the physical pion mass and fine lattice spacing, at nearly-physical pion masses and very fine lattice spacings, and at very large physical"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.03024","kind":"arxiv","version":1},"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/2402.03024/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":"2402.03024","created_at":"2026-07-05T07:41:20.547961+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.03024v1","created_at":"2026-07-05T07:41:20.547961+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.03024","created_at":"2026-07-05T07:41:20.547961+00:00"},{"alias_kind":"pith_short_12","alias_value":"IL4HQTGOWVV4","created_at":"2026-07-05T07:41:20.547961+00:00"},{"alias_kind":"pith_short_16","alias_value":"IL4HQTGOWVV47ZJN","created_at":"2026-07-05T07:41:20.547961+00:00"},{"alias_kind":"pith_short_8","alias_value":"IL4HQTGO","created_at":"2026-07-05T07:41:20.547961+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":10,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.27072","citing_title":"Performance of Low Mode Averaging on Twisted-Mass Fermion Ensembles at the physical pion mass point","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2606.22224","citing_title":"Proton's isovector PDF with updated analysis of large-momentum lattice data","ref_index":24,"is_internal_anchor":false},{"citing_arxiv_id":"2607.02441","citing_title":"Transverse-spin dependent energy-energy correlators in proton-proton collisions within the dihadron fragmentation framework","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02243","citing_title":"Decomposition of the axial-vector current in a finite box","ref_index":10,"is_internal_anchor":false},{"citing_arxiv_id":"2606.00362","citing_title":"Impact of Future Dihadron Production Measurements on the Transversity Distributions and Tensor Charges of the Nucleon","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2411.04268","citing_title":"FLAG Review 2024","ref_index":96,"is_internal_anchor":false},{"citing_arxiv_id":"2604.28131","citing_title":"Simplified approach to extracting nucleon transversity in collinear factorization using near-side energy-energy correlators","ref_index":55,"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":22,"is_internal_anchor":false},{"citing_arxiv_id":"2604.28131","citing_title":"Simplified approach to extracting nucleon transversity in collinear factorization using near-side energy-energy correlators","ref_index":55,"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":16,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5","json":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5.json","graph_json":"https://pith.science/api/pith-number/IL4HQTGOWVV47ZJN2MA6IXRCJ5/graph.json","events_json":"https://pith.science/api/pith-number/IL4HQTGOWVV47ZJN2MA6IXRCJ5/events.json","paper":"https://pith.science/paper/IL4HQTGO"},"agent_actions":{"view_html":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5","download_json":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5.json","view_paper":"https://pith.science/paper/IL4HQTGO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.03024&json=true","fetch_graph":"https://pith.science/api/pith-number/IL4HQTGOWVV47ZJN2MA6IXRCJ5/graph.json","fetch_events":"https://pith.science/api/pith-number/IL4HQTGOWVV47ZJN2MA6IXRCJ5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5/action/storage_attestation","attest_author":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5/action/author_attestation","sign_citation":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5/action/citation_signature","submit_replication":"https://pith.science/pith/IL4HQTGOWVV47ZJN2MA6IXRCJ5/action/replication_record"}},"created_at":"2026-07-05T07:41:20.547961+00:00","updated_at":"2026-07-05T07:41:20.547961+00:00"}