{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:WFD7G5PJTP45LKDQNGTPDO4Z5O","short_pith_number":"pith:WFD7G5PJ","schema_version":"1.0","canonical_sha256":"b147f375e99bf9d5a87069a6f1bb99ebb06ad90640b0f34343d10fe1d9dc6e2e","source":{"kind":"arxiv","id":"1805.10507","version":2},"attestation_state":"computed","paper":{"title":"Nucleon charges with dynamical overlap fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Hiroshi Ohki (JLQCD Collaboration), Nodoka Yamanaka, Shoji Hashimoto, Takashi Kaneko","submitted_at":"2018-05-26T17:09:58Z","abstract_excerpt":"We calculate the scalar and tensor charges of the nucleon in 2+1-flavor lattice QCD, for which the systematics of the renormalization of the disconnected diagram is well controlled. Numerical simulations are performed at a single lattice spacing a = 0.11 fm. We simulate four pion masses, which cover a range of $m_\\pi \\sim$ 290 - 540 MeV, and a single strange quark mass close to its physical value. The statistical accuracy is improved by employing the so-called low-mode averaging technique and the truncated solver method. We study up, down, and strange quark contributions to the nucleon charges"},"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":"1805.10507","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-05-26T17:09:58Z","cross_cats_sorted":["hep-ex","hep-ph","nucl-th"],"title_canon_sha256":"04db869e68a244dcb870bb8bb01f28c2305634181dc7b5ea6353f40cc2cc8b57","abstract_canon_sha256":"59a8536f998ba2f9e9dd39d4152a046b1233ba6d3857fbd90ba523bdf8c52869"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:44.750048Z","signature_b64":"pF173gJJIc2Ml4GTnwAhorup4CBlzFDY49l70akW8CvXp0ISL9P8JjIaGmXF7kWqfcJUOkwbVUwrWhYc+AKpAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b147f375e99bf9d5a87069a6f1bb99ebb06ad90640b0f34343d10fe1d9dc6e2e","last_reissued_at":"2026-05-18T00:04:44.749296Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:44.749296Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nucleon charges with dynamical overlap fermions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Hiroshi Ohki (JLQCD Collaboration), Nodoka Yamanaka, Shoji Hashimoto, Takashi Kaneko","submitted_at":"2018-05-26T17:09:58Z","abstract_excerpt":"We calculate the scalar and tensor charges of the nucleon in 2+1-flavor lattice QCD, for which the systematics of the renormalization of the disconnected diagram is well controlled. Numerical simulations are performed at a single lattice spacing a = 0.11 fm. We simulate four pion masses, which cover a range of $m_\\pi \\sim$ 290 - 540 MeV, and a single strange quark mass close to its physical value. The statistical accuracy is improved by employing the so-called low-mode averaging technique and the truncated solver method. We study up, down, and strange quark contributions to the nucleon charges"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.10507","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":""},"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":"1805.10507","created_at":"2026-05-18T00:04:44.749429+00:00"},{"alias_kind":"arxiv_version","alias_value":"1805.10507v2","created_at":"2026-05-18T00:04:44.749429+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.10507","created_at":"2026-05-18T00:04:44.749429+00:00"},{"alias_kind":"pith_short_12","alias_value":"WFD7G5PJTP45","created_at":"2026-05-18T12:32:59.047623+00:00"},{"alias_kind":"pith_short_16","alias_value":"WFD7G5PJTP45LKDQ","created_at":"2026-05-18T12:32:59.047623+00:00"},{"alias_kind":"pith_short_8","alias_value":"WFD7G5PJ","created_at":"2026-05-18T12:32:59.047623+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.28131","citing_title":"Simplified approach to extracting nucleon transversity in collinear factorization using near-side energy-energy correlators","ref_index":44,"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":35,"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":44,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O","json":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O.json","graph_json":"https://pith.science/api/pith-number/WFD7G5PJTP45LKDQNGTPDO4Z5O/graph.json","events_json":"https://pith.science/api/pith-number/WFD7G5PJTP45LKDQNGTPDO4Z5O/events.json","paper":"https://pith.science/paper/WFD7G5PJ"},"agent_actions":{"view_html":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O","download_json":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O.json","view_paper":"https://pith.science/paper/WFD7G5PJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1805.10507&json=true","fetch_graph":"https://pith.science/api/pith-number/WFD7G5PJTP45LKDQNGTPDO4Z5O/graph.json","fetch_events":"https://pith.science/api/pith-number/WFD7G5PJTP45LKDQNGTPDO4Z5O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O/action/storage_attestation","attest_author":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O/action/author_attestation","sign_citation":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O/action/citation_signature","submit_replication":"https://pith.science/pith/WFD7G5PJTP45LKDQNGTPDO4Z5O/action/replication_record"}},"created_at":"2026-05-18T00:04:44.749429+00:00","updated_at":"2026-05-18T00:04:44.749429+00:00"}