{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:KZOIPD3SYT75WUH7IFGIDFW6AJ","short_pith_number":"pith:KZOIPD3S","schema_version":"1.0","canonical_sha256":"565c878f72c4ffdb50ff414c8196de02571c41045841bab21ec64f61559e25bb","source":{"kind":"arxiv","id":"hep-lat/0011032","version":1},"attestation_state":"computed","paper":{"title":"Eigenvalues of the hermitian Wilson-Dirac operator and chiral properties of the domain-wall fermion","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Ukawa, CP-PACS Collaboration : A. Ali Khan, H.P. Shanahan, J. Noaki, K.-I. Nagai, K. Kanaya, M. Fukugita, M. Okawa, N. Ishizuka, R. Burkhalter, S. Aoki, S. Ejiri, S. Hashimoto, T. Izubuchi, T. Kaneko, T. Manke, T. Yoshi\\'e, Y. Aoki, Y. Iwasaki, Y. Kuramashi, Y. Taniguchi","submitted_at":"2000-11-05T13:51:17Z","abstract_excerpt":"Chiral properties of QCD formulated with the domain-wall fermion (DWQCD) are studied using the anomalous quark mass m_{5q} and the spectrum of the 4-dimensional Wilson-Dirac operator. Numerical simulations are made with the standard plaquette gauge action and a renormalization-group improved gauge action. Results are reported on the density of zero eigenvalue obtained with the accumulation method, and a comparison is made with the results for m_{5q}."},"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":"hep-lat/0011032","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2000-11-05T13:51:17Z","cross_cats_sorted":[],"title_canon_sha256":"0fd2982ca532808449561c8f5d359fa54c8a3384947c08d466d3673fe6670d3d","abstract_canon_sha256":"efc7618fb2a8cc304e287a4a31cc60746953502841a391659e2362826ca77a9d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:20.562289Z","signature_b64":"wIB1plsBAJSQTcCFL7x3zTOO81/KnCvoWmdIdhrSOyEf/eGw1VuenSJgP7M/SU7JQzBhALcuF9XKF65AqUGFCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"565c878f72c4ffdb50ff414c8196de02571c41045841bab21ec64f61559e25bb","last_reissued_at":"2026-05-18T03:47:20.561868Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:20.561868Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Eigenvalues of the hermitian Wilson-Dirac operator and chiral properties of the domain-wall fermion","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Ukawa, CP-PACS Collaboration : A. Ali Khan, H.P. Shanahan, J. Noaki, K.-I. Nagai, K. Kanaya, M. Fukugita, M. Okawa, N. Ishizuka, R. Burkhalter, S. Aoki, S. Ejiri, S. Hashimoto, T. Izubuchi, T. Kaneko, T. Manke, T. Yoshi\\'e, Y. Aoki, Y. Iwasaki, Y. Kuramashi, Y. Taniguchi","submitted_at":"2000-11-05T13:51:17Z","abstract_excerpt":"Chiral properties of QCD formulated with the domain-wall fermion (DWQCD) are studied using the anomalous quark mass m_{5q} and the spectrum of the 4-dimensional Wilson-Dirac operator. Numerical simulations are made with the standard plaquette gauge action and a renormalization-group improved gauge action. Results are reported on the density of zero eigenvalue obtained with the accumulation method, and a comparison is made with the results for m_{5q}."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0011032","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":""},"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":"hep-lat/0011032","created_at":"2026-05-18T03:47:20.561931+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0011032v1","created_at":"2026-05-18T03:47:20.561931+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0011032","created_at":"2026-05-18T03:47:20.561931+00:00"},{"alias_kind":"pith_short_12","alias_value":"KZOIPD3SYT75","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_16","alias_value":"KZOIPD3SYT75WUH7","created_at":"2026-05-18T12:25:50.254431+00:00"},{"alias_kind":"pith_short_8","alias_value":"KZOIPD3S","created_at":"2026-05-18T12:25:50.254431+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ","json":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ.json","graph_json":"https://pith.science/api/pith-number/KZOIPD3SYT75WUH7IFGIDFW6AJ/graph.json","events_json":"https://pith.science/api/pith-number/KZOIPD3SYT75WUH7IFGIDFW6AJ/events.json","paper":"https://pith.science/paper/KZOIPD3S"},"agent_actions":{"view_html":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ","download_json":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ.json","view_paper":"https://pith.science/paper/KZOIPD3S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0011032&json=true","fetch_graph":"https://pith.science/api/pith-number/KZOIPD3SYT75WUH7IFGIDFW6AJ/graph.json","fetch_events":"https://pith.science/api/pith-number/KZOIPD3SYT75WUH7IFGIDFW6AJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ/action/storage_attestation","attest_author":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ/action/author_attestation","sign_citation":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ/action/citation_signature","submit_replication":"https://pith.science/pith/KZOIPD3SYT75WUH7IFGIDFW6AJ/action/replication_record"}},"created_at":"2026-05-18T03:47:20.561931+00:00","updated_at":"2026-05-18T03:47:20.561931+00:00"}