{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:B3FCHWFIJW4IWTZTISVHX2BAAC","short_pith_number":"pith:B3FCHWFI","schema_version":"1.0","canonical_sha256":"0eca23d8a84db88b4f3344aa7be820009e441adcb077e91591ec83f6c0d9d5d6","source":{"kind":"arxiv","id":"hep-lat/0309141","version":1},"attestation_state":"computed","paper":{"title":"Study of finite volume effects in the non-perturbative determination of $\\csw$ with the SF method in full three-flavor lattice QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Ukawa, CP-PACS, JLQCD Collaboration: K-I. Ishikawa, K. Kanaya, M. Fukugita, M. Okawa, N. Ishizuka, N. Tsutsui, N. Yamada, S. Aoki, S. Hashimoto, T.Kaneko, T. Umeda, T. Yoshi\\'e, V. Lesk, Y. Iwasaki, Y. Kuramashi","submitted_at":"2003-09-22T05:47:13Z","abstract_excerpt":"The non-perturbative $\\csw$ determined by the Schr\\\"{o}dinger functional (SF) method with the RG-improved gauge action in dynamical $N_f=3$ QCD shows a finite volume effect when the numerical simulations are carried out at a constant lattice size $L/a$. We remove the unwanted finite volume effect by keeping physical lattice extent $L$ at a constant. The details of the method and the result obtained for non-perturbative $\\csw$ with a constant $L$ are reported."},"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/0309141","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"2003-09-22T05:47:13Z","cross_cats_sorted":[],"title_canon_sha256":"ecc3e76ce713e27b9ee618ed005cf27e9cd837b7ff5acee3d2012e56fefdffb1","abstract_canon_sha256":"2031783dc767c63083920b09ab91b5ba3d235bdabb05edae4facf0f9e228a72a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:20.318956Z","signature_b64":"mk1gGqHRxrArnwXgwW0NThuQUkm7gRsAROPFscOHjGBPNZv+t/Nz+UUobT43jtwVUB1QF4G9lE9O0gFfFm9oDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0eca23d8a84db88b4f3344aa7be820009e441adcb077e91591ec83f6c0d9d5d6","last_reissued_at":"2026-05-18T03:47:20.318187Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:20.318187Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Study of finite volume effects in the non-perturbative determination of $\\csw$ with the SF method in full three-flavor lattice QCD","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Ukawa, CP-PACS, JLQCD Collaboration: K-I. Ishikawa, K. Kanaya, M. Fukugita, M. Okawa, N. Ishizuka, N. Tsutsui, N. Yamada, S. Aoki, S. Hashimoto, T.Kaneko, T. Umeda, T. Yoshi\\'e, V. Lesk, Y. Iwasaki, Y. Kuramashi","submitted_at":"2003-09-22T05:47:13Z","abstract_excerpt":"The non-perturbative $\\csw$ determined by the Schr\\\"{o}dinger functional (SF) method with the RG-improved gauge action in dynamical $N_f=3$ QCD shows a finite volume effect when the numerical simulations are carried out at a constant lattice size $L/a$. We remove the unwanted finite volume effect by keeping physical lattice extent $L$ at a constant. The details of the method and the result obtained for non-perturbative $\\csw$ with a constant $L$ are reported."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/0309141","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/0309141","created_at":"2026-05-18T03:47:20.318299+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/0309141v1","created_at":"2026-05-18T03:47:20.318299+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/0309141","created_at":"2026-05-18T03:47:20.318299+00:00"},{"alias_kind":"pith_short_12","alias_value":"B3FCHWFIJW4I","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"B3FCHWFIJW4IWTZT","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"B3FCHWFI","created_at":"2026-05-18T12:25:51.375804+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/B3FCHWFIJW4IWTZTISVHX2BAAC","json":"https://pith.science/pith/B3FCHWFIJW4IWTZTISVHX2BAAC.json","graph_json":"https://pith.science/api/pith-number/B3FCHWFIJW4IWTZTISVHX2BAAC/graph.json","events_json":"https://pith.science/api/pith-number/B3FCHWFIJW4IWTZTISVHX2BAAC/events.json","paper":"https://pith.science/paper/B3FCHWFI"},"agent_actions":{"view_html":"https://pith.science/pith/B3FCHWFIJW4IWTZTISVHX2BAAC","download_json":"https://pith.science/pith/B3FCHWFIJW4IWTZTISVHX2BAAC.json","view_paper":"https://pith.science/paper/B3FCHWFI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/0309141&json=true","fetch_graph":"https://pith.science/api/pith-number/B3FCHWFIJW4IWTZTISVHX2BAAC/graph.json","fetch_events":"https://pith.science/api/pith-number/B3FCHWFIJW4IWTZTISVHX2BAAC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B3FCHWFIJW4IWTZTISVHX2BAAC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B3FCHWFIJW4IWTZTISVHX2BAAC/action/storage_attestation","attest_author":"https://pith.science/pith/B3FCHWFIJW4IWTZTISVHX2BAAC/action/author_attestation","sign_citation":"https://pith.science/pith/B3FCHWFIJW4IWTZTISVHX2BAAC/action/citation_signature","submit_replication":"https://pith.science/pith/B3FCHWFIJW4IWTZTISVHX2BAAC/action/replication_record"}},"created_at":"2026-05-18T03:47:20.318299+00:00","updated_at":"2026-05-18T03:47:20.318299+00:00"}