{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:EWVKKVKUDHG73PNMUSLWFONQLK","short_pith_number":"pith:EWVKKVKU","schema_version":"1.0","canonical_sha256":"25aaa5555419cdfdbdaca49762b9b05aa6be431e9187b422a5beb02025b6e144","source":{"kind":"arxiv","id":"hep-lat/9901019","version":1},"attestation_state":"computed","paper":{"title":"Non-perturbative determination of quark masses in quenched lattice QCD with the Kogut-Susskind fermion action","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Ukawa, JLQCD Collaboration: S. Aoki, K-I. Ishikawa, K. Kanaya, M. Fukugita, M. Okawa, N. Ishizuka, N. Tsutsui, N. Yamada, S. Hashimoto, S. Kaya, S. Tominaga, T. Kaneda, T. Onogi, T. Yoshi\\'e, Y. Iwasaki, Y. Kuramashi","submitted_at":"1999-01-25T08:25:48Z","abstract_excerpt":"We report results of quark masses in quenched lattice QCD with the Kogut-Susskind fermion action, employing the Reguralization Independent scheme (RI) of Martinelli et al. to non-perturbatively evaluate the renormalization factor relating the bare quark mass on the lattice to that in the continuum. Calculations are carried out at \\beta=6.0, 6.2, and 6.4, from which we find $m^{\\bar{MS}}_{ud} (2 GeV)= 4.23(29) MeV$ for the average up and down quark mass and, with the $\\phi$ meson mass as input, $m^{\\bar{MS}}_{s} (2 GeV)= 129(12) MeV$ for the strange mass in the continuum limit. These values are"},"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/9901019","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1999-01-25T08:25:48Z","cross_cats_sorted":[],"title_canon_sha256":"471349b5bb4b76e4a7f5296617df4144d582290e5516544cd9cb9150f22bfbe3","abstract_canon_sha256":"c4c19af7d0f1aa5b6299af57171ea7c96ccba58c013e3bc6c7830468caf6b817"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:17.203466Z","signature_b64":"LVaG6nX0HLhDeXy7gbNcm9GwfX1DB6sKh0uD553hvYyq+3ayktWhx2OUOALXs0Hdn3B9Lc4TdIxFlI51ZRp2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"25aaa5555419cdfdbdaca49762b9b05aa6be431e9187b422a5beb02025b6e144","last_reissued_at":"2026-05-18T01:09:17.202773Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:17.202773Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-perturbative determination of quark masses in quenched lattice QCD with the Kogut-Susskind fermion action","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Ukawa, JLQCD Collaboration: S. Aoki, K-I. Ishikawa, K. Kanaya, M. Fukugita, M. Okawa, N. Ishizuka, N. Tsutsui, N. Yamada, S. Hashimoto, S. Kaya, S. Tominaga, T. Kaneda, T. Onogi, T. Yoshi\\'e, Y. Iwasaki, Y. Kuramashi","submitted_at":"1999-01-25T08:25:48Z","abstract_excerpt":"We report results of quark masses in quenched lattice QCD with the Kogut-Susskind fermion action, employing the Reguralization Independent scheme (RI) of Martinelli et al. to non-perturbatively evaluate the renormalization factor relating the bare quark mass on the lattice to that in the continuum. Calculations are carried out at \\beta=6.0, 6.2, and 6.4, from which we find $m^{\\bar{MS}}_{ud} (2 GeV)= 4.23(29) MeV$ for the average up and down quark mass and, with the $\\phi$ meson mass as input, $m^{\\bar{MS}}_{s} (2 GeV)= 129(12) MeV$ for the strange mass in the continuum limit. These values are"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9901019","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/9901019","created_at":"2026-05-18T01:09:17.202884+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9901019v1","created_at":"2026-05-18T01:09:17.202884+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9901019","created_at":"2026-05-18T01:09:17.202884+00:00"},{"alias_kind":"pith_short_12","alias_value":"EWVKKVKUDHG7","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"EWVKKVKUDHG73PNM","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"EWVKKVKU","created_at":"2026-05-18T12:25:49.631198+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/EWVKKVKUDHG73PNMUSLWFONQLK","json":"https://pith.science/pith/EWVKKVKUDHG73PNMUSLWFONQLK.json","graph_json":"https://pith.science/api/pith-number/EWVKKVKUDHG73PNMUSLWFONQLK/graph.json","events_json":"https://pith.science/api/pith-number/EWVKKVKUDHG73PNMUSLWFONQLK/events.json","paper":"https://pith.science/paper/EWVKKVKU"},"agent_actions":{"view_html":"https://pith.science/pith/EWVKKVKUDHG73PNMUSLWFONQLK","download_json":"https://pith.science/pith/EWVKKVKUDHG73PNMUSLWFONQLK.json","view_paper":"https://pith.science/paper/EWVKKVKU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-lat/9901019&json=true","fetch_graph":"https://pith.science/api/pith-number/EWVKKVKUDHG73PNMUSLWFONQLK/graph.json","fetch_events":"https://pith.science/api/pith-number/EWVKKVKUDHG73PNMUSLWFONQLK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EWVKKVKUDHG73PNMUSLWFONQLK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EWVKKVKUDHG73PNMUSLWFONQLK/action/storage_attestation","attest_author":"https://pith.science/pith/EWVKKVKUDHG73PNMUSLWFONQLK/action/author_attestation","sign_citation":"https://pith.science/pith/EWVKKVKUDHG73PNMUSLWFONQLK/action/citation_signature","submit_replication":"https://pith.science/pith/EWVKKVKUDHG73PNMUSLWFONQLK/action/replication_record"}},"created_at":"2026-05-18T01:09:17.202884+00:00","updated_at":"2026-05-18T01:09:17.202884+00:00"}