{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:X2BGSUTXVMMA3H4R6R5QPXSKVM","short_pith_number":"pith:X2BGSUTX","schema_version":"1.0","canonical_sha256":"be82695277ab180d9f91f47b07de4aab10bd1eeaee058358cf92e2ba4f9f5435","source":{"kind":"arxiv","id":"1312.7628","version":2},"attestation_state":"computed","paper":{"title":"Non-perturbative renormalization of overlap quark bilinears on 2+1-flavor domain wall fermion configurations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Anyi Li, Jian-Bo Zhang (chiQCD Collaboration), Keh-Fei Liu, Michael Glatzmaier, Ming Gong, Shao-Jing Dong, Yi-Bo Yang, Ying Chen, Zhaofeng Liu","submitted_at":"2013-12-30T05:04:34Z","abstract_excerpt":"We present renormalization constants of overlap quark bilinear operators on 2+1-flavor domain wall fermion configurations. This setup is being used by the chiQCD collaboration in calculations of physical quantities such as strangeness in the nucleon and the strange and charm quark masses. The scale independent renormalization constant for the axial vector current is computed using the Ward Identity. The renormalization constants for scalar, pseudoscalar and vector current are calculated in the RI-MOM scheme. Results in the MS-bar scheme are also given. The step scaling function of quark masses"},"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":"1312.7628","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2013-12-30T05:04:34Z","cross_cats_sorted":[],"title_canon_sha256":"e5f3065d93d7d3555463c467fdeee703a74ef8c99dbf34c224ec09192fc045a8","abstract_canon_sha256":"571642ad2322c854299287fdc79dd4f2d4dc1266d85ff0558bd1088f17b2ecd2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:44:09.013037Z","signature_b64":"wYRJh96N28icqaQGqlY1YEzHUL2qWZpP0mcyEzgHxSPl6nuT3YkKvo38XTIDd0CUw3pwT5Mi1926awOFla4SCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"be82695277ab180d9f91f47b07de4aab10bd1eeaee058358cf92e2ba4f9f5435","last_reissued_at":"2026-05-18T02:44:09.012615Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:44:09.012615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-perturbative renormalization of overlap quark bilinears on 2+1-flavor domain wall fermion configurations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Anyi Li, Jian-Bo Zhang (chiQCD Collaboration), Keh-Fei Liu, Michael Glatzmaier, Ming Gong, Shao-Jing Dong, Yi-Bo Yang, Ying Chen, Zhaofeng Liu","submitted_at":"2013-12-30T05:04:34Z","abstract_excerpt":"We present renormalization constants of overlap quark bilinear operators on 2+1-flavor domain wall fermion configurations. This setup is being used by the chiQCD collaboration in calculations of physical quantities such as strangeness in the nucleon and the strange and charm quark masses. The scale independent renormalization constant for the axial vector current is computed using the Ward Identity. The renormalization constants for scalar, pseudoscalar and vector current are calculated in the RI-MOM scheme. Results in the MS-bar scheme are also given. The step scaling function of quark masses"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.7628","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":"1312.7628","created_at":"2026-05-18T02:44:09.012681+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.7628v2","created_at":"2026-05-18T02:44:09.012681+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.7628","created_at":"2026-05-18T02:44:09.012681+00:00"},{"alias_kind":"pith_short_12","alias_value":"X2BGSUTXVMMA","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_16","alias_value":"X2BGSUTXVMMA3H4R","created_at":"2026-05-18T12:28:06.772260+00:00"},{"alias_kind":"pith_short_8","alias_value":"X2BGSUTX","created_at":"2026-05-18T12:28:06.772260+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/X2BGSUTXVMMA3H4R6R5QPXSKVM","json":"https://pith.science/pith/X2BGSUTXVMMA3H4R6R5QPXSKVM.json","graph_json":"https://pith.science/api/pith-number/X2BGSUTXVMMA3H4R6R5QPXSKVM/graph.json","events_json":"https://pith.science/api/pith-number/X2BGSUTXVMMA3H4R6R5QPXSKVM/events.json","paper":"https://pith.science/paper/X2BGSUTX"},"agent_actions":{"view_html":"https://pith.science/pith/X2BGSUTXVMMA3H4R6R5QPXSKVM","download_json":"https://pith.science/pith/X2BGSUTXVMMA3H4R6R5QPXSKVM.json","view_paper":"https://pith.science/paper/X2BGSUTX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.7628&json=true","fetch_graph":"https://pith.science/api/pith-number/X2BGSUTXVMMA3H4R6R5QPXSKVM/graph.json","fetch_events":"https://pith.science/api/pith-number/X2BGSUTXVMMA3H4R6R5QPXSKVM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X2BGSUTXVMMA3H4R6R5QPXSKVM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X2BGSUTXVMMA3H4R6R5QPXSKVM/action/storage_attestation","attest_author":"https://pith.science/pith/X2BGSUTXVMMA3H4R6R5QPXSKVM/action/author_attestation","sign_citation":"https://pith.science/pith/X2BGSUTXVMMA3H4R6R5QPXSKVM/action/citation_signature","submit_replication":"https://pith.science/pith/X2BGSUTXVMMA3H4R6R5QPXSKVM/action/replication_record"}},"created_at":"2026-05-18T02:44:09.012681+00:00","updated_at":"2026-05-18T02:44:09.012681+00:00"}