{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:EUHWGQTYXLI3BVKN6JK6YTEJJW","short_pith_number":"pith:EUHWGQTY","schema_version":"1.0","canonical_sha256":"250f634278bad1b0d54df255ec4c894d9c35d5c9b81b140c7fade36669018339","source":{"kind":"arxiv","id":"1710.08678","version":2},"attestation_state":"computed","paper":{"title":"RI/MOM and RI/SMOM renormalization of overlap quark bilinears on domain wall fermion configurations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Hao Cai, Keh-Fei Liu, Ming Gong, Yi-Bo Yang, Ying Chen, Yujiang Bi, Zhaofeng Liu","submitted_at":"2017-10-24T09:47:29Z","abstract_excerpt":"Renormalization constants (RCs) of overlap quark bilinear operators on 2+1-flavor domain wall fermion configurations are calculated by using the RI/MOM and RI/SMOM schemes. The scale independent RC for the axial vector current is computed by using a Ward identity. Then the RCs for the quark field and the vector, tensor, scalar and pseudoscalar operators are calculated in both the RI/MOM and RI/SMOM schemes. The RCs are converted to the $\\overline{\\rm MS}$ scheme and we compare the numerical results from using the two intermediate schemes. The lattice size is $48^3\\times96$ and the inverse spac"},"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":"1710.08678","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-10-24T09:47:29Z","cross_cats_sorted":[],"title_canon_sha256":"05c8f10dde34bc9ee577f96c9e09d1a8a5ce8604ed5027ddf4120270ea1f05f7","abstract_canon_sha256":"a4d32f8bc98bbe66abb58cca754abfb4acfc028b2510c908d288dcadee22b718"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:16:30.792698Z","signature_b64":"97XjPl31XlB+JL89K9bs9phca1moOn28yLS4Og7YxQ42kzMsww62uF131b2thQtcn4c2J9QiMp21vAH+vZUrAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"250f634278bad1b0d54df255ec4c894d9c35d5c9b81b140c7fade36669018339","last_reissued_at":"2026-05-18T00:16:30.792013Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:16:30.792013Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"RI/MOM and RI/SMOM renormalization of overlap quark bilinears on domain wall fermion configurations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Hao Cai, Keh-Fei Liu, Ming Gong, Yi-Bo Yang, Ying Chen, Yujiang Bi, Zhaofeng Liu","submitted_at":"2017-10-24T09:47:29Z","abstract_excerpt":"Renormalization constants (RCs) of overlap quark bilinear operators on 2+1-flavor domain wall fermion configurations are calculated by using the RI/MOM and RI/SMOM schemes. The scale independent RC for the axial vector current is computed by using a Ward identity. Then the RCs for the quark field and the vector, tensor, scalar and pseudoscalar operators are calculated in both the RI/MOM and RI/SMOM schemes. The RCs are converted to the $\\overline{\\rm MS}$ scheme and we compare the numerical results from using the two intermediate schemes. The lattice size is $48^3\\times96$ and the inverse spac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.08678","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":"1710.08678","created_at":"2026-05-18T00:16:30.792113+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.08678v2","created_at":"2026-05-18T00:16:30.792113+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.08678","created_at":"2026-05-18T00:16:30.792113+00:00"},{"alias_kind":"pith_short_12","alias_value":"EUHWGQTYXLI3","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_16","alias_value":"EUHWGQTYXLI3BVKN","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_8","alias_value":"EUHWGQTY","created_at":"2026-05-18T12:31:12.930513+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/EUHWGQTYXLI3BVKN6JK6YTEJJW","json":"https://pith.science/pith/EUHWGQTYXLI3BVKN6JK6YTEJJW.json","graph_json":"https://pith.science/api/pith-number/EUHWGQTYXLI3BVKN6JK6YTEJJW/graph.json","events_json":"https://pith.science/api/pith-number/EUHWGQTYXLI3BVKN6JK6YTEJJW/events.json","paper":"https://pith.science/paper/EUHWGQTY"},"agent_actions":{"view_html":"https://pith.science/pith/EUHWGQTYXLI3BVKN6JK6YTEJJW","download_json":"https://pith.science/pith/EUHWGQTYXLI3BVKN6JK6YTEJJW.json","view_paper":"https://pith.science/paper/EUHWGQTY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.08678&json=true","fetch_graph":"https://pith.science/api/pith-number/EUHWGQTYXLI3BVKN6JK6YTEJJW/graph.json","fetch_events":"https://pith.science/api/pith-number/EUHWGQTYXLI3BVKN6JK6YTEJJW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EUHWGQTYXLI3BVKN6JK6YTEJJW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EUHWGQTYXLI3BVKN6JK6YTEJJW/action/storage_attestation","attest_author":"https://pith.science/pith/EUHWGQTYXLI3BVKN6JK6YTEJJW/action/author_attestation","sign_citation":"https://pith.science/pith/EUHWGQTYXLI3BVKN6JK6YTEJJW/action/citation_signature","submit_replication":"https://pith.science/pith/EUHWGQTYXLI3BVKN6JK6YTEJJW/action/replication_record"}},"created_at":"2026-05-18T00:16:30.792113+00:00","updated_at":"2026-05-18T00:16:30.792113+00:00"}