{"as_of":"2026-08-18T16:24:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:7cf6fcf15ae905c7c0da30b42ff16d8f884e7fdf901a711a67120d66b596722e","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":4,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":4,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-18T06:34:40.430872+00:00","state":"measured"},{"denominator":4,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":4,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-11T16:18:17.984982Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-11T22:06:24.790629Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2003.13359","last_updated":"2020-03-30T11:41:48Z","snapshot_observed_at":"2026-07-06T09:08:17.524888Z","submitted_at":"2020-03-30T11:41:48Z","title":"Remarks on strange-quark simulations with Wilson fermions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.13359","snapshot_observed_at":"2026-08-11T16:18:17.984982Z","title":"Remarks on strange-quark simulations with Wilson fermions,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.10215","last_updated":"2025-07-10T12:39:37Z","snapshot_observed_at":"2026-08-17T13:06:33.345450Z","submitted_at":"2024-12-13T15:39:13Z","title":"The determination of potential scales in 2+1 flavor QCD","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-11T16:18:17.984982Z"},"links":{"cited_paper":"/paper/2003.13359","citing_paper":"/paper/2412.10215"},"observation_digest":"sha256:8915b76b3d747899928cc13fdb5fb5f5f6d98ccdae59daa9cf435cf27eb21bc4","observation_id":"5f5237ea-8166-4b31-92ce-c6bc0c236105","resolution":{"observed_at":"2026-08-11T16:18:17.984982Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.13359","last_updated":"2020-03-30T11:41:48Z","snapshot_observed_at":"2026-07-06T09:08:17.524888Z","submitted_at":"2020-03-30T11:41:48Z","title":"Remarks on strange-quark simulations with Wilson fermions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.13359","snapshot_observed_at":"2026-08-07T19:16:22.878276Z","title":"Mohler and S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.10159","last_updated":"2025-02-14T13:40:15Z","snapshot_observed_at":"2026-08-17T12:26:18.734761Z","submitted_at":"2025-02-14T13:40:15Z","title":"The hadronic contribution to the running of $\\alpha$ and the electroweak mixing angle","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-07T19:16:22.878276Z"},"links":{"cited_paper":"/paper/2003.13359","citing_paper":"/paper/2502.10159"},"observation_digest":"sha256:af447223a99a09f1deb49f71d7b5f6868c678e8e20fce237904b9652341a37e6","observation_id":"31c05b08-4729-4732-a522-a5c94728f698","resolution":{"observed_at":"2026-08-07T19:16:22.878276Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.13359","last_updated":"2020-03-30T11:41:48Z","snapshot_observed_at":"2026-07-06T09:08:17.524888Z","submitted_at":"2020-03-30T11:41:48Z","title":"Remarks on strange-quark simulations with Wilson fermions","version":1},"cited_work":{"arxiv_id":"2003.13359","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2003.13359","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Mohler and S","venue":null,"work_id":"4c43a373-b4ae-41da-a743-085d83a9b473","year":2020},"citing_paper":{"arxiv_id":"2605.06559","last_updated":"2026-05-07T16:53:53Z","snapshot_observed_at":"2026-08-14T03:02:08.390694Z","submitted_at":"2026-05-07T16:53:53Z","title":"The strange and flavor-singlet axial form factors of the nucleon from lattice QCD","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-05-08T03:24:57.532684Z"},"links":{"cited_paper":"/paper/2003.13359","citing_paper":"/paper/2605.06559"},"observation_digest":"sha256:819c2cd5489c4c3f20905a2e88742cb26add3fa9adb03062fc2ec236941f4033","observation_id":"94f3f477-1916-4208-aefc-c0959c7e22d5","resolution":{"observed_at":"2026-05-11T22:06:24.793919Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2003.13359","last_updated":"2020-03-30T11:41:48Z","snapshot_observed_at":"2026-07-06T09:08:17.524888Z","submitted_at":"2020-03-30T11:41:48Z","title":"Remarks on strange-quark simulations with Wilson fermions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.13359","snapshot_observed_at":"2026-07-12T02:57:50.266827Z","title":null,"venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2607.03370","last_updated":"2026-07-03T14:24:23Z","snapshot_observed_at":"2026-08-13T05:14:40.868595Z","submitted_at":"2026-07-03T14:24:23Z","title":"The running of the electroweak gauge couplings from first principles","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-07-12T02:57:50.266827Z"},"links":{"cited_paper":"/paper/2003.13359","citing_paper":"/paper/2607.03370"},"observation_digest":"sha256:8c2460e05c0512dc5d7c72f8c0b7a07222fe6ec129494990bad03b0009d04a21","observation_id":"f5965401-9846-49c3-9865-2bebcc1b7887","resolution":{"observed_at":"2026-07-12T02:57:50.266827Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2003.13359/citation-record","integrity":"/paper/2003.13359/integrity","json":"/paper/2003.13359/citation-record.json","paper":"/paper/2003.13359"},"outbound":[],"paper":{"arxiv_id":"2003.13359","last_updated":"2020-03-30T11:41:48Z","latest_version":1,"primary_category":"hep-lat","snapshot_observed_at":"2026-07-06T09:08:17.524888Z","submitted_at":"2020-03-30T11:41:48Z","title":"Remarks on strange-quark simulations with Wilson fermions"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"thesis":"As of 18 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2003.13359."}