{"as_of":"2026-08-10T12:04:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:e7ea90c7792cfa4a263236c9318d919eff127ca7b9c5ef85f4c6fe9baeee077f","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":"2026-08-10T06:31:04.303077+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":"2026-08-09T22:54:53.783844Z","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":"2026-05-21T19:50:34.049286Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2210.09091","last_updated":"2022-12-07T01:17:05Z","snapshot_observed_at":"2026-08-10T10:17:15.724154Z","submitted_at":"2022-10-17T13:35:35Z","title":"Upper critical dimension of the 3-state Potts model","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.09091","snapshot_observed_at":"2026-08-09T22:54:53.783844Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2501.18711","last_updated":"2026-07-13T09:14:33Z","snapshot_observed_at":"2026-08-10T09:19:04.045941Z","submitted_at":"2025-01-30T19:14:45Z","title":"The tricritical Ising CFT and conformal bootstrap","version":3},"reference_index":127,"source":"pdf_text","source_observed_at":"2026-08-09T22:54:53.783844Z"},"links":{"cited_paper":"/paper/2210.09091","citing_paper":"/paper/2501.18711"},"observation_digest":"sha256:b48fca4815607ccefa565b587a1d9f10aa40338913c74c728dfb63f8f534369a","observation_id":"0a503de5-e1a7-4341-a82e-251f0f0815e0","resolution":{"observed_at":"2026-08-09T22:54:53.783844Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.09091","last_updated":"2022-12-07T01:17:05Z","snapshot_observed_at":"2026-08-10T10:17:15.724154Z","submitted_at":"2022-10-17T13:35:35Z","title":"Upper critical dimension of the 3-state Potts model","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.09091","snapshot_observed_at":"2026-08-06T19:14:31.654090Z","title":"Upper critical dimension of the 3-state Potts model,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.06283","last_updated":"2025-07-08T18:00:00Z","snapshot_observed_at":"2026-08-09T09:39:39.050083Z","submitted_at":"2025-07-08T18:00:00Z","title":"Bootstrapping the Simplest Deconfined Quantum Critical Point","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-06T19:14:31.654090Z"},"links":{"cited_paper":"/paper/2210.09091","citing_paper":"/paper/2507.06283"},"observation_digest":"sha256:069eddebf32aff93f5be93d0aec963692285e7fdb50d7ed8678c78e2aeb8287f","observation_id":"78259179-cf10-4fee-b6b3-4c8c1ad14ef4","resolution":{"observed_at":"2026-08-06T19:14:31.654090Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.09091","last_updated":"2022-12-07T01:17:05Z","snapshot_observed_at":"2026-08-10T10:17:15.724154Z","submitted_at":"2022-10-17T13:35:35Z","title":"Upper critical dimension of the 3-state Potts model","version":3},"cited_work":{"arxiv_id":"2210.09091","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2210.09091","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"bc82d0c4-7b8e-449f-941e-74aeee2353a2","year":2025},"citing_paper":{"arxiv_id":"2511.00386","last_updated":"2026-05-19T13:08:03Z","snapshot_observed_at":"2026-07-06T22:34:38.619949Z","submitted_at":"2025-11-01T03:39:10Z","title":"Conformal Bootstrap with Duality-Inspired Fusion Rule","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-05-21T19:45:34.507657Z"},"links":{"cited_paper":"/paper/2210.09091","citing_paper":"/paper/2511.00386"},"observation_digest":"sha256:471d6b97cf4716984b25e199785641f415492fb5884b8ffc4ce926d9eb47d304","observation_id":"aa4c46d5-8d54-478c-b539-12ea3163e33a","resolution":{"observed_at":"2026-05-21T19:50:34.050941Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2210.09091","last_updated":"2022-12-07T01:17:05Z","snapshot_observed_at":"2026-08-10T10:17:15.724154Z","submitted_at":"2022-10-17T13:35:35Z","title":"Upper critical dimension of the 3-state Potts model","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.09091","snapshot_observed_at":"2026-08-08T15:59:33.064888Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.05294","last_updated":"2026-08-05T18:00:07Z","snapshot_observed_at":"2026-08-10T06:03:31.407805Z","submitted_at":"2026-08-05T18:00:07Z","title":"Self-dual $S_3$ gauge theory in 2+1d: lattice model and topological phase transitions","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-08T15:59:33.064888Z"},"links":{"cited_paper":"/paper/2210.09091","citing_paper":"/paper/2608.05294"},"observation_digest":"sha256:f2df3fb2861c6cf6956e7a8043c3d48d7f64764e7a5511ffaa2f1d75c884c05d","observation_id":"0e2cb7c8-8676-4504-bb01-1e9d2c05963a","resolution":{"observed_at":"2026-08-08T15:59:33.064888Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2210.09091/citation-record","integrity":"/paper/2210.09091/integrity","json":"/paper/2210.09091/citation-record.json","paper":"/paper/2210.09091"},"outbound":[],"paper":{"arxiv_id":"2210.09091","last_updated":"2022-12-07T01:17:05Z","latest_version":3,"primary_category":"hep-th","snapshot_observed_at":"2026-08-10T10:17:15.724154Z","submitted_at":"2022-10-17T13:35:35Z","title":"Upper critical dimension of the 3-state Potts model"},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2210.09091."}