{"as_of":"2026-08-19T22:08:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:67f0be197055b6e319143040035e566ab60e72ef5ccd86ec623ae5df6abb29e9","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":7,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":7,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-19T06:32:44.657259+00:00","state":"measured"},{"denominator":7,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":7,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T14:05:42.930961Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-07-04T14:19:54.237135Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1808.02594","last_updated":"2018-08-08T01:44:04Z","snapshot_observed_at":"2026-08-14T18:43:33.143520Z","submitted_at":"2018-08-08T01:44:04Z","title":"The dynamical sine-Gordon model in the full subcritical regime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.02594","snapshot_observed_at":"2026-08-14T14:05:42.930961Z","title":"Chandra, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.03944","last_updated":"2021-06-22T14:07:37Z","snapshot_observed_at":"2026-08-15T15:18:49.239266Z","submitted_at":"2019-08-11T18:04:07Z","title":"On the parabolic and hyperbolic Liouville equations","version":3},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T14:05:42.930961Z"},"links":{"cited_paper":"/paper/1808.02594","citing_paper":"/paper/1908.03944"},"observation_digest":"sha256:2cd6d637cd6a0704dc023f97cb4f7a3de3a991506994ad949cd29d269981d25b","observation_id":"8c34a361-ad6f-485e-8c59-729e0c51c724","resolution":{"observed_at":"2026-08-14T14:05:42.930961Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.02594","last_updated":"2018-08-08T01:44:04Z","snapshot_observed_at":"2026-08-14T18:43:33.143520Z","submitted_at":"2018-08-08T01:44:04Z","title":"The dynamical sine-Gordon model in the full subcritical regime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.02594","snapshot_observed_at":"2026-08-11T10:46:03.883561Z","title":"Chandra, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.16404","last_updated":"2024-12-20T23:39:00Z","snapshot_observed_at":"2026-08-17T23:49:27.660822Z","submitted_at":"2024-12-20T23:39:00Z","title":"A simple construction of the sine-Gordon model via stochastic quantization","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-11T10:46:03.883561Z"},"links":{"cited_paper":"/paper/1808.02594","citing_paper":"/paper/2412.16404"},"observation_digest":"sha256:2157e5fa29d6749f5b20638860dd7fcccf90b080cee31dd49ba6e24b06a29430","observation_id":"54f2fcfd-71a9-4a38-b7b2-26b347f372f1","resolution":{"observed_at":"2026-08-11T10:46:03.883561Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.02594","last_updated":"2018-08-08T01:44:04Z","snapshot_observed_at":"2026-08-14T18:43:33.143520Z","submitted_at":"2018-08-08T01:44:04Z","title":"The dynamical sine-Gordon model in the full subcritical regime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.02594","snapshot_observed_at":"2026-08-10T21:04:19.034829Z","title":"Chandra , M","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2501.06612","last_updated":"2025-08-16T18:03:48Z","snapshot_observed_at":"2026-08-17T23:48:02.602914Z","submitted_at":"2025-01-11T18:22:35Z","title":"Non-Gaussianity of invariant measures to SPDEs in Da Prato-Debussche regime","version":2},"reference_index":23,"source":"arxiv_source","source_observed_at":"2026-08-10T21:04:19.034829Z"},"links":{"cited_paper":"/paper/1808.02594","citing_paper":"/paper/2501.06612"},"observation_digest":"sha256:4d598eab1211c5d54e5cde46e14fe5c5350378ef8b7cbb3cca075cfc5357d6bf","observation_id":"5b63a57e-0ba5-4e9e-bb72-1f68fa0a3555","resolution":{"observed_at":"2026-08-10T21:04:19.034829Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.02594","last_updated":"2018-08-08T01:44:04Z","snapshot_observed_at":"2026-08-14T18:43:33.143520Z","submitted_at":"2018-08-08T01:44:04Z","title":"The dynamical sine-Gordon model in the full subcritical regime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.02594","snapshot_observed_at":"2026-08-10T17:32:15.626558Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2501.12172","last_updated":"2025-04-09T11:24:29Z","snapshot_observed_at":"2026-08-14T10:42:03.158094Z","submitted_at":"2025-01-21T14:30:56Z","title":"A quadratic BSDE approach to normalization for the finite volume 2D sine-Gordon model in the finite ultraviolet regime","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-10T17:32:15.626558Z"},"links":{"cited_paper":"/paper/1808.02594","citing_paper":"/paper/2501.12172"},"observation_digest":"sha256:3c7311530c3a5c38707b10b90bf4976394235201da3d980348ce91aa5f4ac71a","observation_id":"1177b3b9-bd47-4237-928d-6c2801d382d5","resolution":{"observed_at":"2026-08-10T17:32:15.626558Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.02594","last_updated":"2018-08-08T01:44:04Z","snapshot_observed_at":"2026-08-14T18:43:33.143520Z","submitted_at":"2018-08-08T01:44:04Z","title":"The dynamical sine-Gordon model in the full subcritical regime","version":1},"cited_work":{"arxiv_id":"1808.02594","doi":null,"metadata_source":"pith","pith_arxiv_id":"1808.02594","snapshot_observed_at":"2026-07-04T14:19:54.237135Z","title":"The dynamical sine-Gordon model in the full subcritical regime","venue":"math.PR","work_id":"94876580-7638-49de-975a-853021790ed5","year":2018},"citing_paper":{"arxiv_id":"2606.26681","last_updated":"2026-07-07T02:00:59Z","snapshot_observed_at":"2026-08-19T13:38:24.399258Z","submitted_at":"2026-06-25T07:13:39Z","title":"Global well-posedness for generalized parabolic Anderson model on the whole plane","version":1},"reference_index":5,"source":"arxiv_source","source_observed_at":"2026-06-26T04:07:50.151762Z"},"links":{"cited_paper":"/paper/1808.02594","citing_paper":"/paper/2606.26681"},"observation_digest":"sha256:f6e357fd388918ae4d1455206345b38e641599a67ea434735df9dac5881e1a58","observation_id":"939c900a-8fe8-4834-a1d0-e04bdcf14f1f","resolution":{"observed_at":"2026-07-04T14:19:54.238391Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1808.02594","last_updated":"2018-08-08T01:44:04Z","snapshot_observed_at":"2026-08-14T18:43:33.143520Z","submitted_at":"2018-08-08T01:44:04Z","title":"The dynamical sine-Gordon model in the full subcritical regime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.02594","snapshot_observed_at":"2026-07-12T11:56:58.346375Z","title":"Chandra, M","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2606.26681","last_updated":"2026-07-07T02:00:59Z","snapshot_observed_at":"2026-08-19T13:38:24.399258Z","submitted_at":"2026-06-25T07:13:39Z","title":"Global well-posedness for generalized parabolic Anderson model on the whole plane","version":2},"reference_index":5,"source":"arxiv_source","source_observed_at":"2026-07-12T11:56:58.346375Z"},"links":{"cited_paper":"/paper/1808.02594","citing_paper":"/paper/2606.26681"},"observation_digest":"sha256:dececb161b8b17778129ed8004ebf613b936d11de77aced8c6d13deb7b7daec1","observation_id":"575e965d-044d-4e35-b9fd-12288c90b599","resolution":{"observed_at":"2026-07-12T11:56:58.346375Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.02594","last_updated":"2018-08-08T01:44:04Z","snapshot_observed_at":"2026-08-14T18:43:33.143520Z","submitted_at":"2018-08-08T01:44:04Z","title":"The dynamical sine-Gordon model in the full subcritical regime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.02594","snapshot_observed_at":"2026-08-01T09:56:22.128168Z","title":"The Dynamical Sine-","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.20632","last_updated":"2026-07-22T18:03:53Z","snapshot_observed_at":"2026-08-11T07:36:49.646456Z","submitted_at":"2026-07-22T18:03:53Z","title":"An FBSDE Construction of the Sine-Gordon EQFT for $\\beta^{2} < \\frac{6}{7}\\, 8\\pi$ and Perturbative Renormalization in the Full Subcritical Regime","version":1},"reference_index":19,"source":"arxiv_source","source_observed_at":"2026-08-01T09:56:22.128168Z"},"links":{"cited_paper":"/paper/1808.02594","citing_paper":"/paper/2607.20632"},"observation_digest":"sha256:3cf2cee537b73e5f99df4125e55d918ca2e3043324720d42c63a6e9408b5df26","observation_id":"6842f101-7489-41e3-a153-5ed0304fc3fb","resolution":{"observed_at":"2026-08-01T09:56:22.128168Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1808.02594/citation-record","integrity":"/paper/1808.02594/integrity","json":"/paper/1808.02594/citation-record.json","paper":"/paper/1808.02594"},"outbound":[],"paper":{"arxiv_id":"1808.02594","last_updated":"2018-08-08T01:44:04Z","latest_version":1,"primary_category":"math.PR","snapshot_observed_at":"2026-08-14T18:43:33.143520Z","submitted_at":"2018-08-08T01:44:04Z","title":"The dynamical sine-Gordon model in the full subcritical regime"},"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":"2026-08-19T06:32:44.657259+00:00","source":"crossref"},{"observed_at":"2026-08-19T06:32:39.956319+00:00","source":"retraction_watch"}],"thesis":"As of 19 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 7 inbound Pith citation observations for arXiv:1808.02594."}