{"as_of":"2026-08-22T21:25:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:deb301566811c28dcd56ecb90e3c97ddfb72c9083a5f3eef19e1ddc716e9d50a","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":"2026-08-22T06:32:14.747728+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":"2026-08-15T22:21:39.688475Z","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":"2026-08-15T18:34:48.693933Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2502.20310","last_updated":"2025-05-25T13:37:31Z","snapshot_observed_at":"2026-08-20T18:37:28.388250Z","submitted_at":"2025-02-27T17:35:57Z","title":"Dual Non-Lorentzian Backgrounds for Matrix Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.20310","snapshot_observed_at":"2026-08-15T22:21:39.688475Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.07458","last_updated":"2025-08-25T20:40:39Z","snapshot_observed_at":"2026-08-20T15:06:11.805292Z","submitted_at":"2025-05-12T11:46:01Z","title":"Heterotic String Sigma Models: Discrete Light Cone Quantization and Its Current-Current Deformation","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-15T22:21:39.688475Z"},"links":{"cited_paper":"/paper/2502.20310","citing_paper":"/paper/2505.07458"},"observation_digest":"sha256:76eb49c7902f411d4937edb471218e7d5d9ca651a39dcd063f2908c02dd20bab","observation_id":"b2db6f97-9faf-4dcb-bd06-3b9a230de7ce","resolution":{"observed_at":"2026-08-15T22:21:39.688475Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.20310","last_updated":"2025-05-25T13:37:31Z","snapshot_observed_at":"2026-08-20T18:37:28.388250Z","submitted_at":"2025-02-27T17:35:57Z","title":"Dual Non-Lorentzian Backgrounds for Matrix Theories","version":2},"cited_work":{"arxiv_id":"2502.20310","doi":null,"metadata_source":"pith","pith_arxiv_id":"2502.20310","snapshot_observed_at":"2026-08-15T18:34:48.693933Z","title":"Dual Non-Lorentzian Backgrounds for Matrix Theories","venue":"hep-th","work_id":"76734253-46f5-48a1-b7dd-0acc225421e7","year":2025},"citing_paper":{"arxiv_id":"2506.19720","last_updated":"2026-06-05T09:56:37Z","snapshot_observed_at":"2026-08-18T03:41:08.717404Z","submitted_at":"2025-06-24T15:30:13Z","title":"Carroll Geometry Meets De Sitter Space via Holography","version":3},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-15T18:34:47.508724Z"},"links":{"cited_paper":"/paper/2502.20310","citing_paper":"/paper/2506.19720"},"observation_digest":"sha256:ee423fde9d629c184edc946d89725c8ea2624afea2ba72ac1ffb7ab3d4b4ad71","observation_id":"957551f1-ce57-47ea-9ec5-097b2dc68c7c","resolution":{"observed_at":"2026-08-15T18:34:48.697727Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-22T06:32:14.747728+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2502.20310","last_updated":"2025-05-25T13:37:31Z","snapshot_observed_at":"2026-08-20T18:37:28.388250Z","submitted_at":"2025-02-27T17:35:57Z","title":"Dual Non-Lorentzian Backgrounds for Matrix Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.20310","snapshot_observed_at":"2026-08-02T17:32:32.613440Z","title":"Dual non-Lorentzian backgrounds for matrix theories","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2603.24657","last_updated":"2026-07-15T13:05:52Z","snapshot_observed_at":"2026-08-15T05:26:37.762506Z","submitted_at":"2026-03-25T18:00:00Z","title":"An Introduction to String Newton-Cartan Holography and Integrability","version":2},"reference_index":136,"source":"pdf_text","source_observed_at":"2026-08-02T17:32:32.613440Z"},"links":{"cited_paper":"/paper/2502.20310","citing_paper":"/paper/2603.24657"},"observation_digest":"sha256:41e8f7da3098c368c788130e40028a8e0ae82b2931fb10ace4c366885822b668","observation_id":"e05ea38e-924e-4a6d-a7e3-f9c8b3eea0dc","resolution":{"observed_at":"2026-08-02T17:32:32.613440Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.20310","last_updated":"2025-05-25T13:37:31Z","snapshot_observed_at":"2026-08-20T18:37:28.388250Z","submitted_at":"2025-02-27T17:35:57Z","title":"Dual Non-Lorentzian Backgrounds for Matrix Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.20310","snapshot_observed_at":"2026-07-11T08:34:51.771594Z","title":"Dual non-Lorentzian backgrounds for matrix theories,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.05115","last_updated":"2026-08-05T14:54:54Z","snapshot_observed_at":"2026-08-19T05:44:34.602127Z","submitted_at":"2026-07-06T14:06:25Z","title":"From Galilei to Euclidean Carroll and the Alice Particle: The Times They Are a-Changin'","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-07-11T08:34:51.771594Z"},"links":{"cited_paper":"/paper/2502.20310","citing_paper":"/paper/2607.05115"},"observation_digest":"sha256:6c37bfdbbedc21fd5bff76177aa09cb2e49260d19a4ce8c80d4038c0c2823483","observation_id":"67407d64-edb6-4ed0-ba71-61b714d47d24","resolution":{"observed_at":"2026-07-11T08:34:51.771594Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2502.20310/citation-record","integrity":"/paper/2502.20310/integrity","json":"/paper/2502.20310/citation-record.json","paper":"/paper/2502.20310"},"outbound":[],"paper":{"arxiv_id":"2502.20310","last_updated":"2025-05-25T13:37:31Z","latest_version":2,"primary_category":"hep-th","snapshot_observed_at":"2026-08-20T18:37:28.388250Z","submitted_at":"2025-02-27T17:35:57Z","title":"Dual Non-Lorentzian Backgrounds for Matrix Theories"},"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":"2026-08-22T06:32:14.747728+00:00","source":"crossref"},{"observed_at":"2026-08-22T06:32:06.552537+00:00","source":"retraction_watch"}],"thesis":"As of 22 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2502.20310."}