{"as_of":"2026-08-13T09:27:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:c614a120ae897b15b5b0b39c3f5a3265e141d0549b0df417090fe2c46f6ee2be","coverage":[{"denominator":45,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":45,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-12T11:06:54.043258Z","state":"measured"},{"denominator":57,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":57,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-13T06:32:02.005865+00:00","state":"measured"},{"denominator":12,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":12,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T11:11:41.937303Z","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":"2026-07-04T19:00:04.400597Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-08-04T11:11:41.937303Z","title":"Einstein gravity from a matrix integral – Part II,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2510.06704","last_updated":"2026-07-01T06:20:29Z","snapshot_observed_at":"2026-08-08T02:16:52.301628Z","submitted_at":"2025-10-08T06:58:29Z","title":"Bootstrapping Yang-Mills matrix integrals","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-04T11:11:41.937303Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2510.06704"},"observation_digest":"sha256:87031820634f8e231a5d2c0fd21dde8ab39195ab2212454ce54a1487c3157807","observation_id":"7dcda7c7-c723-4c5c-9c9d-1faf7e025041","resolution":{"observed_at":"2026-08-04T11:11:41.937303Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-08-02T20:50:55.556446Z","title":"Komatsu, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.22318","last_updated":"2026-07-16T17:13:18Z","snapshot_observed_at":"2026-08-10T19:57:37.892469Z","submitted_at":"2026-02-25T19:00:02Z","title":"Twisting BFSS & IKKT","version":3},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-02T20:50:55.556446Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2602.22318"},"observation_digest":"sha256:3f17dd995b8a6aad2292c97967a46ad9d761137058f6187d8f7da8babd77935d","observation_id":"b01e9532-4522-4206-bfea-feebdb36cf20","resolution":{"observed_at":"2026-08-02T20:50:55.556446Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-13T08:29:23.093718Z","title":"Einstein gravity from a matrix integral. Part II,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.07500","last_updated":"2026-06-05T19:51:19Z","snapshot_observed_at":"2026-08-12T12:59:33.769752Z","submitted_at":"2026-04-08T18:37:26Z","title":"From Matrix Models to Gaussian Molecules and the Einstein-Hilbert Action","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-07-13T08:29:23.093718Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2604.07500"},"observation_digest":"sha256:8a0b85d2bc5e8cc2614fe20a7fc9a7f4e17e11fdeb4379155c1d7c1c7adf183e","observation_id":"b3b5fce6-b5b2-42af-ac02-b91f036bb12f","resolution":{"observed_at":"2026-07-13T08:29:23.093718Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":"2411.18678","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-04T19:00:04.400597Z","title":"Komatsu, A","venue":null,"work_id":"452a2e31-fcbc-4c09-8f59-f24553ad594f","year":2025},"citing_paper":{"arxiv_id":"2604.19836","last_updated":"2026-04-21T08:10:12Z","snapshot_observed_at":"2026-07-06T23:06:26.596990Z","submitted_at":"2026-04-21T08:10:12Z","title":"The emergence of (3+1)-dimensional expanding spacetime from complex Langevin simulations of the Lorentzian type IIB matrix model with deformations","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-05-10T02:39:49.953743Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2604.19836"},"observation_digest":"sha256:bb4a15a2213c3f0fa0b1be7bb55a64324fb5be1df3c7a24a99e424c2a8a087d7","observation_id":"4c3f2d8b-a231-4a87-9d52-c50a1db728e8","resolution":{"observed_at":"2026-05-11T12:51:08.117326Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":"2411.18678","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-04T19:00:04.400597Z","title":"Komatsu, A","venue":null,"work_id":"452a2e31-fcbc-4c09-8f59-f24553ad594f","year":2025},"citing_paper":{"arxiv_id":"2604.25052","last_updated":"2026-05-04T20:57:27Z","snapshot_observed_at":"2026-07-06T23:10:57.164248Z","submitted_at":"2026-04-27T23:06:44Z","title":"Path integral for the closed superstring and the matrix model","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-05-08T02:20:18.623525Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2604.25052"},"observation_digest":"sha256:0c231cd5210967835f6f2e29f9115696148b5dcaccd1b1718c29d83854f3f867","observation_id":"0e64d5ae-8fed-4ed0-b013-bdd7ed80b091","resolution":{"observed_at":"2026-05-11T22:51:22.812120Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":"2411.18678","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-04T19:00:04.400597Z","title":"Komatsu, A","venue":null,"work_id":"452a2e31-fcbc-4c09-8f59-f24553ad594f","year":2025},"citing_paper":{"arxiv_id":"2605.10720","last_updated":"2026-07-07T21:40:11Z","snapshot_observed_at":"2026-08-07T18:51:28.810868Z","submitted_at":"2026-05-11T15:29:26Z","title":"Regularized Master-Field Approximation for Large-$N$ Reduced Matrix Models","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-05-12T04:17:02.143135Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2605.10720"},"observation_digest":"sha256:b0c40236a31280fef02c5691858adae6d06304842009b3cd340096cdf40cc0cb","observation_id":"668d1a80-bd00-496b-82de-7ce722729858","resolution":{"observed_at":"2026-05-12T06:26:25.564987Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":"2411.18678","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-04T19:00:04.400597Z","title":"Komatsu, A","venue":null,"work_id":"452a2e31-fcbc-4c09-8f59-f24553ad594f","year":2025},"citing_paper":{"arxiv_id":"2605.10720","last_updated":"2026-07-07T21:40:11Z","snapshot_observed_at":"2026-08-07T18:51:28.810868Z","submitted_at":"2026-05-11T15:29:26Z","title":"Regularized Master-Field Approximation for Large-$N$ Reduced Matrix Models","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-06-30T22:29:22.990935Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2605.10720"},"observation_digest":"sha256:0b8f0596ff7537d3a1e3358cf5a714be1898b086797dd0d17ea5b05d8d681b73","observation_id":"df5d4ccb-66db-412e-8788-2d78a3b3abd0","resolution":{"observed_at":"2026-07-01T13:55:46.647305Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":"2411.18678","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-04T19:00:04.400597Z","title":"Komatsu, A","venue":null,"work_id":"452a2e31-fcbc-4c09-8f59-f24553ad594f","year":2025},"citing_paper":{"arxiv_id":"2605.13294","last_updated":"2026-05-13T10:07:26Z","snapshot_observed_at":"2026-07-06T23:24:52.373554Z","submitted_at":"2026-05-13T10:07:26Z","title":"Quantum spacetime and quantum fluctuations in the IKKT model at weak coupling","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-05-14T18:45:25.446400Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2605.13294"},"observation_digest":"sha256:f70986c3e1c15c9cd73e4480171e4034af37fc4a6fe14ada34b7401433bc8301","observation_id":"b90761bc-cd88-412f-83d6-cafd6497d313","resolution":{"observed_at":"2026-05-14T18:47:36.356111Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":"2411.18678","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-04T19:00:04.400597Z","title":"Komatsu, A","venue":null,"work_id":"452a2e31-fcbc-4c09-8f59-f24553ad594f","year":2025},"citing_paper":{"arxiv_id":"2606.24577","last_updated":"2026-06-24T01:41:46Z","snapshot_observed_at":"2026-08-12T15:26:21.057546Z","submitted_at":"2026-06-23T13:42:13Z","title":"Description of curved spacetimes by finite-size matrices in the type IIB matrix model","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-06-25T22:17:14.418193Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2606.24577"},"observation_digest":"sha256:c98c7682d8affad8c1a18ad9cafb65d3143cd8c3d9253100ccacabc2166003ce","observation_id":"420d52a0-7443-4837-9311-6521535305d3","resolution":{"observed_at":"2026-07-04T19:00:04.403135Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":"2411.18678","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-04T19:00:04.400597Z","title":"Komatsu, A","venue":null,"work_id":"452a2e31-fcbc-4c09-8f59-f24553ad594f","year":2025},"citing_paper":{"arxiv_id":"2606.27333","last_updated":"2026-06-25T17:45:36Z","snapshot_observed_at":"2026-07-07T00:01:34.696890Z","submitted_at":"2026-06-25T17:45:36Z","title":"The IKKT renormalization group flow is IIB: toward zero-d holography","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-06-26T02:17:48.500904Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2606.27333"},"observation_digest":"sha256:50e27329bb82bb9f574b0162c6d660d54d3a65308809fd5aca86dbdf772caa75","observation_id":"fbff5969-3b62-40a1-9bc4-9c20a1964ac3","resolution":{"observed_at":"2026-07-04T14:49:56.024387Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-08-01T07:02:47.123217Z","title":"Einstein gravity from a matrix integral – Part II,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.21593","last_updated":"2026-07-23T17:59:53Z","snapshot_observed_at":"2026-08-02T21:38:12.178035Z","submitted_at":"2026-07-23T17:59:53Z","title":"On the strong coupling limit of Yang-Mills matrix models","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-01T07:02:47.123217Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2607.21593"},"observation_digest":"sha256:55d654faade1bfbf20bd0bbd01e78ea9430d95e6b7766532acbd6ab555227ecf","observation_id":"4a3b7fcd-7a6e-4408-8f6f-ae98953f9ac4","resolution":{"observed_at":"2026-08-01T07:02:47.123217Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.18678","snapshot_observed_at":"2026-07-31T00:53:54.269563Z","title":"Einstein gravity from a matrix integral – Part II,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.25116","last_updated":"2026-07-27T22:22:57Z","snapshot_observed_at":"2026-08-10T12:53:14.460041Z","submitted_at":"2026-07-27T22:22:57Z","title":"Derivation of the NS5-brane limit of the plane wave matrix model","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-07-31T00:53:54.269563Z"},"links":{"cited_paper":"/paper/2411.18678","citing_paper":"/paper/2607.25116"},"observation_digest":"sha256:12acee91bbeb993470523c7363bc104a1cc9e264af9b53815f8485e15f353eba","observation_id":"12f5941f-1092-4bcf-8e0b-0410a0fc43a4","resolution":{"observed_at":"2026-07-31T00:53:54.269563Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2411.18678/citation-record","integrity":"/paper/2411.18678/integrity","json":"/paper/2411.18678/citation-record.json","paper":"/paper/2411.18678"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9310026","last_updated":"2009-03-20T21:49:19Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"1993-10-19T14:17:10Z","title":"Dimensional Reduction in Quantum Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9310026","snapshot_observed_at":"2026-08-12T11:06:53.865539Z","title":"Dimensional reduction in quantum gravity,","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.865539Z"},"links":{"cited_paper":"/paper/gr-qc/9310026","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:7891593533ba681b983fcb84c1b9ce3776996a9d1ed86b7b686ed825062fa3fc","observation_id":"53d6afcb-1fcc-4526-b5ff-1ce9e134b1a4","resolution":{"observed_at":"2026-08-12T11:06:53.865539Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9409089","last_updated":"1994-09-28T01:12:55Z","snapshot_observed_at":"2026-07-07T05:06:21.473375Z","submitted_at":"1994-09-15T23:14:18Z","title":"The World as a Hologram","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9409089","snapshot_observed_at":"2026-08-12T11:06:53.870442Z","title":"The World as a hologram,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.870442Z"},"links":{"cited_paper":"/paper/hep-th/9409089","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:0d23378dd722760364839d8d62812d94d20469b996dad15b0aaf745f1094b9e2","observation_id":"ac25a59e-e7ff-4e34-b0c6-6a924de43ae8","resolution":{"observed_at":"2026-08-12T11:06:53.870442Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9711200","last_updated":"1998-01-22T15:42:41Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"1997-11-27T23:53:13Z","title":"The Large N Limit of Superconformal Field Theories and Supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9711200","snapshot_observed_at":"2026-08-12T11:06:53.874885Z","title":"The Large N limit of superconformal field theories and supergravity,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.874885Z"},"links":{"cited_paper":"/paper/hep-th/9711200","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:15a802a8d61836c5ffc5b763c7bda87b3c386f462ceee5a72717a0a6644f5675","observation_id":"9867442d-ec69-4d9f-b757-0f01309aa67d","resolution":{"observed_at":"2026-08-12T11:06:53.874885Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.676456Z","title":"A Planar Diagram Theory for Strong Interactions,","venue":null,"work_id":"09002ef2-0d9e-48ae-a9d1-8898ea3b8431","year":1974},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.879497Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:86cbf3286e1bdcd22b22f6c529bccd1c85d17c661fc9ea029672a2fd1ef9c182","observation_id":"16689f69-dc1b-4584-b354-84f136b194fb","resolution":{"observed_at":"2026-08-12T11:06:54.680888Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2410.18173","last_updated":"2025-07-26T21:43:04Z","snapshot_observed_at":"2026-08-12T22:16:28.489873Z","submitted_at":"2024-10-23T18:00:01Z","title":"Einstein gravity from a matrix integral -- Part I","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.18173","snapshot_observed_at":"2026-08-12T11:06:53.883382Z","title":"Einstein gravity from a matrix integral – Part I,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.883382Z"},"links":{"cited_paper":"/paper/2410.18173","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:fc2047304ef1d7989a494b8737f31613accec2b9718f00936f35cea8c6c87e44","observation_id":"86184a4f-0423-4700-9589-f47a48ebe9b4","resolution":{"observed_at":"2026-08-12T11:06:53.883382Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.663503Z","title":"Strings in Less Than One-Dimension,","venue":null,"work_id":"1f0368d2-63dc-4603-9ced-f6fd88cb77e6","year":1990},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.887437Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:0b44ffd9bbe68b2f396ba8a76b3d7e2b18c9b724ed192435d286f7f34646566c","observation_id":"2ed47ae4-8189-452d-b5d1-4c0a547e014b","resolution":{"observed_at":"2026-08-12T11:06:54.667407Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.651470Z","title":"Exactly Solvable Field Theories of Closed Strings,","venue":null,"work_id":"36e7bda6-4a91-48e1-af7c-bc154f1b1a2d","year":1990},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.891338Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:206f111511571f8b0a79f0ed022423d7324dbf4b46710e381625201071538778","observation_id":"49f18534-2b01-4885-8b1a-4905d4d0cfae","resolution":{"observed_at":"2026-08-12T11:06:54.655656Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2212.05999","last_updated":"2023-03-19T16:46:40Z","snapshot_observed_at":"2026-08-06T03:39:21.390874Z","submitted_at":"2022-12-12T16:00:55Z","title":"Deriving the Simplest Gauge-String Duality -- I: Open-Closed-Open Triality","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.05999","snapshot_observed_at":"2026-08-12T11:06:53.895609Z","title":"Deriving the Simplest Gauge-String Duality – I: Open-Closed-Open Triality,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.895609Z"},"links":{"cited_paper":"/paper/2212.05999","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:e6c638b6fc38213316bf2020dc76cf9dbd4a1d4d209f07201e9447b46fee6021","observation_id":"5647b2b8-7fd8-409b-bb96-675a57d1f6bd","resolution":{"observed_at":"2026-08-12T11:06:53.895609Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.10846","last_updated":"2024-01-16T13:25:23Z","snapshot_observed_at":"2026-07-06T16:20:44.981294Z","submitted_at":"2023-09-19T18:00:04Z","title":"The Virasoro Minimal String","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.10846","snapshot_observed_at":"2026-08-12T11:06:53.899647Z","title":"The Virasoro minimal string,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.899647Z"},"links":{"cited_paper":"/paper/2309.10846","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:8fdb87f6086095de5a5e459117ea91e6891ba7391b104471deedeadef5919a01","observation_id":"1ce6ba46-e7cc-4cd2-92d6-57d675df2d5e","resolution":{"observed_at":"2026-08-12T11:06:53.899647Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:53.904128Z","title":"A large-n reduced model as superstring,","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.904128Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:da095ba203b5d71ec4d6295391ba1b56ba6c0f81012d3bd79d4a87729f03179a","observation_id":"aa94cf7a-d83c-4d85-b105-0123aae1d94b","resolution":{"observed_at":"2026-08-12T11:06:53.904128Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1126-6708/2002/08/022","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.086285Z","title":"Matrix strings in pp-wave backgrounds from deformed super yang-mills theory,","venue":null,"work_id":"03b47f16-5cd4-4072-bd23-ba173ca08511","year":2002},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.907968Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:ff2e10455a6bb9adcc2fba83869114e306f7ecf7b805f4277366c5c0c4769450","observation_id":"c9bafc46-ea2c-4a21-b4e3-7e56036cc94d","resolution":{"observed_at":"2026-08-12T11:06:54.090187Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.18706","last_updated":"2024-09-27T12:50:47Z","snapshot_observed_at":"2026-08-12T22:36:05.120246Z","submitted_at":"2024-09-27T12:50:47Z","title":"The Polarised IKKT Matrix Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.18706","snapshot_observed_at":"2026-08-12T11:06:53.911908Z","title":"The Polarised IKKT Matrix Model,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.911908Z"},"links":{"cited_paper":"/paper/2409.18706","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:f56c82c8c33588029687a4fc50ce395d911cc7d079c560b20a15c65c6cb556a2","observation_id":"73ef2438-47e1-4da2-b0aa-e3d00b94ee88","resolution":{"observed_at":"2026-08-12T11:06:53.911908Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.639742Z","title":"A Possible constructive approach to (SUPER phi**3) in four-dimensions. 1. Euclidean formulation of the model,","venue":null,"work_id":"6c798d00-5ccd-4f22-b32c-6c52ab8e50f7","year":1978},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.915833Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:aca90c359b00e0c32187ffacc9c936050050690277e750845e9a6e95610c63b0","observation_id":"8fac6aed-ebdb-49ea-8ba6-8fb045e31b31","resolution":{"observed_at":"2026-08-12T11:06:54.643706Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0301120","last_updated":"2003-01-29T04:24:49Z","snapshot_observed_at":"2026-08-04T01:06:16.029780Z","submitted_at":"2003-01-17T02:11:12Z","title":"Instantons of M(atrix) Theory in PP-Wave Background","version":2},"cited_work":{"arxiv_id":"hep-th/0301120","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/0301120","snapshot_observed_at":"2026-08-12T11:06:54.513422Z","title":"Instantons of M(atrix) Theory in PP-Wave Background","venue":"hep-th","work_id":"974e501d-3a21-47c9-ae6b-78ebf432f6d6","year":2003},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.919687Z"},"links":{"cited_paper":"/paper/hep-th/0301120","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:73833697f6421042594b1d8b00f5f1ae5c5ca0f6ba5cab4e97299127f4d06836","observation_id":"a28c1965-48d7-4007-ae65-20d3717716d0","resolution":{"observed_at":"2026-08-12T11:06:54.517706Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0103159","last_updated":"2001-04-23T09:10:56Z","snapshot_observed_at":"2026-07-07T04:39:24.857155Z","submitted_at":"2001-03-20T10:07:18Z","title":"Convergent Yang-Mills Matrix Theories","version":2},"cited_work":{"arxiv_id":"hep-th/0103159","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/0103159","snapshot_observed_at":"2026-08-12T11:06:54.497347Z","title":"Convergent Yang-Mills Matrix Theories","venue":"hep-th","work_id":"283ae115-c4f2-40a4-aa6d-fa057c7012d4","year":2001},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.923712Z"},"links":{"cited_paper":"/paper/hep-th/0103159","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:5af5d9eb5f5570f7127cb516654025d252cabd0c6f613cc73d4f27fb49772149","observation_id":"cb6c3f19-ca70-4940-8901-ef447e1c85a5","resolution":{"observed_at":"2026-08-12T11:06:54.501249Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1401.5079","last_updated":"2014-03-10T11:41:01Z","snapshot_observed_at":"2026-07-06T03:33:51.219885Z","submitted_at":"2014-01-20T21:00:27Z","title":"Emergent bubbling geometries in the plane wave matrix model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1401.5079","snapshot_observed_at":"2026-08-12T11:06:53.927658Z","title":"Emergent bubbling geometries in the plane wave matrix model,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.927658Z"},"links":{"cited_paper":"/paper/1401.5079","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:efd8fcaf9441b25acf4258796a567ee1a9a39d971e2f3497ee05306efe3ab920","observation_id":"31d1dd92-1da0-4c55-922b-1716f7e66a4f","resolution":{"observed_at":"2026-08-12T11:06:53.927658Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.1337","last_updated":"2014-07-05T20:02:21Z","snapshot_observed_at":"2026-08-08T04:51:47.658651Z","submitted_at":"2014-06-05T11:13:36Z","title":"Emergent bubbling geometries in gauge theories with SU(2|4) symmetry","version":2},"cited_work":{"arxiv_id":"1406.1337","doi":null,"metadata_source":"pith","pith_arxiv_id":"1406.1337","snapshot_observed_at":"2026-08-12T11:06:54.468842Z","title":"Emergent bubbling geometries in gauge theories with SU(2|4) symmetry","venue":"hep-th","work_id":"eb3b5578-0ccb-4d6c-a6f1-30038dd80a9b","year":2014},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.931973Z"},"links":{"cited_paper":"/paper/1406.1337","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:51ff5743e02812f79e3dc4fdababbe29f843ad081aec327ac35c607ea8e98948","observation_id":"ba8589d9-81b9-4acd-8f20-0800fea6d211","resolution":{"observed_at":"2026-08-12T11:06:54.473479Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0806.4191","last_updated":"2008-07-31T06:42:45Z","snapshot_observed_at":"2026-07-06T01:41:35.334177Z","submitted_at":"2008-06-26T19:56:12Z","title":"Spectral curves, emergent geometry, and bubbling solutions for Wilson loops","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0806.4191","snapshot_observed_at":"2026-08-12T11:06:53.936321Z","title":"Spectral curves, emergent geometry, and bubbling solutions for Wilson loops,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.936321Z"},"links":{"cited_paper":"/paper/0806.4191","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:b657ba58baa30cc15cdb00174342a78417a05ff8df40beb1ad7409ce64c46160","observation_id":"5fb534e7-eb22-44bd-bc71-cbfb71b3c420","resolution":{"observed_at":"2026-08-12T11:06:53.936321Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:53.940555Z","title":"SolvingN = 4 SYM BCFT matrix models at large N,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.940555Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:0ee72452a9de18437e5b726e3c2645c9c0cce18f91b290e935a5cfd1df4d0fe5","observation_id":"cea7d789-3dda-44c4-aba6-472b8d2a462e","resolution":{"observed_at":"2026-08-12T11:06:53.940555Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9908038","last_updated":"1999-08-04T18:31:22Z","snapshot_observed_at":"2026-08-08T15:45:07.008054Z","submitted_at":"1999-08-04T18:31:22Z","title":"IIB Matrix Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9908038","snapshot_observed_at":"2026-08-12T11:06:53.944164Z","title":"IIB matrix model,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.944164Z"},"links":{"cited_paper":"/paper/hep-th/9908038","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:739c1bb2a4f07630fc95192e159efad40ed75a8d792cf1366385729ffbfab062","observation_id":"1bbd3a86-33c7-473f-9a5b-f7f66082d53a","resolution":{"observed_at":"2026-08-12T11:06:53.944164Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9711107","last_updated":"1998-01-30T15:10:55Z","snapshot_observed_at":"2026-07-07T05:15:11.082503Z","submitted_at":"1997-11-17T23:48:12Z","title":"D-particle bound states and the D-instanton measure","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9711107","snapshot_observed_at":"2026-08-12T11:06:53.948084Z","title":"D Particle bound states and the D instanton measure,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.948084Z"},"links":{"cited_paper":"/paper/hep-th/9711107","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:9c17279e406862459c3abfec76400df781c63f708061e9a97d1ed724ed4b2910","observation_id":"acbd8f9b-19bf-4c69-9217-5b021f3e5cd0","resolution":{"observed_at":"2026-08-12T11:06:53.948084Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9803265","last_updated":"1998-04-20T22:20:13Z","snapshot_observed_at":"2026-08-03T14:42:10.804127Z","submitted_at":"1998-04-01T00:41:16Z","title":"D-particle bound states and generalized instantons","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9803265","snapshot_observed_at":"2026-08-12T11:06:53.951979Z","title":"D particle bound states and generalized instantons,","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.951979Z"},"links":{"cited_paper":"/paper/hep-th/9803265","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:50b157537cec99232c7ad1d139f251f806b40ed8782fc12cc386cd1a79f91694","observation_id":"f1080dd4-44b2-40b3-88af-6ef309f01d91","resolution":{"observed_at":"2026-08-12T11:06:53.951979Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9804123","last_updated":"1998-04-30T12:53:31Z","snapshot_observed_at":"2026-07-07T05:16:31.129096Z","submitted_at":"1998-04-20T20:23:53Z","title":"D-instanton partition functions","version":2},"cited_work":{"arxiv_id":"hep-th/9804123","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/9804123","snapshot_observed_at":"2026-08-12T11:06:54.343031Z","title":"D-instanton partition functions","venue":"hep-th","work_id":"a4f342b4-e102-4e28-a9bf-149eb2e9f4c7","year":1998},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.955586Z"},"links":{"cited_paper":"/paper/hep-th/9804123","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:604917db128b99476302ab4ceb4168e10b82b2e3bc6892b5bd00fe7f6868f3db","observation_id":"f4ae4dd5-d33f-4a58-bf6f-2330f29918e7","resolution":{"observed_at":"2026-08-12T11:06:54.346973Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0101071","last_updated":"2001-01-15T10:20:30Z","snapshot_observed_at":"2026-08-12T14:47:39.774769Z","submitted_at":"2001-01-11T17:23:35Z","title":"The Convergence of Yang-Mills Integrals","version":2},"cited_work":{"arxiv_id":"hep-th/0101071","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/0101071","snapshot_observed_at":"2026-08-12T11:06:54.326368Z","title":"The Convergence of Yang-Mills Integrals","venue":"hep-th","work_id":"c1df32cd-6c7e-414f-86ba-c0044b93515a","year":2001},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.959173Z"},"links":{"cited_paper":"/paper/hep-th/0101071","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:d7e635671e6ec131d33f2f135dc31e735d0e91f627a01ca546e18e97cea2979b","observation_id":"e5930a6a-bcf8-4c39-b599-1320ff1b597a","resolution":{"observed_at":"2026-08-12T11:06:54.330658Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9803117","last_updated":"1998-04-01T19:11:43Z","snapshot_observed_at":"2026-08-09T04:16:42.464814Z","submitted_at":"1998-03-13T17:26:31Z","title":"Monte Carlo Approach to M-Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9803117","snapshot_observed_at":"2026-08-12T11:06:53.962782Z","title":"Monte Carlo approach to M theory,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.962782Z"},"links":{"cited_paper":"/paper/hep-th/9803117","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:80a302d9f6be0da3ee09fdc763edce0ab8d843a30802a087cc0dc4d83194a62f","observation_id":"ef190d93-baa0-4746-8b33-74f7427db7cf","resolution":{"observed_at":"2026-08-12T11:06:53.962782Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.627245Z","title":"Hardy, An introduction to the theory of numbers","venue":null,"work_id":"7e7260ba-32ee-4a59-8a35-ecd4bb0d065d","year":1979},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.967066Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:d43c1d9d43baaf352919df716636b02a81d4f29d766d0cf4fdc1a4f3d3683e61","observation_id":"6ce272c4-da9d-4748-82e9-22cf7927906b","resolution":{"observed_at":"2026-08-12T11:06:54.631726Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0202021","last_updated":"2002-02-26T21:57:42Z","snapshot_observed_at":"2026-07-07T04:42:32.986757Z","submitted_at":"2002-02-04T18:38:18Z","title":"Strings in flat space and pp waves from ${\\cal N}=4$ Super Yang Mills","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0202021","snapshot_observed_at":"2026-08-12T11:06:53.970665Z","title":"Strings in flat space and pp waves from N=4 superYang-Mills,","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.970665Z"},"links":{"cited_paper":"/paper/hep-th/0202021","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:e96b968d5262b42a4ba65dfa88d8166aeea0e4de61b1d369b858fec26ada0e12","observation_id":"f54ce327-e717-4bd3-8e71-28c8efa227f9","resolution":{"observed_at":"2026-08-12T11:06:53.970665Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1211.0364","last_updated":"2012-11-22T08:35:31Z","snapshot_observed_at":"2026-07-06T02:59:01.101873Z","submitted_at":"2012-11-02T04:32:55Z","title":"Exact results for perturbative partition functions of theories with SU(2|4) symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1211.0364","snapshot_observed_at":"2026-08-12T11:06:53.974857Z","title":"Exact results for perturbative partition functions of theories with SU(2|4) symmetry,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.974857Z"},"links":{"cited_paper":"/paper/1211.0364","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:3bacdb4b7814fb2eb761db424744cd19c0cf6b1ed1a6a7c58b7acd356173c2fa","observation_id":"8f04bd37-7f51-43c0-ace8-ad4f04b9712d","resolution":{"observed_at":"2026-08-12T11:06:53.974857Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0712.2824","last_updated":"2012-09-20T05:34:12Z","snapshot_observed_at":"2026-08-07T22:53:33.873038Z","submitted_at":"2007-12-17T21:12:42Z","title":"Localization of gauge theory on a four-sphere and supersymmetric Wilson loops","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0712.2824","snapshot_observed_at":"2026-08-12T11:06:53.982479Z","title":"Localization of gauge theory on a four-sphere and supersymmetric Wilson loops,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.982479Z"},"links":{"cited_paper":"/paper/0712.2824","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:f44e6ad0a772e1556ff43d53c652611766c99b6687221f03b7ee6def43ea6f44","observation_id":"a04f2886-9f94-467a-8288-426834d8fa81","resolution":{"observed_at":"2026-08-12T11:06:53.982479Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9308128","last_updated":"1993-09-05T20:38:00Z","snapshot_observed_at":"2026-07-07T05:03:46.654645Z","submitted_at":"1993-08-27T10:32:00Z","title":"A Ten-Dimensional Super-Yang-Mills Action with Off-Shell Supersymmetry","version":3},"cited_work":{"arxiv_id":"hep-th/9308128","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/9308128","snapshot_observed_at":"2026-08-12T11:06:54.262551Z","title":"A Ten-Dimensional Super-Yang-Mills Action with Off-Shell Supersymmetry","venue":"hep-th","work_id":"e69062ab-fd82-4289-b19d-bafb570a3f60","year":1993},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.986268Z"},"links":{"cited_paper":"/paper/hep-th/9308128","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:157023ec968c67fe1ad996c45c90cf730a43fa012dd25665631eb7580b670438","observation_id":"ba13078f-e1fd-4060-9df6-f738efd5ccf2","resolution":{"observed_at":"2026-08-12T11:06:54.266875Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.614415Z","title":"An Introduction to Localisation and Supersymmetry in Curved Space,","venue":null,"work_id":"149e8342-ce8b-4cab-9d94-29396566a61e","year":2013},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.989920Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:8f4b827d4ca638704b414f095c2c3927f2f5536e6a25417221e56783393d5b26","observation_id":"57f75784-a749-4922-ac29-5e67fdc59de6","resolution":{"observed_at":"2026-08-12T11:06:54.618958Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0908.0684","last_updated":"2010-01-05T12:51:49Z","snapshot_observed_at":"2026-08-12T19:30:19.273629Z","submitted_at":"2009-08-05T19:22:27Z","title":"Scattering into the fifth dimension of N=4 super Yang-Mills","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0908.0684","snapshot_observed_at":"2026-08-12T11:06:53.993291Z","title":"Scattering into the fifth dimension of N=4 super Yang-Mills,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.993291Z"},"links":{"cited_paper":"/paper/0908.0684","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:3b915af2e6c04d4565da2dd18281305dc24e1202160cc72e874f24c9b77ef9cb","observation_id":"3c09ada5-2746-4460-a581-12812b613f38","resolution":{"observed_at":"2026-08-12T11:06:53.993291Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0909.4559","last_updated":"2010-12-17T21:32:28Z","snapshot_observed_at":"2026-07-06T02:01:56.136724Z","submitted_at":"2009-09-24T21:33:30Z","title":"Exact Results for Wilson Loops in Superconformal Chern-Simons Theories with Matter","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0909.4559","snapshot_observed_at":"2026-08-12T11:06:53.997441Z","title":"Exact Results for Wilson Loops in Superconformal Chern-Simons Theories with Matter,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:53.997441Z"},"links":{"cited_paper":"/paper/0909.4559","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:a27ac326968cc37b69ad037e26776be513df1ea803e726cded03ab810506ef67","observation_id":"afcb2da2-34d5-4b2e-a2e3-912495583c31","resolution":{"observed_at":"2026-08-12T11:06:53.997441Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1143/ptp.99.713","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.071341Z","title":"Space-time structures from iib matrix model,","venue":null,"work_id":"6f9d613e-f0db-4749-aa30-446e0e96677f","year":1998},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.001248Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:9cb2af65f003f8f00284170fee5f698cff4884288b1fb6389a3193421698b509","observation_id":"cc97e005-38dc-41f0-b806-b66553c45d88","resolution":{"observed_at":"2026-08-12T11:06:54.077917Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.16471","last_updated":"2024-01-29T19:00:00Z","snapshot_observed_at":"2026-08-13T04:32:24.218237Z","submitted_at":"2024-01-29T19:00:00Z","title":"Gravity from quantum mechanics of finite matrices","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.16471","snapshot_observed_at":"2026-08-12T11:06:54.004953Z","title":"Gravity from quantum mechanics of finite matrices,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.004953Z"},"links":{"cited_paper":"/paper/2401.16471","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:1639833c9329c7f08a6d78bddd205f92b08e7ed2a911835c9a25881b95ab31e6","observation_id":"ab83822f-1a31-42bb-ac3e-2a6933d387ec","resolution":{"observed_at":"2026-08-12T11:06:54.004953Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.0055","last_updated":"2015-08-28T18:49:24Z","snapshot_observed_at":"2026-07-06T03:34:53.400053Z","submitted_at":"2014-02-01T06:20:20Z","title":"On the Ground State Wave Function of Matrix Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.0055","snapshot_observed_at":"2026-08-12T11:06:54.008780Z","title":"On the Ground State Wave Function of Matrix Theory,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.008780Z"},"links":{"cited_paper":"/paper/1402.0055","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:daa4f5f47b4af823667d81f9e538f16f30f4828f1bdcbcf8f5c0a261c5a0d7cc","observation_id":"24108fbe-bc43-42c6-9d71-6deac7c5aa50","resolution":{"observed_at":"2026-08-12T11:06:54.008780Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0108128","last_updated":"2001-09-04T15:11:47Z","snapshot_observed_at":"2026-07-07T04:40:58.562909Z","submitted_at":"2001-08-17T14:26:07Z","title":"Yang-Mills Matrix Theory","version":2},"cited_work":{"arxiv_id":"hep-th/0108128","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/0108128","snapshot_observed_at":"2026-08-12T11:06:54.198272Z","title":"Yang-Mills Matrix Theory","venue":"hep-th","work_id":"a543d46c-db3e-46d9-b486-c3e66b408979","year":2001},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.012992Z"},"links":{"cited_paper":"/paper/hep-th/0108128","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:1b07c376392b1061441d030949473738a76e7934ac8fb84d9f8c5cdba021b2e2","observation_id":"0f1e88e1-c0b7-4354-af6c-2d580073fafe","resolution":{"observed_at":"2026-08-12T11:06:54.202251Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0509235","last_updated":"2006-08-10T16:20:48Z","snapshot_observed_at":"2026-08-01T04:25:08.435504Z","submitted_at":"2005-09-30T16:29:29Z","title":"Fivebranes from gauge theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0509235","snapshot_observed_at":"2026-08-12T11:06:54.016830Z","title":"Fivebranes from gauge theory,","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.016830Z"},"links":{"cited_paper":"/paper/hep-th/0509235","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:3d9c20a6bad216cfdabf70d7343b5236bee5542b1013dbf2828b8682a5c1f63b","observation_id":"37ddb46c-d6cf-4bcb-b9f9-2c4ea34c041b","resolution":{"observed_at":"2026-08-12T11:06:54.016830Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.3566","last_updated":"2014-02-03T05:58:35Z","snapshot_observed_at":"2026-07-06T03:25:30.591661Z","submitted_at":"2013-10-14T05:42:45Z","title":"Notes on Mayer Expansions and Matrix Models","version":2},"cited_work":{"arxiv_id":"1310.3566","doi":null,"metadata_source":"pith","pith_arxiv_id":"1310.3566","snapshot_observed_at":"2026-08-12T11:06:54.168827Z","title":"Notes on Mayer Expansions and Matrix Models","venue":"hep-th","work_id":"8bebd166-dc77-49b8-9675-dc7a03a9102c","year":2013},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.020576Z"},"links":{"cited_paper":"/paper/1310.3566","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:7925e1ced2ef657e57bdeb8f740eacc15ff853f2d8097d409bc0c863624f7404","observation_id":"7f5935ea-15c8-41de-8d23-273ecb116d81","resolution":{"observed_at":"2026-08-12T11:06:54.173797Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1910.08555","last_updated":"2019-10-18T18:00:00Z","snapshot_observed_at":"2026-08-05T10:30:31.652784Z","submitted_at":"2019-10-18T18:00:00Z","title":"Supersymmetric Yang-Mills, Spherical Branes, and Precision Holography","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.08555","snapshot_observed_at":"2026-08-12T11:06:54.024496Z","title":"Supersymmetric Yang-Mills, Spherical Branes, and Precision Holography,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.024496Z"},"links":{"cited_paper":"/paper/1910.08555","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:c06c4304d400d137c9ec899d7f7ad51b41977a4589e2e4f75b23fdcb66fd369a","observation_id":"90cc6efb-6a81-4151-9ba3-bc4717566fde","resolution":{"observed_at":"2026-08-12T11:06:54.024496Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.09974","last_updated":"2024-05-31T21:28:10Z","snapshot_observed_at":"2026-07-06T15:04:56.367057Z","submitted_at":"2023-03-17T13:47:42Z","title":"Scaling similarities and quasinormal modes of D0 black hole solutions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.09974","snapshot_observed_at":"2026-08-12T11:06:54.028407Z","title":"Scaling similarities and quasinormal modes of D0 black hole solutions,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.028407Z"},"links":{"cited_paper":"/paper/2303.09974","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:22a7be6da425127c96dc260e30f522499082dfd04b5052066ea94a2518093ab4","observation_id":"7258c5b8-4503-49f1-89d8-6138e802e506","resolution":{"observed_at":"2026-08-12T11:06:54.028407Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.21376","last_updated":"2024-12-09T20:17:07Z","snapshot_observed_at":"2026-08-12T22:13:31.971296Z","submitted_at":"2024-10-28T18:00:01Z","title":"Spherical Branes and the BMN Matrix Quantum Mechanics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.21376","snapshot_observed_at":"2026-08-12T11:06:54.032074Z","title":"Spherical Branes and the BMN Matrix Quantum Mechanics,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.032074Z"},"links":{"cited_paper":"/paper/2410.21376","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:86a78761dd287fd35d0a44019b30ad352001d60f721ffb87849889dc46d4f507","observation_id":"c82b01df-2d0c-47d2-881c-978bfd593bdf","resolution":{"observed_at":"2026-08-12T11:06:54.032074Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.01372","last_updated":"2022-06-28T18:54:52Z","snapshot_observed_at":"2026-08-09T05:03:23.794769Z","submitted_at":"2022-02-03T02:15:39Z","title":"No Ensemble Averaging Below the Black Hole Threshold","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.01372","snapshot_observed_at":"2026-08-12T11:06:54.036070Z","title":"No ensemble averaging below the black hole threshold,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.036070Z"},"links":{"cited_paper":"/paper/2202.01372","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:98a2f915b4edb1e67814417263c81d3ec5e810e721d74349e0d53904e9454e36","observation_id":"9a55c481-d84e-467b-bfb0-27179b4add02","resolution":{"observed_at":"2026-08-12T11:06:54.036070Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-12T11:06:54.039622Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.039622Z"},"links":{"citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:513e73a46f03439b6cbcdd233096e2918d982ff1e9eba587237e5279dfcf2768","observation_id":"cc8087b4-4cd8-451d-bde7-894f42b069c4","resolution":{"observed_at":"2026-08-12T11:06:54.039622Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0610038","last_updated":"2007-12-14T11:04:19Z","snapshot_observed_at":"2026-08-02T14:58:45.582030Z","submitted_at":"2006-10-03T06:47:07Z","title":"Embedding of theories with SU(2|4) symmetry into the plane wave matrix model","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0610038","snapshot_observed_at":"2026-08-12T11:06:54.043258Z","title":"Embedding of theories with SU(2|4) symmetry into the plane wave matrix model,","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-12T11:06:54.043258Z"},"links":{"cited_paper":"/paper/hep-th/0610038","citing_paper":"/paper/2411.18678"},"observation_digest":"sha256:1ad78c1085c2e6cb800b2f84e10b1d28cfff7c3a8f785ce9bd2d838700b0ea9f","observation_id":"45ff1358-d4d6-4e6c-b2c5-86de5ad27319","resolution":{"observed_at":"2026-08-12T11:06:54.043258Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2411.18678","last_updated":"2025-07-26T21:48:51Z","latest_version":2,"primary_category":"hep-th","snapshot_observed_at":"2026-08-12T10:57:15.847298Z","submitted_at":"2024-11-27T19:00:00Z","title":"Einstein gravity from a matrix integral -- Part II"},"reference_resolution":{"displayed":45,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":29,"verified_exact":10,"verified_fuzzy":6},"total_outbound_references":45},"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":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 45 of 45 outbound references and 12 inbound Pith citation observations for arXiv:2411.18678."}