{"as_of":"2026-08-10T15:12:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:c1fe553629da2a432c0c6aafa8b67149a9101ecf50ed21d283fd6d704d6caa21","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":10,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":10,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":10,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":10,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-09T18:51:30.770886Z","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":"2026-06-30T00:24:04.831782Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-08-09T18:51:30.770886Z","title":"Okyay and A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.00521","last_updated":"2025-06-18T05:58:38Z","snapshot_observed_at":"2026-08-09T23:53:27.006973Z","submitted_at":"2025-02-01T18:49:33Z","title":"Formation of regular black hole from baryonic matter","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-09T18:51:30.770886Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2502.00521"},"observation_digest":"sha256:5a06ff4e51ae75308a88d15f5e820eb3b5ba3eed3f239fbcbf01cbaf01183edd","observation_id":"876ad47e-3817-4871-80fa-c9fa5dde4ac5","resolution":{"observed_at":"2026-08-09T18:51:30.770886Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-08-08T23:50:42.609437Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinor- mal modes and greybody factors,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.04044","last_updated":"2025-06-20T14:27:02Z","snapshot_observed_at":"2026-08-09T23:47:13.741408Z","submitted_at":"2025-02-06T13:04:15Z","title":"Analyzing Deflection Angles and Photon Sphere Dynamics of Magnetically Charged Black Holes in Nonlinear Electrodynamic","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-08T23:50:42.609437Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2502.04044"},"observation_digest":"sha256:1f4cc7c2b1dca654c8315480b2f8066cf544ec9652a73ee6ea4510cb1fda2139","observation_id":"513232fd-b490-40ea-b3c5-506ed1946414","resolution":{"observed_at":"2026-08-08T23:50:42.609437Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-08-06T16:19:57.191378Z","title":"Okyay and A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.13953","last_updated":"2025-07-18T14:21:03Z","snapshot_observed_at":"2026-08-10T00:57:13.314174Z","submitted_at":"2025-07-18T14:21:03Z","title":"Strong gravitational lensing by black hole in F(R) Euler Heisenberg Gravity's Rainbow","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-06T16:19:57.191378Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2507.13953"},"observation_digest":"sha256:8adfee06bd5687e015724b0c8697a91fafd16e3c47d81551c73313cb381642d8","observation_id":"7fcb4973-63df-4ca6-a295-e4fe98ce897b","resolution":{"observed_at":"2026-08-06T16:19:57.191378Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-07-15T12:04:34.107907Z","title":"Okyay and A","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2603.10097","last_updated":"2026-03-10T17:21:07Z","snapshot_observed_at":"2026-08-10T00:47:22.539744Z","submitted_at":"2026-03-10T17:21:07Z","title":"Optical and orbital characterization of spherically symmetric static black holes of self-gravitating new nonlinear electrodynamics model","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-07-15T12:04:34.107907Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2603.10097"},"observation_digest":"sha256:da2c45178a0b676bb485bf81fd8b19a5f022ad50222a9c166f2a3dd0e0cef3fa","observation_id":"06d948c9-c3f4-493f-b473-9616e62b9be9","resolution":{"observed_at":"2026-07-15T12:04:34.107907Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-07-13T16:36:36.896932Z","title":"Okyay and A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2603.27935","last_updated":"2026-04-05T14:31:48Z","snapshot_observed_at":"2026-08-07T04:42:45.230903Z","submitted_at":"2026-03-30T01:08:05Z","title":"Connection Between the Shadow Radius and Quasinormal Frequencies for Black Holes in STVG with Perfect Fluid Dark Matter","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-07-13T16:36:36.896932Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2603.27935"},"observation_digest":"sha256:7a2141ca1504def447261ebd4060066c9205041b1cc67dd1af5d25a5c56279e8","observation_id":"429c90d3-b44f-4250-8f6f-62e737d12ba2","resolution":{"observed_at":"2026-07-13T16:36:36.896932Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":"2108.07766","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-06-30T00:24:04.831782Z","title":"Okyay and A","venue":null,"work_id":"dc735880-df28-4ff6-9fbb-94192a6f4863","year":2022},"citing_paper":{"arxiv_id":"2604.02164","last_updated":"2026-06-21T15:56:24Z","snapshot_observed_at":"2026-07-31T14:54:12.582793Z","submitted_at":"2026-04-02T15:30:54Z","title":"Echoes of a hairy black hole from gravitational decoupling","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-13T20:49:33.386272Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2604.02164"},"observation_digest":"sha256:0c4a84c2c3542a2ccdb6148fc6bf6bd41bf46264ef74efceeafa9c595d0ca600","observation_id":"806ec9cd-6fe8-4eb2-96e1-9b4441c7471b","resolution":{"observed_at":"2026-05-13T20:53:16.028550Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-07-13T13:56:52.487777Z","title":"Okyay and A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2604.02164","last_updated":"2026-06-21T15:56:24Z","snapshot_observed_at":"2026-07-31T14:54:12.582793Z","submitted_at":"2026-04-02T15:30:54Z","title":"Echoes of a hairy black hole from gravitational decoupling","version":3},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-07-13T13:56:52.487777Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2604.02164"},"observation_digest":"sha256:3d50719b6d36c74b5a671c8aba596ac3eaaf7d41dfda95e1f8d1b324cf5bc4eb","observation_id":"cf7d4e6b-cc3c-4693-9931-3d0e501f5a5c","resolution":{"observed_at":"2026-07-13T13:56:52.487777Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":"2108.07766","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-06-30T00:24:04.831782Z","title":"Okyay and A","venue":null,"work_id":"dc735880-df28-4ff6-9fbb-94192a6f4863","year":2022},"citing_paper":{"arxiv_id":"2605.17647","last_updated":"2026-05-17T20:52:06Z","snapshot_observed_at":"2026-08-05T12:08:40.255345Z","submitted_at":"2026-05-17T20:52:06Z","title":"Scattering, absorption and greybody factor of scalar particles by Lorentz-violating charged black holes","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-05-19T22:47:53.234005Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2605.17647"},"observation_digest":"sha256:dbd346cedc2002c41416058498fcdfdcef025aeea0b1153d2fc8b1cec3f1e28d","observation_id":"91e1d008-b2e1-427a-bd6f-4cc77d61188b","resolution":{"observed_at":"2026-05-19T22:52:50.588282Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":"2108.07766","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-06-30T00:24:04.831782Z","title":"Okyay and A","venue":null,"work_id":"dc735880-df28-4ff6-9fbb-94192a6f4863","year":2022},"citing_paper":{"arxiv_id":"2605.26369","last_updated":"2026-05-25T22:34:51Z","snapshot_observed_at":"2026-08-07T10:28:00.576831Z","submitted_at":"2026-05-25T22:34:51Z","title":"Energy extraction from NED-deformed rotating black holes via the Comisso-Asenjo reconnection process","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-06-29T20:20:54.407011Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2605.26369"},"observation_digest":"sha256:2fef07923bc9ebe64bafa38483eb48eff36bc7507f504a358e25259046897b1a","observation_id":"53df2a06-4911-4994-b466-bdd61916c26e","resolution":{"observed_at":"2026-06-30T00:24:04.833278Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.07766","snapshot_observed_at":"2026-08-01T17:57:55.296252Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinor- mal modes and greybody factors,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.17483","last_updated":"2026-07-20T02:14:13Z","snapshot_observed_at":"2026-08-10T09:45:16.546038Z","submitted_at":"2026-07-20T02:14:13Z","title":"Shadow of the generalized Vaidya black hole","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-01T17:57:55.296252Z"},"links":{"cited_paper":"/paper/2108.07766","citing_paper":"/paper/2607.17483"},"observation_digest":"sha256:4d3d34c73c02aadb68f5726ca9cc82f4ada8b9fbd4b0575cc01294670677a850","observation_id":"7d19d15c-e3d9-458e-bac8-f9e55071d99c","resolution":{"observed_at":"2026-08-01T17:57:55.296252Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2108.07766/citation-record","integrity":"/paper/2108.07766/integrity","json":"/paper/2108.07766/citation-record.json","paper":"/paper/2108.07766"},"outbound":[],"paper":{"arxiv_id":"2108.07766","last_updated":"2022-01-04T20:57:09Z","latest_version":3,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-08T13:59:34.847479Z","submitted_at":"2021-08-17T17:17:19Z","title":"Nonlinear electrodynamics effects on the black hole shadow, deflection angle, quasinormal modes and greybody factors"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 10 inbound Pith citation observations for arXiv:2108.07766."}