{"as_of":"2026-08-22T01:33:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:f48d727d320b619e6ac697b7956d8293395320610053d280925f2da692a6782c","coverage":[{"denominator":103,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T13:01:40.743390Z","state":"measured"},{"denominator":101,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":101,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-06-28T12:04:26.176993Z","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":"2026-07-02T01:26:24.255632Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"cited_work":{"arxiv_id":"1908.07381","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1908.07381","snapshot_observed_at":"2026-07-02T01:26:24.255632Z","title":"Capozziello and G","venue":null,"work_id":"2e646879-1d30-484a-94ad-5ef3793f8c38","year":2019},"citing_paper":{"arxiv_id":"2606.02660","last_updated":"2026-06-01T07:16:50Z","snapshot_observed_at":"2026-08-15T04:24:25.921810Z","submitted_at":"2026-06-01T07:16:50Z","title":"Late-Time Cosmology and Structure Formation in Quadratic $f(Q)$ Gravity","version":1},"reference_index":118,"source":"pdf_text","source_observed_at":"2026-06-28T12:04:26.176993Z"},"links":{"cited_paper":"/paper/1908.07381","citing_paper":"/paper/2606.02660"},"observation_digest":"sha256:ec3d1e78de424422dfd91b0d725461c5bc2c78b3e4e31b7831c7c8ac25b1a2bc","observation_id":"c9e3d267-1169-4bb5-b7af-cb081d67c276","resolution":{"observed_at":"2026-07-02T01:26:24.257183Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/1908.07381/citation-record","integrity":"/paper/1908.07381/integrity","json":"/paper/1908.07381/citation-record.json","paper":"/paper/1908.07381"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1706.01773","last_updated":"2017-07-18T12:11:44Z","snapshot_observed_at":"2026-08-21T19:20:21.051728Z","submitted_at":"2017-06-03T16:27:11Z","title":"$D$-dimensional charged Anti-de-Sitter black holes in $f(T)$ gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.01773","snapshot_observed_at":"2026-08-14T13:01:40.229520Z","title":"D-dimens ional charged Anti-de-Sitter black holes in f (T ) gravity,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.229520Z"},"links":{"cited_paper":"/paper/1706.01773","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:fbb40e8f655b6b8139d8599d1e7a06b3d819bac165385233da62521d35e06972","observation_id":"fc12cf69-45e5-4ce4-ac92-be393f42a5fa","resolution":{"observed_at":"2026-08-14T13:01:40.229520Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1605.07614","last_updated":"2016-05-24T17:51:52Z","snapshot_observed_at":"2026-08-21T17:21:05.674455Z","submitted_at":"2016-05-24T17:51:52Z","title":"Solar System tests in $f(T)$ gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1605.07614","snapshot_observed_at":"2026-08-14T13:01:40.235127Z","title":"Solar System tests in f (T ) gravity,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.235127Z"},"links":{"cited_paper":"/paper/1605.07614","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:8e98b4f36b50e9fcb6564ed2c8230b32cdcb174c01cca0a2dad0c50d8ae320dc","observation_id":"1c787f20-3fa9-4155-a07c-80dcc2b2d050","resolution":{"observed_at":"2026-08-14T13:01:40.235127Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9805201","last_updated":"1998-05-15T03:59:02Z","snapshot_observed_at":"2026-08-14T08:08:09.999762Z","submitted_at":"1998-05-15T03:59:02Z","title":"Observational Evidence from Supernovae for an Accelerating Universe and a Cosmological Constant","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9805201","snapshot_observed_at":"2026-08-14T13:01:40.241093Z","title":"Observational evidence from sup ernovae for an accelerating universe and a cosmological constant,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.241093Z"},"links":{"cited_paper":"/paper/astro-ph/9805201","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:369e1f9aac1ec4205493431dc3569f1517e89fdd8c93698f20bc4f6b01a64b09","observation_id":"1cce7928-258b-4f05-ac1c-53f9b63bd6cd","resolution":{"observed_at":"2026-08-14T13:01:40.241093Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9812133","last_updated":"1998-12-08T03:27:34Z","snapshot_observed_at":"2026-08-14T18:17:06.144059Z","submitted_at":"1998-12-08T03:27:34Z","title":"Measurements of Omega and Lambda from 42 High-Redshift Supernovae","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9812133","snapshot_observed_at":"2026-08-14T13:01:40.246579Z","title":"Measurements of Ωand Λfrom 42 High-Redshift Supernovae,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.246579Z"},"links":{"cited_paper":"/paper/astro-ph/9812133","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:2d005d2d6cb8ab1517671341cbf6c2f54ac7f5aeec286db643a770a44026dd6c","observation_id":"e70fa9ec-5858-48f6-a201-2c6a2011d296","resolution":{"observed_at":"2026-08-14T13:01:40.246579Z","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":"2026-08-14T13:01:40.205057Z","title":"(7) The Lagrangian of TEGR theory is constructed from the torsio n scalar given by Eq","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.205057Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:bf63fc10151205b96354a8d9e685bcb0d1b608464c2568e6bb1f056cdcafeb52","observation_id":"49445b3b-8b18-4ef0-8ca7-e5c118a9f175","resolution":{"observed_at":"2026-08-14T13:01:40.205057Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0501171","last_updated":"2005-01-10T21:25:29Z","snapshot_observed_at":"2026-08-16T17:08:58.010532Z","submitted_at":"2005-01-10T21:25:29Z","title":"Detection of the Baryon Acoustic Peak in the Large-Scale Correlation Function of SDSS Luminous Red Galaxies","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0501171","snapshot_observed_at":"2026-08-14T13:01:40.259255Z","title":"Detection of the Baryon Acoustic Peak in the Large- Scale Correlation Function of SDSS Luminous Red Galaxies,","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.259255Z"},"links":{"cited_paper":"/paper/astro-ph/0501171","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:8b6987cbe9aa376786111ae7414cd6a149a1cdad72eeb14c33acf40637983c02","observation_id":"f332ced7-48ca-44ef-814b-026b11811fe2","resolution":{"observed_at":"2026-08-14T13:01:40.259255Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0809.0657","last_updated":"2008-12-16T19:43:43Z","snapshot_observed_at":"2026-08-18T21:18:36.522986Z","submitted_at":"2008-09-03T16:04:26Z","title":"Model-Independent Distance Measurements from Gamma-Ray Bursts and Constraints on Dark Energy","version":3},"cited_work":{"arxiv_id":"0809.0657","doi":null,"metadata_source":"pith","pith_arxiv_id":"0809.0657","snapshot_observed_at":"2026-08-14T13:01:42.356246Z","title":"Model-Independent Distance Measurements from Gamma-Ray Bursts and Constraints on Dark Energy","venue":"astro-ph","work_id":"b9da9927-3fe5-4169-b952-dfe6e83a8695","year":2008},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.265565Z"},"links":{"cited_paper":"/paper/0809.0657","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:6ec598d91d7da017744f30aab9350f4450a3fd8ab411b6e4be762db70f3e1b18","observation_id":"151bc612-7184-4515-a3df-3df88d284f5f","resolution":{"observed_at":"2026-08-14T13:01:42.361662Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0207347","last_updated":"2002-11-20T20:31:52Z","snapshot_observed_at":"2026-08-21T09:57:39.427633Z","submitted_at":"2002-07-16T21:40:00Z","title":"The Cosmological Constant and Dark Energy","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0207347","snapshot_observed_at":"2026-08-14T13:01:40.271572Z","title":"The cosmological constant an d dark energy,","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.271572Z"},"links":{"cited_paper":"/paper/astro-ph/0207347","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:039314d55c64735b6374780ae25f770387512f89c83fe03f1a0f6b774462b251","observation_id":"9f9a28df-d76d-40bd-ada5-46afeda2e897","resolution":{"observed_at":"2026-08-14T13:01:40.271572Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.5226","last_updated":"2013-06-04T19:07:35Z","snapshot_observed_at":"2026-08-21T07:58:09.218936Z","submitted_at":"2012-12-20T20:24:52Z","title":"Nine-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Cosmological Parameter Results","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.5226","snapshot_observed_at":"2026-08-14T13:01:40.252691Z","title":"Nine-year Wilkinson Microwave Anisotropy Probe (WMAP) Ob servations: Cosmological Parameter Results,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.252691Z"},"links":{"cited_paper":"/paper/1212.5226","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:89621a31327b14de03f106b83c25f88a837969354df184e1ce250f6fa7bde448","observation_id":"9dff90be-14e6-4eb1-8c22-66c91d8a8c02","resolution":{"observed_at":"2026-08-14T13:01:40.252691Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1409.7871","last_updated":"2014-09-28T05:18:45Z","snapshot_observed_at":"2026-08-20T17:01:51.418024Z","submitted_at":"2014-09-28T05:18:45Z","title":"Was Einstein Right? A Centenary Assessment","version":1},"cited_work":{"arxiv_id":"1409.7871","doi":null,"metadata_source":"pith","pith_arxiv_id":"1409.7871","snapshot_observed_at":"2026-08-14T13:01:42.312296Z","title":"Was Einstein Right? A Centenary Assessment","venue":"gr-qc","work_id":"17773da2-b749-4d5e-9d56-0cda7159eae4","year":2014},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.282203Z"},"links":{"cited_paper":"/paper/1409.7871","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:7c388d87af9403674cdaa762ebf664c2976e9a8a1a6bdc7c8026d14addea09a2","observation_id":"5eedfeb6-b6b6-48aa-955b-0b2204ef7faf","resolution":{"observed_at":"2026-08-14T13:01:42.317498Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0706.1146","last_updated":"2007-07-16T15:29:42Z","snapshot_observed_at":"2026-08-15T10:39:11.736066Z","submitted_at":"2007-06-08T09:59:25Z","title":"Extended Theories of Gravity and their Cosmological and Astrophysical Applications","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0706.1146","snapshot_observed_at":"2026-08-14T13:01:40.288512Z","title":"Extended theorie s of gravity and their cosmological and astrophysical appli cations,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.288512Z"},"links":{"cited_paper":"/paper/0706.1146","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:53804f93f3090f92392a6c22552136818a31efd9d67fcf1b109c66e5a209c854","observation_id":"e253886e-c1e0-45e9-a401-b8136628b2a5","resolution":{"observed_at":"2026-08-14T13:01:40.288512Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0011087","last_updated":"2000-11-24T11:26:53Z","snapshot_observed_at":"2026-08-18T14:19:58.713962Z","submitted_at":"2000-11-24T11:26:53Z","title":"Teleparallel Gravity: An Overview","version":1},"cited_work":{"arxiv_id":"gr-qc/0011087","doi":null,"metadata_source":"pith","pith_arxiv_id":"gr-qc/0011087","snapshot_observed_at":"2026-08-14T13:01:42.269773Z","title":"Teleparallel Gravity: An Overview","venue":"gr-qc","work_id":"cebb9c36-bff9-4df4-a240-e676296b3331","year":2000},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.293822Z"},"links":{"cited_paper":"/paper/gr-qc/0011087","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:d0ca0310d1108c912c7ec3c518b72f5d897b118054b7609bdd86c42bdb6b142a","observation_id":"12286777-9e8b-43ac-87dc-c630905ef94c","resolution":{"observed_at":"2026-08-14T13:01:42.275672Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T13:01:40.276883Z","title":"Binney and S","venue":null,"work_id":null,"year":1987},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.276883Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:b10ec481d06e2568e45a56cc802a095fe3f39c45fb2a28c7d90286c44932ee34","observation_id":"a9e0287c-976b-4da6-9686-0e7279701fa1","resolution":{"observed_at":"2026-08-14T13:01:40.276883Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0312008","last_updated":"2003-12-01T16:12:01Z","snapshot_observed_at":"2026-07-07T03:18:35.419334Z","submitted_at":"2003-12-01T16:12:01Z","title":"Selected Topics in Teleparallel Gravity","version":1},"cited_work":{"arxiv_id":"gr-qc/0312008","doi":null,"metadata_source":"pith","pith_arxiv_id":"gr-qc/0312008","snapshot_observed_at":"2026-08-14T13:01:42.243750Z","title":"Selected Topics in Teleparallel Gravity","venue":"gr-qc","work_id":"09b052ea-2b84-475c-9732-376440edfbdb","year":2003},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.304503Z"},"links":{"cited_paper":"/paper/gr-qc/0312008","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:116cb95c4e88987ff37dd355a766ec0d61c84a48bc5888f9eb03642ad9142b9c","observation_id":"831f0244-6239-4808-a8cb-6c0ca95050a2","resolution":{"observed_at":"2026-08-14T13:01:42.249414Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T13:01:40.212486Z","title":"It is worth noticing that the electric field of linear electrodyna mics is obtained as E = Ftr = ℵPPtr","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.212486Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:da0c98d98713a8c4f8ea0c3bc67d658ee8abc8a762d4d6496503d13b37e2565a","observation_id":"26d77e58-17eb-4edd-bf80-adebbb88ede6","resolution":{"observed_at":"2026-08-14T13:01:40.212486Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"physics/0503046","last_updated":"2005-03-06T19:44:56Z","snapshot_observed_at":"2026-08-10T09:14:04.220387Z","submitted_at":"2005-03-06T19:44:56Z","title":"Translation of Einstein's Attempt of a Unified Field Theory with Teleparallelism","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"physics/0503046","snapshot_observed_at":"2026-08-14T13:01:40.315463Z","title":"Translation of Einstein’s Att empt of a Unified Field Theory with Teleparallelism,","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.315463Z"},"links":{"cited_paper":"/paper/physics/0503046","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:58f1871770246430d55d943a9afcd855fe86dd14af0d1e7953619c39d63980a8","observation_id":"462711be-c9e3-4bdb-99a4-926ffcdf3360","resolution":{"observed_at":"2026-08-14T13:01:40.315463Z","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":"2026-08-14T13:01:40.218212Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.218212Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:ca202cbe93557405c5e5fde71ce9b92227d0588d1010aa76125a42da6799fc0d","observation_id":"5c4ec2ad-a106-49df-b15d-596e7cb2777a","resolution":{"observed_at":"2026-08-14T13:01:40.218212Z","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":"2026-08-14T13:01:40.299327Z","title":"Charged and Non-Charged Black Hole Solu tions in Mimetic Gravitational Theory,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.299327Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:3689da4d21315bd5ca527b8004828d294776fa6dbd2e6865e9bead277fb8e7a3","observation_id":"be332e9b-ff49-4a10-b586-7fc84efcb63d","resolution":{"observed_at":"2026-08-14T13:01:40.299327Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1303.3897","last_updated":"2013-03-15T20:18:27Z","snapshot_observed_at":"2026-08-15T00:25:00.028435Z","submitted_at":"2013-03-15T20:18:27Z","title":"The teleparallel equivalent of general relativity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1303.3897","snapshot_observed_at":"2026-08-14T13:01:40.309929Z","title":"The teleparallel equivalent of general re lativity,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.309929Z"},"links":{"cited_paper":"/paper/1303.3897","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:7444dbed4934184a072f3fb5d7e48013e13f70f1fffca1fac92f88b7382e63d8","observation_id":"09b60b0c-1d31-4bab-996f-7eb8a35fcfe7","resolution":{"observed_at":"2026-08-14T13:01:40.309929Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1981","last_updated":"2008-12-10T17:37:22Z","snapshot_observed_at":"2026-08-15T05:59:37.459123Z","submitted_at":"2008-12-10T17:37:22Z","title":"On Born-Infeld Gravity in Weitzenbock spacetime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1981","snapshot_observed_at":"2026-08-14T13:01:40.337313Z","title":"Born-Infeld gravity in Weit zenb¨ ock spacetime,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.337313Z"},"links":{"cited_paper":"/paper/0812.1981","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:5b9a9ac70bb2b9555e82629fb11b310db0f0c26bdf92ceb807c56b16b9c0af52","observation_id":"9c155743-236e-4b39-aeb0-45f23aa0def5","resolution":{"observed_at":"2026-08-14T13:01:40.337313Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0301008","last_updated":"2003-01-11T08:55:20Z","snapshot_observed_at":"2026-07-07T03:17:11.181957Z","submitted_at":"2003-01-04T08:49:38Z","title":"Stability of the Vacuum Non Singular Black Hole","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0301008","snapshot_observed_at":"2026-08-14T13:01:40.320822Z","title":"Stability of the vacuum nonsingula r black hole,","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.320822Z"},"links":{"cited_paper":"/paper/gr-qc/0301008","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:90ee79870aea91c0e235359b37dadcb238ce9966adb75153844b1d1aa1fbd748","observation_id":"37838673-05fe-4fe4-8ae8-b63a6c6767d3","resolution":{"observed_at":"2026-08-14T13:01:40.320822Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9703059","last_updated":"1997-06-23T19:44:46Z","snapshot_observed_at":"2026-08-17T01:07:04.911520Z","submitted_at":"1997-03-21T15:12:18Z","title":"Gravitational Lorentz Force and the Description of the Gravitational Interaction","version":2},"cited_work":{"arxiv_id":"gr-qc/9703059","doi":null,"metadata_source":"pith","pith_arxiv_id":"gr-qc/9703059","snapshot_observed_at":"2026-08-14T13:01:42.159479Z","title":"Gravitational Lorentz Force and the Description of the Gravitational Interaction","venue":"gr-qc","work_id":"d501c4bf-14ff-4c14-8c6a-bd098eaff9e3","year":1997},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.326512Z"},"links":{"cited_paper":"/paper/gr-qc/9703059","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:923bf3533e0fc9e684af80da709662a235fd18ecb76641d9f49d7c4053ddbb65","observation_id":"c6cbb4ef-c78b-4b62-b523-0db52236faac","resolution":{"observed_at":"2026-08-14T13:01:42.166177Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1704.05919","last_updated":"2017-04-24T11:25:27Z","snapshot_observed_at":"2026-08-19T02:31:12.497517Z","submitted_at":"2017-04-19T20:02:16Z","title":"Black Holes, Dark Wormholes and Solitons in f(T) Gravities","version":2},"cited_work":{"arxiv_id":"1704.05919","doi":null,"metadata_source":"pith","pith_arxiv_id":"1704.05919","snapshot_observed_at":"2026-08-14T13:01:42.133547Z","title":"Black Holes, Dark Wormholes and Solitons in f(T) Gravities","venue":"hep-th","work_id":"011453b9-ebf3-4351-96bc-9acc48077a71","year":2017},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.332105Z"},"links":{"cited_paper":"/paper/1704.05919","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:a1f8d06dabbd1c6beebe0bc7f2f3d1e2c07543bfcf04002d4207f7cec9abef43","observation_id":"567efd92-bfb5-49d9-b7a5-45d6f90efab7","resolution":{"observed_at":"2026-08-14T13:01:42.139554Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1612.05106","last_updated":"2017-01-29T08:07:18Z","snapshot_observed_at":"2026-08-18T22:19:31.077314Z","submitted_at":"2016-12-09T09:50:15Z","title":"Analytic rotating black hole solutions in $N$-dimensional $f(T)$ gravity","version":3},"cited_work":{"arxiv_id":"1612.05106","doi":null,"metadata_source":"pith","pith_arxiv_id":"1612.05106","snapshot_observed_at":"2026-08-14T13:01:42.025081Z","title":"Analytic rotating black hole solutions in $N$-dimensional $f(T)$ gravity","venue":"gr-qc","work_id":"4c6e0103-1465-4c25-bb51-9b7e4d3e8e37","year":2016},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.358107Z"},"links":{"cited_paper":"/paper/1612.05106","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:d5047fc8dc1438eefd112eac8133a60b68ccc0e96f358143ba1c08b389c3ce67","observation_id":"25fd76a7-e3eb-4c6c-8c90-ef4ba170257b","resolution":{"observed_at":"2026-08-14T13:01:42.031157Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0904.1767","last_updated":"2009-04-10T23:46:35Z","snapshot_observed_at":"2026-08-15T05:50:43.814858Z","submitted_at":"2009-04-10T23:46:35Z","title":"A type of Born-Infeld regular gravity and its cosmological consequences","version":1},"cited_work":{"arxiv_id":"0904.1767","doi":null,"metadata_source":"pith","pith_arxiv_id":"0904.1767","snapshot_observed_at":"2026-08-14T13:01:42.087437Z","title":"A type of Born-Infeld regular gravity and its cosmological consequences","venue":"gr-qc","work_id":"fffed67c-0121-4b3e-a35c-0c3e55349c98","year":2009},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.342570Z"},"links":{"cited_paper":"/paper/0904.1767","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:b63d8b7877908e574f949acfa005f0b18b778fe94b72b7c469835ec7d93eb956","observation_id":"f07ac9c5-6b0c-4cec-ae01-8e79fe6e8bb7","resolution":{"observed_at":"2026-08-14T13:01:42.093483Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1204.5294","last_updated":"2012-04-24T08:14:22Z","snapshot_observed_at":"2026-08-15T04:12:07.926154Z","submitted_at":"2012-04-24T08:14:22Z","title":"Accelerating f(T) gravity models constrained by recent cosmological data","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1204.5294","snapshot_observed_at":"2026-08-14T13:01:40.348055Z","title":"Accelerati ng f(T) gravity models constrained by recent cosmological d ata,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.348055Z"},"links":{"cited_paper":"/paper/1204.5294","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:7f2b0870833a0b048c935fdd08f817f9f1d1227631d78bcd449bf4acd711e178","observation_id":"56924899-7fb6-4f98-8e57-13ff22f68773","resolution":{"observed_at":"2026-08-14T13:01:40.348055Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1006.1120","last_updated":"2011-09-17T10:06:39Z","snapshot_observed_at":"2026-08-19T04:39:44.997511Z","submitted_at":"2010-06-06T17:13:07Z","title":"Accelerating universe from F(T) gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1006.1120","snapshot_observed_at":"2026-08-14T13:01:40.353062Z","title":"Accelerating universe from F(T ) gravity,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.353062Z"},"links":{"cited_paper":"/paper/1006.1120","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:13f37e70ec326a60b94696688823b8f9ef69c6270b7298850fab80b59e2f9f5a","observation_id":"908e09c8-102e-4bab-8dd0-22405f7c68a1","resolution":{"observed_at":"2026-08-14T13:01:40.353062Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1009.2459","last_updated":"2011-08-18T04:59:19Z","snapshot_observed_at":"2026-08-15T05:08:56.546378Z","submitted_at":"2010-09-13T17:44:02Z","title":"f(T) modified teleparallel gravity models as an alternative for holographic and new agegraphic dark energy models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1009.2459","snapshot_observed_at":"2026-08-14T13:01:40.379409Z","title":"f (T ) modified teleparallel gravity as an alternative for hologr aphic and new agegraphic dark energy models,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.379409Z"},"links":{"cited_paper":"/paper/1009.2459","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:16eb91590e61f1592649a546aa7f88b72c5debb2602cf3583addee5b4b2ef75f","observation_id":"4ccaea05-9fb3-4b4c-a0a9-5170226f6a53","resolution":{"observed_at":"2026-08-14T13:01:40.379409Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1007.3571","last_updated":"2011-11-09T14:07:17Z","snapshot_observed_at":"2026-08-15T05:13:23.114394Z","submitted_at":"2010-07-21T07:26:08Z","title":"New types of $f(T)$ gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1007.3571","snapshot_observed_at":"2026-08-14T13:01:40.363200Z","title":"New types of f( T) gravity,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.363200Z"},"links":{"cited_paper":"/paper/1007.3571","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:f81e02a340a03fc50ad4dac955a57967f9a710517da8dd56e9f3bec375993a0c","observation_id":"1de2758b-bc6c-4d1b-91d4-30b1492f2bbb","resolution":{"observed_at":"2026-08-14T13:01:40.363200Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1008.3188","last_updated":"2010-12-13T14:01:26Z","snapshot_observed_at":"2026-08-15T05:11:09.446904Z","submitted_at":"2010-08-18T23:46:58Z","title":"Observational information for f(T) theories and Dark Torsion","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1008.3188","snapshot_observed_at":"2026-08-14T13:01:40.368587Z","title":"Observational information for f (T ) theories and dark torsion,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.368587Z"},"links":{"cited_paper":"/paper/1008.3188","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:f61b32d938be893b3224b4fbcc8e94871ab49b40ff3a655d870f25b751fe5d8a","observation_id":"c291aa55-a441-4b85-af18-a4a9db316be7","resolution":{"observed_at":"2026-08-14T13:01:40.368587Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1007.0482","last_updated":"2010-10-15T03:34:50Z","snapshot_observed_at":"2026-08-18T15:15:07.550967Z","submitted_at":"2010-07-03T08:52:18Z","title":"Generic feature of future crossing of phantom divide in viable $f(R)$ gravity models","version":2},"cited_work":{"arxiv_id":"1007.0482","doi":null,"metadata_source":"pith","pith_arxiv_id":"1007.0482","snapshot_observed_at":"2026-08-14T13:01:41.959089Z","title":"Generic feature of future crossing of phantom divide in viable $f(R)$ gravity models","venue":"astro-ph.CO","work_id":"5c93ed51-5702-4ecb-81ac-902619a000fc","year":2010},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.374127Z"},"links":{"cited_paper":"/paper/1007.0482","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:3a76a230bda076d50d3cd5c241bfe21e71959cd6436659a50d7da0f8593c5c9d","observation_id":"e1c65e8d-6896-426f-a046-c82356fd3b8e","resolution":{"observed_at":"2026-08-14T13:01:41.964902Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1308.5789","last_updated":"2013-10-17T00:41:34Z","snapshot_observed_at":"2026-08-15T00:05:22.959181Z","submitted_at":"2013-08-27T08:24:41Z","title":"Conformal symmetry and accelerating cosmology in teleparallel gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.5789","snapshot_observed_at":"2026-08-14T13:01:40.399956Z","title":"Conform al symmetry and accelerating cosmology in teleparallel gra vity,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.399956Z"},"links":{"cited_paper":"/paper/1308.5789","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:7011d2f2c387e1ebb0c3479bf6e0bd2b58ac5b3c25f98368a36e19a9629e7759","observation_id":"1da545ed-1ac2-459e-824f-456e2acfea50","resolution":{"observed_at":"2026-08-14T13:01:40.399956Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1010.2215","last_updated":"2010-12-20T16:49:16Z","snapshot_observed_at":"2026-08-15T05:06:22.674430Z","submitted_at":"2010-10-11T20:02:15Z","title":"f(T) gravity mimicking dynamical dark energy. Background and perturbation analysis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1010.2215","snapshot_observed_at":"2026-08-14T13:01:40.384486Z","title":"f (T ) gravity mimicking dynamical dark energy. Background and p erturbation analysis,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.384486Z"},"links":{"cited_paper":"/paper/1010.2215","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:bfac8ea54089ec4cfbe5376086f0abf785425fe6c77686dbc4d448ac861d01d8","observation_id":"d2511755-00bf-42a4-a7c2-6bc4b5ec541d","resolution":{"observed_at":"2026-08-14T13:01:40.384486Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1104.4349","last_updated":"2011-10-05T21:46:17Z","snapshot_observed_at":"2026-08-15T04:48:40.154378Z","submitted_at":"2011-04-21T20:01:17Z","title":"Matter Bounce Cosmology with the f(T) Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1104.4349","snapshot_observed_at":"2026-08-14T13:01:40.389710Z","title":"Matter bounce cosmology with the f (T ) gravity,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.389710Z"},"links":{"cited_paper":"/paper/1104.4349","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:8f0588e20b913c376f8be9e61d996f15fff8fc53e68f3e513f4d71974f4f601d","observation_id":"335c9ce3-f2b5-435e-a842-fa71ca7040a7","resolution":{"observed_at":"2026-08-14T13:01:40.389710Z","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":"2026-08-14T13:01:40.223825Z","title":"This feature comes out from the fact that it mixes compact and noncompact coordinates","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.223825Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:fac8851686062137dd24c1dbdd9378c91e19d2a0feec1fc2100553aaeb9cd15a","observation_id":"ca23dafb-236a-4028-a19d-a50c64f53b78","resolution":{"observed_at":"2026-08-14T13:01:40.223825Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1108.2789","last_updated":"2011-08-13T13:17:49Z","snapshot_observed_at":"2026-08-21T06:38:42.254182Z","submitted_at":"2011-08-13T13:17:49Z","title":"Cosmography in f(T)-gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1108.2789","snapshot_observed_at":"2026-08-14T13:01:40.394769Z","title":"Cosmography in f (T ) gravity,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.394769Z"},"links":{"cited_paper":"/paper/1108.2789","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:1ae71b507c3a9e90dec5eb202aec3bb67cef7bea40737b8b35201368129ad308","observation_id":"a37a07d3-007b-434e-8fcb-54006b3655c6","resolution":{"observed_at":"2026-08-14T13:01:40.394769Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1311.1004","last_updated":"2014-04-10T10:04:26Z","snapshot_observed_at":"2026-08-14T23:56:24.840270Z","submitted_at":"2013-11-05T10:03:51Z","title":"Detectability of Torsion Gravity via Galaxy Clustering and Cosmic Shear Measurements","version":2},"cited_work":{"arxiv_id":"1311.1004","doi":null,"metadata_source":"pith","pith_arxiv_id":"1311.1004","snapshot_observed_at":"2026-08-14T13:01:41.841708Z","title":"Detectability of Torsion Gravity via Galaxy Clustering and Cosmic Shear Measurements","venue":"astro-ph.CO","work_id":"18d83736-153b-4c83-8b5f-a6ee0870d5c9","year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.405288Z"},"links":{"cited_paper":"/paper/1311.1004","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:7dfe20ee17b93bbb138540c363895fb5dcc75ebc97dcd8de349041d0e825e5a5","observation_id":"f5d7710a-809b-442d-bfa6-4c622486f2cb","resolution":{"observed_at":"2026-08-14T13:01:41.848148Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1506.08695","last_updated":"2015-06-26T10:14:51Z","snapshot_observed_at":"2026-08-14T22:42:50.636233Z","submitted_at":"2015-06-26T10:14:51Z","title":"FRW in quadratic form of $f(T)$ gravitational theories","version":1},"cited_work":{"arxiv_id":"1506.08695","doi":null,"metadata_source":"pith","pith_arxiv_id":"1506.08695","snapshot_observed_at":"2026-08-14T13:01:41.815554Z","title":"FRW in quadratic form of $f(T)$ gravitational theories","venue":"gr-qc","work_id":"e8815957-a592-474e-96ea-050c69c4401a","year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.410846Z"},"links":{"cited_paper":"/paper/1506.08695","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:8d26c5a315be8270cb2acbf24caf86ba5278ee917f1d94da2fca5f6e3d83a037","observation_id":"caa338dc-e721-4cb6-9db2-b085564b44e3","resolution":{"observed_at":"2026-08-14T13:01:41.821489Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1311.3131","last_updated":"2013-11-13T13:57:46Z","snapshot_observed_at":"2026-08-14T23:55:28.922996Z","submitted_at":"2013-11-13T13:57:46Z","title":"A spherically-symmetric charged-dS solution in f(T) gravity theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1311.3131","snapshot_observed_at":"2026-08-14T13:01:40.416351Z","title":"Spherically symmetric charged-dS sol ution in f (T ) gravity theories,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.416351Z"},"links":{"cited_paper":"/paper/1311.3131","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:c27e46581d91b782bdfbc8285aaa28e370a0b33fee188642270d52e4ce646964","observation_id":"1dcb5e96-f4d6-4034-92d0-416d24032c11","resolution":{"observed_at":"2026-08-14T13:01:40.416351Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9601044","last_updated":"1996-01-29T08:28:10Z","snapshot_observed_at":"2026-08-18T06:42:46.423465Z","submitted_at":"1996-01-29T08:28:10Z","title":"Energy of General Spherically Symmetric Solution in Tetrad Theory of Gravitation","version":1},"cited_work":{"arxiv_id":"gr-qc/9601044","doi":null,"metadata_source":"pith","pith_arxiv_id":"gr-qc/9601044","snapshot_observed_at":"2026-08-14T13:01:41.766535Z","title":"Energy of General Spherically Symmetric Solution in Tetrad Theory of Gravitation","venue":"gr-qc","work_id":"d4ab5842-0510-4aba-94d0-58ace598555f","year":1996},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.421757Z"},"links":{"cited_paper":"/paper/gr-qc/9601044","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:1a236edde2db86c2744831b75b6522fa5db441129480cc426d33acf416e293aa","observation_id":"62827b63-be7f-4d60-a8ac-0b43a3aec240","resolution":{"observed_at":"2026-08-14T13:01:41.772411Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1102.4410","last_updated":"2011-07-20T10:45:46Z","snapshot_observed_at":"2026-08-15T14:30:49.847840Z","submitted_at":"2011-02-22T05:14:44Z","title":"Static Solutions with Spherical Symmetry in f(T) Theories","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1102.4410","snapshot_observed_at":"2026-08-14T13:01:40.427387Z","title":"Static solutions with spherical symmetry in f (T ) theories,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.427387Z"},"links":{"cited_paper":"/paper/1102.4410","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:60e8b0b102c6b7485ee2021a25d1346b2e3adecb120e25b729a157b7a8c35107","observation_id":"c90b5044-0aff-4eaf-8042-d95bb1cd0dea","resolution":{"observed_at":"2026-08-14T13:01:40.427387Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1109.4209","last_updated":"2011-10-17T18:13:31Z","snapshot_observed_at":"2026-08-15T04:34:47.321817Z","submitted_at":"2011-09-20T05:44:41Z","title":"Spherically symmetric static spacetimes in vacuum f(T) gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1109.4209","snapshot_observed_at":"2026-08-14T13:01:40.432849Z","title":"Spherically symmetric stat ic spacetimes in vacuum f (T ) gravity,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.432849Z"},"links":{"cited_paper":"/paper/1109.4209","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:1acd37eadbbaa9d83944b246dc7e50b97655a5bac26016fddcf70c820ef0e7bc","observation_id":"504ece30-a612-4d1c-8e1d-df22740acc0f","resolution":{"observed_at":"2026-08-14T13:01:40.432849Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.02289","last_updated":"2018-11-30T10:47:35Z","snapshot_observed_at":"2026-08-14T18:31:51.274674Z","submitted_at":"2018-09-07T03:07:10Z","title":"Charged rotating black holes coupled with nonlinear electrodynamics Maxwell field in the mimetic gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.02289","snapshot_observed_at":"2026-08-14T13:01:40.438181Z","title":"Charg ed rotating black holes coupled with nonlinear electrodyna mics Maxwell field in the mimetic gravity,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.438181Z"},"links":{"cited_paper":"/paper/1809.02289","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:68f660730b4cf38d965e56499e1ca036564ad16dc9e4dea4cd5e5f2a02407266","observation_id":"53bb34c6-9695-477b-a446-0dbf7315b38f","resolution":{"observed_at":"2026-08-14T13:01:40.438181Z","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":"2026-08-14T13:01:40.443314Z","title":"Constraini ng f (T ) gravity in the solar system,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.443314Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:a68decbb960cdd79b53a9b2f98a797f58a6c39112e21cfdc2bfbe58ed256f999","observation_id":"02a91545-9ff4-4828-b4d5-17da70db5368","resolution":{"observed_at":"2026-08-14T13:01:40.443314Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1710.06620","last_updated":"2018-04-14T16:05:34Z","snapshot_observed_at":"2026-08-14T20:22:38.863479Z","submitted_at":"2017-10-18T08:35:24Z","title":"Charged Anti-de Sitter BTZ black holes in Maxwell-$f(T)$ gravity","version":2},"cited_work":{"arxiv_id":"1710.06620","doi":null,"metadata_source":"pith","pith_arxiv_id":"1710.06620","snapshot_observed_at":"2026-08-14T13:01:41.685771Z","title":"Charged Anti-de Sitter BTZ black holes in Maxwell-$f(T)$ gravity","venue":"gr-qc","work_id":"3cf0b55a-1f9c-45df-be53-389bf9c229da","year":2017},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.448567Z"},"links":{"cited_paper":"/paper/1710.06620","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:30e5379a2238600baf1bd9edafa5b3be9bf6c7c6b64607ddf4728f3d7c3cce6c","observation_id":"b5eb34a8-e661-4c65-8d02-f3e931180dd2","resolution":{"observed_at":"2026-08-14T13:01:41.691775Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T13:01:40.453941Z","title":"Phase portraits of general f (T ) cosmology,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.453941Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:c62af36793d0b9c1096fdd04e694528231f62ae3861e0057f1d2eb8c71fdef74","observation_id":"1308b2a0-8686-4b2b-8a43-dc755c4fbd68","resolution":{"observed_at":"2026-08-14T13:01:40.453941Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1110.4024","last_updated":"2012-07-10T20:55:09Z","snapshot_observed_at":"2026-08-15T06:44:58.466427Z","submitted_at":"2011-10-18T15:34:21Z","title":"Circularly symmetric solutions in three-dimensional Teleparallel, f(T) and Maxwell-f(T) gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1110.4024","snapshot_observed_at":"2026-08-14T13:01:40.459519Z","title":"Circularly symmetric solutions in three-dimensional telepara llel, f (T ) and Maxwell- f (T ) gravity,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.459519Z"},"links":{"cited_paper":"/paper/1110.4024","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:19832d30211b616980fbe1253a61b8d661b6be2de27d1f2c3f1eeece4f0002ac","observation_id":"93f69f4b-bc33-4ca4-b7bc-1eb9328ee754","resolution":{"observed_at":"2026-08-14T13:01:40.459519Z","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":"2026-08-14T13:01:40.465381Z","title":"Rotating ch arged ads solutions in quadratic f (T ) gravity,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.465381Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:8865c51da33d3154a9ac012b915acc8acde99a24ee7f1759f5f479bb06f053fb","observation_id":"1873573b-28cf-4172-8794-818f05f2dbf7","resolution":{"observed_at":"2026-08-14T13:01:40.465381Z","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":"2026-08-14T13:01:40.470661Z","title":"Generic phase portrait analysis of finite-time singularities and generalized tele parallel gravity,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.470661Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:e67104f92af9c14694ff874ff185f7f552dc9e178590c91296686a91bc4c400d","observation_id":"fe9a1a6d-d7b1-4136-bb6d-9b290366dbc5","resolution":{"observed_at":"2026-08-14T13:01:40.470661Z","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":"2026-08-14T13:01:40.475840Z","title":"Constraining the Schwarzschild de Sitter solution in m odels of modified gravity,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.475840Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:6ef1f86f2eb8b4d745bca5963f973125681a3d27c870167d35b06cd1ae472663","observation_id":"0c8f37eb-7ba8-4577-8b06-68e317c231b8","resolution":{"observed_at":"2026-08-14T13:01:40.475840Z","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":"2026-08-14T13:01:40.480830Z","title":"Bo rn-infeld and charged black holes with non-linear source in f (T ) gravity,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.480830Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:9b3683b2ea2f0b86f0905740de585f8ae0fafc317be2e15a2047f0a51d3aa57b","observation_id":"82404977-86b6-4de4-bbe0-4e139b825e15","resolution":{"observed_at":"2026-08-14T13:01:40.480830Z","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":"2026-08-14T13:01:40.485832Z","title":"f (T, T ) gravity and cosmology,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.485832Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:53b03bf0d7d948fe922ed28b1c176202b266966abc92f2986a1b355957aa41f3","observation_id":"24d23fea-e822-47b4-b90e-0625107ecdaa","resolution":{"observed_at":"2026-08-14T13:01:40.485832Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1210.1098","last_updated":"2012-10-03T13:11:02Z","snapshot_observed_at":"2026-08-21T18:59:40.593077Z","submitted_at":"2012-10-03T13:11:02Z","title":"Exact charged black-hole solutions in D-dimensional f(T) gravity: torsion vs curvature analysis","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1210.1098","snapshot_observed_at":"2026-08-14T13:01:40.490718Z","title":"Exact charged black-hole solutions in D-dimensi onal f (T ) gravity: torsion vs curvature analysis,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.490718Z"},"links":{"cited_paper":"/paper/1210.1098","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:773c6164b4e6343adf0be9545de4882dfa78a7e9eb8502deceb8fac43eaacc48","observation_id":"d8a86b7e-b243-40cf-b86f-1ad3771b20e5","resolution":{"observed_at":"2026-08-14T13:01:40.490718Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1306.2280","last_updated":"2013-10-29T16:52:20Z","snapshot_observed_at":"2026-08-15T00:14:34.121223Z","submitted_at":"2013-06-10T18:50:08Z","title":"Charged Black Holes in Generalized Teleparallel Gravity","version":4},"cited_work":{"arxiv_id":"1306.2280","doi":null,"metadata_source":"pith","pith_arxiv_id":"1306.2280","snapshot_observed_at":"2026-08-14T13:01:41.619856Z","title":"Charged Black Holes in Generalized Teleparallel Gravity","venue":"gr-qc","work_id":"eb426d9b-80ea-413c-a605-0a7b81c237f3","year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.496106Z"},"links":{"cited_paper":"/paper/1306.2280","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:955bac97c8860d8ae7b0e04b9e8505cab4be7f983280e75b7ec6d71e4235248f","observation_id":"4cc18d70-2ced-4347-b3ae-315a4958606f","resolution":{"observed_at":"2026-08-14T13:01:41.625836Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1502.05219","last_updated":"2015-02-17T10:26:13Z","snapshot_observed_at":"2026-08-18T05:30:18.555426Z","submitted_at":"2015-02-17T10:26:13Z","title":"A special exact spherically symmetric solution in f(T) gravity theories","version":1},"cited_work":{"arxiv_id":"1502.05219","doi":null,"metadata_source":"pith","pith_arxiv_id":"1502.05219","snapshot_observed_at":"2026-08-14T13:01:41.593453Z","title":"A special exact spherically symmetric solution in f(T) gravity theories","venue":"gr-qc","work_id":"683b8502-adc7-45ed-9d32-4470bdb716ee","year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.502056Z"},"links":{"cited_paper":"/paper/1502.05219","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:13aafeec3049f1d74d832cb333e49a6c715c649226ceb3ce8a80764ea26bf974","observation_id":"ff010e9f-f157-427a-8e15-bb3a4fc9e627","resolution":{"observed_at":"2026-08-14T13:01:41.599630Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1503.01379","last_updated":"2015-03-03T14:42:45Z","snapshot_observed_at":"2026-08-15T16:09:21.368945Z","submitted_at":"2015-03-03T14:42:45Z","title":"Stationary Axisymmetric Solutions and their Energy Contents in Teleparallel Equivalent of Einstein Theory","version":1},"cited_work":{"arxiv_id":"1503.01379","doi":null,"metadata_source":"pith","pith_arxiv_id":"1503.01379","snapshot_observed_at":"2026-08-14T13:01:41.567046Z","title":"Stationary Axisymmetric Solutions and their Energy Contents in Teleparallel Equivalent of Einstein Theory","venue":"gr-qc","work_id":"d9e563a3-3fae-4a9c-8247-e3cfb0bf34db","year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.507237Z"},"links":{"cited_paper":"/paper/1503.01379","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:220be94fcf45f0b82de3ed1fb01c15405c17463f95357f2df0e9c6f5ce005014","observation_id":"713c8d3d-a065-4649-ae75-7359c953edb6","resolution":{"observed_at":"2026-08-14T13:01:41.573260Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1503.07857","last_updated":"2015-10-30T17:15:51Z","snapshot_observed_at":"2026-08-21T07:59:32.466851Z","submitted_at":"2015-03-26T00:52:57Z","title":"Regular black holes in $f(T)$ Gravity through a nonlinear electrodynamics source","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.07857","snapshot_observed_at":"2026-08-14T13:01:40.512483Z","title":"Re gular black holes in f (T ) gravity through a nonlinear electrodynamics source,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.512483Z"},"links":{"cited_paper":"/paper/1503.07857","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:9272b0242ea916ac6d22850823087b6fa4b212e937423082ef6050f56016eedc","observation_id":"86d00701-d9ae-489b-80a3-05d7d8ff6dc3","resolution":{"observed_at":"2026-08-14T13:01:40.512483Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1412.0641","last_updated":"2015-02-05T21:40:29Z","snapshot_observed_at":"2026-08-14T23:09:26.868621Z","submitted_at":"2014-12-01T20:50:03Z","title":"Kerr geometry in f(T) gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1412.0641","snapshot_observed_at":"2026-08-14T13:01:40.517703Z","title":"Kerr geomet ry in gravity,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.517703Z"},"links":{"cited_paper":"/paper/1412.0641","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:c90a108fa0377b2b3519e160ff46f6769d0d35836e8b0b712502bfcdad126805","observation_id":"89bc6723-bd75-4ec0-8cfe-deedf3bac734","resolution":{"observed_at":"2026-08-14T13:01:40.517703Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.0003","last_updated":"2016-10-21T10:58:59Z","snapshot_observed_at":"2026-08-15T04:30:33.779478Z","submitted_at":"2011-10-30T16:01:08Z","title":"Spherically Symmetric Solutions on a Non-Trivial Frame in f(T) Theories of Gravity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.0003","snapshot_observed_at":"2026-08-14T13:01:40.522892Z","title":"Spherically Symmetric Solutions on a No n-Trivial Frame in f (T ) Theories of Gravity,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.522892Z"},"links":{"cited_paper":"/paper/1111.0003","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:9e18d86c4264e0cb02c969052a9266c84a3271c9aa1606e0798462d0ae00b1a4","observation_id":"37d04198-3d4b-4272-bad1-8e21c0493e2c","resolution":{"observed_at":"2026-08-14T13:01:40.522892Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1501.00974","last_updated":"2015-01-05T08:14:21Z","snapshot_observed_at":"2026-08-19T12:24:32.828023Z","submitted_at":"2015-01-05T08:14:21Z","title":"Schwarzschild solution in extended teleparallel gravity","version":1},"cited_work":{"arxiv_id":"1501.00974","doi":null,"metadata_source":"pith","pith_arxiv_id":"1501.00974","snapshot_observed_at":"2026-08-14T13:01:41.482042Z","title":"Schwarzschild solution in extended teleparallel gravity","venue":"gr-qc","work_id":"7b1fa42c-a378-4c5a-b7af-9d2da741a5f1","year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.528418Z"},"links":{"cited_paper":"/paper/1501.00974","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:82f65ac393234cabcb60f33cd38cc2b44fb7ff722e047a7ffd6dfc3ff8ad5e47","observation_id":"ff1bc33f-e466-484b-8a00-5c776bffc4bf","resolution":{"observed_at":"2026-08-14T13:01:41.487803Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1203.5781","last_updated":"2012-08-29T16:04:55Z","snapshot_observed_at":"2026-08-15T04:14:59.258363Z","submitted_at":"2012-03-26T15:01:03Z","title":"Solar system constraints on f(T) gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1203.5781","snapshot_observed_at":"2026-08-14T13:01:40.533527Z","title":"Solar system constraints on f (T ) gravity,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.533527Z"},"links":{"cited_paper":"/paper/1203.5781","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:aab55e68ebb84ae922df0a4b487222c13bd485f87511d6cc51b3887c0fd12f43","observation_id":"b0e9213a-5f9e-4dec-a80d-893663a65c2e","resolution":{"observed_at":"2026-08-14T13:01:40.533527Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1312.4103","last_updated":"2013-12-15T02:56:37Z","snapshot_observed_at":"2026-08-14T23:51:38.795326Z","submitted_at":"2013-12-15T02:56:37Z","title":"$f(T)$ gravity: effects on astronomical observation and Solar System experiments and upper-bounds","version":1},"cited_work":{"arxiv_id":"1312.4103","doi":null,"metadata_source":"pith","pith_arxiv_id":"1312.4103","snapshot_observed_at":"2026-08-14T13:01:41.434318Z","title":"$f(T)$ gravity: effects on astronomical observation and Solar System experiments and upper-bounds","venue":"gr-qc","work_id":"4faa19ab-0758-44c9-954b-b94f3caefc90","year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.538756Z"},"links":{"cited_paper":"/paper/1312.4103","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:647a3b077463cd65c6418a73d76dba8a3689b72ecec775fec73a9cc866951ad8","observation_id":"8d18c408-5a1f-40bb-bc78-5736c521e7f9","resolution":{"observed_at":"2026-08-14T13:01:41.440185Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1204.4593","last_updated":"2012-04-20T11:59:38Z","snapshot_observed_at":"2026-08-15T04:12:26.709364Z","submitted_at":"2012-04-20T11:59:38Z","title":"Good and bad tetrads in f(T) gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1204.4593","snapshot_observed_at":"2026-08-14T13:01:40.544386Z","title":"Good and bad tetrads in f (T ) gravity,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.544386Z"},"links":{"cited_paper":"/paper/1204.4593","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:e76902d56ad8810cc2041c0dc0078326a2f382b57a558e808d0765ff91782281","observation_id":"f8bb5b77-072c-412d-9011-4d6bfd1fa70a","resolution":{"observed_at":"2026-08-14T13:01:40.544386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1501.02198","last_updated":"2015-04-21T17:44:56Z","snapshot_observed_at":"2026-08-16T06:28:39.352471Z","submitted_at":"2015-01-09T16:48:49Z","title":"Weak-Field Spherically Symmetric Solutions in $f(T)$ gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1501.02198","snapshot_observed_at":"2026-08-14T13:01:40.549419Z","title":"Weak-field sphericall y symmetric solutions in f (T ) gravity,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.549419Z"},"links":{"cited_paper":"/paper/1501.02198","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:809ea1a5098fc7cb908d953f4f3d3dea3034df8e207f0189e08276c27bff03fc","observation_id":"148df1bd-7c96-47a2-bd6e-f98e5d3aae6c","resolution":{"observed_at":"2026-08-14T13:01:40.549419Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.06996","last_updated":"2015-07-14T08:05:46Z","snapshot_observed_at":"2026-08-14T22:47:19.966743Z","submitted_at":"2015-05-24T15:28:42Z","title":"Constraining f(T) gravity in the Solar System","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.06996","snapshot_observed_at":"2026-08-14T13:01:40.555602Z","title":"Constraini ng f (T ) gravity in the Solar System,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.555602Z"},"links":{"cited_paper":"/paper/1505.06996","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:972f3dea380ac4381f0dfaecf5d3e2026bde05ff39d802fd7284b58d7835d166","observation_id":"94c5faa2-52f8-4142-8521-09cde77711b0","resolution":{"observed_at":"2026-08-14T13:01:40.555602Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.03658","last_updated":"2019-06-09T14:51:15Z","snapshot_observed_at":"2026-08-14T18:01:57.324082Z","submitted_at":"2018-11-08T19:35:26Z","title":"Rotating AdS black holes in Maxwell-$f(T)$ gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.03658","snapshot_observed_at":"2026-08-14T13:01:40.560917Z","title":"Rotating AdS black h oles in Maxwell- f (T ) gravity,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.560917Z"},"links":{"cited_paper":"/paper/1811.03658","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:4a44fe905788111b895f47685e857a051136099c28057b9202b87eddbbecacfc","observation_id":"4548bcb0-607c-483e-8288-8d6260b6417f","resolution":{"observed_at":"2026-08-14T13:01:40.560917Z","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":"2026-08-14T13:01:40.566844Z","title":"Pleba´ nski,Lectures on non-linear electrodynamics: an extended versi on of lectures given at the Niels Bohr Institute and NORDITA, Copenhagen, in October 1968 (NORDITA, 1970)","venue":null,"work_id":null,"year":1968},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.566844Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:d018536c93b9028b6af5ae03b8fc9a24aaf0f06801913d56d93ead37d33b2423","observation_id":"2e52884a-f225-436d-987c-9e0d074947c6","resolution":{"observed_at":"2026-08-14T13:01:40.566844Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9911174","last_updated":"1999-11-22T19:47:27Z","snapshot_observed_at":"2026-07-07T05:21:30.904101Z","submitted_at":"1999-11-22T19:47:27Z","title":"New Regular Black Hole Solution from Nonlinear Electrodynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9911174","snapshot_observed_at":"2026-08-14T13:01:40.572127Z","title":"New regular black hole solution from no nlinear electrodynamics,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.572127Z"},"links":{"cited_paper":"/paper/hep-th/9911174","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:6eac553bab7626407c18cae105fba11e1a50eaff448d5a0925c4558867acb3c0","observation_id":"133602d1-f008-4b45-8e66-972a1e46931e","resolution":{"observed_at":"2026-08-14T13:01:40.572127Z","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":"2026-08-14T13:01:40.577427Z","title":"Duality rotations and type D solutions to Einstein equations with n onlinear electromagnetic sources,","venue":null,"work_id":null,"year":1987},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.577427Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:87dcda440bf32c2e4a5229f2a254732c74cf7b33be2455cedbdfe78c8d9c53ab","observation_id":"0a40aaed-9988-424a-9a33-b01f95fae3b4","resolution":{"observed_at":"2026-08-14T13:01:40.577427Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.6142","last_updated":"2013-12-16T10:36:40Z","snapshot_observed_at":"2026-08-21T09:36:01.354453Z","submitted_at":"2013-08-28T12:30:06Z","title":"Viable f(T) models are practically indistinguishable from LCDM","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.6142","snapshot_observed_at":"2026-08-14T13:01:40.582293Z","title":"Viable f (T ) models are practically indistinguishable from ΛCDM,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.582293Z"},"links":{"cited_paper":"/paper/1308.6142","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:f7b8fa0fa9c7ec5c031bc5560cc70569d25c9995c4535ba68364057c2c32b07e","observation_id":"2ae85a22-7025-4f48-992d-7ec10bb4eebc","resolution":{"observed_at":"2026-08-14T13:01:40.582293Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1606.04359","last_updated":"2016-08-09T08:06:40Z","snapshot_observed_at":"2026-08-14T21:53:47.769663Z","submitted_at":"2016-06-07T19:18:29Z","title":"New observational constraints on f(T) gravity from cosmic chronometers","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.04359","snapshot_observed_at":"2026-08-14T13:01:40.587740Z","title":"New observatio nal constraints on f (T ) gravity from cosmic chronometers,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.587740Z"},"links":{"cited_paper":"/paper/1606.04359","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:49d60b2ca56f6d95637408cb798cee6ab9701aae992e6be6788f5372225ca55d","observation_id":"e0729c28-6a1c-4f49-8dcc-1668a2b5a078","resolution":{"observed_at":"2026-08-14T13:01:40.587740Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.09278","last_updated":"2018-07-24T20:07:05Z","snapshot_observed_at":"2026-08-14T19:32:43.928210Z","submitted_at":"2018-03-25T15:43:57Z","title":"Updated constraints on $f(T)$ models using direct and indirect measurements of the Hubble parameter","version":2},"cited_work":{"arxiv_id":"1803.09278","doi":null,"metadata_source":"pith","pith_arxiv_id":"1803.09278","snapshot_observed_at":"2026-08-14T13:01:41.273041Z","title":"Updated constraints on $f(T)$ models using direct and indirect measurements of the Hubble parameter","venue":"astro-ph.CO","work_id":"411f82e3-bf01-4b9e-bb3c-4af4ae0c9824","year":2018},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.593003Z"},"links":{"cited_paper":"/paper/1803.09278","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:ea4ac9f0c6bda3764fd67ad647859eaea1d57df0189a749604582e9a834dd6a5","observation_id":"765682b4-485b-4d26-a418-134da63425af","resolution":{"observed_at":"2026-08-14T13:01:41.279179Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9404041","last_updated":"1995-05-17T01:05:44Z","snapshot_observed_at":"2026-07-07T03:24:40.793068Z","submitted_at":"1994-04-23T00:40:06Z","title":"Cylindrical Black Hole in General Relativity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9404041","snapshot_observed_at":"2026-08-14T13:01:40.598424Z","title":"Cylindrical black hole in general relat ivity,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.598424Z"},"links":{"cited_paper":"/paper/gr-qc/9404041","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:0ca6d0032e6a1c498d3d386e3c4cdb208af633ae1a0aff315dedd9b2db46080e","observation_id":"07607e31-184e-4992-95e4-4faeee61e141","resolution":{"observed_at":"2026-08-14T13:01:40.598424Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0209238","last_updated":"2003-06-05T18:07:38Z","snapshot_observed_at":"2026-08-16T20:49:24.371667Z","submitted_at":"2002-09-27T04:45:57Z","title":"Higher Dimensional Charged Rotating Solutions in (A)dS Space-times","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0209238","snapshot_observed_at":"2026-08-14T13:01:40.603642Z","title":"Higher dimensional charged rotating sol utions in (A)dS space-times,","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.603642Z"},"links":{"cited_paper":"/paper/hep-th/0209238","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:cc3beb60fab7c439f3009e95d39922bf1d62bedce13536106bfae49abdf7ce3b","observation_id":"6c520de9-95b6-4adf-ab0f-aef761ae9ed5","resolution":{"observed_at":"2026-08-14T13:01:40.603642Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9807010","last_updated":"1998-07-05T19:06:35Z","snapshot_observed_at":"2026-08-19T03:13:50.687274Z","submitted_at":"1998-07-05T19:06:35Z","title":"The Action of Instantons with Nut Charge","version":1},"cited_work":{"arxiv_id":"gr-qc/9807010","doi":null,"metadata_source":"pith","pith_arxiv_id":"gr-qc/9807010","snapshot_observed_at":"2026-08-14T13:01:41.207362Z","title":"The Action of Instantons with Nut Charge","venue":"gr-qc","work_id":"a4e90422-5e30-4d26-9136-6d9e7d404c6a","year":1998},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.608943Z"},"links":{"cited_paper":"/paper/gr-qc/9807010","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:72471e25b8d59a43f265a6b3f16c550612b9c29de4766e4f52169eaf88fa8862","observation_id":"413252f9-5346-4ef4-b4c0-18bb5a151186","resolution":{"observed_at":"2026-08-14T13:01:41.213224Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9809035","last_updated":"1998-09-24T22:41:54Z","snapshot_observed_at":"2026-08-18T23:32:27.056755Z","submitted_at":"1998-09-04T23:24:37Z","title":"Nut Charge, Anti-de Sitter Space and Entropy","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9809035","snapshot_observed_at":"2026-08-14T13:01:40.614114Z","title":"Nut charge, anti-de Sitter space and entropy,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.614114Z"},"links":{"cited_paper":"/paper/hep-th/9809035","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:59cf13cb661f96f47f4d4497d529f09721f2003aa18de7ba68f5066673df42ae","observation_id":"b72d1bb6-f4e6-4d27-bf92-efe0d7505771","resolution":{"observed_at":"2026-08-14T13:01:40.614114Z","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":"2026-08-14T13:01:40.619483Z","title":"Black holes and the second law,","venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.619483Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:25f4fd47c98c8ea241fd6433a7093b19f867513c8a4f0f588b8c231ec99164fe","observation_id":"376e42f5-945e-4583-876c-cc273fdec81e","resolution":{"observed_at":"2026-08-14T13:01:40.619483Z","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":"2026-08-14T13:01:40.624605Z","title":"Black holes and entropy,","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.624605Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:25a7ea6107679068b63d79083594a08a90056c14bd4928f95d9da8704f16da41","observation_id":"8b683b3b-e7f2-4226-96a1-5cfe73befe83","resolution":{"observed_at":"2026-08-14T13:01:40.624605Z","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":"2026-08-14T13:01:40.629768Z","title":"Cosmological Event Hor izons, Thermodynamics, and Particle Creation,","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.629768Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:e3e78241b1c2cf0079bc795ac7eb838e0bb8f6570d3f7ef0a95b43ba5f0eb37b","observation_id":"bc4947a4-5cc1-4cc3-9435-545715fd3148","resolution":{"observed_at":"2026-08-14T13:01:40.629768Z","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":"2026-08-14T13:01:40.634633Z","title":"De Sitter-Schwarzschild Black Hole:. i ts Particlelike Core and Thermodynamical Properties,","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.634633Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:5f2b4165436efd90afdbdfed6b5742cbf0cd3b57ddb81711747bb9af27d0c837","observation_id":"94f93b28-fe39-44a9-9bef-13d1c330510c","resolution":{"observed_at":"2026-08-14T13:01:40.634633Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0112052","last_updated":"2001-12-20T10:41:11Z","snapshot_observed_at":"2026-08-15T05:58:58.399506Z","submitted_at":"2001-12-20T10:41:11Z","title":"Cosmological term as a source of mass","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0112052","snapshot_observed_at":"2026-08-14T13:01:40.639726Z","title":"Cosmological term as a source of mass,","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.639726Z"},"links":{"cited_paper":"/paper/gr-qc/0112052","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:e673b2baadb02f3e7d7e2b2c1451ce0d1ce29e09241911506b68e9afd302426b","observation_id":"974e52cf-a556-440c-bbf5-97e72557bcb2","resolution":{"observed_at":"2026-08-14T13:01:40.639726Z","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":"2026-08-14T13:01:40.645463Z","title":"Generic Features of Thermodynamics of H orizons in Regular Spherical Space-Times of the Kerr-Schil d Class,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.645463Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:e019f03c660f2d4416a5b1eec0c7755c0a452adb3256e1fc52af095e09a00604","observation_id":"0308136e-3b68-498d-a9b8-dc1f12b1a1cb","resolution":{"observed_at":"2026-08-14T13:01:40.645463Z","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":"2026-08-14T13:01:40.650639Z","title":"Thermodynamics of th e Schwarzschild and the ReissnerNordstrm black holes with q uintessence,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.650639Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:590f48cbc0a2a97bd415abcc4f39be8cc0a6c1645c4bafc8ff6f6e1ea33c0371","observation_id":"36d43671-d91f-4628-847b-afa108b46263","resolution":{"observed_at":"2026-08-14T13:01:40.650639Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0506126","last_updated":"2005-12-26T21:08:24Z","snapshot_observed_at":"2026-07-07T03:21:09.268337Z","submitted_at":"2005-06-28T10:23:55Z","title":"Formation and evaporation of non-singular black holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0506126","snapshot_observed_at":"2026-08-14T13:01:40.655461Z","title":"Formation and evaporation of regular bl ack holes,","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.655461Z"},"links":{"cited_paper":"/paper/gr-qc/0506126","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:4276ae5dbc6a2d94f3ebde507f6302309285fd4c6fdfd4c0dcdbbd483d076e97","observation_id":"32e6e8a7-86d7-490c-972f-fabfaafb2c18","resolution":{"observed_at":"2026-08-14T13:01:40.655461Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0803.3849","last_updated":"2008-03-27T00:53:54Z","snapshot_observed_at":"2026-08-18T22:34:26.902249Z","submitted_at":"2008-03-27T00:53:54Z","title":"Anomaly and Hawking radiation from regular black holes","version":1},"cited_work":{"arxiv_id":"0803.3849","doi":null,"metadata_source":"pith","pith_arxiv_id":"0803.3849","snapshot_observed_at":"2026-08-14T13:01:41.120615Z","title":"Anomaly and Hawking radiation from regular black holes","venue":"gr-qc","work_id":"90de8c21-ae20-4a5f-a134-809de2d699eb","year":2008},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.661600Z"},"links":{"cited_paper":"/paper/0803.3849","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:7064c71e684303620e51bcb9d927b4bf9c83e2d51894eecc124cf700924e7d56","observation_id":"54ef4acd-4c98-4c3f-9dc0-728e836c3225","resolution":{"observed_at":"2026-08-14T13:01:41.127562Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0708.3145","last_updated":"2008-09-21T15:27:05Z","snapshot_observed_at":"2026-08-15T10:33:44.889962Z","submitted_at":"2007-08-23T09:00:14Z","title":"Thermodynamics of regular black hole","version":4},"cited_work":{"arxiv_id":"0708.3145","doi":null,"metadata_source":"pith","pith_arxiv_id":"0708.3145","snapshot_observed_at":"2026-08-14T13:01:41.093388Z","title":"Thermodynamics of regular black hole","venue":"gr-qc","work_id":"62981870-f03d-4c90-8d8c-63e76f1d5412","year":2007},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.667415Z"},"links":{"cited_paper":"/paper/0708.3145","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:681e0dc09f6d1fa60a2013f25e20359e12efd1de9c0ec5db5fb866e9f7d71a7b","observation_id":"665ec9b0-e8a6-4b3e-97c6-234123fa92ae","resolution":{"observed_at":"2026-08-14T13:01:41.099527Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0510112","last_updated":"2005-11-12T07:59:01Z","snapshot_observed_at":"2026-08-11T10:35:24.971521Z","submitted_at":"2005-10-26T09:55:41Z","title":"Noncommutative geometry inspired Schwarzschild black hole","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0510112","snapshot_observed_at":"2026-08-14T13:01:40.673172Z","title":"Noncommu tative geometry inspired Schwarzschild black hole,","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.673172Z"},"links":{"cited_paper":"/paper/gr-qc/0510112","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:84afcecb63a2b2e0b5c33ab15b14c04e285b8990a10e6adf2fa974fc3cef5c39","observation_id":"9163ebf1-5424-4d7b-9b6b-004fd3076bd6","resolution":{"observed_at":"2026-08-14T13:01:40.673172Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1109.6627","last_updated":"2011-09-28T07:20:18Z","snapshot_observed_at":"2026-08-15T04:33:58.096637Z","submitted_at":"2011-09-28T07:20:18Z","title":"Thermodynamics of a Bardeen black hole in noncommutative space","version":1},"cited_work":{"arxiv_id":"1109.6627","doi":null,"metadata_source":"pith","pith_arxiv_id":"1109.6627","snapshot_observed_at":"2026-08-14T13:01:41.043745Z","title":"Thermodynamics of a Bardeen black hole in noncommutative space","venue":"gr-qc","work_id":"858daf59-7a6e-4540-bdf4-c72c36443303","year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.678426Z"},"links":{"cited_paper":"/paper/1109.6627","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:6a5d9a28cc9ae8dd11201b43ae0f417452f261f0dec14c6be14b2a6c022dd2b0","observation_id":"a4785baf-e986-4eb9-a43e-4efc03ac9be0","resolution":{"observed_at":"2026-08-14T13:01:41.049859Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1107.0515","last_updated":"2011-11-17T15:55:18Z","snapshot_observed_at":"2026-08-15T04:42:08.391584Z","submitted_at":"2011-07-04T02:21:31Z","title":"Violation of the first law of black hole thermodynamics in $f(T)$ gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.0515","snapshot_observed_at":"2026-08-14T13:01:40.683479Z","title":"Violation of the first law of black hole thermodynamics in f (T ) gravity,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.683479Z"},"links":{"cited_paper":"/paper/1107.0515","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:2375ffda151f358582d199a8da4274a41956deb831a3dfdbf1d0bdefbbe85b54","observation_id":"ae25caa8-7ea6-4c24-b18c-3402652aea16","resolution":{"observed_at":"2026-08-14T13:01:40.683479Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0706.2749","last_updated":"2007-11-22T12:20:45Z","snapshot_observed_at":"2026-08-18T03:32:09.608169Z","submitted_at":"2007-06-19T09:44:51Z","title":"Black holes thermodynamics to all orders in the Planck length in extra dimensions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0706.2749","snapshot_observed_at":"2026-08-14T13:01:40.689381Z","title":"Black holes thermodynamics to all order in the Planck length in extra dimensions,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.689381Z"},"links":{"cited_paper":"/paper/0706.2749","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:f94e302bd249ddb3a9425708d43db35cd33c64aa27a018c14de9dfe173ce0d99","observation_id":"07cbeb6e-c06f-4b27-9e10-a7fb534b767f","resolution":{"observed_at":"2026-08-14T13:01:40.689381Z","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":"2026-08-14T13:01:40.695093Z","title":"Thermodynamics of regul ar cosmological black holes with the de sitter interior,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.695093Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:6c416fc574f77613361ca1aa7cf317096d5c2af3d198a0d3cf5972aaa1aefbdd","observation_id":"71fed9ea-027c-4df8-bf3a-5d3420ef7d36","resolution":{"observed_at":"2026-08-14T13:01:40.695093Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9902170","last_updated":"1999-03-09T15:53:58Z","snapshot_observed_at":"2026-08-03T08:04:07.245723Z","submitted_at":"1999-02-24T00:58:47Z","title":"Charged AdS Black Holes and Catastrophic Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9902170","snapshot_observed_at":"2026-08-14T13:01:40.700494Z","title":"Charged AdS black holes and catastrophic holography,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.700494Z"},"links":{"cited_paper":"/paper/hep-th/9902170","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:53a2612a9b46f31bc1db27a9deffe919a556bf9d468b269feded1ed95fc9059c","observation_id":"2f5b9634-453a-42da-b086-668084d91b0f","resolution":{"observed_at":"2026-08-14T13:01:40.700494Z","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":"2026-08-14T13:01:40.705599Z","title":"Particle Creation by Black Holes,","venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.705599Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:38ad8ce4e1dd6675b2d72a737b6cac61b2489bdc98a32bf915f71c77b6d375fe","observation_id":"41f9edd6-1f03-47a9-816a-9b4a439161ae","resolution":{"observed_at":"2026-08-14T13:01:40.705599Z","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":"2026-08-14T13:01:42.498468Z","title":"Thermodynamics of Black Holes,","venue":null,"work_id":"55cbf185-0d30-46ad-8d8b-382c7b15a797","year":1977},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.710464Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:2f27092f56367b5e7d3afdaad2949f11028d392c04ce6e48d0c4f369fe9afb0b","observation_id":"dc6b9c19-12e3-4e56-85a0-9b6bd712c573","resolution":{"observed_at":"2026-08-14T13:01:42.506677Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+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":"2026-08-14T13:01:42.480801Z","title":"Thermodynamics of Black H oles in anti-De Sitter Space,","venue":null,"work_id":"39ec7f01-cc7a-4918-9f09-2ec01c368b7a","year":1983},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.715822Z"},"links":{"citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:fbcc0934aedfb9736c006442822cd8a0a0ec48ae2f6a7101e2f12912e82b9008","observation_id":"aecfa3f9-8ec4-4126-a156-a290fdfecc9b","resolution":{"observed_at":"2026-08-14T13:01:42.486240Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1207.5318","last_updated":"2012-11-07T08:26:54Z","snapshot_observed_at":"2026-08-18T19:27:40.293287Z","submitted_at":"2012-07-23T08:43:23Z","title":"Phase transition of quantum corrected Schwarzschild black hole","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.5318","snapshot_observed_at":"2026-08-14T13:01:40.720729Z","title":"Phase transition of quantum-correct ed Schwarzschild black hole,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.720729Z"},"links":{"cited_paper":"/paper/1207.5318","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:fd8dd2ebb8985d9f64f2f22c180e247882611e7983f0db56dcfcc57c4fe172eb","observation_id":"ff4998cc-d8da-48e1-b84e-175bd2b5740c","resolution":{"observed_at":"2026-08-14T13:01:40.720729Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1401.2586","last_updated":"2014-01-12T02:45:03Z","snapshot_observed_at":"2026-08-18T19:27:40.840329Z","submitted_at":"2014-01-12T02:45:03Z","title":"Thermodynamics of rotating black holes and black rings: phase transitions and thermodynamic volume","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1401.2586","snapshot_observed_at":"2026-08-14T13:01:40.725964Z","title":"Thermodynamics of Rotating Black Holes and Black Rin gs: Phase Transitions and Thermodynamic V olume,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.725964Z"},"links":{"cited_paper":"/paper/1401.2586","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:83b63745d3f513c8f2384cd21931bfb20bf9e84765185a8f333aeb8833cbffca","observation_id":"5c7c7cf5-3000-45a8-8f7c-e7df6cfaa185","resolution":{"observed_at":"2026-08-14T13:01:40.725964Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0112045","last_updated":"2002-01-21T15:30:26Z","snapshot_observed_at":"2026-08-06T10:01:38.446887Z","submitted_at":"2001-12-06T19:53:12Z","title":"Black Hole Thermodynamics and Negative Entropy in deSitter and Anti-deSitter Einstein-Gauss-Bonnet gravity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0112045","snapshot_observed_at":"2026-08-14T13:01:40.731176Z","title":"Black hole th ermodynamics and negative entropy in de sitter and anti-de s itter einstein-gauss- bonnet gravity,","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.731176Z"},"links":{"cited_paper":"/paper/hep-th/0112045","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:2f28cd46575262437b2c456720d92cb52c5e5ec767f4ff687a5553d7c14a46e7","observation_id":"0d0e071a-b861-4ab1-99b3-8db0dd8c4c97","resolution":{"observed_at":"2026-08-14T13:01:40.731176Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0105117","last_updated":"2001-05-14T04:52:01Z","snapshot_observed_at":"2026-08-09T06:17:54.436058Z","submitted_at":"2001-05-14T04:52:01Z","title":"Holographic entropy and brane FRW-dynamics from AdS black hole in d5 higher derivative gravity","version":1},"cited_work":{"arxiv_id":"hep-th/0105117","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/0105117","snapshot_observed_at":"2026-08-14T13:01:40.899197Z","title":"Holographic entropy and brane FRW-dynamics from AdS black hole in d5 higher derivative gravity","venue":"hep-th","work_id":"586ceb02-4192-49a1-8531-926275291809","year":2001},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.737321Z"},"links":{"cited_paper":"/paper/hep-th/0105117","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:7f096502e22489a6938cb02bca88191e2235acd6f7fd9034693aaded1d12cfd0","observation_id":"c27ecf8b-9a95-4e1b-95bb-12d2dafb0095","resolution":{"observed_at":"2026-08-14T13:01:40.904988Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0204112","last_updated":"2002-05-01T13:38:15Z","snapshot_observed_at":"2026-08-15T22:53:25.442729Z","submitted_at":"2002-04-13T14:54:49Z","title":"(Anti-) de Sitter Black Holes in higher derivative gravity and dual Conformal Field Theories","version":3},"cited_work":{"arxiv_id":"hep-th/0204112","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/0204112","snapshot_observed_at":"2026-08-14T13:01:40.869919Z","title":"(Anti-) de Sitter Black Holes in higher derivative gravity and dual Conformal Field Theories","venue":"hep-th","work_id":"69d5e022-019f-4709-802d-3ed1c31c6a7b","year":2002},"citing_paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics","version":2},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-14T13:01:40.743390Z"},"links":{"cited_paper":"/paper/hep-th/0204112","citing_paper":"/paper/1908.07381"},"observation_digest":"sha256:e888995475d195ede9c9866523b7667a5dca7bffe6c3cf101d11a98ad775b08d","observation_id":"8b4173a0-ef99-427d-8069-b5fd59a66a8e","resolution":{"observed_at":"2026-08-14T13:01:40.875683Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"1908.07381","last_updated":"2019-10-19T14:06:20Z","latest_version":2,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-18T19:29:11.555182Z","submitted_at":"2019-08-17T09:54:02Z","title":"Rotating and non-rotating AdS black holes in $f({\\cal T})$ gravity non-linear electrodynamics"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":73,"verified_exact":25,"verified_fuzzy":2},"total_outbound_references":103},"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":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"thesis":"As of 22 August 2026, this Paper Citation Record lists 100 of 103 outbound references and 1 inbound Pith citation observation for arXiv:1908.07381."}