{"as_of":"2026-08-09T13:23:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:847fc0d75aac502a7190bad2fc22d380dc3dbef0d50f43898f9e561735e7827c","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":17,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":17,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-09T06:31:02.800959+00:00","state":"measured"},{"denominator":17,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":17,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T00:41:00.121908Z","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":"2026-07-04T08:29:41.634607Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-08-07T13:42:43.200025Z","title":"Krssak, R","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.21359","last_updated":"2025-05-27T15:52:14Z","snapshot_observed_at":"2026-08-07T14:16:21.746867Z","submitted_at":"2025-05-27T15:52:14Z","title":"Teleparallel dark energy in a nonflat universe","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-07T13:42:43.200025Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2505.21359"},"observation_digest":"sha256:3fc7d0edae8e49978cd31bb4e592270382a88ef05f50363c227c0bdbe0669e4b","observation_id":"87c8dde8-4daa-4cbc-95d7-6e26d5d924b8","resolution":{"observed_at":"2026-08-07T13:42:43.200025Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2505.24732","last_updated":"2026-04-11T09:17:44Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-05-30T15:54:16Z","title":"The Quintom theory of dark energy after DESI DR2","version":3},"reference_index":178,"source":"pdf_text","source_observed_at":"2026-05-19T13:08:20.192767Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2505.24732"},"observation_digest":"sha256:4152114848b4bacd70e0d3ead16708f8105822896ab4eec1eadf4399b73038af","observation_id":"8756877c-26d4-42d0-87f8-5746fcd4aa49","resolution":{"observed_at":"2026-05-19T13:12:18.808827Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2507.23672","last_updated":"2026-05-07T17:50:14Z","snapshot_observed_at":"2026-07-06T22:05:52.712231Z","submitted_at":"2025-07-31T15:49:32Z","title":"Teleparallel gravity from the principal bundle viewpoint","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-05-19T02:14:33.371203Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2507.23672"},"observation_digest":"sha256:28d6da76b11d6bfc65887ccce8e965c6f346eb53744f076688d4c68a7994ea6b","observation_id":"5f47b979-53d5-4070-bbad-7c52419ceb1b","resolution":{"observed_at":"2026-05-19T02:16:59.258357Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-08-05T22:53:16.197017Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2508.06290","last_updated":"2026-06-06T16:55:48Z","snapshot_observed_at":"2026-08-06T13:05:21.838711Z","submitted_at":"2025-08-08T13:10:50Z","title":"Traversable Wormhole Solutions in massive $F(T)$ gravity","version":3},"reference_index":4,"source":"arxiv_source","source_observed_at":"2026-08-05T22:53:16.197017Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2508.06290"},"observation_digest":"sha256:c2a0e1219a26912041e4efd23f257b8375dd9b31a30d437846a774d31d0f107a","observation_id":"6af48666-05e5-446c-9087-7f29837b115c","resolution":{"observed_at":"2026-08-05T22:53:16.197017Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2508.20314","last_updated":"2025-08-27T23:03:09Z","snapshot_observed_at":"2026-07-06T22:19:43.531487Z","submitted_at":"2025-08-27T23:03:09Z","title":"On black holes in new general relativity","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-05-18T20:21:02.339813Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2508.20314"},"observation_digest":"sha256:e23401bad1a17793f3882382605a4a440670aec94f799470ca8635469a786cf6","observation_id":"a7d2c02b-5341-48e5-8dfa-1c3fdb5521da","resolution":{"observed_at":"2026-05-18T20:21:49.978819Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2509.02646","last_updated":"2026-04-20T16:52:47Z","snapshot_observed_at":"2026-08-03T04:18:44.539165Z","submitted_at":"2025-09-02T10:58:37Z","title":"Gauge invariant perturbations of $F(T,T_G)$ Cosmology","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-05-18T19:47:37.738359Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2509.02646"},"observation_digest":"sha256:afb521f27ccbd1f74e87b93afd14ca2244254dc0e2939914b80a4cbb8ac0fcbc","observation_id":"78b5d2eb-4d91-469b-a77f-840af41a3f7d","resolution":{"observed_at":"2026-05-18T19:51:49.694252Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2602.12496","last_updated":"2026-04-22T22:37:59Z","snapshot_observed_at":"2026-07-06T22:45:44.135338Z","submitted_at":"2026-02-13T00:36:29Z","title":"On non-vacuum black holes in new general relativity","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-05-15T23:05:25.823433Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2602.12496"},"observation_digest":"sha256:6b525c9d67965c8bc9272f4eaedfe67b69d105da40e0c0240217ad824e6819b1","observation_id":"b2d5eef5-1c4a-4731-a547-355849908b33","resolution":{"observed_at":"2026-05-15T23:06:51.131454Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2604.07858","last_updated":"2026-04-09T06:16:57Z","snapshot_observed_at":"2026-07-06T22:57:05.146373Z","submitted_at":"2026-04-09T06:16:57Z","title":"Quasinormal modes of the thick braneworld in $f(T)$ gravity","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-05-10T17:36:53.184074Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2604.07858"},"observation_digest":"sha256:0a6dbc911dac77574c7144473645d6155ef9d9bc959599563333d684ef33675a","observation_id":"fe241657-ea38-4178-8e45-c618b35e0716","resolution":{"observed_at":"2026-05-11T06:31:00.468091Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2606.01360","last_updated":"2026-07-18T02:00:49Z","snapshot_observed_at":"2026-08-02T12:39:56.892030Z","submitted_at":"2026-05-31T17:31:59Z","title":"A short review on Quintom dark energy theory","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-06-28T16:17:39.285285Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2606.01360"},"observation_digest":"sha256:1ba3f3a8ad69cf05fdc9c6b529f123e3590eedc489b810d2a83fe5be66d7ddaf","observation_id":"35330409-b62a-4dd3-a32c-f7ada3a7cc74","resolution":{"observed_at":"2026-07-01T21:46:16.036516Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-08-02T12:40:08.491667Z","title":"Krssak, R","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2606.01360","last_updated":"2026-07-18T02:00:49Z","snapshot_observed_at":"2026-08-02T12:39:56.892030Z","submitted_at":"2026-05-31T17:31:59Z","title":"A short review on Quintom dark energy theory","version":2},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-02T12:40:08.491667Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2606.01360"},"observation_digest":"sha256:e6800fb9d95363286f80c4789ae19d9a749ff8779e0fa60c39481dd176acc686","observation_id":"7a32c46d-fc23-447a-a141-4d94eff22890","resolution":{"observed_at":"2026-08-02T12:40:08.491667Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2606.19905","last_updated":"2026-06-18T08:02:10Z","snapshot_observed_at":"2026-08-08T07:09:29.361155Z","submitted_at":"2026-06-18T08:02:10Z","title":"Cosmological Constraints on Minimal Cubic Galileon Models in Teleparallel Gravity","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-06-26T16:55:10.910021Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2606.19905"},"observation_digest":"sha256:6dbf48cc325e259dd6ffa6b909edf78ac9dae7eb735c6023d101b8c6ed1559d5","observation_id":"0525be92-89b1-4f9c-8c49-ff29dd5fc2d4","resolution":{"observed_at":"2026-07-04T04:39:34.168278Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2606.22121","last_updated":"2026-06-20T16:03:38Z","snapshot_observed_at":"2026-08-08T06:15:04.818080Z","submitted_at":"2026-06-20T16:03:38Z","title":"Horizon Singularities in the Schwarzschild Geometry of the Teleparallel Equivalent of General Relativity","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-06-26T11:39:53.368639Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2606.22121"},"observation_digest":"sha256:cd5cd53936d20fd77db762cac3715baf7e9240ed5ff1fc79eedd607e9155af05","observation_id":"a515b57b-c012-4129-a135-cfec96d51fc0","resolution":{"observed_at":"2026-07-04T08:29:41.636878Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2606.30717","last_updated":"2026-07-01T13:17:27Z","snapshot_observed_at":"2026-08-05T16:03:14.276555Z","submitted_at":"2026-06-29T18:00:01Z","title":"The auxiliary-deformed Breitenlohner-Maison model: duality frames and higher-dimensional origin","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-07-01T02:06:12.922104Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2606.30717"},"observation_digest":"sha256:aa26aab8ae5f5e0f7836c1f5172182df57c319531e0e2728d57d1c374e75d22e","observation_id":"e0b231ee-c2c0-4536-b334-dfc3500541c8","resolution":{"observed_at":"2026-07-01T12:25:43.570584Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2606.30717","last_updated":"2026-07-01T13:17:27Z","snapshot_observed_at":"2026-08-05T16:03:14.276555Z","submitted_at":"2026-06-29T18:00:01Z","title":"The auxiliary-deformed Breitenlohner-Maison model: duality frames and higher-dimensional origin","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-07-02T20:22:09.814152Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2606.30717"},"observation_digest":"sha256:d15f4b0286b805b031d2443919ce5e20e48a9772ab872c2b76baf1dcd4021953","observation_id":"42f2e1a6-f295-4977-aba2-b59ee4ab00f4","resolution":{"observed_at":"2026-07-02T20:27:21.803252Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2606.31330","last_updated":"2026-06-30T08:32:30Z","snapshot_observed_at":"2026-07-07T00:05:02.977105Z","submitted_at":"2026-06-30T08:32:30Z","title":"Two-scalar-field $f(R)$ Thick Branes, Gravitational Resonances and Quasinormal Modes","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-07-01T05:00:36.912861Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2606.31330"},"observation_digest":"sha256:3309cea1b15cafe5fecbf8080f2a1ac2dd3da1410b8f8d4f373daf6f92105484","observation_id":"d79049fe-e24c-4ed3-8759-530ee07a657b","resolution":{"observed_at":"2026-07-01T10:55:41.773766Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":"1810.12932","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-07-04T08:29:41.634607Z","title":"Krssak, R","venue":null,"work_id":"cfd10be0-b077-461f-8180-2144fa463484","year":2019},"citing_paper":{"arxiv_id":"2607.02017","last_updated":"2026-07-02T10:49:34Z","snapshot_observed_at":"2026-08-04T23:24:53.378082Z","submitted_at":"2026-07-02T10:49:34Z","title":"Boson Stars in Teleparallel Gravity with a Nonminimally Coupled Field: The Violation of Energy Conditions and Gravitational Waveforms from EMRIs","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-07-03T08:30:26.651482Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2607.02017"},"observation_digest":"sha256:f6013e988bb79fdefa712cadc980f5984aa3015990d19cbe9f995ef3b444e577","observation_id":"335224bf-009c-49cf-812c-f27e1cc0b4cb","resolution":{"observed_at":"2026-07-03T08:37:46.517504Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.12932","snapshot_observed_at":"2026-08-08T00:41:00.121908Z","title":"Krssak, R","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.04094","last_updated":"2026-08-04T18:00:03Z","snapshot_observed_at":"2026-08-09T01:42:49.912019Z","submitted_at":"2026-08-04T18:00:03Z","title":"Disformal Maps: Classification and Singular Dynamics","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-08T00:41:00.121908Z"},"links":{"cited_paper":"/paper/1810.12932","citing_paper":"/paper/2608.04094"},"observation_digest":"sha256:b81011b0509402fee0c63a977aff264912697d1913fa413642ca6739b5522cab","observation_id":"e4e52cc0-b9b7-4e22-aae6-6a9a6d030d8b","resolution":{"observed_at":"2026-08-08T00:41:00.121908Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/1810.12932/citation-record","integrity":"/paper/1810.12932/integrity","json":"/paper/1810.12932/citation-record.json","paper":"/paper/1810.12932"},"outbound":[],"paper":{"arxiv_id":"1810.12932","last_updated":"2019-09-24T12:01:30Z","latest_version":2,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-03T01:56:35.699306Z","submitted_at":"2018-10-30T18:01:21Z","title":"Teleparallel Theories of Gravity: Illuminating a Fully Invariant Approach"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"thesis":"As of 9 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 17 inbound Pith citation observations for arXiv:1810.12932."}