{"as_of":"2026-08-08T22:24:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:fbfacd89d32ee94bf8fedb0d4c27f542e92b74b5d6f4f4bbecb55ca00aa8a8f8","coverage":[{"denominator":57,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":57,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-07T14:40:27.598587Z","state":"measured"},{"denominator":58,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":58,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-08T06:32:00.761636+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":"2026-08-07T14:40:27.598587Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-08-07T14:40:28.369728Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"cited_work":{"arxiv_id":"2505.18285","doi":null,"metadata_source":"pith","pith_arxiv_id":"2505.18285","snapshot_observed_at":"2026-08-07T14:40:28.369728Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","venue":"gr-qc","work_id":"1ed5e94b-4985-48ae-a77a-6e0a52e7e1d8","year":2025},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.598587Z"},"links":{"cited_paper":"/paper/2505.18285","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:2852d80f438343ba5c59912b01116ff7f3aeeb488789366cdff37eb43995bfb5","observation_id":"a294c7a8-8e9d-469d-b370-34d4b79f83ac","resolution":{"observed_at":"2026-08-07T14:40:28.412652Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2505.18285/citation-record","integrity":"/paper/2505.18285/integrity","json":"/paper/2505.18285/citation-record.json","paper":"/paper/2505.18285"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:32.628351Z","title":"This formalism generalizes GR by allowing for non-Riemannian geometries, s uch as those that include torsion and Gauss-Bonnet, in addition to curvature","venue":null,"work_id":"230cfdbd-2770-4fd2-8c21-f5c06a0d5d88","year":null},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:22.243553Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:c78553e9f86423ab6e8c579f2f0ba92cfe2b2b97cd89cff28ed4e162ea549096","observation_id":"c0734378-95c7-4575-9a79-cef64c41b069","resolution":{"observed_at":"2026-08-07T14:40:32.663329Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:32.529372Z","title":"The variation of the action with respect to the vielbein eµ A leads to the field equations governing the dynamics of the system","venue":null,"work_id":"c4c32212-6098-452c-b8fe-34698735da35","year":null},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:22.365562Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:12ce42f6583d3ff3a94d535d17b0b41ebf500f6ea37642146f7ca81ecebe39d6","observation_id":"2814f626-346a-4d1a-9b07-610a3988b840","resolution":{"observed_at":"2026-08-07T14:40:32.586863Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:32.422183Z","title":null,"venue":null,"work_id":"4bfe3d35-5706-4958-b810-8dfa1dd386a3","year":null},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:22.483301Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:548fda54e88a0b33e2336c9e9847bc8cb2525058b02d67183df366ac8b740f65","observation_id":"e7d2e0e2-b8bd-4089-9b9c-5ad7ad4bc3f7","resolution":{"observed_at":"2026-08-07T14:40:32.468806Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:32.133315Z","title":"In this formalism, the connection is not symm etric, and torsion arises due to the antisymmetric part of the connection","venue":null,"work_id":"b782c7a8-a61d-4abc-8a39-d9dfc889c586","year":null},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:22.567872Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:442e5a6381c2ec1cdc5c50bcf12f6b8c56796ed14d46fe2a91c666ae01f29648","observation_id":"a7419302-3e5f-4ddd-bcb3-0350fbc1c924","resolution":{"observed_at":"2026-08-07T14:40:32.320121Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:32.049415Z","title":null,"venue":null,"work_id":"bdb8b060-fed7-47cc-af72-33ee3e487195","year":null},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:22.675323Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:78da02a21385b79631eaca025ce1a8d3e3440cc4a19db01ea75dd89565ab0ec8","observation_id":"9a7884c8-d2ad-4f81-8f8c-9ae767bee002","resolution":{"observed_at":"2026-08-07T14:40:32.088203Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:31.963738Z","title":"(39) For large a, the cosmological constant ρΛ becomes dominant","venue":null,"work_id":"2996d5ce-8a0c-4584-a20d-84eeea9f13b0","year":null},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:22.761685Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:c1888311a71ce87eeeab873f10339cd65d023b3b2684ffba35075a6cda54261d","observation_id":"8d982cc7-6b9d-4586-8e56-8e846c86eb71","resolution":{"observed_at":"2026-08-07T14:40:32.014109Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0812.1205","last_updated":"2009-05-21T19:41:47Z","snapshot_observed_at":"2026-08-03T09:06:19.016196Z","submitted_at":"2008-12-05T19:39:54Z","title":"Dark torsion as the cosmic speed-up","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.1205","snapshot_observed_at":"2026-08-07T14:40:22.845522Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:22.845522Z"},"links":{"cited_paper":"/paper/0812.1205","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:b95acba781cbbe798708247baa902143f98e1d9873e4c27b2383bfc6b8cf1a52","observation_id":"dff112a8-faee-4483-b2fb-c3d3ef2605fc","resolution":{"observed_at":"2026-08-07T14:40:22.845522Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0610067","last_updated":"2007-03-29T17:14:29Z","snapshot_observed_at":"2026-08-08T13:53:24.642421Z","submitted_at":"2006-10-12T20:27:38Z","title":"Modified teleparallel gravity: inflation without inflaton","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0610067","snapshot_observed_at":"2026-08-07T14:40:22.948724Z","title":"Ferraro and F","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:22.948724Z"},"links":{"cited_paper":"/paper/gr-qc/0610067","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:06dfcfeb9b9a2a171a8373c2ad315b5e67e0a15d0d25a4167d5f5fd45bd2afaf","observation_id":"91a99731-d549-42e1-b846-6a04328d8ef8","resolution":{"observed_at":"2026-08-07T14:40:22.948724Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.1039","last_updated":"2012-11-17T21:07:09Z","snapshot_observed_at":"2026-07-06T02:51:14.232244Z","submitted_at":"2012-06-28T18:51:56Z","title":"FRW Cosmology in F(R,T) gravity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.1039","snapshot_observed_at":"2026-08-07T14:40:23.070760Z","title":"Myrzakulov, Eur","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.070760Z"},"links":{"cited_paper":"/paper/1207.1039","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:12f455fd8a2f5a18a82d31896ad3b6e77aee4bec9e53ba3196ed38934abf25c0","observation_id":"4cea7425-2d6c-450d-8b47-3ff86d153aaf","resolution":{"observed_at":"2026-08-07T14:40:23.070760Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1401.7378","last_updated":"2014-02-21T01:36:21Z","snapshot_observed_at":"2026-07-06T03:34:36.736577Z","submitted_at":"2014-01-29T00:49:37Z","title":"Trace-anomaly driven inflation in $f(T)$ gravity and in minimal massive bigravity","version":2},"cited_work":{"arxiv_id":"1401.7378","doi":null,"metadata_source":"pith","pith_arxiv_id":"1401.7378","snapshot_observed_at":"2026-08-07T14:40:31.336823Z","title":"Trace-anomaly driven inflation in $f(T)$ gravity and in minimal massive bigravity","venue":"gr-qc","work_id":"362af7fb-2569-4af7-bd18-e630e77a928b","year":2014},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.170490Z"},"links":{"cited_paper":"/paper/1401.7378","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:836b78d8312ed0a51d587bb54df968bae8c6f2785ee47fa1a03de5ad4f133627","observation_id":"61de7e2b-bf69-43b8-8419-8842140f372f","resolution":{"observed_at":"2026-08-07T14:40:31.418233Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1308.6142","last_updated":"2013-12-16T10:36:40Z","snapshot_observed_at":"2026-07-06T03:21:38.164769Z","submitted_at":"2013-08-28T12:30:06Z","title":"Viable f(T) models are practically indistinguishable from LCDM","version":3},"cited_work":{"arxiv_id":"1308.6142","doi":null,"metadata_source":"pith","pith_arxiv_id":"1308.6142","snapshot_observed_at":"2026-08-07T14:40:31.206775Z","title":"Viable f(T) models are practically indistinguishable from LCDM","venue":"astro-ph.CO","work_id":"501bff39-2a7c-457a-9e6b-335e11cc3dd3","year":2013},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.268422Z"},"links":{"cited_paper":"/paper/1308.6142","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:ff3faae4aba8cb9f0a186c600759657038bc607b79eb81d56eb37821676f432a","observation_id":"2ecb3dac-d5a7-4d10-ba60-17e0a1fd8fcb","resolution":{"observed_at":"2026-08-07T14:40:31.286618Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1510.08432","last_updated":"2016-05-05T11:30:13Z","snapshot_observed_at":"2026-07-06T04:34:36.474437Z","submitted_at":"2015-10-28T19:39:52Z","title":"The covariant formulation of f(T) gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.08432","snapshot_observed_at":"2026-08-07T14:40:23.410612Z","title":"Kr /caron.ts1s/caron.ts1s/acute.ts1ak and E","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.410612Z"},"links":{"cited_paper":"/paper/1510.08432","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:04e409b9019f1aa89c6fb9ed0151d6b40e49fb6bfea48ba2fcd2cd0a7bd9c400","observation_id":"d471cb26-c8a0-4277-afe9-de6f472a305f","resolution":{"observed_at":"2026-08-07T14:40:23.410612Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.07586","last_updated":"2016-09-08T17:34:46Z","snapshot_observed_at":"2026-07-06T04:37:35.431681Z","submitted_at":"2015-11-24T06:36:47Z","title":"f(T) teleparallel gravity and cosmology","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.07586","snapshot_observed_at":"2026-08-07T14:40:23.514334Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.514334Z"},"links":{"cited_paper":"/paper/1511.07586","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:77f76393d24ccca1d0b7f38f146707c8bf89bde211bc13b42eb13d1148c99c5f","observation_id":"816314bf-3a77-4bc6-8168-5aa83a548486","resolution":{"observed_at":"2026-08-07T14:40:23.514334Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.07171","last_updated":"2018-03-19T21:31:34Z","snapshot_observed_at":"2026-07-06T06:29:08.725216Z","submitted_at":"2018-03-19T21:31:34Z","title":"Effective gravitational coupling in modified teleparallel theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.07171","snapshot_observed_at":"2026-08-07T14:40:23.631639Z","title":"Abedi, S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.631639Z"},"links":{"cited_paper":"/paper/1803.07171","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:d0ce8f3b71a55370eeb9b12cdeddb150734d1999ab4a5a0bffbe870f0c899385","observation_id":"3b51aea5-5dd6-485e-9cc5-d40a7730674d","resolution":{"observed_at":"2026-08-07T14:40:23.631639Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.05933","last_updated":"2018-06-01T20:01:11Z","snapshot_observed_at":"2026-07-06T06:14:40.571088Z","submitted_at":"2017-12-16T10:37:21Z","title":"Gravitational waves in modified teleparallel theories of gravity","version":2},"cited_work":{"arxiv_id":"1712.05933","doi":null,"metadata_source":"pith","pith_arxiv_id":"1712.05933","snapshot_observed_at":"2026-08-07T14:40:30.944937Z","title":"Gravitational waves in modified teleparallel theories of gravity","venue":"gr-qc","work_id":"6a4125d1-3263-491a-b086-41d5d8d9e5f0","year":2017},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.709973Z"},"links":{"cited_paper":"/paper/1712.05933","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:31208a49ae1a0950dac00237e4230ac81a138bf644db86bae9e76d19a3df51cd","observation_id":"bd0aadab-a0c8-4202-af90-542158926f49","resolution":{"observed_at":"2026-08-07T14:40:31.037236Z","resolver_source":"local_arxiv","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2020.13582","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:30.754052Z","title":"Capozziello, M","venue":null,"work_id":"b7a30fdd-ac9b-4b37-a0ab-c12f55a9614b","year":2020},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.824614Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:c2fe2477e5691ff1710192ba89bfbfa20bf8146bcfae7d983a9be4b6caaf0579","observation_id":"0e573054-f1b5-4cec-bba3-ebe730e284eb","resolution":{"observed_at":"2026-08-07T14:40:30.845417Z","resolver_source":"raw_fallback","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1507.06123","last_updated":"2015-07-27T21:53:06Z","snapshot_observed_at":"2026-07-06T04:24:33.642334Z","submitted_at":"2015-07-22T10:53:38Z","title":"Constraining $f(R)$ gravity by the Large Scale Structure","version":2},"cited_work":{"arxiv_id":"1507.06123","doi":null,"metadata_source":"pith","pith_arxiv_id":"1507.06123","snapshot_observed_at":"2026-08-07T14:40:30.526361Z","title":"Constraining $f(R)$ gravity by the Large Scale Structure","venue":"gr-qc","work_id":"3d1276b8-6133-4ef0-b568-63f564b6481c","year":2015},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:23.930145Z"},"links":{"cited_paper":"/paper/1507.06123","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:2f3812fe4fc840c82af000e213f407e29fa70ae570063ccc33854048a1df4abf","observation_id":"bd5dbdea-dcb3-42ee-a013-63f172fc2b94","resolution":{"observed_at":"2026-08-07T14:40:30.543288Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1412.1471","last_updated":"2015-05-04T20:19:28Z","snapshot_observed_at":"2026-07-06T04:02:33.136517Z","submitted_at":"2014-12-03T20:44:28Z","title":"Noether Symmetry Approach for teleparallel-curvature cosmology","version":2},"cited_work":{"arxiv_id":"1412.1471","doi":null,"metadata_source":"pith","pith_arxiv_id":"1412.1471","snapshot_observed_at":"2026-08-07T14:40:30.448692Z","title":"Noether Symmetry Approach for teleparallel-curvature cosmology","venue":"gr-qc","work_id":"03062b16-accc-413d-a1ff-6f98a1e88289","year":2014},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.019770Z"},"links":{"cited_paper":"/paper/1412.1471","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:3d1b72858d6d8cc8a75f6bfb8d184f9d56f88c67ff7a44b77fb85894348a3489","observation_id":"c89ff0d8-3b1a-4ba0-a96b-ab0ced356f65","resolution":{"observed_at":"2026-08-07T14:40:30.511501Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1210.1098","last_updated":"2012-10-03T13:11:02Z","snapshot_observed_at":"2026-07-06T02:56:52.410992Z","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":"2026-08-07T14:40:24.126382Z","title":"Capozziello, P","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.126382Z"},"links":{"cited_paper":"/paper/1210.1098","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:d44d4be379bb2f2d5cd32e670fca66ee0d100660cf403ab9c58757293c21f98b","observation_id":"190e359d-c267-4fa2-aafa-10daae8ae2fa","resolution":{"observed_at":"2026-08-07T14:40:24.126382Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1308.5789","last_updated":"2013-10-17T00:41:34Z","snapshot_observed_at":"2026-07-06T03:21:31.510137Z","submitted_at":"2013-08-27T08:24:41Z","title":"Conformal symmetry and accelerating cosmology in teleparallel gravity","version":2},"cited_work":{"arxiv_id":"1308.5789","doi":null,"metadata_source":"pith","pith_arxiv_id":"1308.5789","snapshot_observed_at":"2026-08-07T14:40:30.271622Z","title":"Conformal symmetry and accelerating cosmology in teleparallel gravity","venue":"gr-qc","work_id":"2a3d2f7d-608b-4c4c-9a08-a5a7a49ce684","year":2013},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.224481Z"},"links":{"cited_paper":"/paper/1308.5789","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:0e655fa9c2b21d5be8ba8f728204e29e520fcc66dd377b19d4ec88d5cb5a9f97","observation_id":"4a57f79c-6750-4f05-8e5d-54a36a328bed","resolution":{"observed_at":"2026-08-07T14:40:30.353889Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1304.6191","last_updated":"2013-07-24T07:41:50Z","snapshot_observed_at":"2026-07-06T03:11:47.265163Z","submitted_at":"2013-04-23T07:44:36Z","title":"Effective $F(T)$ gravity from the higher-dimensional Kaluza-Klein and Randall-Sundrum theories","version":3},"cited_work":{"arxiv_id":"1304.6191","doi":null,"metadata_source":"pith","pith_arxiv_id":"1304.6191","snapshot_observed_at":"2026-08-07T14:40:30.060012Z","title":"Effective $F(T)$ gravity from the higher-dimensional Kaluza-Klein and Randall-Sundrum theories","venue":"gr-qc","work_id":"99231e62-6019-4f96-85c9-f8c243a1c8d0","year":2013},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.340597Z"},"links":{"cited_paper":"/paper/1304.6191","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:5771f24e17ae853ae4710f3a669c855dde2629b45db2b920f48b31dbe393de35","observation_id":"1517f515-933e-49d6-b908-6128f638180a","resolution":{"observed_at":"2026-08-07T14:40:30.168161Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:24.449263Z","title":"Reconstruction of f (T ) gravity: Rip cosmology, finite-time future singularities and thermo dynamics,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.449263Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:b1280e6e001289b7336bcb82c777ef6b11f6d31be976c5cc8a194bdeeb6a218d","observation_id":"e85ad505-0cb1-420c-aea4-a56bad07a57e","resolution":{"observed_at":"2026-08-07T14:40:24.449263Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.17277","last_updated":"2024-10-12T10:26:22Z","snapshot_observed_at":"2026-08-07T22:46:36.208802Z","submitted_at":"2023-12-27T19:28:25Z","title":"Observational Constraints and Cosmographic Analysis of $f({T},{T}_{{G}})$ Gravity and Cosmology","version":2},"cited_work":{"arxiv_id":"2312.17277","doi":null,"metadata_source":"pith","pith_arxiv_id":"2312.17277","snapshot_observed_at":"2026-08-07T14:40:29.834907Z","title":"Observational Constraints and Cosmographic Analysis of $f({T},{T}_{{G}})$ Gravity and Cosmology","venue":"gr-qc","work_id":"499f3334-da0a-40cb-be20-3ab2123d9c0b","year":2023},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.576473Z"},"links":{"cited_paper":"/paper/2312.17277","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:b4c92c88adf151cdb265bfa0fb472e41b89886d2c25f410586dbbce2cfb59f7c","observation_id":"302704cf-662c-4f8d-b919-bd97051fd930","resolution":{"observed_at":"2026-08-07T14:40:29.944480Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2312.15552","last_updated":"2024-06-01T07:19:20Z","snapshot_observed_at":"2026-07-06T17:07:48.292847Z","submitted_at":"2023-12-24T21:48:22Z","title":"Finsler-Randers-Sasaki gravity and cosmology","version":2},"cited_work":{"arxiv_id":"2312.15552","doi":null,"metadata_source":"pith","pith_arxiv_id":"2312.15552","snapshot_observed_at":"2026-08-07T14:40:29.669438Z","title":"Finsler-Randers-Sasaki gravity and cosmology","venue":"gr-qc","work_id":"86dcc7ef-9d8b-4f39-ac52-04be54a1839a","year":2023},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.659615Z"},"links":{"cited_paper":"/paper/2312.15552","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:21139b93136de65e78671cedb3642f1e0b884d8fd55ed9dcb2e2baa4ea1c7917","observation_id":"55ef5150-ede9-47ac-b471-c8e8d81091bf","resolution":{"observed_at":"2026-08-07T14:40:29.708238Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2211.11420","last_updated":"2023-05-01T02:59:38Z","snapshot_observed_at":"2026-08-03T05:17:09.614105Z","submitted_at":"2022-11-21T13:07:43Z","title":"General Effective Field Theory of Teleparallel Gravity","version":2},"cited_work":{"arxiv_id":"2211.11420","doi":null,"metadata_source":"pith","pith_arxiv_id":"2211.11420","snapshot_observed_at":"2026-08-07T14:40:29.569958Z","title":"General Effective Field Theory of Teleparallel Gravity","venue":"gr-qc","work_id":"d35fcc91-be4d-41a5-a096-798068532d80","year":2022},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.763612Z"},"links":{"cited_paper":"/paper/2211.11420","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:3d55733e5848d3960809cf0cf1a431d920513e5d2b5b7bc526655df3f8487699","observation_id":"745e636a-e80d-475b-ac69-4eef9e16b45a","resolution":{"observed_at":"2026-08-07T14:40:29.613009Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2209.01595","last_updated":"2022-09-04T11:14:17Z","snapshot_observed_at":"2026-08-08T18:37:23.670043Z","submitted_at":"2022-09-04T11:14:17Z","title":"Big Bang Nucleosynthesis constraints on $f(T,T_G)$ gravity","version":1},"cited_work":{"arxiv_id":"2209.01595","doi":null,"metadata_source":"pith","pith_arxiv_id":"2209.01595","snapshot_observed_at":"2026-08-07T14:40:29.460892Z","title":"Big Bang Nucleosynthesis constraints on $f(T,T_G)$ gravity","venue":"gr-qc","work_id":"18191424-e237-4dcb-8b8d-671ad5843474","year":2022},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.856876Z"},"links":{"cited_paper":"/paper/2209.01595","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:0f88c016a416c8650af76f3a544200ca4844685839d6dfb1ac3e5f58391c0ea7","observation_id":"864b2700-7bf0-4fec-bd0d-522ce2c709c6","resolution":{"observed_at":"2026-08-07T14:40:29.508688Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1475-7516/2022/10/087","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:28.255804Z","title":"Q uasinormal modes of black holes in f(T) gravity,","venue":null,"work_id":"48657d80-ee9b-4358-886a-6a3e287fde98","year":2022},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:24.966102Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:eae351146549310b9432bdae1d0da841c373ba453459b729dcccdfb19a9c9dad","observation_id":"491a3249-8544-4773-ac34-3794ab91f659","resolution":{"observed_at":"2026-08-07T14:40:28.299748Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2203.14866","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:29.372292Z","title":"Unified dark sec- tors in scalar-torsion theories of gravity,","venue":null,"work_id":"d048ab62-89be-4b4c-b08b-06c007754626","year":2022},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:25.082520Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:23ec2b3a9d783703c33144ad1e8804c83b89a8540f9f166280275a7ed061860b","observation_id":"a8ea3cbc-646e-4e03-84ff-27adc80c05b5","resolution":{"observed_at":"2026-08-07T14:40:29.400599Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2203.01926","last_updated":"2022-06-30T14:34:27Z","snapshot_observed_at":"2026-08-06T14:14:04.532599Z","submitted_at":"2022-03-03T18:58:36Z","title":"Gaussian processes and effective field theory of $f(T)$ gravity under the $H_0$ tension","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.01926","snapshot_observed_at":"2026-08-07T14:40:25.174661Z","title":"G aussian processes and effec- tive field theory of f (T ) gravity under the H0 tension,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:25.174661Z"},"links":{"cited_paper":"/paper/2203.01926","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:1c8bc93450b0feb37415f56bd08c30cfedaaa325d222131a1eca2d262fd9d439","observation_id":"2984553f-4f1d-4556-b2bb-ed9529b1a1cc","resolution":{"observed_at":"2026-08-07T14:40:25.174661Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.06359","last_updated":"2022-04-17T10:00:28Z","snapshot_observed_at":"2026-07-06T12:07:42.057797Z","submitted_at":"2021-11-11T18:17:54Z","title":"Stability of motion and thermodynamics in charged black holes in $f(T)$ gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.06359","snapshot_observed_at":"2026-08-07T14:40:25.365176Z","title":"Stability of motion and thermodynamics in charged black holes in f(T) gravity,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:25.365176Z"},"links":{"cited_paper":"/paper/2111.06359","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:7fac27d6953caf0eee95b8d0aa66562f8e94fcede42c539dd173d43eac6c7152","observation_id":"633bd823-5d4e-4c26-8321-93097c887d3d","resolution":{"observed_at":"2026-08-07T14:40:25.365176Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.01937","last_updated":"2021-07-05T11:08:53Z","snapshot_observed_at":"2026-07-06T11:25:58.411215Z","submitted_at":"2021-07-05T11:08:53Z","title":"Gravitationally Induced Particle Production through a Nonminimal Torsion-Matter Coupling","version":1},"cited_work":{"arxiv_id":"2107.01937","doi":null,"metadata_source":"pith","pith_arxiv_id":"2107.01937","snapshot_observed_at":"2026-08-07T14:40:29.107725Z","title":"Gravitationally Induced Particle Production through a Nonminimal Torsion-Matter Coupling","venue":"gr-qc","work_id":"7e25d05c-a239-4ee5-bf8c-32acf5afd488","year":2021},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:25.483129Z"},"links":{"cited_paper":"/paper/2107.01937","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:f2ddab7f014d8fc61284b79bd9dc44036026f2275ebc530a21910919974f0788","observation_id":"dfc4d4e2-b278-4f78-8be3-3fa8b4ee44a9","resolution":{"observed_at":"2026-08-07T14:40:29.142488Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:25.598694Z","title":"Metric-Affine Gravity,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:25.598694Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:1a52beb269b9fd2582404e23a8f6e722123a8ee00993c069c99b3070a9adf478","observation_id":"d3fba9f8-a55e-4823-9a65-fc37cfab96d2","resolution":{"observed_at":"2026-08-07T14:40:25.598694Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1475-7516/2021/09/019","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:28.138992Z","title":"f(T) cosmology: from P seudo-Bang to Pseudo-Rip,","venue":null,"work_id":"d4b85f6f-262d-4b28-ae5f-73d33dbebcc7","year":2021},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:25.681654Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:9b51c3f2a96362c5d9359b1fc0fed348edc04c3191776d7104801f92e64b1939","observation_id":"3cc8a449-b2ee-45c6-afcd-f76d2fe24ca0","resolution":{"observed_at":"2026-08-07T14:40:28.186860Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.102.023525","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:27.964126Z","title":"Cosmological applications of F (R, T) gravity with dynamical curvature and torsion,","venue":null,"work_id":"5ddf1ef9-3f87-4d29-9cc1-3f99f16c01d3","year":2020},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:25.803780Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:d09f93602b64004be2414d889a7e774f9d7aa4f8aaff0d71af1a176a5890c758","observation_id":"354a17af-639f-420e-a9bf-ed89d8c82d14","resolution":{"observed_at":"2026-08-07T14:40:28.024029Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1909.06388","last_updated":"2020-08-05T13:35:49Z","snapshot_observed_at":"2026-07-06T08:21:38.125492Z","submitted_at":"2019-09-13T18:01:16Z","title":"Interpreting cosmological tensions from the effective field theory of torsional gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.06388","snapshot_observed_at":"2026-08-07T14:40:25.931319Z","title":"Interpreting cosmological tensions from the effective field theory of torsi onal gravity,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:25.931319Z"},"links":{"cited_paper":"/paper/1909.06388","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:9a92683d88f9f1ffa2f8827e89fd422d138bc02497b740761b402a26e37cf4a2","observation_id":"8520404c-d0e8-43b7-82d6-361817defaf0","resolution":{"observed_at":"2026-08-07T14:40:25.931319Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1908.05741","last_updated":"2019-08-14T06:55:53Z","snapshot_observed_at":"2026-08-02T17:03:46.062831Z","submitted_at":"2019-08-14T06:55:53Z","title":"Conformal Gravity and Transformations in the Symmetric Teleparallel Framework","version":1},"cited_work":{"arxiv_id":"1908.05741","doi":null,"metadata_source":"pith","pith_arxiv_id":"1908.05741","snapshot_observed_at":"2026-08-07T14:40:28.993681Z","title":"Conformal Gravity and Transformations in the Symmetric Teleparallel Framework","venue":"gr-qc","work_id":"12cab486-ec45-4420-bbeb-956610b758bd","year":2019},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.025518Z"},"links":{"cited_paper":"/paper/1908.05741","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:bcb4815fcc5d9c5085f542a750e78ef806d32448a0e93aa4d13b3e02fb315496","observation_id":"75d33261-67e5-45b1-b552-31c355e8a50a","resolution":{"observed_at":"2026-08-07T14:40:29.037401Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.12225","last_updated":"2020-11-19T16:04:41Z","snapshot_observed_at":"2026-08-06T06:04:41.824486Z","submitted_at":"2019-07-29T06:21:29Z","title":"New test on general relativity and $f(T)$ torsional gravity from galaxy-galaxy weak lensing surveys","version":3},"cited_work":{"arxiv_id":"1907.12225","doi":null,"metadata_source":"pith","pith_arxiv_id":"1907.12225","snapshot_observed_at":"2026-08-07T14:40:28.871618Z","title":"New test on general relativity and $f(T)$ torsional gravity from galaxy-galaxy weak lensing surveys","venue":"astro-ph.CO","work_id":"bca91bdc-5c85-49a8-9523-002e5159628e","year":2019},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.129414Z"},"links":{"cited_paper":"/paper/1907.12225","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:89fd4a878765d4a8032c2fcf1e195c8233dbddac5c6861dfb5d0cb42b5784fe5","observation_id":"3ba87fae-3ef6-4918-b3fa-81f556a6557c","resolution":{"observed_at":"2026-08-07T14:40:28.927847Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1811.03658","last_updated":"2019-06-09T14:51:15Z","snapshot_observed_at":"2026-08-05T13:48:12.585224Z","submitted_at":"2018-11-08T19:35:26Z","title":"Rotating AdS black holes in Maxwell-$f(T)$ gravity","version":3},"cited_work":{"arxiv_id":"1811.03658","doi":null,"metadata_source":"pith","pith_arxiv_id":"1811.03658","snapshot_observed_at":"2026-08-07T14:40:28.784274Z","title":"Rotating AdS black holes in Maxwell-$f(T)$ gravity","venue":"gr-qc","work_id":"1ee825d3-29f0-491b-aeb8-927215644a97","year":2018},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.266937Z"},"links":{"cited_paper":"/paper/1811.03658","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:7bca91cfc69fe40b27a15965bb2688371ac1482311789ffc82faf6d212c4d2c1","observation_id":"40a8c0a4-880c-41d1-923c-bff0f3f6a139","resolution":{"observed_at":"2026-08-07T14:40:28.812667Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1810.08220","last_updated":"2019-08-07T08:25:15Z","snapshot_observed_at":"2026-08-08T06:55:35.763874Z","submitted_at":"2018-10-18T18:06:25Z","title":"Polarization of gravitational waves in symmetric teleparallel theories of gravity and their modifications","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.08220","snapshot_observed_at":"2026-08-07T14:40:26.376698Z","title":"Polarization of gravitational waves in symmetric teleparallel theories of gravity and the ir modifications,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.376698Z"},"links":{"cited_paper":"/paper/1810.08220","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:9bd60cb2e1bb61df4edcffee20f5a9d7806c8b75539fcf5acca19651b5a07b8f","observation_id":"e1b9d9b1-5d16-4aed-a8e3-d48d5e2a864f","resolution":{"observed_at":"2026-08-07T14:40:26.376698Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.07365","last_updated":"2018-06-28T08:28:21Z","snapshot_observed_at":"2026-07-06T06:34:24.166201Z","submitted_at":"2018-04-19T20:16:36Z","title":"Gravitational Waves in Modified Teleparallel Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.07365","snapshot_observed_at":"2026-08-07T14:40:26.471900Z","title":"Gravitational Waves in Modified Teleparallel Theories,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.471900Z"},"links":{"cited_paper":"/paper/1804.07365","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:cfb85e984c0d85bd026a1b967d5aadb020ce7f73392e65c7c4c54120b0761d6c","observation_id":"63de4549-4cbd-4636-8cac-78a2e0a47db1","resolution":{"observed_at":"2026-08-07T14:40:26.471900Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/jhep02(2019)009","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:27.860779Z","title":"Dark matter and energy from the effective field theory of torsion,","venue":null,"work_id":"eca2f827-0421-462c-86d4-69451c704b4b","year":2019},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.581921Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:14f8fe7f4fa82a5e605e20856a62f2f6e1ae71212411342dcd892c1124a70160","observation_id":"0646cb4c-73e6-4641-9003-f428aaf97e84","resolution":{"observed_at":"2026-08-07T14:40:27.898127Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2404.09698","last_updated":"2024-04-15T11:59:36Z","snapshot_observed_at":"2026-08-04T03:02:16.350716Z","submitted_at":"2024-04-15T11:59:36Z","title":"Myrzakulov $F(T,Q)$ gravity: cosmological implications and constraints","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.09698","snapshot_observed_at":"2026-08-07T14:40:26.666323Z","title":"Myrzakulov F(T,Q) Gravity: Cosmological Implications and Constraints,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.666323Z"},"links":{"cited_paper":"/paper/2404.09698","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:91a5730cd2e5d53a6af470550831c0ae746d2c6684728a92eb880902a1fc032b","observation_id":"17e8fd67-7d63-4592-85b3-c2ac0f7e9938","resolution":{"observed_at":"2026-08-07T14:40:26.666323Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.02123","last_updated":"2024-02-03T11:17:19Z","snapshot_observed_at":"2026-08-05T23:06:30.729811Z","submitted_at":"2024-02-03T11:17:19Z","title":"Exact Cosmology in Myrzakulov Gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.02123","snapshot_observed_at":"2026-08-07T14:40:26.713843Z","title":"Exact Cosmology in Myrzak ulov Gravity,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.713843Z"},"links":{"cited_paper":"/paper/2402.02123","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:aef233b6eb5f46a68764aec9dbd2f5705dea256159d28d66106516f278a3ceda","observation_id":"86f299eb-2510-4082-a99e-331c003fae14","resolution":{"observed_at":"2026-08-07T14:40:26.713843Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00686","last_updated":"2024-02-19T06:29:57Z","snapshot_observed_at":"2026-07-06T17:10:28.919468Z","submitted_at":"2024-01-01T07:20:42Z","title":"Transit cosmological models in Myrzakulov F(R,T) gravity theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.00686","snapshot_observed_at":"2026-08-07T14:40:26.759031Z","title":"Transit Cosmological Mod els in Myrzakulov F(R,T) Gravity Theory,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.759031Z"},"links":{"cited_paper":"/paper/2401.00686","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:47bd13160ce6e01bca754256ecb9e66ae05c7c6087814042ecb9259506d63579","observation_id":"a12a197f-8078-4383-8044-e68732a76608","resolution":{"observed_at":"2026-08-07T14:40:26.759031Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.09230","last_updated":"2024-11-17T17:34:08Z","snapshot_observed_at":"2026-08-03T01:14:45.840954Z","submitted_at":"2023-09-17T10:02:05Z","title":"Cosmological Study in Myrzakulov $F(R, T)$ Quasi-dilaton Massive Gravity","version":2},"cited_work":{"arxiv_id":"2309.09230","doi":null,"metadata_source":"pith","pith_arxiv_id":"2309.09230","snapshot_observed_at":"2026-08-07T14:40:28.637092Z","title":"Cosmological Study in Myrzakulov $F(R, T)$ Quasi-dilaton Massive Gravity","venue":"gr-qc","work_id":"8e61375a-2728-4453-a0c5-569e04e35560","year":2023},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.804182Z"},"links":{"cited_paper":"/paper/2309.09230","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:7ddfc77ca2fdddb3b205b4950a8dca54318de6f07fdaeeec840ec6a84c21cc6c","observation_id":"08fecce4-dfa6-49d7-87f2-9648360144a8","resolution":{"observed_at":"2026-08-07T14:40:28.683343Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2202.10871","last_updated":"2022-10-19T10:39:23Z","snapshot_observed_at":"2026-07-06T12:40:23.619725Z","submitted_at":"2022-02-22T13:09:19Z","title":"Dynamical system analysis of Myrzakulov gravity","version":2},"cited_work":{"arxiv_id":"2202.10871","doi":null,"metadata_source":"pith","pith_arxiv_id":"2202.10871","snapshot_observed_at":"2026-08-07T14:40:29.211355Z","title":"Dynamical system analysis of Myrzakulov gravity","venue":"gr-qc","work_id":"b490028d-caa6-4fdb-9e8d-0808b0e1b581","year":2022},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:26.910874Z"},"links":{"cited_paper":"/paper/2202.10871","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:e40b3c197c95953a912fb47b6a1781865923e573a534150b2a661859acb04660","observation_id":"2b42ebae-13cc-4a31-9417-4999e0a4980a","resolution":{"observed_at":"2026-08-07T14:40:29.261515Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2108.00957","last_updated":"2021-07-30T07:32:50Z","snapshot_observed_at":"2026-08-08T01:56:52.740652Z","submitted_at":"2021-07-30T07:32:50Z","title":"Metric-Affine Myrzakulov Gravity Theories","version":1},"cited_work":{"arxiv_id":"2108.00957","doi":null,"metadata_source":"pith","pith_arxiv_id":"2108.00957","snapshot_observed_at":"2026-08-07T14:40:28.545235Z","title":"Metric-Affine Myrzakulov Gravity Theories","venue":"gr-qc","work_id":"1f93c905-7879-42c3-89c8-c3578f4ff497","year":2021},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.043818Z"},"links":{"cited_paper":"/paper/2108.00957","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:c1f83dd1443c1a1878561841c89145c6ce1006e674dd4cf1b42397ff9a588248","observation_id":"5d108daa-f412-4325-a360-df2d32f51f41","resolution":{"observed_at":"2026-08-07T14:40:28.583157Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1205.5266","last_updated":"2024-05-31T09:36:19Z","snapshot_observed_at":"2026-07-06T02:48:40.122616Z","submitted_at":"2012-05-23T18:53:30Z","title":"Metric-affine Myrzakulov gravity and its generalizations","version":8},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1205.5266","snapshot_observed_at":"2026-08-07T14:40:27.118961Z","title":"Myrzakulov, [arXiv:1205.5266 [physics.gen-ph]]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.118961Z"},"links":{"cited_paper":"/paper/1205.5266","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:2fdfd5fce8ed7bf262b072659903d7ad2e1415b4a30933deee6f202dd558df31","observation_id":"d1acaa84-b37c-4851-a626-8e917c41afd2","resolution":{"observed_at":"2026-08-07T14:40:27.118961Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.79.1240","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:27.759837Z","title":null,"venue":null,"work_id":"6415a985-4121-4388-aa6e-918ae328163c","year":2009},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.173320Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:07e7428c7ab4a811a986898059c66bc3b3ff2371b338ae51ddc2ed46c8639e83","observation_id":"d93720cc-5a4a-4377-8d02-4b96e458410a","resolution":{"observed_at":"2026-08-07T14:40:27.808561Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/j.physrep.2010.01.001","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-07T14:40:27.676467Z","title":null,"venue":null,"work_id":"128d675a-91de-4e94-a02a-415d4e1c8bac","year":2010},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.221686Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:bf30a99e14e3d9b2e9ba27e9d9f9f31c0314c7de4d49f3735ee54e42ed16b069","observation_id":"4489a838-d215-48cf-bf8c-075388605bc8","resolution":{"observed_at":"2026-08-07T14:40:27.718054Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2504.02002","last_updated":"2025-04-01T15:06:30Z","snapshot_observed_at":"2026-08-07T16:17:10.391598Z","submitted_at":"2025-04-01T15:06:30Z","title":"Metric-Affine Myrzakulov Gravity Theories: Models, Applications and Theoretical Developments","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.02002","snapshot_observed_at":"2026-08-07T14:40:27.290790Z","title":"Momeni and R","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.290790Z"},"links":{"cited_paper":"/paper/2504.02002","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:aeee63ab3d9aaf3f80b56f5ecf28d069f05047314aeffeeb6234e54eb5871cd6","observation_id":"358c26e2-7a07-4e1c-b28d-b10391a872a7","resolution":{"observed_at":"2026-08-07T14:40:27.290790Z","resolver_source":null,"status":"malformed_identifier"},"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":"2026-08-07T14:40:27.335837Z","title":"Momeni and R","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.335837Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:2d09ed77f96e1354e64f600e54cc1db443fafa0d2f1d59138990e467de426489","observation_id":"0af6b6d9-6cea-4c96-a9c6-ee1ebd2d5750","resolution":{"observed_at":"2026-08-07T14:40:27.335837Z","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":"2026-08-07T14:40:31.813059Z","title":"Teleparallel equivalen t of Gauss-Bonnet gravity and its modifications,","venue":null,"work_id":"a633e3cf-b717-41d7-9c18-62b1e6aa9120","year":2014},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.380500Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:1e6425245417586d6978f2dc32025538d81762ec8b9292109a27e54d1d14c951","observation_id":"ce58343a-a4d2-473b-8904-690191d93094","resolution":{"observed_at":"2026-08-07T14:40:31.898219Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:31.703137Z","title":"Nojiri and S","venue":null,"work_id":"9d711f08-7584-48a2-9edf-434b0465bc5e","year":2005},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.434420Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:3dab4c248da4ee597e11ac2ea035f5a5bd8b5cd8fd3a3498d13e30e71e0dab4d","observation_id":"e31d4d8c-b205-447b-9f19-7d2794d5c45b","resolution":{"observed_at":"2026-08-07T14:40:31.748101Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:31.608874Z","title":"Capozziello and M","venue":null,"work_id":"e95be559-4819-4798-a110-7b9e96c0973a","year":2008},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.501117Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:d98667846817528696253df108b47a147732825bc69378838c54b8a951ab6a9c","observation_id":"ffa2dcb4-f71f-4213-8d7a-455302841c52","resolution":{"observed_at":"2026-08-07T14:40:31.657910Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-07T14:40:31.516756Z","title":"Fonseca et al., A new neutron star mass measurement from X-ray timing observ ations, Nature 593, 211-214 (2021)","venue":null,"work_id":"0f162ebe-2680-4906-81c7-79b121f5113a","year":2021},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.546333Z"},"links":{"citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:dc2cc641e92700c40a4a184b21d02ea3d9cd8a01a8692210fb53bc99583b4c4e","observation_id":"33fa75e6-ae87-4112-a28a-2dabc4dda867","resolution":{"observed_at":"2026-08-07T14:40:31.555711Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"cited_work":{"arxiv_id":"2505.18285","doi":null,"metadata_source":"pith","pith_arxiv_id":"2505.18285","snapshot_observed_at":"2026-08-07T14:40:28.369728Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","venue":"gr-qc","work_id":"1ed5e94b-4985-48ae-a77a-6e0a52e7e1d8","year":2025},"citing_paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-07T14:40:27.598587Z"},"links":{"cited_paper":"/paper/2505.18285","citing_paper":"/paper/2505.18285"},"observation_digest":"sha256:2852d80f438343ba5c59912b01116ff7f3aeeb488789366cdff37eb43995bfb5","observation_id":"a294c7a8-8e9d-469d-b370-34d4b79f83ac","resolution":{"observed_at":"2026-08-07T14:40:28.412652Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2505.18285","last_updated":"2025-05-23T18:30:14Z","latest_version":1,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-07T14:31:42.926116Z","submitted_at":"2025-05-23T18:30:14Z","title":"Einstein-Gauss-Bonnet-Myrzakulov Gravity from $R + F(T, G)$: Numerical Insights and Torsion-Gauss-Bonnet Dynamics in Weitzenb\\\"ock Spacetime"},"reference_resolution":{"displayed":57,"state_counts":{"malformed_identifier":2,"metadata_mismatch":1,"parse_uncertain":0,"unresolved":21,"verified_exact":25,"verified_fuzzy":8},"total_outbound_references":57},"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":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"thesis":"As of 8 August 2026, this Paper Citation Record lists 57 of 57 outbound references and 1 inbound Pith citation observation for arXiv:2505.18285."}