{"as_of":"2026-08-12T15:33:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:5d352893675c0c0f8c6fc154124327aab9ae2900d2f1621b87980a9a7809b91d","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":7,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":7,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-12T06:34:41.77262+00:00","state":"measured"},{"denominator":7,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":7,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T19:52:41.721794Z","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":"2026-07-01T14:45:49.778348Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2103.10983","last_updated":"2021-08-12T17:17:49Z","snapshot_observed_at":"2026-08-12T08:46:30.687318Z","submitted_at":"2021-03-19T18:40:25Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant","version":2},"cited_work":{"arxiv_id":"2103.10983","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2103.10983","snapshot_observed_at":"2026-07-01T14:45:49.778348Z","title":"Hajian, H","venue":null,"work_id":"c25936cf-e490-43eb-94ef-8fde050b5f84","year":2021},"citing_paper":{"arxiv_id":"2509.08390","last_updated":"2026-04-17T03:14:17Z","snapshot_observed_at":"2026-07-06T22:27:30.075376Z","submitted_at":"2025-09-10T08:33:14Z","title":"Gravitational constant as a conserved charge in black hole thermodynamics","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-05-18T18:21:41.604721Z"},"links":{"cited_paper":"/paper/2103.10983","citing_paper":"/paper/2509.08390"},"observation_digest":"sha256:b9be10955acf4c23e84cc1291911b326fe8c5bb33eb269691847a26bac0e42ec","observation_id":"81a709e3-0826-4f32-8a5f-f734fb73a403","resolution":{"observed_at":"2026-05-18T18:22:46.998979Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2103.10983","last_updated":"2021-08-12T17:17:49Z","snapshot_observed_at":"2026-08-12T08:46:30.687318Z","submitted_at":"2021-03-19T18:40:25Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.10983","snapshot_observed_at":"2026-08-03T19:52:41.721794Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2511.22558","last_updated":"2026-06-15T17:31:54Z","snapshot_observed_at":"2026-08-08T12:44:12.866902Z","submitted_at":"2025-11-27T15:48:35Z","title":"A Universal Smarr Formula via Coupling Constants","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-03T19:52:41.721794Z"},"links":{"cited_paper":"/paper/2103.10983","citing_paper":"/paper/2511.22558"},"observation_digest":"sha256:66f61ff34b6dd627792fb1a91eeebe72ad7a19ca67ec57f6e69e48fc92cb7cfe","observation_id":"8bb35357-2048-479d-a2bc-c583a1bb0668","resolution":{"observed_at":"2026-08-03T19:52:41.721794Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.10983","last_updated":"2021-08-12T17:17:49Z","snapshot_observed_at":"2026-08-12T08:46:30.687318Z","submitted_at":"2021-03-19T18:40:25Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant","version":2},"cited_work":{"arxiv_id":"2103.10983","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2103.10983","snapshot_observed_at":"2026-07-01T14:45:49.778348Z","title":"Hajian, H","venue":null,"work_id":"c25936cf-e490-43eb-94ef-8fde050b5f84","year":2021},"citing_paper":{"arxiv_id":"2601.15592","last_updated":"2026-05-14T06:03:01Z","snapshot_observed_at":"2026-08-06T02:45:15.570062Z","submitted_at":"2026-01-22T02:33:28Z","title":"Extended symmetry of the Maxwell theory with a gauge coupling constant as a conserved charge","version":4},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-05-16T12:37:00.127066Z"},"links":{"cited_paper":"/paper/2103.10983","citing_paper":"/paper/2601.15592"},"observation_digest":"sha256:4e86ebed5bec704640adb93b74da6e965f913146cd1b778d0e1ba04361d7a6e3","observation_id":"5c04f9e8-4601-4e68-bc89-a5dcdf94a894","resolution":{"observed_at":"2026-05-16T12:37:52.993240Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2103.10983","last_updated":"2021-08-12T17:17:49Z","snapshot_observed_at":"2026-08-12T08:46:30.687318Z","submitted_at":"2021-03-19T18:40:25Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant","version":2},"cited_work":{"arxiv_id":"2103.10983","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2103.10983","snapshot_observed_at":"2026-07-01T14:45:49.778348Z","title":"Hajian, H","venue":null,"work_id":"c25936cf-e490-43eb-94ef-8fde050b5f84","year":2021},"citing_paper":{"arxiv_id":"2605.15005","last_updated":"2026-05-14T16:06:36Z","snapshot_observed_at":"2026-07-06T23:26:23.179482Z","submitted_at":"2026-05-14T16:06:36Z","title":"An Exact Single-Rotating Near-Horizon Geometry in Einstein-Gauss-Bonnet Gravity","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-06-30T20:05:01.418811Z"},"links":{"cited_paper":"/paper/2103.10983","citing_paper":"/paper/2605.15005"},"observation_digest":"sha256:fcb11c015d4ea6435b5af7854fc6b2e352576fee31d1b7578dcb169042220880","observation_id":"5278c868-4880-42ee-af9f-93037b6e4468","resolution":{"observed_at":"2026-07-01T14:45:49.780385Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2103.10983","last_updated":"2021-08-12T17:17:49Z","snapshot_observed_at":"2026-08-12T08:46:30.687318Z","submitted_at":"2021-03-19T18:40:25Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant","version":2},"cited_work":{"arxiv_id":"2103.10983","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2103.10983","snapshot_observed_at":"2026-07-01T14:45:49.778348Z","title":"Hajian, H","venue":null,"work_id":"c25936cf-e490-43eb-94ef-8fde050b5f84","year":2021},"citing_paper":{"arxiv_id":"2606.30507","last_updated":"2026-07-15T23:58:35Z","snapshot_observed_at":"2026-08-07T02:34:29.444345Z","submitted_at":"2026-06-29T16:13:54Z","title":"The Role of the Volume in Black Hole Thermodynamics","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-06-30T04:52:40.574118Z"},"links":{"cited_paper":"/paper/2103.10983","citing_paper":"/paper/2606.30507"},"observation_digest":"sha256:5fe5ceb1ee3d259389d6ac1f3b401d9506c02ba57c2de0aa98531e944066ec62","observation_id":"42534f5d-10f1-40c2-b0f3-54e3b6f13cdc","resolution":{"observed_at":"2026-06-30T04:54:16.657735Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2103.10983","last_updated":"2021-08-12T17:17:49Z","snapshot_observed_at":"2026-08-12T08:46:30.687318Z","submitted_at":"2021-03-19T18:40:25Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.10983","snapshot_observed_at":"2026-08-02T09:33:10.974457Z","title":"Hajian, H","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2606.30507","last_updated":"2026-07-15T23:58:35Z","snapshot_observed_at":"2026-08-07T02:34:29.444345Z","submitted_at":"2026-06-29T16:13:54Z","title":"The Role of the Volume in Black Hole Thermodynamics","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-02T09:33:10.974457Z"},"links":{"cited_paper":"/paper/2103.10983","citing_paper":"/paper/2606.30507"},"observation_digest":"sha256:ec3eb88a844e2eaefad66fe2f7a4782e49d93c086ecf9c72f042d7edf8840ea1","observation_id":"5a6efb40-5a71-4914-8ace-e074d5e377c5","resolution":{"observed_at":"2026-08-02T09:33:10.974457Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.10983","last_updated":"2021-08-12T17:17:49Z","snapshot_observed_at":"2026-08-12T08:46:30.687318Z","submitted_at":"2021-03-19T18:40:25Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant","version":2},"cited_work":{"arxiv_id":"2103.10983","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2103.10983","snapshot_observed_at":"2026-07-01T14:45:49.778348Z","title":"Hajian, H","venue":null,"work_id":"c25936cf-e490-43eb-94ef-8fde050b5f84","year":2021},"citing_paper":{"arxiv_id":"2606.30707","last_updated":"2026-06-29T14:36:48Z","snapshot_observed_at":"2026-08-03T18:12:50.541578Z","submitted_at":"2026-06-29T14:36:48Z","title":"Dynamical Completion of Coupling-Charge Thermodynamics","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-07-01T02:14:56.293536Z"},"links":{"cited_paper":"/paper/2103.10983","citing_paper":"/paper/2606.30707"},"observation_digest":"sha256:f4433022a92404f0dec1e26086a23be833178a86d5a564fd5b13a63264b24a6f","observation_id":"2858ca10-7e13-4187-a4c8-cd6d3a214df6","resolution":{"observed_at":"2026-07-01T12:15:44.144906Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2103.10983/citation-record","integrity":"/paper/2103.10983/integrity","json":"/paper/2103.10983/citation-record.json","paper":"/paper/2103.10983"},"outbound":[],"paper":{"arxiv_id":"2103.10983","last_updated":"2021-08-12T17:17:49Z","latest_version":2,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-12T08:46:30.687318Z","submitted_at":"2021-03-19T18:40:25Z","title":"First law of black hole thermodynamics and Smarr formula with a cosmological constant"},"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":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"thesis":"As of 12 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 7 inbound Pith citation observations for arXiv:2103.10983."}