{"as_of":"2026-08-08T03:58:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:5a1f16f271152949f52fd092b09f19a134eb7fd902c3378940f772e43c6bc2e3","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":"2026-08-07T06:34:17.273281+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":"2026-08-07T00:33:57.019800Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-06-29T21:03:58.610213Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2409.18178","last_updated":"2025-03-24T03:36:47Z","snapshot_observed_at":"2026-08-04T22:12:15.403086Z","submitted_at":"2024-09-26T18:00:01Z","title":"Dual Dressed Black Holes as the end point of the Charged Superradiant instability in ${\\cal N} = 4$ Yang Mills","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.18178","snapshot_observed_at":"2026-08-07T00:33:57.019800Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2506.13887","last_updated":"2025-06-16T18:10:02Z","snapshot_observed_at":"2026-08-07T15:09:30.907217Z","submitted_at":"2025-06-16T18:10:02Z","title":"Probing Non-Graviton Spectra in $\\mathcal{N}=4$ SYM via BMN truncation and S-Duality","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-07T00:33:57.019800Z"},"links":{"cited_paper":"/paper/2409.18178","citing_paper":"/paper/2506.13887"},"observation_digest":"sha256:7cadd2096da82497e9040f1065030158fd5d5fbfccf8d0e9ec5c5e9a9d58d501","observation_id":"172d8f74-76f7-403f-85b1-9962e2aee859","resolution":{"observed_at":"2026-08-07T00:33:57.019800Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.18178","last_updated":"2025-03-24T03:36:47Z","snapshot_observed_at":"2026-08-04T22:12:15.403086Z","submitted_at":"2024-09-26T18:00:01Z","title":"Dual Dressed Black Holes as the end point of the Charged Superradiant instability in ${\\cal N} = 4$ Yang Mills","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.18178","snapshot_observed_at":"2026-08-06T20:02:11.983358Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.04131","last_updated":"2025-07-05T19:04:18Z","snapshot_observed_at":"2026-08-07T10:38:17.151890Z","submitted_at":"2025-07-05T19:04:18Z","title":"Instability of Black Holes in AdS$_3 \\times S^3$","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T20:02:11.983358Z"},"links":{"cited_paper":"/paper/2409.18178","citing_paper":"/paper/2507.04131"},"observation_digest":"sha256:6d7d62133b975524133a9731e0816185528602b619e6c5a65b2f3788bfc35b62","observation_id":"52b36164-45d9-4b93-bef8-ff4a1d64bdc2","resolution":{"observed_at":"2026-08-06T20:02:11.983358Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.18178","last_updated":"2025-03-24T03:36:47Z","snapshot_observed_at":"2026-08-04T22:12:15.403086Z","submitted_at":"2024-09-26T18:00:01Z","title":"Dual Dressed Black Holes as the end point of the Charged Superradiant instability in ${\\cal N} = 4$ Yang Mills","version":2},"cited_work":{"arxiv_id":"2409.18178","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2409.18178","snapshot_observed_at":"2026-06-29T21:03:58.610213Z","title":null,"venue":null,"work_id":"f9ccf271-ef59-4bd6-8b08-3687acf71029","year":2025},"citing_paper":{"arxiv_id":"2510.19939","last_updated":"2026-04-14T06:06:53Z","snapshot_observed_at":"2026-08-02T04:44:07.461925Z","submitted_at":"2025-10-22T18:08:32Z","title":"Covariant phase space and the semi-classical Einstein equation","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-05-18T04:26:54.007695Z"},"links":{"cited_paper":"/paper/2409.18178","citing_paper":"/paper/2510.19939"},"observation_digest":"sha256:b5dc48ba5bec6228de8c8090d90e15c6c39f1456b9ece43f268307e69341e005","observation_id":"7c72456c-ec92-4eaa-a669-2f317c1b0dae","resolution":{"observed_at":"2026-05-18T04:30:53.510238Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.18178","last_updated":"2025-03-24T03:36:47Z","snapshot_observed_at":"2026-08-04T22:12:15.403086Z","submitted_at":"2024-09-26T18:00:01Z","title":"Dual Dressed Black Holes as the end point of the Charged Superradiant instability in ${\\cal N} = 4$ Yang Mills","version":2},"cited_work":{"arxiv_id":"2409.18178","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2409.18178","snapshot_observed_at":"2026-06-29T21:03:58.610213Z","title":null,"venue":null,"work_id":"f9ccf271-ef59-4bd6-8b08-3687acf71029","year":2025},"citing_paper":{"arxiv_id":"2604.00095","last_updated":"2026-04-30T01:25:15Z","snapshot_observed_at":"2026-07-06T22:51:22.254518Z","submitted_at":"2026-03-31T18:18:42Z","title":"Instanton condensation and a new phase of BPS black holes","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-05-13T22:44:48.684585Z"},"links":{"cited_paper":"/paper/2409.18178","citing_paper":"/paper/2604.00095"},"observation_digest":"sha256:54b70baa578df5070264c40f27e5ade518da370d222b45afd4bf37335340f9d1","observation_id":"44485115-2252-405a-ae94-2239476f6f0d","resolution":{"observed_at":"2026-05-13T22:48:23.143638Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.18178","last_updated":"2025-03-24T03:36:47Z","snapshot_observed_at":"2026-08-04T22:12:15.403086Z","submitted_at":"2024-09-26T18:00:01Z","title":"Dual Dressed Black Holes as the end point of the Charged Superradiant instability in ${\\cal N} = 4$ Yang Mills","version":2},"cited_work":{"arxiv_id":"2409.18178","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2409.18178","snapshot_observed_at":"2026-06-29T21:03:58.610213Z","title":null,"venue":null,"work_id":"f9ccf271-ef59-4bd6-8b08-3687acf71029","year":2025},"citing_paper":{"arxiv_id":"2605.25560","last_updated":"2026-06-08T09:13:16Z","snapshot_observed_at":"2026-07-06T23:35:31.372756Z","submitted_at":"2026-05-25T08:16:18Z","title":"Finite-$N$ BMN index across all vacuum sectors","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-06-29T20:59:46.811368Z"},"links":{"cited_paper":"/paper/2409.18178","citing_paper":"/paper/2605.25560"},"observation_digest":"sha256:6c851545455da70b17427637b4b21500ef0673281af7eac7178d4f8181bad558","observation_id":"82a5b5e3-4ac9-4cc0-ad9c-c08cb0ba72ba","resolution":{"observed_at":"2026-06-29T21:03:58.611556Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.18178","last_updated":"2025-03-24T03:36:47Z","snapshot_observed_at":"2026-08-04T22:12:15.403086Z","submitted_at":"2024-09-26T18:00:01Z","title":"Dual Dressed Black Holes as the end point of the Charged Superradiant instability in ${\\cal N} = 4$ Yang Mills","version":2},"cited_work":{"arxiv_id":"2409.18178","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2409.18178","snapshot_observed_at":"2026-06-29T21:03:58.610213Z","title":null,"venue":null,"work_id":"f9ccf271-ef59-4bd6-8b08-3687acf71029","year":2025},"citing_paper":{"arxiv_id":"2605.28737","last_updated":"2026-05-27T16:57:30Z","snapshot_observed_at":"2026-07-06T23:38:19.096349Z","submitted_at":"2026-05-27T16:57:30Z","title":"Complex BPS Black Holes in AdS$_3\\times S^3$","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-06-29T11:10:03.677163Z"},"links":{"cited_paper":"/paper/2409.18178","citing_paper":"/paper/2605.28737"},"observation_digest":"sha256:c4edfaa94ecef7f8c266b44a384e069d6f9e514832e7f8cda29a2fd1ac4085c4","observation_id":"f7806c3e-a18c-4a9f-92d9-3b3670c19baa","resolution":{"observed_at":"2026-06-29T11:13:20.912549Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.18178","last_updated":"2025-03-24T03:36:47Z","snapshot_observed_at":"2026-08-04T22:12:15.403086Z","submitted_at":"2024-09-26T18:00:01Z","title":"Dual Dressed Black Holes as the end point of the Charged Superradiant instability in ${\\cal N} = 4$ Yang Mills","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.18178","snapshot_observed_at":"2026-07-12T00:18:24.986106Z","title":"Dual dressed black holes as the end point of the charged superradiant instability inN = 4Yang–Mills,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.03735","last_updated":"2026-07-04T06:44:40Z","snapshot_observed_at":"2026-08-07T11:55:50.120902Z","submitted_at":"2026-07-04T06:44:40Z","title":"Equal-charge projection of the $\\mathcal{N}=4$ index: exact large-$N$ formula and finite-rank $U(3)$ coefficients","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-07-12T00:18:24.986106Z"},"links":{"cited_paper":"/paper/2409.18178","citing_paper":"/paper/2607.03735"},"observation_digest":"sha256:1240a9e84cc575b1fa18b39d642028e8cc53375b6ef37c68fc9aa45bffa9127b","observation_id":"89d5178a-8c07-43ee-961e-98fa72325c9d","resolution":{"observed_at":"2026-07-12T00:18:24.986106Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2409.18178/citation-record","integrity":"/paper/2409.18178/integrity","json":"/paper/2409.18178/citation-record.json","paper":"/paper/2409.18178"},"outbound":[],"paper":{"arxiv_id":"2409.18178","last_updated":"2025-03-24T03:36:47Z","latest_version":2,"primary_category":"hep-th","snapshot_observed_at":"2026-08-04T22:12:15.403086Z","submitted_at":"2024-09-26T18:00:01Z","title":"Dual Dressed Black Holes as the end point of the Charged Superradiant instability in ${\\cal N} = 4$ Yang Mills"},"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":"2026-08-07T06:34:17.273281+00:00","source":"crossref"},{"observed_at":"2026-08-07T06:34:11.927384+00:00","source":"retraction_watch"}],"thesis":"As of 8 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 7 inbound Pith citation observations for arXiv:2409.18178."}