{"as_of":"2026-08-18T15:52:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6ddb3f9a3cd2924f0f95f13351eb4f95bb637450f3280cdfabca08889d5b5eac","coverage":[{"denominator":62,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":62,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-15T17:46:39.687728Z","state":"measured"},{"denominator":63,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":63,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-18T06:34:40.430872+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-06-27T09:18:17.003491Z","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":"2026-07-03T11:48:05.686275Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"cited_work":{"arxiv_id":"2508.10998","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2508.10998","snapshot_observed_at":"2026-07-03T11:48:05.686275Z","title":null,"venue":null,"work_id":"e07d17d1-b5e3-41e0-84f1-d81fe13d6150","year":null},"citing_paper":{"arxiv_id":"2606.12172","last_updated":"2026-06-10T15:00:26Z","snapshot_observed_at":"2026-08-16T16:28:01.415589Z","submitted_at":"2026-06-10T15:00:26Z","title":"$\\boldsymbol{T\\overline{T}}$ correlators from tensionless strings","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-06-27T09:18:17.003491Z"},"links":{"cited_paper":"/paper/2508.10998","citing_paper":"/paper/2606.12172"},"observation_digest":"sha256:f126191ef4177cdcd2c4aabf3cbccf7771c6f2d9fef135d05b335487fbb81eea","observation_id":"7425d6f8-7872-45d3-aabe-4fe2e0f84dc8","resolution":{"observed_at":"2026-07-03T11:48:05.687700Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2508.10998/citation-record","integrity":"/paper/2508.10998/integrity","json":"/paper/2508.10998/citation-record.json","paper":"/paper/2508.10998"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T17:46:39.384262Z","title":"Gibbons and S.W","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.384262Z"},"links":{"citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:12dd34be342a7259ddf6a35292e8fa24c930121755c081deffa462a77d4ca7b4","observation_id":"c232a568-803c-440a-85f3-710402ca2f72","resolution":{"observed_at":"2026-08-15T17:46:39.384262Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T17:46:39.389823Z","title":"Hawking and D.N","venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.389823Z"},"links":{"citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:0c46e8e6d23e966a469a7980e1136d46a2ae33a73142cc9b52ca4c6a8c2afb7c","observation_id":"783d9780-bb18-4a8b-a995-fb5534c38cd6","resolution":{"observed_at":"2026-08-15T17:46:39.389823Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.05576","last_updated":"2020-07-14T15:16:09Z","snapshot_observed_at":"2026-08-17T18:48:19.006513Z","submitted_at":"2017-01-19T19:35:30Z","title":"$T\\bar T$ and LST","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.05576","snapshot_observed_at":"2026-08-15T17:46:39.395109Z","title":"Giveon, N","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.395109Z"},"links":{"cited_paper":"/paper/1701.05576","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:c91d137f137e7128e5f51dc94bd1c4342f33779ec9d43a0e3e0a5e0305ecbf9f","observation_id":"67e211c9-6151-4469-bd2e-8321a6cd5e39","resolution":{"observed_at":"2026-08-15T17:46:39.395109Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.05800","last_updated":"2017-07-18T18:09:25Z","snapshot_observed_at":"2026-08-14T20:46:50.089159Z","submitted_at":"2017-07-18T18:09:25Z","title":"A Solvable Irrelevant Deformation of $AdS_3/CFT_2$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.05800","snapshot_observed_at":"2026-08-15T17:46:39.400558Z","title":"Giveon, N","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.400558Z"},"links":{"cited_paper":"/paper/1707.05800","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:80d97f784bcf8bd83ab3aa462bc2732b0e1358359a9676444f08732d15f5a354","observation_id":"f60600bc-eced-4efc-8f6d-77590294b6fc","resolution":{"observed_at":"2026-08-15T17:46:39.400558Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02690","last_updated":"2017-11-27T21:52:04Z","snapshot_observed_at":"2026-08-17T19:29:32.088785Z","submitted_at":"2017-11-07T19:14:44Z","title":"Holography Beyond AdS","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02690","snapshot_observed_at":"2026-08-15T17:46:39.406616Z","title":"Asrat, A","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.406616Z"},"links":{"cited_paper":"/paper/1711.02690","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:acd539473613a9e764066526368c02a8c08c0e4fc387b6c8061e17fbbe1a3db4","observation_id":"2532fae6-c3b4-4ed2-be72-8ba08be987fe","resolution":{"observed_at":"2026-08-15T17:46:39.406616Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.07221","last_updated":"2019-12-04T19:48:16Z","snapshot_observed_at":"2026-08-17T07:46:12.860376Z","submitted_at":"2019-07-16T19:12:35Z","title":"$T \\bar{T},J \\bar T$, $T \\bar{J}$ Partition Sums From String Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.07221","snapshot_observed_at":"2026-08-15T17:46:39.411656Z","title":"Hashimoto and D","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.411656Z"},"links":{"cited_paper":"/paper/1907.07221","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:5402cded3161372dc3e262a06e42e561b1bc4e6cfeef555a630faee7efa56337","observation_id":"e287be24-c291-4f92-9333-c93a686a5f6c","resolution":{"observed_at":"2026-08-15T17:46:39.411656Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.11118","last_updated":"2019-12-10T17:40:20Z","snapshot_observed_at":"2026-08-18T00:40:06.896450Z","submitted_at":"2019-09-24T18:46:39Z","title":"Strings, Symmetric Products, $T \\bar{T}$ deformations and Hecke Operators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.11118","snapshot_observed_at":"2026-08-15T17:46:39.417090Z","title":"Hashimoto and D","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.417090Z"},"links":{"cited_paper":"/paper/1909.11118","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:03425f12a1061e67e6f3b424dea7022f5f1b278e4ad4a1ab978f19a11e90e92b","observation_id":"1b15f36c-18b0-45c6-be19-90cf7ef740af","resolution":{"observed_at":"2026-08-15T17:46:39.417090Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1911.12359","last_updated":"2025-01-07T04:40:37Z","snapshot_observed_at":"2026-08-18T05:22:10.209622Z","submitted_at":"2019-11-27T18:59:13Z","title":"TsT, $T\\bar{T}$ and black strings","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1911.12359","snapshot_observed_at":"2026-08-15T17:46:39.422273Z","title":"Apolo, S","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.422273Z"},"links":{"cited_paper":"/paper/1911.12359","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:84453a509d9f30fefe7180b94c0c427c6d7b5a3f0523a7c26f3c3ce564f2dbe9","observation_id":"5610792f-1ea5-488c-8848-a57f42fa6d42","resolution":{"observed_at":"2026-08-15T17:46:39.422273Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.03995","last_updated":"2021-02-07T08:24:08Z","snapshot_observed_at":"2026-08-18T01:53:24.649605Z","submitted_at":"2020-12-07T19:08:07Z","title":"$\\frac{SL(2,\\mathbb{R})\\times U(1)}{U(1)}$ CFT, NS5$+$F1 system and single trace $T\\bar{T}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.03995","snapshot_observed_at":"2026-08-15T17:46:39.427345Z","title":"Chakraborty, SL(2,R)×U(1) U(1) CFT, NS5+F1 system and single trace TT , JHEP 03 (2021) 113 [2012.03995]","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.427345Z"},"links":{"cited_paper":"/paper/2012.03995","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:9aa643074e0e222a288526e62719955f055e6bd192a67b93a39bb54471168bab","observation_id":"ebe46af6-3edf-4c2b-9914-bb9f9d289e85","resolution":{"observed_at":"2026-08-15T17:46:39.427345Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.03041","last_updated":"2023-04-26T05:14:22Z","snapshot_observed_at":"2026-08-17T04:48:32.322543Z","submitted_at":"2023-02-06T19:00:00Z","title":"Holography and Irrelevant Operators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.03041","snapshot_observed_at":"2026-08-15T17:46:39.432620Z","title":"Chang, C","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.432620Z"},"links":{"cited_paper":"/paper/2302.03041","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:9db6b1b48ee2cc73a96c74600cc7330b02bb83fb904d2fe9afaf26b3bba94c82","observation_id":"6b059d17-53c9-4129-ad56-8b29bbf5b577","resolution":{"observed_at":"2026-08-15T17:46:39.432620Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.00823","last_updated":"2025-01-13T15:43:52Z","snapshot_observed_at":"2026-08-16T13:29:08.108703Z","submitted_at":"2024-08-01T18:00:00Z","title":"Tensionless AdS$_3$/CFT$_2$ and Single Trace $T\\overline{T}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.00823","snapshot_observed_at":"2026-08-15T17:46:39.437408Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.437408Z"},"links":{"cited_paper":"/paper/2408.00823","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:33c1ab4666674f056a3ac73468f22494ca8428f599e8ad323c033b5536753826","observation_id":"85c05738-02fb-4903-be7c-2d06dbe460d2","resolution":{"observed_at":"2026-08-15T17:46:39.437408Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T17:46:39.442273Z","title":"Dei and E.J","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.442273Z"},"links":{"citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:8b7b0903acbbe075764095721397e7cf5748a3ecdfa3bf448fb73299c7958be7","observation_id":"a5553f25-70a6-4549-80d8-e5f40b1a6eb4","resolution":{"observed_at":"2026-08-15T17:46:39.442273Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0209067","last_updated":"2002-10-11T03:34:36Z","snapshot_observed_at":"2026-08-07T06:17:05.281617Z","submitted_at":"2002-09-09T13:31:06Z","title":"Lecture Notes on Holographic Renormalization","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0209067","snapshot_observed_at":"2026-08-15T17:46:39.446922Z","title":"Skenderis, Lecture notes on holographic renormalization, Class","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.446922Z"},"links":{"cited_paper":"/paper/hep-th/0209067","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:9c54234ab6a31c2ea8c444d70ff04204fae0529fd78ddb8ea019f5278065ee8a","observation_id":"6ccccd7d-1a3d-489a-bf71-c9b32ea8f66c","resolution":{"observed_at":"2026-08-15T17:46:39.446922Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9906127","last_updated":"1999-09-01T16:23:00Z","snapshot_observed_at":"2026-08-16T07:07:48.856533Z","submitted_at":"1999-06-16T23:55:42Z","title":"The Gravitational Action in Asymptotically AdS and Flat Spacetimes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9906127","snapshot_observed_at":"2026-08-15T17:46:39.452016Z","title":"Kraus, F","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.452016Z"},"links":{"cited_paper":"/paper/hep-th/9906127","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:f306bcd64c526fbae2865068c4d2cd825c3babf758a0ca44d633043f7e240799","observation_id":"439dd89c-34ac-4914-8d3b-8597c9a07bc4","resolution":{"observed_at":"2026-08-15T17:46:39.452016Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9912013","last_updated":"1999-12-02T05:35:52Z","snapshot_observed_at":"2026-08-18T01:54:39.830124Z","submitted_at":"1999-12-02T05:35:52Z","title":"Surface counterterms and boundary stress-energy tensors for asymptotically non-anti-de Sitter spaces","version":1},"cited_work":{"arxiv_id":"hep-th/9912013","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/9912013","snapshot_observed_at":"2026-08-15T17:46:40.581582Z","title":"Surface counterterms and boundary stress-energy tensors for asymptotically non-anti-de Sitter spaces","venue":"hep-th","work_id":"4e87b403-e696-4cca-a21a-39ac17416581","year":1999},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.457061Z"},"links":{"cited_paper":"/paper/hep-th/9912013","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:99c965cc94553e494aa3ac0a710d5995a83d110205c359e57d2037c04945bd31","observation_id":"7ab2f8b8-d985-46d8-b4d0-68abdc253a58","resolution":{"observed_at":"2026-08-15T17:46:40.586846Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0511096","last_updated":"2006-01-13T18:12:03Z","snapshot_observed_at":"2026-07-07T04:55:40.466354Z","submitted_at":"2005-11-08T16:45:45Z","title":"Holographic Renormalization of Asymptotically Flat Spacetimes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0511096","snapshot_observed_at":"2026-08-15T17:46:39.461760Z","title":"Mann and D","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.461760Z"},"links":{"cited_paper":"/paper/hep-th/0511096","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:fde5efc0989357be7b3b60de785c07fe31dba2fbb494d7bce886ba3652399634","observation_id":"5d206ede-e7bb-471b-abac-4994159d1c74","resolution":{"observed_at":"2026-08-15T17:46:39.461760Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0607041","last_updated":"2006-07-26T20:40:57Z","snapshot_observed_at":"2026-08-18T01:54:54.047159Z","submitted_at":"2006-07-10T23:19:55Z","title":"Covariant Counterterms and Conserved Charges in Asymptotically Flat Spacetimes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0607041","snapshot_observed_at":"2026-08-15T17:46:39.466277Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.466277Z"},"links":{"cited_paper":"/paper/gr-qc/0607041","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:d23d580701f16c64ab5afd6218a282492970972512caef5353572a692ce79bac","observation_id":"9e31ced3-313d-4d2c-bf76-bd8c183ed4ae","resolution":{"observed_at":"2026-08-15T17:46:39.466277Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0608037","last_updated":"2006-08-17T04:21:25Z","snapshot_observed_at":"2026-08-15T20:23:32.860392Z","submitted_at":"2006-08-04T18:36:44Z","title":"Note on counterterms in asymptotically flat spacetimes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0608037","snapshot_observed_at":"2026-08-15T17:46:39.470891Z","title":"Astefanesei, R.B","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.470891Z"},"links":{"cited_paper":"/paper/hep-th/0608037","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:790e2a3e62239b80f14e71ff6ec00b80cefdfa35665aebac32605e0526e1c08a","observation_id":"32822d3e-32c0-402a-8a13-58131e4ee63d","resolution":{"observed_at":"2026-08-15T17:46:39.470891Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0703251","last_updated":"2007-06-13T18:05:09Z","snapshot_observed_at":"2026-08-15T10:43:42.243281Z","submitted_at":"2007-03-28T08:20:21Z","title":"Holographic Renormalization of Gravity in Little String Theory Duals","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0703251","snapshot_observed_at":"2026-08-15T17:46:39.475174Z","title":"Marolf and A","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.475174Z"},"links":{"cited_paper":"/paper/hep-th/0703251","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:eb935c9c16fe761bacc42e56eb3c11c7447476932ce83d82d131e0451af10410","observation_id":"1f3c2377-7b9a-4026-98c2-3bbf955535b9","resolution":{"observed_at":"2026-08-15T17:46:39.475174Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0801.4412","last_updated":"2008-04-21T16:03:44Z","snapshot_observed_at":"2026-08-18T01:52:19.719103Z","submitted_at":"2008-01-29T17:02:50Z","title":"Asymptotically Plane Wave Spacetimes and their Actions","version":3},"cited_work":{"arxiv_id":"0801.4412","doi":null,"metadata_source":"pith","pith_arxiv_id":"0801.4412","snapshot_observed_at":"2026-08-15T17:46:40.490822Z","title":"Asymptotically Plane Wave Spacetimes and their Actions","venue":"hep-th","work_id":"d04445cd-1350-4c63-af5e-cdab0756b77b","year":2008},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.480029Z"},"links":{"cited_paper":"/paper/0801.4412","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:b41d0e04466ee3f09798e9f092968d03a687213e88ebe424c5fe0487ca7af187","observation_id":"0f40b29b-b3d7-4f6e-b5b8-ce5af5129ef4","resolution":{"observed_at":"2026-08-15T17:46:40.495958Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0804.2079","last_updated":"2008-04-13T18:16:33Z","snapshot_observed_at":"2026-08-15T10:17:41.103760Z","submitted_at":"2008-04-13T18:16:33Z","title":"On the Stress Tensor for Asymptotically Flat Gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0804.2079","snapshot_observed_at":"2026-08-15T17:46:39.484997Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.484997Z"},"links":{"cited_paper":"/paper/0804.2079","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:a612afce474e78995da219e452c6fe5b8cfc9d00f6579750850ccd09c6301cd5","observation_id":"972bc3ce-6917-4d50-8767-b66341564eaa","resolution":{"observed_at":"2026-08-15T17:46:39.484997Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0807.3324","last_updated":"2008-10-02T14:47:21Z","snapshot_observed_at":"2026-08-15T10:10:33.094979Z","submitted_at":"2008-07-21T19:01:30Z","title":"Precision holography for non-conformal branes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0807.3324","snapshot_observed_at":"2026-08-15T17:46:39.490368Z","title":"Kanitscheider, K","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.490368Z"},"links":{"cited_paper":"/paper/0807.3324","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:9ca2e353c4f4d364b5d288ea28447e9c823991c1d8f5e976d295e1fe24e064ae","observation_id":"fa13fc92-4027-4b86-9ad5-9ea3323951f3","resolution":{"observed_at":"2026-08-15T17:46:39.490368Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0807.0755","last_updated":"2008-07-04T14:04:08Z","snapshot_observed_at":"2026-08-15T10:11:52.893309Z","submitted_at":"2008-07-04T14:04:08Z","title":"Holographic renormalization for coincident Dp-branes","version":1},"cited_work":{"arxiv_id":"0807.0755","doi":null,"metadata_source":"pith","pith_arxiv_id":"0807.0755","snapshot_observed_at":"2026-08-15T17:46:40.436594Z","title":"Holographic renormalization for coincident Dp-branes","venue":"hep-th","work_id":"50e8303f-79ba-4ab6-aeee-8d6c0e9a3e13","year":2008},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.495527Z"},"links":{"cited_paper":"/paper/0807.0755","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:4b098a99c09e2d852db78146ef8b3c7057a470879070980a6ee6ccafb9f24961","observation_id":"2d52b59c-0425-4fa1-8fb8-112afc2e2b84","resolution":{"observed_at":"2026-08-15T17:46:40.441485Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0905.3848","last_updated":"2009-05-23T20:52:05Z","snapshot_observed_at":"2026-08-15T05:47:47.403504Z","submitted_at":"2009-05-23T20:52:05Z","title":"Boundary Terms Unbound! Holographic Renormalization of Asymptotically Linear Dilaton Gravity","version":1},"cited_work":{"arxiv_id":"0905.3848","doi":null,"metadata_source":"pith","pith_arxiv_id":"0905.3848","snapshot_observed_at":"2026-08-15T17:46:40.414335Z","title":"Boundary Terms Unbound! Holographic Renormalization of Asymptotically Linear Dilaton Gravity","venue":"hep-th","work_id":"8d0803b8-ca59-4200-9552-bfd0a644c418","year":2009},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.500487Z"},"links":{"cited_paper":"/paper/0905.3848","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:9ae98697b6387bcb268f32e8defa3841efe0ea8c022a09662aedae91509834f6","observation_id":"417ee93a-ffb2-4f88-9f1b-eb159f64415d","resolution":{"observed_at":"2026-08-15T17:46:40.419533Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+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":"2026-08-15T17:46:40.972179Z","title":"Regge and C","venue":null,"work_id":"dd287446-fe20-42b4-997d-156b99ca86d0","year":1974},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.505396Z"},"links":{"citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:f19bbbc1a562abaec90b2326d3f938cabf437cc4a8ffeb1c6f0ce7688376c4b8","observation_id":"56d83503-314a-473f-a8cd-31849f9040d6","resolution":{"observed_at":"2026-08-15T17:46:40.978803Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9204099","last_updated":"2001-03-20T23:56:53Z","snapshot_observed_at":"2026-08-02T06:01:22.609920Z","submitted_at":"1992-04-29T23:16:12Z","title":"The Black Hole in Three Dimensional Space Time","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9204099","snapshot_observed_at":"2026-08-15T17:46:39.510702Z","title":"Banados, C","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.510702Z"},"links":{"cited_paper":"/paper/hep-th/9204099","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:0a0d798134790272ba92d4894f9adbcf2b57bfa8f218a0c57461c90a32fe5fee","observation_id":"68f8bf83-e167-4258-a082-ab24f5d3fd75","resolution":{"observed_at":"2026-08-15T17:46:39.510702Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0505190","last_updated":"2005-09-22T15:27:07Z","snapshot_observed_at":"2026-08-12T08:24:34.587482Z","submitted_at":"2005-05-23T13:42:54Z","title":"Thermodynamics of Asymptotically Locally AdS Spacetimes","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0505190","snapshot_observed_at":"2026-08-15T17:46:39.515658Z","title":"Papadimitriou and K","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.515658Z"},"links":{"cited_paper":"/paper/hep-th/0505190","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:85fe879c1752418a657e356be621e0f3dfc0fcd7ff86420360748b9c1355f8f9","observation_id":"ef534fae-616f-45a2-9bab-d8060bbdc7b3","resolution":{"observed_at":"2026-08-15T17:46:39.515658Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.01665","last_updated":"2025-07-17T09:31:19Z","snapshot_observed_at":"2026-08-16T18:20:01.930180Z","submitted_at":"2021-06-03T08:15:11Z","title":"The two-sphere partition function in two-dimensional quantum gravity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.01665","snapshot_observed_at":"2026-08-15T17:46:39.520741Z","title":"Anninos, T","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.520741Z"},"links":{"cited_paper":"/paper/2106.01665","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:b58ab9fe4d454871d2a30731fd0f0a35668676b32658b6ac526e4957f0711154","observation_id":"ddce804d-74f0-47c2-b767-21b5842e15ea","resolution":{"observed_at":"2026-08-15T17:46:39.520741Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.01172","last_updated":"2021-07-02T16:21:48Z","snapshot_observed_at":"2026-08-16T18:12:41.785341Z","submitted_at":"2021-07-02T16:21:48Z","title":"Sphere and disk partition functions in Liouville and in matrix integrals","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.01172","snapshot_observed_at":"2026-08-15T17:46:39.525739Z","title":"Mahajan, D","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.525739Z"},"links":{"cited_paper":"/paper/2107.01172","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:37e106712dc09aca895e65e845a9f4c1278545e2cf511ba8476108e0fde3552a","observation_id":"b36c967d-9798-44a9-aca6-f8cdd7fc2e9e","resolution":{"observed_at":"2026-08-15T17:46:39.525739Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.03000","last_updated":"2023-12-18T09:04:29Z","snapshot_observed_at":"2026-08-16T15:18:14.279080Z","submitted_at":"2023-07-06T14:04:01Z","title":"Holographic Weyl anomaly in string theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.03000","snapshot_observed_at":"2026-08-15T17:46:39.530557Z","title":"Eberhardt and S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.530557Z"},"links":{"cited_paper":"/paper/2307.03000","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:740188e15fd03e264692dcd410d829fac48b8089c274a188b91db3955da5bb82","observation_id":"3451e16e-b0c7-4394-8cac-c1908b57502c","resolution":{"observed_at":"2026-08-15T17:46:39.530557Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.00712","last_updated":"2026-06-17T13:39:03Z","snapshot_observed_at":"2026-08-18T01:53:46.381170Z","submitted_at":"2024-06-02T11:31:21Z","title":"A Worldsheet Derivation of the Classical Off-shell Boundary Action for the Dilaton in Half-Space","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.00712","snapshot_observed_at":"2026-08-15T17:46:39.535688Z","title":"Ahmadain and R","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.535688Z"},"links":{"cited_paper":"/paper/2406.00712","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:aab3cf8d7147d5911ed82367c1a87eb47bd185d4c20cf6a6f2642a3f611f5c38","observation_id":"02762245-ca1f-47ae-9728-5c4582ae00f9","resolution":{"observed_at":"2026-08-15T17:46:39.535688Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9902121","last_updated":"1999-12-28T23:45:33Z","snapshot_observed_at":"2026-08-07T23:20:44.277480Z","submitted_at":"1999-02-17T00:48:44Z","title":"A Stress Tensor for Anti-de Sitter Gravity","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9902121","snapshot_observed_at":"2026-08-15T17:46:39.540949Z","title":"Balasubramanian and P","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.540949Z"},"links":{"cited_paper":"/paper/hep-th/9902121","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:9e7fb9082b3e9f4a12b8336ae6cc26fdf7b66e4a83ca7ad8369d62de2a38d014","observation_id":"757d968a-a204-471f-95db-2e1d3498b918","resolution":{"observed_at":"2026-08-15T17:46:39.540949Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T17:46:39.545937Z","title":"Brown and M","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.545937Z"},"links":{"citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:5e02ca3f40c8a3db0456b1f52eefed9ffccce4afc1b4fb4a3cfb8fb94e857a2b","observation_id":"a85dc46c-9330-4ffe-a1ca-fae9d4e8c303","resolution":{"observed_at":"2026-08-15T17:46:39.545937Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9806087","last_updated":"1998-06-17T14:04:39Z","snapshot_observed_at":"2026-08-08T14:43:10.631138Z","submitted_at":"1998-06-11T21:51:07Z","title":"The Holographic Weyl anomaly","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9806087","snapshot_observed_at":"2026-08-15T17:46:39.551103Z","title":"Henningson and K","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.551103Z"},"links":{"cited_paper":"/paper/hep-th/9806087","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:2ff6752c300a191e09513cb000b0cb365d24e648b28c72f0544b68ea66c7e838","observation_id":"423324a0-99c0-4398-9a74-05fce680776a","resolution":{"observed_at":"2026-08-15T17:46:39.551103Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9503052","last_updated":"1995-03-27T20:25:29Z","snapshot_observed_at":"2026-07-07T03:25:18.614600Z","submitted_at":"1995-03-27T20:25:29Z","title":"A comparison of Noether charge and Euclidean methods for Computing the Entropy of Stationary Black Holes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9503052","snapshot_observed_at":"2026-08-15T17:46:39.555782Z","title":"Iyer and R.M","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.555782Z"},"links":{"cited_paper":"/paper/gr-qc/9503052","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:ab95d3eab6065a4e19b873606ad619c6b35ab3499c197551f711cb95286122b2","observation_id":"8f374bdf-0b9d-4573-ac19-8b60b83f392e","resolution":{"observed_at":"2026-08-15T17:46:39.555782Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.01258","last_updated":"2023-08-05T01:57:47Z","snapshot_observed_at":"2026-08-16T15:27:15.865583Z","submitted_at":"2023-06-02T03:49:18Z","title":"On-shell action of $\\text{T}\\bar{\\text{T}}$-deformed Holographic CFTs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.01258","snapshot_observed_at":"2026-08-15T17:46:39.560877Z","title":"Tian, On-shell action of T ¯T-deformed Holographic CFTs, 2306.01258","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.560877Z"},"links":{"cited_paper":"/paper/2306.01258","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:96f34c4ab361560a26ac65ff0e49eceb158d242f96fc79233212a3e36b705413","observation_id":"c5889454-62e5-4053-8424-d18daa931118","resolution":{"observed_at":"2026-08-15T17:46:39.560877Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.16391","last_updated":"2024-07-29T05:15:19Z","snapshot_observed_at":"2026-08-16T14:00:24.517334Z","submitted_at":"2024-07-23T11:25:26Z","title":"Holographic Action Principle for $T\\bar{T}$-deformation","version":2},"cited_work":{"arxiv_id":"2407.16391","doi":null,"metadata_source":"pith","pith_arxiv_id":"2407.16391","snapshot_observed_at":"2026-08-15T17:46:40.116977Z","title":"Holographic Action Principle for $T\\bar{T}$-deformation","venue":"hep-th","work_id":"0e9de1d9-ab6f-4c7b-85bd-dfb21a8f7c79","year":2024},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.565464Z"},"links":{"cited_paper":"/paper/2407.16391","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:60292fe8f4505dbe3b15429fea5d8e54d2b77e76493b5dbdbe819d77ccc3e032","observation_id":"49549ebf-bb37-488b-bb80-e808ba3ee9df","resolution":{"observed_at":"2026-08-15T17:46:40.122324Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2006.13249","last_updated":"2020-08-14T13:57:49Z","snapshot_observed_at":"2026-08-18T01:53:42.439966Z","submitted_at":"2020-06-23T18:07:16Z","title":"$T\\bar T$, Black Holes and Negative Strings","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.13249","snapshot_observed_at":"2026-08-15T17:46:39.570691Z","title":"Chakraborty, A","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.570691Z"},"links":{"cited_paper":"/paper/2006.13249","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:1f0020c9fff179aa79071ce94ac098dfc745aa3175528f9246d3a118a7e75042","observation_id":"d759e8f5-f352-41b4-a54b-9ac20fd49951","resolution":{"observed_at":"2026-08-15T17:46:39.570691Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.03024","last_updated":"2022-09-12T12:33:57Z","snapshot_observed_at":"2026-08-16T17:08:47.213589Z","submitted_at":"2022-04-06T18:16:12Z","title":"Solvable time-like cosets and holography beyond $AdS$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.03024","snapshot_observed_at":"2026-08-15T17:46:39.574903Z","title":"Chakraborty and M","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.574903Z"},"links":{"cited_paper":"/paper/2204.03024","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:0280351b32e7ae5d218f487ec713f9b28e2af9c6893214354dfedfde680dd7aa","observation_id":"215e6a93-19f3-484d-a123-9136b9ac4127","resolution":{"observed_at":"2026-08-15T17:46:39.574903Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.03673","last_updated":"2020-12-03T10:02:29Z","snapshot_observed_at":"2026-08-18T01:52:51.958051Z","submitted_at":"2020-07-07T17:59:59Z","title":"Universal flow equations and chaos bound saturation in 2d dilaton gravity","version":3},"cited_work":{"arxiv_id":"2007.03673","doi":null,"metadata_source":"pith","pith_arxiv_id":"2007.03673","snapshot_observed_at":"2026-08-15T17:46:40.064540Z","title":"Universal flow equations and chaos bound saturation in 2d dilaton gravity","venue":"hep-th","work_id":"3068479f-5acd-4abe-9940-0f31f8c798af","year":2020},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.579529Z"},"links":{"cited_paper":"/paper/2007.03673","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:3e0b35e5bceddedfd4ce79458006e4536f67549f7826455640cb1f4d08295934","observation_id":"a8e019b1-19d9-49d9-b98a-4b5689200443","resolution":{"observed_at":"2026-08-15T17:46:40.069490Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1705.10844","last_updated":"2020-06-06T19:17:06Z","snapshot_observed_at":"2026-08-18T01:53:25.210467Z","submitted_at":"2017-05-30T19:58:54Z","title":"String Theory of Supertubes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.10844","snapshot_observed_at":"2026-08-15T17:46:39.583967Z","title":"Martinec and S","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.583967Z"},"links":{"cited_paper":"/paper/1705.10844","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:26ee9b51167baad3729976a2d2e8d03861c617f1158d165a2e6375d73730ae7b","observation_id":"4dd22f77-cd91-4745-bc29-0de5632badfe","resolution":{"observed_at":"2026-08-15T17:46:39.583967Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2506.20765","last_updated":"2025-06-29T02:09:37Z","snapshot_observed_at":"2026-08-10T10:59:04.025075Z","submitted_at":"2025-06-25T18:57:48Z","title":"Holography with Null Boundaries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2506.20765","snapshot_observed_at":"2026-08-15T17:46:39.589137Z","title":"Ferko and S","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.589137Z"},"links":{"cited_paper":"/paper/2506.20765","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:3593dd051c7f8b74df00672a2dc2562b55139d9290815084fe2586ec246737c7","observation_id":"a1c6eaec-2507-4bad-ad63-4ec06f990232","resolution":{"observed_at":"2026-08-15T17:46:39.589137Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9705221","last_updated":"1997-06-03T16:02:23Z","snapshot_observed_at":"2026-07-07T05:13:49.124126Z","submitted_at":"1997-05-28T17:32:19Z","title":"Matrix Description of M-theory on $T^5$ and $T^5/Z_2$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9705221","snapshot_observed_at":"2026-08-15T17:46:39.594240Z","title":"Seiberg, New theories in six-dimensions and matrix description of M theory on T**5 and T**5 / Z(2) , Phys","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.594240Z"},"links":{"cited_paper":"/paper/hep-th/9705221","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:bc5b35d59ffc68fec8321d226e1531bd61918e99d7aab95a6f9b5023538047ce","observation_id":"adb258f8-ee82-4d91-b079-e2196f2d2342","resolution":{"observed_at":"2026-08-15T17:46:39.594240Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9808149","last_updated":"1998-09-09T20:30:48Z","snapshot_observed_at":"2026-07-07T05:17:33.090196Z","submitted_at":"1998-08-24T23:28:10Z","title":"Linear Dilatons, NS5-branes and Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9808149","snapshot_observed_at":"2026-08-15T17:46:39.599382Z","title":"Aharony, M","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.599382Z"},"links":{"cited_paper":"/paper/hep-th/9808149","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:922190c223bc722a1ca614cdcaffeabc0ccc2816ca535dd24e1e420a1dca89f4","observation_id":"0eebceb4-e726-4e22-a8b7-0df1dfd8d201","resolution":{"observed_at":"2026-08-15T17:46:39.599382Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9907178","last_updated":"1999-11-02T00:39:01Z","snapshot_observed_at":"2026-08-12T17:48:52.398819Z","submitted_at":"1999-07-22T17:45:49Z","title":"Holography for Non-Critical Superstrings","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9907178","snapshot_observed_at":"2026-08-15T17:46:39.604470Z","title":"Giveon, D","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.604470Z"},"links":{"cited_paper":"/paper/hep-th/9907178","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:63d9e4d9a604df59d8688cc4078e13b11eefd15773691c7b3ab4b8fec3833010","observation_id":"d32a7bf5-f05b-4b0f-ba83-2e2c414924ce","resolution":{"observed_at":"2026-08-15T17:46:39.604470Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9601177","last_updated":"1996-09-09T15:00:02Z","snapshot_observed_at":"2026-08-17T11:34:33.520707Z","submitted_at":"1996-02-01T01:06:27Z","title":"Extreme dyonic black holes in string theory","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9601177","snapshot_observed_at":"2026-08-15T17:46:39.610012Z","title":"Tseytlin, Extreme dyonic black holes in string theory , Mod","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.610012Z"},"links":{"cited_paper":"/paper/hep-th/9601177","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:5ea17d4af82da236158e827c08aaaa4aa896752080c4e1da853b5bc5ffcf3653","observation_id":"1988c730-76b9-405b-b113-011cf640dc39","resolution":{"observed_at":"2026-08-15T17:46:39.610012Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0011217","last_updated":"2001-02-04T20:20:01Z","snapshot_observed_at":"2026-08-18T02:31:20.740978Z","submitted_at":"2000-11-23T20:48:48Z","title":"Supersymmetric Conical Defects: Towards a string theoretic description of black hole formation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0011217","snapshot_observed_at":"2026-08-15T17:46:39.615031Z","title":"Balasubramanian, J","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.615031Z"},"links":{"cited_paper":"/paper/hep-th/0011217","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:d3043e88e8bcce4629d506937515575d283fd6aaed926ea42d5a1c61b7ac16c6","observation_id":"b2e8653d-fa4d-4c97-8cac-671c7c7670c4","resolution":{"observed_at":"2026-08-15T17:46:39.615031Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0012025","last_updated":"2003-03-29T00:00:31Z","snapshot_observed_at":"2026-07-07T04:38:33.980959Z","submitted_at":"2000-12-04T23:04:30Z","title":"De-singularization by rotation","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0012025","snapshot_observed_at":"2026-08-15T17:46:39.620037Z","title":"Maldacena and L","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.620037Z"},"links":{"cited_paper":"/paper/hep-th/0012025","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:4b3240eacdb930d53a923ed1c0798c186b28ba28984e97f458e011340daf482f","observation_id":"b8417dfa-78cd-46ce-8147-ee76ff18ced6","resolution":{"observed_at":"2026-08-15T17:46:39.620037Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0212210","last_updated":"2002-12-17T23:22:25Z","snapshot_observed_at":"2026-08-18T13:36:28.903594Z","submitted_at":"2002-12-17T23:22:25Z","title":"Gravity solutions for the D1-D5 system with angular momentum","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0212210","snapshot_observed_at":"2026-08-15T17:46:39.624841Z","title":"Lunin, J.M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.624841Z"},"links":{"cited_paper":"/paper/hep-th/0212210","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:776670d648252329327cbb71544123bab0e07e5e841b5a616106e8d13ca548fb","observation_id":"1fe6de06-68b1-4fb8-bf23-e0fc500e57c2","resolution":{"observed_at":"2026-08-15T17:46:39.624841Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0609074","last_updated":"2006-09-20T16:16:25Z","snapshot_observed_at":"2026-08-15T11:03:46.403738Z","submitted_at":"2006-09-11T15:36:57Z","title":"Lectures on black holes and the AdS_3 / CFT_2 correspondence","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0609074","snapshot_observed_at":"2026-08-15T17:46:39.630303Z","title":"Kraus, Lectures on black holes and the AdS(3) / CFT(2) correspondence , Lect","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.630303Z"},"links":{"cited_paper":"/paper/hep-th/0609074","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:1fe23a55a381b48dda276d6b8d58605e53495f067503bfbe53d444b64c7a2d62","observation_id":"2905c72e-1c4e-4ee4-b467-23c0c17a964e","resolution":{"observed_at":"2026-08-15T17:46:39.630303Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9302012","last_updated":"1993-02-10T15:26:26Z","snapshot_observed_at":"2026-08-17T11:53:51.492434Z","submitted_at":"1993-02-10T15:26:26Z","title":"Geometry of the 2+1 Black Hole","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9302012","snapshot_observed_at":"2026-08-15T17:46:39.635019Z","title":"Banados, M","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.635019Z"},"links":{"cited_paper":"/paper/gr-qc/9302012","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:20416498a3a194b4ac420b7bb9a52b43dd59901ab5161c51f9c4d6da21c116b6","observation_id":"a352ce04-34ff-46a2-853c-1544a3ae4f64","resolution":{"observed_at":"2026-08-15T17:46:39.635019Z","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":"2026-08-15T17:46:40.935791Z","title":"York, Jr., Role of conformal three geometry in the dynamics of gravitation , Phys","venue":null,"work_id":"e62a835b-60b5-46f1-9634-e1f96fd95773","year":1972},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.639708Z"},"links":{"citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:9e7e7dc71239d33cf1d953e7cac295717129f1e93b5e4e6706b82c9d8cfb5dfc","observation_id":"18230341-f506-4f30-b1af-267ca3fd69c8","resolution":{"observed_at":"2026-08-15T17:46:40.941073Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.06400","last_updated":"2026-06-17T13:03:55Z","snapshot_observed_at":"2026-08-18T01:52:54.456278Z","submitted_at":"2024-11-10T09:20:58Z","title":"The GHY boundary term from the string worldsheet to linear order","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.06400","snapshot_observed_at":"2026-08-15T17:46:39.644506Z","title":"Ahmadain, S","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.644506Z"},"links":{"cited_paper":"/paper/2411.06400","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:503d54c6eea2e184b90754bfa5e75a02e793df0a2298428684345ba29acb1500","observation_id":"4a2bebae-31d0-4836-9d70-c9f4e77c18e0","resolution":{"observed_at":"2026-08-15T17:46:39.644506Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.18866","last_updated":"2024-07-26T16:53:23Z","snapshot_observed_at":"2026-08-18T01:52:24.615467Z","submitted_at":"2024-07-26T16:53:23Z","title":"A Comment on Deriving the Gibbons-Hawking-York Term From the String Worldsheet","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.18866","snapshot_observed_at":"2026-08-15T17:46:39.650263Z","title":"Ahmadain, V","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.650263Z"},"links":{"cited_paper":"/paper/2407.18866","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:652b79f9db2a25bdeb87319cf1362835bb413d19779773a69483b0f57a944398","observation_id":"8e54f0e9-8732-4457-9a1d-79af4307d40f","resolution":{"observed_at":"2026-08-15T17:46:39.650263Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9405070","last_updated":"1994-05-30T00:19:30Z","snapshot_observed_at":"2026-08-18T01:55:10.419332Z","submitted_at":"1994-05-30T00:19:30Z","title":"Aspects of Black Hole Quantum Mechanics and Thermodynamics in 2+1 Dimensions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9405070","snapshot_observed_at":"2026-08-15T17:46:39.655267Z","title":"Carlip and C","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.655267Z"},"links":{"cited_paper":"/paper/gr-qc/9405070","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:5c72c832f7f0faeda1a12176f3e2c92722e46817729c15bcf052b214e238bf78","observation_id":"75c0cfc4-f4f9-46fd-8d7e-afd3e79b373e","resolution":{"observed_at":"2026-08-15T17:46:39.655267Z","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":"2026-08-15T17:46:40.917245Z","title":"Mathematica packages for differential geometry and general relativity","venue":null,"work_id":"f6f2927b-df0e-482e-82f7-07da3bc4b70a","year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.660324Z"},"links":{"citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:e483a8d9265bbeac9781798987c035043ef28d09a5541eecfe6b2f9e0aa6480b","observation_id":"3643b725-9a34-4dc4-97f2-3d4f4fc29526","resolution":{"observed_at":"2026-08-15T17:46:40.923509Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9906112","last_updated":"1999-06-15T12:15:08Z","snapshot_observed_at":"2026-07-07T05:20:04.670828Z","submitted_at":"1999-06-15T12:15:08Z","title":"Point Mass Geometries, Spectral Flow and AdS_3-CFT_2 Correspondence","version":1},"cited_work":{"arxiv_id":"hep-th/9906112","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-th/9906112","snapshot_observed_at":"2026-08-15T17:46:39.804987Z","title":"Point Mass Geometries, Spectral Flow and AdS_3-CFT_2 Correspondence","venue":"hep-th","work_id":"ce7ab974-2813-4650-9e37-bea52144e884","year":1999},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.664895Z"},"links":{"cited_paper":"/paper/hep-th/9906112","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:1e70ccc60e7f203340889ebaf5e4bde40aa9dde44e56760c5296ab08d39c13e1","observation_id":"592d3a16-f580-4493-83b1-309ce223b9e7","resolution":{"observed_at":"2026-08-15T17:46:39.812055Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0401146","last_updated":"2004-01-21T18:26:01Z","snapshot_observed_at":"2026-07-07T04:49:32.283438Z","submitted_at":"2004-01-21T18:26:01Z","title":"Expectation value of composite field $T{\\bar T}$ in two-dimensional quantum field theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0401146","snapshot_observed_at":"2026-08-15T17:46:39.669719Z","title":"Zamolodchikov, Expectation value of composite field T anti-T in two-dimensional quantum field theory , hep-th/0401146","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.669719Z"},"links":{"cited_paper":"/paper/hep-th/0401146","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:ed61679bc9394f37145d1d6a2c616d8530bb084d133ac0376f09c457f17a89be","observation_id":"226b1645-612b-4928-a31a-a8d62334f2a2","resolution":{"observed_at":"2026-08-15T17:46:39.669719Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.05499","last_updated":"2016-11-13T14:52:30Z","snapshot_observed_at":"2026-08-14T21:43:35.329420Z","submitted_at":"2016-08-19T05:52:29Z","title":"On space of integrable quantum field theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.05499","snapshot_observed_at":"2026-08-15T17:46:39.674176Z","title":"Smirnov and A.B","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.674176Z"},"links":{"cited_paper":"/paper/1608.05499","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:4e0a9678c3464ed5a119b8518305dcd42eb5ac583e482becbf69c1d89f5242f2","observation_id":"89b0a7da-23f2-44ad-83f3-de8f5b8271b5","resolution":{"observed_at":"2026-08-15T17:46:39.674176Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.05534","last_updated":"2016-09-03T18:58:39Z","snapshot_observed_at":"2026-08-16T21:49:58.731473Z","submitted_at":"2016-08-19T08:45:13Z","title":"$T \\bar{T}$-deformed 2D Quantum Field Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.05534","snapshot_observed_at":"2026-08-15T17:46:39.678562Z","title":"Cavagli` a, S","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.678562Z"},"links":{"cited_paper":"/paper/1608.05534","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:5c4bc7ca467ce1fb19d1ac8e54ed279b7cf0b163ddfbf458c7437408c5c70d97","observation_id":"7bc75b47-9af6-4a52-a1fb-e205b858a3ce","resolution":{"observed_at":"2026-08-15T17:46:39.678562Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1904.13376","last_updated":"2021-02-15T14:00:58Z","snapshot_observed_at":"2026-08-18T03:11:34.641613Z","submitted_at":"2019-04-30T17:17:26Z","title":"A pedagogical review on solvable irrelevant deformations of 2d quantum field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1904.13376","snapshot_observed_at":"2026-08-15T17:46:39.682883Z","title":"Jiang, A pedagogical review on solvable irrelevant deformations of 2D quantum field theory, Commun","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.682883Z"},"links":{"cited_paper":"/paper/1904.13376","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:46f712d0e4244772dd067bdd48b8d8d93e5f61c2dedecb51e2fe982aede024d1","observation_id":"9913e2fc-7cc3-4cee-829d-f83650642f7b","resolution":{"observed_at":"2026-08-15T17:46:39.682883Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.09997","last_updated":"2025-05-12T13:36:26Z","snapshot_observed_at":"2026-08-16T12:50:32.003939Z","submitted_at":"2025-03-13T03:11:07Z","title":"$T\\overline{T}$ Deformation: Introduction and Some Recent Advances","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.09997","snapshot_observed_at":"2026-08-15T17:46:39.687728Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-15T17:46:39.687728Z"},"links":{"cited_paper":"/paper/2503.09997","citing_paper":"/paper/2508.10998"},"observation_digest":"sha256:743c2667fe6dc255d5650e2f10842e159265c1a1ffd7f40643945bba9ec2c45b","observation_id":"fe50e0da-6b18-4d9d-a181-e3562e79ac4d","resolution":{"observed_at":"2026-08-15T17:46:39.687728Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2508.10998","last_updated":"2025-08-30T10:09:54Z","latest_version":2,"primary_category":"hep-th","snapshot_observed_at":"2026-08-18T00:41:01.068428Z","submitted_at":"2025-08-14T18:04:43Z","title":"The On-shell Gravity Action and Linear Dilaton Holography"},"reference_resolution":{"displayed":62,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":52,"verified_exact":7,"verified_fuzzy":3},"total_outbound_references":62},"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":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"thesis":"As of 18 August 2026, this Paper Citation Record lists 62 of 62 outbound references and 1 inbound Pith citation observation for arXiv:2508.10998."}