{"as_of":"2026-08-15T01:39:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:8c8525ff16db3fc64527397eb0ecda1ab4bef8b70287b82c0a32fb51a91b2921","coverage":[{"denominator":90,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":90,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T11:20:24.045473Z","state":"measured"},{"denominator":90,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":90,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/1908.09310/citation-record","integrity":"/paper/1908.09310/integrity","json":"/paper/1908.09310/citation-record.json","paper":"/paper/1908.09310"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:20:23.615921Z","title":null,"venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.615921Z"},"links":{"citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:f6e42e63b4b0aaae67e3623f80773702e56e87604a15d55d9068ad918213d563","observation_id":"82ce3f6d-ec0d-4cb9-881c-40e3984c68a8","resolution":{"observed_at":"2026-08-14T11:20:23.615921Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9802150","last_updated":"1998-04-06T20:45:58Z","snapshot_observed_at":"2026-08-02T14:27:11.943858Z","submitted_at":"1998-02-20T22:41:01Z","title":"Anti De Sitter Space And Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9802150","snapshot_observed_at":"2026-08-14T11:20:23.621544Z","title":"Witten, Anti-de Sitter space and holography, Adv","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.621544Z"},"links":{"cited_paper":"/paper/hep-th/9802150","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:2c49a18cfd9565151ed13f487b2171642aaedc96972e266ab2a673128225e3f6","observation_id":"dc3446c5-e12d-47fc-a4ed-70f65be9008e","resolution":{"observed_at":"2026-08-14T11:20:23.621544Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9802109","last_updated":"1998-03-27T22:25:16Z","snapshot_observed_at":"2026-08-14T17:07:25.590053Z","submitted_at":"1998-02-16T18:38:17Z","title":"Gauge Theory Correlators from Non-Critical String Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9802109","snapshot_observed_at":"2026-08-14T11:20:23.626215Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.626215Z"},"links":{"cited_paper":"/paper/hep-th/9802109","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:f367b00ffaca353b26d87a66bfa4433e5ea2122320cfc0857e68bc90d5fcc68f","observation_id":"36e43404-f252-4bb7-aa97-fbb146f9f931","resolution":{"observed_at":"2026-08-14T11:20:23.626215Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0603001","last_updated":"2006-03-07T19:21:09Z","snapshot_observed_at":"2026-07-07T04:56:49.142200Z","submitted_at":"2006-02-28T21:29:24Z","title":"Holographic Derivation of Entanglement Entropy from AdS/CFT","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0603001","snapshot_observed_at":"2026-08-14T11:20:23.631080Z","title":"Ryu and T","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.631080Z"},"links":{"cited_paper":"/paper/hep-th/0603001","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:8c8f4f07c15132e4a89ad199854c543f657b94c63792d36d4c00dbb64fdd19ec","observation_id":"6da4cb32-dc51-452f-9501-ee1f72aa7be6","resolution":{"observed_at":"2026-08-14T11:20:23.631080Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1005.3035","last_updated":"2025-07-07T17:31:58Z","snapshot_observed_at":"2026-08-14T07:39:28.331748Z","submitted_at":"2010-05-17T20:17:32Z","title":"Building up spacetime with quantum entanglement","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1005.3035","snapshot_observed_at":"2026-08-14T11:20:23.636172Z","title":"Van Raamsdonk, Building up spacetime with quantum entanglement, Gen","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.636172Z"},"links":{"cited_paper":"/paper/1005.3035","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:4275877bc5cc92e6c4cc9dd4d4e152cf91b30dab250ff8fc0c465203f5640fdf","observation_id":"c7a2e461-1be1-4141-a548-3682cadc3215","resolution":{"observed_at":"2026-08-14T11:20:23.636172Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.0690","last_updated":"2014-11-03T21:01:35Z","snapshot_observed_at":"2026-08-14T23:13:04.787872Z","submitted_at":"2014-11-03T21:01:35Z","title":"Entanglement is not Enough","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.0690","snapshot_observed_at":"2026-08-14T11:20:23.640908Z","title":"Susskind, Entanglement is not enough, Fortsch","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.640908Z"},"links":{"cited_paper":"/paper/1411.0690","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:1c4b7dc18a2bef5cc5476a228e16c645d28d713a95a3f9529622e60608bea738","observation_id":"20890f43-0f49-4920-83bf-849b93055e9e","resolution":{"observed_at":"2026-08-14T11:20:23.640908Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.5695","last_updated":"2014-03-22T18:33:06Z","snapshot_observed_at":"2026-08-14T23:40:19.705925Z","submitted_at":"2014-03-22T18:33:06Z","title":"Addendum to Computational Complexity and Black Hole Horizons","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.5695","snapshot_observed_at":"2026-08-14T11:20:23.646719Z","title":"Susskind, Computational Complexity and Black Hole Horizons, [Fortsch","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.646719Z"},"links":{"cited_paper":"/paper/1403.5695","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:4cf56c73a357b03efc3a4a3cb271c1a8b07fe5ba864163ba095a750d87bade52","observation_id":"f7c6b4ea-86d9-4dd8-840f-2414bb67b753","resolution":{"observed_at":"2026-08-14T11:20:23.646719Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1406.2678","last_updated":"2014-06-12T00:20:40Z","snapshot_observed_at":"2026-08-14T23:30:51.507316Z","submitted_at":"2014-06-10T19:51:42Z","title":"Complexity and Shock Wave Geometries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1406.2678","snapshot_observed_at":"2026-08-14T11:20:23.651598Z","title":"Stanford and L","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.651598Z"},"links":{"cited_paper":"/paper/1406.2678","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:2be2629973f9497da8c46b4327c0a9044e83da7ac8eb8c2d9aec8a553cb2a706","observation_id":"28c67aa0-056b-49aa-9cf0-dd55fdc8f65e","resolution":{"observed_at":"2026-08-14T11:20:23.651598Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.07876","last_updated":"2016-05-10T21:49:25Z","snapshot_observed_at":"2026-08-14T22:30:46.093501Z","submitted_at":"2015-09-25T20:06:58Z","title":"Complexity Equals Action","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.07876","snapshot_observed_at":"2026-08-14T11:20:23.656476Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.656476Z"},"links":{"cited_paper":"/paper/1509.07876","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:8a8c8a190b26667e0e4d64ed9863e0913b99b49c8760295922209f356c830ee4","observation_id":"d978a29c-ea1f-4014-abed-61ec54d0c7c2","resolution":{"observed_at":"2026-08-14T11:20:23.656476Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.04993","last_updated":"2016-05-10T23:02:42Z","snapshot_observed_at":"2026-08-14T22:18:21.184431Z","submitted_at":"2015-12-15T22:28:19Z","title":"Complexity, action, and black holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.04993","snapshot_observed_at":"2026-08-14T11:20:23.661104Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.661104Z"},"links":{"cited_paper":"/paper/1512.04993","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:41b22712603f8cd11ecb0f43b7ca824d85ddf5007de401632187bd51c0ffef33","observation_id":"f6801eb2-35df-4ca2-8aa4-1879ad3f5a5a","resolution":{"observed_at":"2026-08-14T11:20:23.661104Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.07137","last_updated":"2017-12-19T19:00:11Z","snapshot_observed_at":"2026-08-14T20:02:00.679768Z","submitted_at":"2017-12-19T19:00:11Z","title":"Divergences in the rate of complexification","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.07137","snapshot_observed_at":"2026-08-14T11:20:23.665877Z","title":"Moosa, Divergences in the rate of complexiﬁcation,Phys","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.665877Z"},"links":{"cited_paper":"/paper/1712.07137","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:1357c2c565092c72b98efbed2bb47445df0442b89e881590ac3baae7f5b44b7b","observation_id":"f220576f-f85d-4cc8-836a-d5e6ae5c4834","resolution":{"observed_at":"2026-08-14T11:20:23.665877Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.09749","last_updated":"2020-06-18T07:53:40Z","snapshot_observed_at":"2026-08-14T20:09:49.349014Z","submitted_at":"2017-11-27T15:16:26Z","title":"Complexity Growth, Butterfly Velocity and Black hole Thermodynamics","version":3},"cited_work":{"arxiv_id":"1711.09749","doi":null,"metadata_source":"pith","pith_arxiv_id":"1711.09749","snapshot_observed_at":"2026-08-14T11:20:25.328176Z","title":"Complexity Growth, Butterfly Velocity and Black hole Thermodynamics","venue":"hep-th","work_id":"88415932-0c90-4664-8a31-8f61cb45e157","year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.670481Z"},"links":{"cited_paper":"/paper/1711.09749","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:6b7d67889b3c69b30328dcf4b935106fd38d4a9990e8a772215cc1b1db8cacaf","observation_id":"baed186f-2c05-4371-beaa-fc87cf555164","resolution":{"observed_at":"2026-08-14T11:20:25.333408Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1808.09917","last_updated":"2018-12-03T12:51:05Z","snapshot_observed_at":"2026-08-14T18:35:32.524122Z","submitted_at":"2018-08-29T16:36:36Z","title":"On the time dependence of holographic complexity in a dynamical Einstein-dilaton model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.09917","snapshot_observed_at":"2026-08-14T11:20:23.675089Z","title":"Mahapatra and P","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.675089Z"},"links":{"cited_paper":"/paper/1808.09917","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:ead553c47571885bbaa23e30ffe31dc23d2770af560fe438b27f7b4cb43f362d","observation_id":"00348c92-24c6-4563-aa8b-ce939ba91afe","resolution":{"observed_at":"2026-08-14T11:20:23.675089Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.08063","last_updated":"2016-11-17T03:20:25Z","snapshot_observed_at":"2026-08-14T21:33:35.082414Z","submitted_at":"2016-10-25T20:00:09Z","title":"Complexity of Formation in Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.08063","snapshot_observed_at":"2026-08-14T11:20:23.679542Z","title":"Chapman, H","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.679542Z"},"links":{"cited_paper":"/paper/1610.08063","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:919094dca04396603970dda7f68e313b66ddba017b8ee66df63d1ddfd055d93d","observation_id":"9ff1f1d1-e07d-4c86-aee2-532cfad59cc1","resolution":{"observed_at":"2026-08-14T11:20:23.679542Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.00433","last_updated":"2019-05-23T20:25:51Z","snapshot_observed_at":"2026-08-14T21:27:32.469490Z","submitted_at":"2016-12-01T20:51:28Z","title":"Comments on Holographic Complexity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.00433","snapshot_observed_at":"2026-08-14T11:20:23.684361Z","title":"Carmi, R","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.684361Z"},"links":{"cited_paper":"/paper/1612.00433","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:ce838194de371d18b9cbbf11ef8a33b95aabf747d6f80eebdc529c423116c72d","observation_id":"d09fd9d9-c763-45e4-b9c5-df892ba162ef","resolution":{"observed_at":"2026-08-14T11:20:23.684361Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.03706","last_updated":"2017-09-19T16:35:26Z","snapshot_observed_at":"2026-08-14T21:21:17.875599Z","submitted_at":"2017-01-13T16:09:42Z","title":"Surface Counterterms and Regularized Holographic Complexity","version":4},"cited_work":{"arxiv_id":"1701.03706","doi":null,"metadata_source":"pith","pith_arxiv_id":"1701.03706","snapshot_observed_at":"2026-08-14T11:20:25.262818Z","title":"Surface Counterterms and Regularized Holographic Complexity","venue":"hep-th","work_id":"1648a666-17fc-432d-9054-fb573754687d","year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.688891Z"},"links":{"cited_paper":"/paper/1701.03706","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:fed4ab0d87ec1a073143b2097ab29b21a52f696df7689fe2bbfa5e9eb4996793","observation_id":"95d11f74-6a50-42b0-9c89-6387cd2ededf","resolution":{"observed_at":"2026-08-14T11:20:25.267682Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1610.05090","last_updated":"2017-05-04T03:35:44Z","snapshot_observed_at":"2026-08-14T21:34:56.616379Z","submitted_at":"2016-10-17T13:02:52Z","title":"Strong energy condition and complexity growth bound in holography","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.05090","snapshot_observed_at":"2026-08-14T11:20:23.693360Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.693360Z"},"links":{"cited_paper":"/paper/1610.05090","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:cc0f262c097a93d511b323f36eabc82de923ce83f800d843b7e8fc35ab22444e","observation_id":"9a836bd1-0712-4b1d-83cf-3917b9409724","resolution":{"observed_at":"2026-08-14T11:20:23.693360Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.07410","last_updated":"2018-04-20T00:27:08Z","snapshot_observed_at":"2026-08-14T19:24:03.044967Z","submitted_at":"2018-04-20T00:27:08Z","title":"Holographic Complexity in Vaidya Spacetimes I","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.07410","snapshot_observed_at":"2026-08-14T11:20:23.697928Z","title":"Chapman, H","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.697928Z"},"links":{"cited_paper":"/paper/1804.07410","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:bbe563bd1a37ccb715ea807a081808b58debd7c9edc744b144a0d889254f62c3","observation_id":"7fbc7b04-a126-4ede-bedc-87ce94e61373","resolution":{"observed_at":"2026-08-14T11:20:23.697928Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.07262","last_updated":"2018-05-18T15:00:38Z","snapshot_observed_at":"2026-08-14T19:13:45.439650Z","submitted_at":"2018-05-18T15:00:38Z","title":"Holographic Complexity in Vaidya Spacetimes II","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.07262","snapshot_observed_at":"2026-08-14T11:20:23.702566Z","title":"Chapman, H","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.702566Z"},"links":{"cited_paper":"/paper/1805.07262","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:7fbe6751af7cc6de47171193f7bef0b6c96779c2b4d5cdc4d295d8a6cdbe8c1c","observation_id":"71b0101b-da2c-4a0e-8555-d11bbf5ced5b","resolution":{"observed_at":"2026-08-14T11:20:23.702566Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02668","last_updated":"2018-03-08T09:22:20Z","snapshot_observed_at":"2026-08-14T20:15:59.054430Z","submitted_at":"2017-11-07T19:00:01Z","title":"Evolution of Complexity Following a Global Quench","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1711.02668","snapshot_observed_at":"2026-08-14T11:20:23.707112Z","title":"Moosa, Evolution of Complexity Following a Global Quench, JHEP 1803, 031 (2018) [arXiv:1711.02668 [hep-th]]","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.707112Z"},"links":{"cited_paper":"/paper/1711.02668","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:ec3adccb589ab249f90c52956f19baaa3fd3e52aec2a1dd937e02248addb73f9","observation_id":"6943e6b9-6df1-4696-b124-7e47cdf9da5a","resolution":{"observed_at":"2026-08-14T11:20:23.707112Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.01473","last_updated":"2019-10-24T13:48:04Z","snapshot_observed_at":"2026-08-14T18:04:27.680775Z","submitted_at":"2018-11-05T01:25:17Z","title":"Holographic complexity under a global quantum quench","version":2},"cited_work":{"arxiv_id":"1811.01473","doi":null,"metadata_source":"pith","pith_arxiv_id":"1811.01473","snapshot_observed_at":"2026-08-14T11:20:25.183118Z","title":"Holographic complexity under a global quantum quench","venue":"hep-th","work_id":"361c3111-ce54-4364-b4a1-2383e048fe70","year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.711589Z"},"links":{"cited_paper":"/paper/1811.01473","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:831cc8c8fd9fc67555380a63729269106e832c8d5e6f2ece1664066cdc803255","observation_id":"9ea996cf-044f-4182-9653-51f64844c823","resolution":{"observed_at":"2026-08-14T11:20:25.188064Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1903.04511","last_updated":"2020-02-27T13:34:25Z","snapshot_observed_at":"2026-08-14T17:04:04.049359Z","submitted_at":"2019-03-11T18:01:08Z","title":"The First Law of Complexity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.04511","snapshot_observed_at":"2026-08-14T11:20:23.716422Z","title":"Bernamonti, F","venue":null,"work_id":null,"year":1903},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.716422Z"},"links":{"cited_paper":"/paper/1903.04511","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:5f70f6982a639c07c6f7933078c2495ca53e5dbcaedf2b5da1a04dd53bffdbab","observation_id":"9e1ea567-cdb2-4bc1-979e-8bd77bbd84e8","resolution":{"observed_at":"2026-08-14T11:20:23.716422Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.09826","last_updated":"2018-02-19T19:28:39Z","snapshot_observed_at":"2026-08-14T19:59:39.090366Z","submitted_at":"2017-12-28T11:12:17Z","title":"Holographic Complexity of Einstein-Maxwell-Dilaton Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.09826","snapshot_observed_at":"2026-08-14T11:20:23.721507Z","title":"Swingle and Y","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.721507Z"},"links":{"cited_paper":"/paper/1712.09826","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:90605d5f16d77c4e0260998ddbc95e03b8447bf656dde1d6185afca812e2cc46","observation_id":"23751ec7-b276-45b9-b9bf-b4bf281b7fd1","resolution":{"observed_at":"2026-08-14T11:20:23.721507Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.06740","last_updated":"2018-07-12T12:03:47Z","snapshot_observed_at":"2026-08-14T19:44:27.863905Z","submitted_at":"2018-02-19T18:07:27Z","title":"Complexity Growth with Lifshitz Scaling and Hyperscaling Violation","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.06740","snapshot_observed_at":"2026-08-14T11:20:23.726409Z","title":"Alishahiha, A","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.726409Z"},"links":{"cited_paper":"/paper/1802.06740","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:9375bc8353707d36047343050ae6d8b245093694fd4cc740a510206c5b72af2f","observation_id":"e66f2378-d151-40f4-a720-2fc0f611160c","resolution":{"observed_at":"2026-08-14T11:20:23.726409Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.03638","last_updated":"2018-03-03T03:59:23Z","snapshot_observed_at":"2026-08-14T19:56:07.589742Z","submitted_at":"2018-01-11T05:40:25Z","title":"The effect of Dilaton on the holographic complexity growth","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.03638","snapshot_observed_at":"2026-08-14T11:20:23.731023Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.731023Z"},"links":{"cited_paper":"/paper/1801.03638","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:9f5f8e3985a94cf6f2446149a05b11b4a4d1634d692203f00f9164f9c67ad639","observation_id":"9fd368ad-5641-4f51-95db-07fa6f7a1a56","resolution":{"observed_at":"2026-08-14T11:20:23.731023Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.00758","last_updated":"2018-10-01T15:27:55Z","snapshot_observed_at":"2026-08-14T18:21:06.921429Z","submitted_at":"2018-10-01T15:27:55Z","title":"Action growth rate for a higher curvature gravitational theory","version":1},"cited_work":{"arxiv_id":"1810.00758","doi":null,"metadata_source":"pith","pith_arxiv_id":"1810.00758","snapshot_observed_at":"2026-08-14T11:20:25.104376Z","title":"Action growth rate for a higher curvature gravitational theory","venue":"hep-th","work_id":"f2b615c7-5a64-41d6-8b45-49aae71f4839","year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.735498Z"},"links":{"cited_paper":"/paper/1810.00758","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:72f1e5a07afb3bad151bbaf815f031704c273a966ae92402a74a22884b3dfc9f","observation_id":"f09664c9-f16d-41d6-94a3-3edcae00898e","resolution":{"observed_at":"2026-08-14T11:20:25.109068Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1710.00600","last_updated":"2017-11-09T10:43:32Z","snapshot_observed_at":"2026-08-14T20:27:43.361860Z","submitted_at":"2017-10-02T12:10:08Z","title":"Comparison of holographic and field theoretic complexities by time dependent thermofield double states","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1710.00600","snapshot_observed_at":"2026-08-14T11:20:23.739967Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.739967Z"},"links":{"cited_paper":"/paper/1710.00600","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:5252272ffc02ade29a1193953c1e0326e22653aecc8fd67ab27e04fbf924c21b","observation_id":"f87c89d6-5ea1-4143-b130-975f30d2e002","resolution":{"observed_at":"2026-08-14T11:20:23.739967Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.07586","last_updated":"2019-03-08T05:04:00Z","snapshot_observed_at":"2026-08-14T17:13:47.918673Z","submitted_at":"2019-02-20T15:03:06Z","title":"Complexity of Holographic Superconductors","version":2},"cited_work":{"arxiv_id":"1902.07586","doi":null,"metadata_source":"pith","pith_arxiv_id":"1902.07586","snapshot_observed_at":"2026-08-14T11:20:25.070231Z","title":"Complexity of Holographic Superconductors","venue":"hep-th","work_id":"21049555-43d1-44b7-a888-8f84a925c939","year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.744591Z"},"links":{"cited_paper":"/paper/1902.07586","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:82a867668145dbe3daeb1668dd2899838b6e1eaa004fd2200326c5e969c31420","observation_id":"2143ad2e-7194-4509-8c09-f65ae35ac5f1","resolution":{"observed_at":"2026-08-14T11:20:25.074794Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1902.07945","last_updated":"2019-08-27T23:38:10Z","snapshot_observed_at":"2026-08-14T17:13:20.635577Z","submitted_at":"2019-02-21T10:11:35Z","title":"Holographic entanglement entropy and complexity in St$\\ddot{u}$ckelberg superconductor","version":2},"cited_work":{"arxiv_id":"1902.07945","doi":null,"metadata_source":"pith","pith_arxiv_id":"1902.07945","snapshot_observed_at":"2026-08-14T11:20:25.049455Z","title":"Holographic entanglement entropy and complexity in St$\\ddot{u}$ckelberg superconductor","venue":"hep-th","work_id":"a86bb949-a3e3-48b4-9882-0f16c3833dde","year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.749098Z"},"links":{"cited_paper":"/paper/1902.07945","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:3a106200ab7cd4064520716b3db33ed5af7436bd4bd2b7d6fdbd41c0dc7b4941","observation_id":"ad40d0ac-ba41-477a-a5ad-c48553d5b238","resolution":{"observed_at":"2026-08-14T11:20:25.054679Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1606.08307","last_updated":"2016-09-27T15:26:32Z","snapshot_observed_at":"2026-08-14T21:51:26.510182Z","submitted_at":"2016-06-23T16:00:09Z","title":"Complexity Growth for AdS Black Holes","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.08307","snapshot_observed_at":"2026-08-14T11:20:23.753907Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.753907Z"},"links":{"cited_paper":"/paper/1606.08307","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:c69517b3f2398453ced631d369d9d743f58a11b8c85b3801ad732aa5a51cd232","observation_id":"27eb6b14-d190-4785-a372-65d89bdd724b","resolution":{"observed_at":"2026-08-14T11:20:23.753907Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.00207","last_updated":"2016-09-01T12:11:54Z","snapshot_observed_at":"2026-08-14T21:41:47.591058Z","submitted_at":"2016-09-01T12:11:54Z","title":"Gravitational action with null boundaries","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.00207","snapshot_observed_at":"2026-08-14T11:20:23.759016Z","title":"Lehner, R","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.759016Z"},"links":{"cited_paper":"/paper/1609.00207","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:126084554e9d4aeadf93fc9a2533ca7470c472e5173a6dff8db78a44072edf7f","observation_id":"8163bf89-7e90-4b03-b5aa-6e3ce79e0511","resolution":{"observed_at":"2026-08-14T11:20:23.759016Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1611.02321","last_updated":"2016-11-23T06:14:20Z","snapshot_observed_at":"2026-08-14T21:31:31.829987Z","submitted_at":"2016-11-07T22:04:26Z","title":"Holographic Complexity and Two Identities of Action Growth","version":2},"cited_work":{"arxiv_id":"1611.02321","doi":null,"metadata_source":"pith","pith_arxiv_id":"1611.02321","snapshot_observed_at":"2026-08-14T11:20:24.999717Z","title":"Holographic Complexity and Two Identities of Action Growth","venue":"hep-th","work_id":"c35ff27e-bbdc-4d62-9574-740b2412ff40","year":2016},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.763757Z"},"links":{"cited_paper":"/paper/1611.02321","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:4762f490ae8fc99957ec919518d82eb04d12574a5f15cd3a0186a877fde9513a","observation_id":"da00979f-2c85-4e32-9403-e9059a89adb0","resolution":{"observed_at":"2026-08-14T11:20:25.004629Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1702.06766","last_updated":"2017-06-04T14:31:30Z","snapshot_observed_at":"2026-08-14T21:15:21.042292Z","submitted_at":"2017-02-22T12:06:20Z","title":"Action growth of charged black holes with a single horizon","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.06766","snapshot_observed_at":"2026-08-14T11:20:23.768276Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.768276Z"},"links":{"cited_paper":"/paper/1702.06766","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:597235d13a7736693cfb8f5f86ab651d9e4562ed412dc715af2c537994f9ae91","observation_id":"ced0887b-e0ad-4654-8653-8d6d9766a2f0","resolution":{"observed_at":"2026-08-14T11:20:23.768276Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.02795","last_updated":"2018-03-28T22:10:55Z","snapshot_observed_at":"2026-08-14T19:38:29.039001Z","submitted_at":"2018-03-07T18:05:12Z","title":"Complexity Growth Rate in Lovelock Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.02795","snapshot_observed_at":"2026-08-14T11:20:23.772999Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.772999Z"},"links":{"cited_paper":"/paper/1803.02795","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:4151530673e0d83a1f66337f271755c28a703029f154caf0048782d6c2d564c3","observation_id":"87af2103-ea41-480d-bc7c-4a5cc8496a77","resolution":{"observed_at":"2026-08-14T11:20:23.772999Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1806.10312","last_updated":"2019-03-23T03:00:36Z","snapshot_observed_at":"2026-08-14T18:58:44.186226Z","submitted_at":"2018-06-27T06:06:29Z","title":"Surface term, corner term, and action growth in F(Riemann) gravity theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1806.10312","snapshot_observed_at":"2026-08-14T11:20:23.777383Z","title":"Jiang and H","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.777383Z"},"links":{"cited_paper":"/paper/1806.10312","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:b6f6ba1520a1f87972fba6e1518aa70971577d5a6343c9f5b9a0ea0e4c075018","observation_id":"a5469c26-e06c-456b-baaa-662c9ec3ec3f","resolution":{"observed_at":"2026-08-14T11:20:23.777383Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.05476","last_updated":"2019-03-12T17:01:46Z","snapshot_observed_at":"2026-08-14T17:03:26.264846Z","submitted_at":"2019-03-12T17:01:46Z","title":"Modified \"complexity equals action\" conjecture","version":1},"cited_work":{"arxiv_id":"1903.05476","doi":null,"metadata_source":"pith","pith_arxiv_id":"1903.05476","snapshot_observed_at":"2026-08-14T11:20:24.936832Z","title":"Modified \"complexity equals action\" conjecture","venue":"hep-th","work_id":"17dee92f-fef1-4e90-836b-11cf459187e6","year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.782031Z"},"links":{"cited_paper":"/paper/1903.05476","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:3089f970371576f376edbbcf7276db915a6ee96977fa0aa79f499ce57bac3ef6","observation_id":"0f35ea67-6319-435d-a33f-667c53ec0662","resolution":{"observed_at":"2026-08-14T11:20:24.941356Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1811.03303","last_updated":"2018-11-15T14:00:45Z","snapshot_observed_at":"2026-08-14T18:02:20.539349Z","submitted_at":"2018-11-08T07:56:50Z","title":"Holographic Complexity Growth Rate in Horndeski Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.03303","snapshot_observed_at":"2026-08-14T11:20:23.786630Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.786630Z"},"links":{"cited_paper":"/paper/1811.03303","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:b1d7c2b6d2c6d621cdaec9d889c85e168e78bdf081488f74a46c4b1ad74a3ece","observation_id":"fd6781fc-c283-45f7-9cde-657cb49fd0cc","resolution":{"observed_at":"2026-08-14T11:20:23.786630Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.06796","last_updated":"2017-05-29T09:43:16Z","snapshot_observed_at":"2026-08-14T21:15:19.766897Z","submitted_at":"2017-02-22T13:51:36Z","title":"On Complexity for Higher Derivative Gravities","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.06796","snapshot_observed_at":"2026-08-14T11:20:23.791396Z","title":"Alishahiha, A","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.791396Z"},"links":{"cited_paper":"/paper/1702.06796","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:3a3f2a1fea2acbae1da2e029288026ef219ed6168186eba7a4b2610cb475f445","observation_id":"505c76fd-7f5c-468f-800b-ca366361ae8e","resolution":{"observed_at":"2026-08-14T11:20:23.791396Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.10184","last_updated":"2017-09-28T22:04:34Z","snapshot_observed_at":"2026-08-14T20:28:34.790085Z","submitted_at":"2017-09-28T22:04:34Z","title":"On the Time Dependence of Holographic Complexity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.10184","snapshot_observed_at":"2026-08-14T11:20:23.796354Z","title":"Carmi, S","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.796354Z"},"links":{"cited_paper":"/paper/1709.10184","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:084998f19abe9d2e5ec601a1ac443a259c090b6ffb3560838a6f0ad1c5717858","observation_id":"9c3b0f01-c34e-49f2-a857-1a25ef457740","resolution":{"observed_at":"2026-08-14T11:20:23.796354Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.08447","last_updated":"2019-05-21T05:38:59Z","snapshot_observed_at":"2026-08-14T16:29:17.098719Z","submitted_at":"2019-05-21T05:38:59Z","title":"Investigating two counting methods of the holographic complexity","version":1},"cited_work":{"arxiv_id":"1905.08447","doi":null,"metadata_source":"pith","pith_arxiv_id":"1905.08447","snapshot_observed_at":"2026-08-14T11:20:24.872242Z","title":"Investigating two counting methods of the holographic complexity","venue":"hep-th","work_id":"192e9ad1-2778-4c76-ba85-3b7f58dae0b1","year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.801174Z"},"links":{"cited_paper":"/paper/1905.08447","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:6e1b2cca10758582bb00575b915a32f7cfb864e271d321165ad02185de49eade","observation_id":"b43d06bd-f356-424e-bb28-4cc2c48bdf67","resolution":{"observed_at":"2026-08-14T11:20:24.876857Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1905.06409","last_updated":"2019-05-28T02:16:40Z","snapshot_observed_at":"2026-08-14T16:31:37.037870Z","submitted_at":"2019-05-15T19:38:55Z","title":"Action Growth of Dyonic Black Holes and Electromagnetic Duality","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.06409","snapshot_observed_at":"2026-08-14T11:20:23.806164Z","title":null,"venue":null,"work_id":null,"year":1905},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.806164Z"},"links":{"cited_paper":"/paper/1905.06409","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:3b65d2295cef69b1296be7b35a668acaf1e618be54e340f786f55d3c94c2c5f9","observation_id":"481722a9-3e0a-40c4-bf73-5bdd3b369ce3","resolution":{"observed_at":"2026-08-14T11:20:23.806164Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1806.08376","last_updated":"2019-06-08T12:30:10Z","snapshot_observed_at":"2026-08-14T19:00:49.482252Z","submitted_at":"2018-06-21T18:11:01Z","title":"Complexity change under conformal transformations in AdS$_{3}$/CFT$_{2}$","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1806.08376","snapshot_observed_at":"2026-08-14T11:20:23.810710Z","title":"Flory and N","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.810710Z"},"links":{"cited_paper":"/paper/1806.08376","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:e9e5fe30c8648c0855fada1d63d06634a972d25ef5f7801d8056c5c2d4cbf0bb","observation_id":"0e0a194b-8993-4ecc-b3eb-9b1719a23065","resolution":{"observed_at":"2026-08-14T11:20:23.810710Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.06499","last_updated":"2019-06-08T11:59:44Z","snapshot_observed_at":"2026-08-14T17:15:02.244749Z","submitted_at":"2019-02-18T10:36:09Z","title":"WdW-patches in AdS$_{3}$ and complexity change under conformal transformations II","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.06499","snapshot_observed_at":"2026-08-14T11:20:23.815435Z","title":"Flory, WdW-patches in AdS3 and complexity change under conformal transforma- tions II, JHEP 1905, 086 (2019) [arXiv:1902.06499 [hep-th]]","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.815435Z"},"links":{"cited_paper":"/paper/1902.06499","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:3278f3360533f5e86fc290a942feca664aa682a62d84507abdd9c4356381538a","observation_id":"42cab377-cec7-4491-b622-55998eec41e9","resolution":{"observed_at":"2026-08-14T11:20:23.815435Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.08164","last_updated":"2018-10-23T03:14:57Z","snapshot_observed_at":"2026-08-14T18:37:28.585271Z","submitted_at":"2018-08-24T15:03:01Z","title":"Complexity growth rate during phase transitions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.08164","snapshot_observed_at":"2026-08-14T11:20:23.820152Z","title":"Ghodrati, Complexity growth rate during phase transitions, Phys","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.820152Z"},"links":{"cited_paper":"/paper/1808.08164","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:0b8b3f70b334e24990fe8a77068dd1aca223360ebc20b2f6a3fd536ce8d85344","observation_id":"94362ddd-a92d-4a37-86e4-206d62c6b5f6","resolution":{"observed_at":"2026-08-14T11:20:23.820152Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.07981","last_updated":"2017-08-26T14:51:18Z","snapshot_observed_at":"2026-08-14T20:38:51.163022Z","submitted_at":"2017-08-26T14:51:18Z","title":"On complexity growth in massive gravity theories, the effects of chirality and more","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.07981","snapshot_observed_at":"2026-08-14T11:20:23.825096Z","title":"Ghodrati, Complexity growth in massive gravity theories, the eﬀects of chirality, and more, Phys","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.825096Z"},"links":{"cited_paper":"/paper/1708.07981","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:6c6f7ea9cf11e4e61e949a2f15416bdd5de092864741d74f17235c2cdc3387cd","observation_id":"6f5b087a-1274-4a9c-803f-a577c2f67741","resolution":{"observed_at":"2026-08-14T11:20:23.825096Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.08453","last_updated":"2019-08-20T09:26:38Z","snapshot_observed_at":"2026-08-14T22:55:34.662943Z","submitted_at":"2019-07-19T10:39:56Z","title":"Evolutions of entanglement and complexity after a thermal quench in massive gravity theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.08453","snapshot_observed_at":"2026-08-14T11:20:23.829944Z","title":null,"venue":null,"work_id":null,"year":1907},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.829944Z"},"links":{"cited_paper":"/paper/1907.08453","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:7320cc8bf6e1a3542858496846608baa597365d0cd943db8add06dd73fc13594","observation_id":"aa4ed25c-20ce-4e9f-ac1b-c382d6eac894","resolution":{"observed_at":"2026-08-14T11:20:23.829944Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.02038","last_updated":"2017-04-12T01:01:37Z","snapshot_observed_at":"2026-08-14T21:36:21.290587Z","submitted_at":"2016-10-06T20:00:02Z","title":"Noether charge, black hole volume, and complexity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.02038","snapshot_observed_at":"2026-08-14T11:20:23.835528Z","title":"Couch, W","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.835528Z"},"links":{"cited_paper":"/paper/1610.02038","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:97714073bbc73be28956dc51026b4f9788335b714dc8472105bddb266951d269","observation_id":"c6d120b4-f640-48d2-b947-a2c895fafa42","resolution":{"observed_at":"2026-08-14T11:20:23.835528Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.03796","last_updated":"2018-05-18T07:09:25Z","snapshot_observed_at":"2026-08-14T19:16:56.532714Z","submitted_at":"2018-05-10T03:05:50Z","title":"On the Noether charge and the gravity duals of quantum complexity","version":2},"cited_work":{"arxiv_id":"1805.03796","doi":null,"metadata_source":"pith","pith_arxiv_id":"1805.03796","snapshot_observed_at":"2026-08-14T11:20:24.750964Z","title":"On the Noether charge and the gravity duals of quantum complexity","venue":"hep-th","work_id":"7c3f107f-41af-4643-9aec-11e9f1b29e1a","year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.840289Z"},"links":{"cited_paper":"/paper/1805.03796","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:17d7ebb96df8887473ebcc57bf8531de3c6c59998e163c633ef2a669bbaf1793","observation_id":"7cba6c5d-ba47-49a8-946f-1700471fe7a9","resolution":{"observed_at":"2026-08-14T11:20:24.755599Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1903.04127","last_updated":"2019-06-20T04:11:22Z","snapshot_observed_at":"2026-08-14T17:04:30.545676Z","submitted_at":"2019-03-11T05:09:59Z","title":"Holographic complexity and thermodynamics of AdS black holes","version":2},"cited_work":{"arxiv_id":"1903.04127","doi":null,"metadata_source":"pith","pith_arxiv_id":"1903.04127","snapshot_observed_at":"2026-08-14T11:20:24.731475Z","title":"Holographic complexity and thermodynamics of AdS black holes","venue":"hep-th","work_id":"8e617ecf-57aa-43da-9021-ca72a6e1f402","year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.845006Z"},"links":{"cited_paper":"/paper/1903.04127","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:949f69a0c2296eebdf47745188951d0cf88e92fc5549b8245fe269a24324d85e","observation_id":"6845ef92-ade9-4ac9-b500-a2a4796ddb4c","resolution":{"observed_at":"2026-08-14T11:20:24.736147Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1707.08570","last_updated":"2018-07-23T17:04:34Z","snapshot_observed_at":"2026-08-14T20:45:05.214090Z","submitted_at":"2017-07-26T18:00:00Z","title":"Circuit complexity in quantum field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.08570","snapshot_observed_at":"2026-08-14T11:20:23.849820Z","title":"Myers, Circuit complexity in quantum ﬁeld theory , JHEP 10 (2017) 107, [arXiv:1707.08570]","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.849820Z"},"links":{"cited_paper":"/paper/1707.08570","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:3895142f6cfa5e176bcd0a564c7912dfbeccb307774867d85eb0a04678c902b7","observation_id":"4aa7fc94-5450-4741-a6d5-d82846da8de0","resolution":{"observed_at":"2026-08-14T11:20:23.849820Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.10638","last_updated":"2018-03-28T14:20:10Z","snapshot_observed_at":"2026-08-14T19:31:30.051680Z","submitted_at":"2018-03-28T14:20:10Z","title":"Circuit complexity for free fermions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.10638","snapshot_observed_at":"2026-08-14T11:20:23.854598Z","title":"Myers, Circuit complexity for free fermions , JHEP07(2018)139, [arXiv:1803.10638]","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.854598Z"},"links":{"cited_paper":"/paper/1803.10638","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:addcbbd0aca9eecd6d49f870c2793fffda9c237180b7ae92c4b72c5387d04fe1","observation_id":"ae1051ff-ea95-432a-ae0b-04f3592cb293","resolution":{"observed_at":"2026-08-14T11:20:23.854598Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.07620","last_updated":"2018-01-23T15:39:08Z","snapshot_observed_at":"2026-08-14T19:52:45.743573Z","submitted_at":"2018-01-23T15:39:08Z","title":"Circuit Complexity in Fermionic Field Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.07620","snapshot_observed_at":"2026-08-14T11:20:23.859233Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.859233Z"},"links":{"cited_paper":"/paper/1801.07620","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:73b0abf83ae90c479402c04e3801458a945fc32c15df1ba6483bdbd1da7b5823","observation_id":"09b51feb-dae6-415a-aa27-b7ee6232a53a","resolution":{"observed_at":"2026-08-14T11:20:23.859233Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1707.08582","last_updated":"2018-11-13T21:07:59Z","snapshot_observed_at":"2026-08-14T20:45:04.888078Z","submitted_at":"2017-07-26T18:00:07Z","title":"Towards Complexity for Quantum Field Theory States","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1707.08582","snapshot_observed_at":"2026-08-14T11:20:23.863960Z","title":"Heller, Hugo Marrochio and Fernando Pastawski, Towards Complexity for Quantum Field Theory States , Phys","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.863960Z"},"links":{"cited_paper":"/paper/1707.08582","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:83a07780293e24bd7c675c9fc3126cd61a81cdc28e2df2f53bbf86cee3700599","observation_id":"d698f7a4-819d-4926-a179-32d1f8af79e4","resolution":{"observed_at":"2026-08-14T11:20:23.863960Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.07677","last_updated":"2018-10-08T18:22:09Z","snapshot_observed_at":"2026-08-14T18:49:43.846815Z","submitted_at":"2018-07-20T00:56:42Z","title":"Circuit Complexity for Coherent States","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.07677","snapshot_observed_at":"2026-08-14T11:20:23.868507Z","title":"Myers and Shan-Ming Ruan, Circuit Com- plexity for Coherent States , JHEP 1810 (2018) 011, [arXiv:1807.07677]","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.868507Z"},"links":{"cited_paper":"/paper/1807.07677","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:6c8332cc56554f7ba7de97c0872f75f8f15dc60b4bd4432aa2454998555f94b6","observation_id":"26ee130e-79c0-4a49-a038-aea887cb594f","resolution":{"observed_at":"2026-08-14T11:20:23.868507Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.05151","last_updated":"2019-02-15T15:02:18Z","snapshot_observed_at":"2026-08-14T18:16:04.479086Z","submitted_at":"2018-10-11T17:52:39Z","title":"Complexity and entanglement for thermofield double states","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.05151","snapshot_observed_at":"2026-08-14T11:20:23.873355Z","title":"Heller, Ro Jeﬀerson, Hugo Mar- rochio and Robert C","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.873355Z"},"links":{"cited_paper":"/paper/1810.05151","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:3282eb986c9fe2817c0be4aaa135b177d05cf0dbb5951375eda3f31eecb7205d","observation_id":"b70d05cb-ca16-4a80-90d7-5696d22d7dcd","resolution":{"observed_at":"2026-08-14T11:20:23.873355Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.03105","last_updated":"2018-10-18T10:11:07Z","snapshot_observed_at":"2026-08-14T18:43:03.541770Z","submitted_at":"2018-08-09T11:59:28Z","title":"Circuit complexity in interacting QFTs and RG flows","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.03105","snapshot_observed_at":"2026-08-14T11:20:23.878023Z","title":"Bhattacharyya, A","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.878023Z"},"links":{"cited_paper":"/paper/1808.03105","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:35c797fe83fdb0f12ca7e42ce6e376dd578b20a2ece4feda7af55837f7cf7c4a","observation_id":"a449a1dc-603a-4ff6-96eb-d52a2dcb8c21","resolution":{"observed_at":"2026-08-14T11:20:23.878023Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.00537","last_updated":"2018-10-01T05:54:11Z","snapshot_observed_at":"2026-08-14T18:21:20.478393Z","submitted_at":"2018-10-01T05:54:11Z","title":"Circuit complexity for free Fermion with a mass quench","version":1},"cited_work":{"arxiv_id":"1810.00537","doi":null,"metadata_source":"pith","pith_arxiv_id":"1810.00537","snapshot_observed_at":"2026-08-14T11:20:24.606796Z","title":"Circuit complexity for free Fermion with a mass quench","venue":"hep-th","work_id":"b4aa4143-a5cd-4dca-a0f0-3fe983ec9875","year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.882725Z"},"links":{"cited_paper":"/paper/1810.00537","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:2e9bda6d19cdb38cfb5719fb4920e6594ff1a9a23285d951fb6b5b53ab242df7","observation_id":"43970f59-9e72-4167-84aa-69e4d094e96b","resolution":{"observed_at":"2026-08-14T11:20:24.612437Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1812.00193","last_updated":"2018-12-01T11:55:58Z","snapshot_observed_at":"2026-08-14T17:50:11.836492Z","submitted_at":"2018-12-01T11:55:58Z","title":"Circuit Complexity for Fermionic Thermofield Double states","version":1},"cited_work":{"arxiv_id":"1812.00193","doi":null,"metadata_source":"pith","pith_arxiv_id":"1812.00193","snapshot_observed_at":"2026-08-14T11:20:24.584134Z","title":"Circuit Complexity for Fermionic Thermofield Double states","venue":"hep-th","work_id":"38be4bcc-28a2-4084-a5a4-2975dbbb8be6","year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.888189Z"},"links":{"cited_paper":"/paper/1812.00193","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:092dd705fc7d322aee1930d7a2ff44f18d8011b190706a30a9b59740ef0bf95d","observation_id":"418d679c-45be-4702-8374-aea32adab5b1","resolution":{"observed_at":"2026-08-14T11:20:24.589527Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1804.00107","last_updated":"2018-06-12T19:45:10Z","snapshot_observed_at":"2026-08-14T19:30:31.480084Z","submitted_at":"2018-03-31T02:29:11Z","title":"Evolution of complexity following a quantum quench in free field theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.00107","snapshot_observed_at":"2026-08-14T11:20:23.892690Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.892690Z"},"links":{"cited_paper":"/paper/1804.00107","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:bac5f01d857c15bbea98b405855264a4d4b8d33bba9a6524913bd6981dd7368e","observation_id":"7d764818-080f-4ff4-ad36-7f0bb8b5326c","resolution":{"observed_at":"2026-08-14T11:20:23.892690Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1807.07075","last_updated":"2019-03-01T10:56:21Z","snapshot_observed_at":"2026-08-14T18:50:22.244753Z","submitted_at":"2018-07-18T18:00:00Z","title":"Complexity as a novel probe of quantum quenches: universal scalings and purifications","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.07075","snapshot_observed_at":"2026-08-14T11:20:23.897467Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.897467Z"},"links":{"cited_paper":"/paper/1807.07075","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:7c0eb4f11f592dfa830bd047d37f9d570bf9af620c75bc3781844e95890c547a","observation_id":"68d042f8-8c5a-4a1a-89fe-77a3977ae844","resolution":{"observed_at":"2026-08-14T11:20:23.897467Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1810.02734","last_updated":"2019-04-08T19:01:32Z","snapshot_observed_at":"2026-08-14T18:18:56.514402Z","submitted_at":"2018-10-05T14:56:01Z","title":"Time Evolution of Complexity: A Critique of Three Methods","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1810.02734","snapshot_observed_at":"2026-08-14T11:20:23.901952Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.901952Z"},"links":{"cited_paper":"/paper/1810.02734","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:ee61cdc26ea6a15da5ea05f464ba562323e5a97a6959661838d4e67f8c50573f","observation_id":"9cf49341-29d0-48a0-9ec8-d61c80b178e6","resolution":{"observed_at":"2026-08-14T11:20:23.901952Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1706.07056","last_updated":"2017-06-21T18:00:04Z","snapshot_observed_at":"2026-08-14T20:52:28.401967Z","submitted_at":"2017-06-21T18:00:04Z","title":"Liouville Action as Path-Integral Complexity: From Continuous Tensor Networks to AdS/CFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1706.07056","snapshot_observed_at":"2026-08-14T11:20:23.906889Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.906889Z"},"links":{"cited_paper":"/paper/1706.07056","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:c39605bff8556cc06882da69e80aa2d61d1268c8f1d2fee0b5ed8dd1a66d459a","observation_id":"ac945eae-ca90-4df0-834a-f32b6503a52d","resolution":{"observed_at":"2026-08-14T11:20:23.906889Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.01999","last_updated":"2018-07-09T19:11:00Z","snapshot_observed_at":"2026-08-14T19:28:50.700705Z","submitted_at":"2018-04-05T18:00:07Z","title":"Path-Integral Complexity for Perturbed CFTs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.01999","snapshot_observed_at":"2026-08-14T11:20:23.911934Z","title":"Bhattacharyya, P","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.911934Z"},"links":{"cited_paper":"/paper/1804.01999","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:ff2aeea2439d1fd82ab6046c56682e7e0010925cce9128dc3fe5a7729d140d04","observation_id":"564fe030-3097-4f5d-a383-259674aaf9b5","resolution":{"observed_at":"2026-08-14T11:20:23.911934Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.01797","last_updated":"2019-02-18T12:42:07Z","snapshot_observed_at":"2026-08-14T19:39:24.185600Z","submitted_at":"2018-03-05T17:39:54Z","title":"Principles and symmetries of complexity in quantum field theory","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.01797","snapshot_observed_at":"2026-08-14T11:20:23.918855Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.918855Z"},"links":{"cited_paper":"/paper/1803.01797","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:c31315a4382b0f0d6e33aba6bce7482b56d38fbc0b701c264d0501e85921333b","observation_id":"80289455-b367-4615-b5bc-859e1948eb9d","resolution":{"observed_at":"2026-08-14T11:20:23.918855Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.06678","last_updated":"2019-02-20T15:22:30Z","snapshot_observed_at":"2026-08-14T18:26:54.724026Z","submitted_at":"2018-09-18T12:59:50Z","title":"More on complexity of operators in quantum field theory","version":2},"cited_work":{"arxiv_id":"1809.06678","doi":null,"metadata_source":"pith","pith_arxiv_id":"1809.06678","snapshot_observed_at":"2026-08-14T11:20:24.467699Z","title":"More on complexity of operators in quantum field theory","venue":"hep-th","work_id":"05ddb474-734d-491b-9322-72ac7116e5de","year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.925968Z"},"links":{"cited_paper":"/paper/1809.06678","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:ac011b388394ec968de1fa75be533f0c7795fff86e4e0f0848cd1f5f9347a098","observation_id":"86f25471-5cea-4bde-89ee-532d361b3ac1","resolution":{"observed_at":"2026-08-14T11:20:24.472898Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1906.02063","last_updated":"2019-06-13T15:27:24Z","snapshot_observed_at":"2026-08-14T16:20:27.251318Z","submitted_at":"2019-06-05T15:03:46Z","title":"To be unitary-invariant or not?: a simple but non-trivial proposal for the complexity between states in quantum mechanics/field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.02063","snapshot_observed_at":"2026-08-14T11:20:23.930739Z","title":null,"venue":null,"work_id":null,"year":1906},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.930739Z"},"links":{"cited_paper":"/paper/1906.02063","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:dce8f826460af17bed2ab636e2fa34bb3ff5d2b23b243476a834d0c8cc89ea42","observation_id":"58bae831-089a-4acf-b5b5-3b625e86f020","resolution":{"observed_at":"2026-08-14T11:20:23.930739Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.11279","last_updated":"2020-07-04T08:11:29Z","snapshot_observed_at":"2026-08-14T16:11:12.133778Z","submitted_at":"2019-06-26T18:13:04Z","title":"Nonanalyticity of circuit complexity across topological phase transitions","version":2},"cited_work":{"arxiv_id":"1906.11279","doi":null,"metadata_source":"pith","pith_arxiv_id":"1906.11279","snapshot_observed_at":"2026-08-14T11:20:24.431572Z","title":"Nonanalyticity of circuit complexity across topological phase transitions","venue":"cond-mat.str-el","work_id":"101425ef-f7d1-4f77-8480-8276a9ba341f","year":2019},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.936281Z"},"links":{"cited_paper":"/paper/1906.11279","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:04425132a8c780652194f292db7969632440981758a77524a76d9830423e8d98","observation_id":"fff5360e-0cbf-40c4-a2dd-e9e087591bed","resolution":{"observed_at":"2026-08-14T11:20:24.436893Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0712.0805","last_updated":"2008-06-13T15:39:13Z","snapshot_observed_at":"2026-08-14T13:23:46.826333Z","submitted_at":"2007-12-05T20:51:34Z","title":"Viscosity Bound Violation in Higher Derivative Gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0712.0805","snapshot_observed_at":"2026-08-14T11:20:23.940974Z","title":"Brigante, H","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.940974Z"},"links":{"cited_paper":"/paper/0712.0805","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:08bb89c620b1f416d3dbf2bc43d3b26c10b2c396536b6316b42a19d253caab74","observation_id":"e73d6598-7ac3-4f39-b9b3-f034a1967bce","resolution":{"observed_at":"2026-08-14T11:20:23.940974Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.3160","last_updated":"2010-02-09T00:23:19Z","snapshot_observed_at":"2026-08-04T18:25:49.652337Z","submitted_at":"2009-11-17T20:46:29Z","title":"Causality constraints in AdS/CFT from conformal collider physics and Gauss-Bonnet gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0911.3160","snapshot_observed_at":"2026-08-14T11:20:23.945734Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.945734Z"},"links":{"cited_paper":"/paper/0911.3160","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:13f5de4b4de5e33c69840d20e46ce4325d033751367e28f0b329cdc1febbd983","observation_id":"890c81e6-4dc4-45c1-a5a1-55fa4ec7159b","resolution":{"observed_at":"2026-08-14T11:20:23.945734Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.4257","last_updated":"2010-01-02T05:33:50Z","snapshot_observed_at":"2026-07-06T02:03:46.397194Z","submitted_at":"2009-11-23T19:21:52Z","title":"Holographic GB gravity in arbitrary dimensions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0911.4257","snapshot_observed_at":"2026-08-14T11:20:23.950192Z","title":"Buchel, J","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.950192Z"},"links":{"cited_paper":"/paper/0911.4257","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:916cf611bd02a1c1124028865a0d3af5241038f4f27bbe68db2196e3830c8339","observation_id":"bf5dc451-a83e-468a-bee8-ff710a877f0b","resolution":{"observed_at":"2026-08-14T11:20:23.950192Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0912.1877","last_updated":"2010-04-15T16:54:28Z","snapshot_observed_at":"2026-08-13T05:22:04.858930Z","submitted_at":"2009-12-10T20:28:19Z","title":"Holographic Lovelock Gravities and Black Holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0912.1877","snapshot_observed_at":"2026-08-14T11:20:23.955438Z","title":"de Boer, M","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.955438Z"},"links":{"cited_paper":"/paper/0912.1877","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:e30919a5a21696597e2703543c0bea739640fdb18effb27ecda86dc0c93a781d","observation_id":"8dd23d84-17f7-42ed-981f-aa9d14ad698e","resolution":{"observed_at":"2026-08-14T11:20:23.955438Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0912.1944","last_updated":"2010-04-27T19:37:59Z","snapshot_observed_at":"2026-07-06T02:01:52.980237Z","submitted_at":"2009-12-10T20:43:20Z","title":"Causality in AdS/CFT and Lovelock theory","version":2},"cited_work":{"arxiv_id":"0912.1944","doi":null,"metadata_source":"pith","pith_arxiv_id":"0912.1944","snapshot_observed_at":"2026-08-14T11:20:24.349098Z","title":"Causality in AdS/CFT and Lovelock theory","venue":"hep-th","work_id":"b680efbf-392f-41cb-a49f-44ac786c46d8","year":2009},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.960151Z"},"links":{"cited_paper":"/paper/0912.1944","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:6f1155fb606c8057edd15ed917422f144a4405d7e174b4e5d058cdae6f0ec28d","observation_id":"e88f3bba-fdc5-454a-b6e6-d946f5e749c2","resolution":{"observed_at":"2026-08-14T11:20:24.353853Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0905.2675","last_updated":"2009-08-31T07:56:47Z","snapshot_observed_at":"2026-07-06T01:54:44.894591Z","submitted_at":"2009-05-16T11:29:51Z","title":"Shear viscosity and instability from third order Lovelock gravity","version":2},"cited_work":{"arxiv_id":"0905.2675","doi":null,"metadata_source":"pith","pith_arxiv_id":"0905.2675","snapshot_observed_at":"2026-08-14T11:20:24.327588Z","title":"Shear viscosity and instability from third order Lovelock gravity","venue":"hep-th","work_id":"9fb98b76-b050-4e38-bc9b-39b794c1fd9f","year":2009},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.964559Z"},"links":{"cited_paper":"/paper/0905.2675","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:77a9af177f8baa5f6cbd8c5df4697782db57e1563e6d9b0e658bc2975c98787e","observation_id":"72e74bf0-23e7-4ea4-8f2f-13f0d0a0c041","resolution":{"observed_at":"2026-08-14T11:20:24.332648Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1101.5781","last_updated":"2011-05-17T14:27:00Z","snapshot_observed_at":"2026-08-03T06:59:19.048048Z","submitted_at":"2011-01-30T16:09:47Z","title":"Holographic Entanglement Entropy in Lovelock Gravities","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1101.5781","snapshot_observed_at":"2026-08-14T11:20:23.969314Z","title":"de Boer, M","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.969314Z"},"links":{"cited_paper":"/paper/1101.5781","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:53899eb7a056daa7988d4f62f9e1d91d0e2d9451eab8ac91bd3d9bfcf06e8bbe","observation_id":"41fcc673-fe55-4556-9ff2-b3b2b7bc62f2","resolution":{"observed_at":"2026-08-14T11:20:23.969314Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1305.6767","last_updated":"2013-08-06T11:04:33Z","snapshot_observed_at":"2026-08-15T00:16:14.627683Z","submitted_at":"2013-05-29T12:24:39Z","title":"Note on generalized gravitational entropy in Lovelock gravity","version":3},"cited_work":{"arxiv_id":"1305.6767","doi":null,"metadata_source":"pith","pith_arxiv_id":"1305.6767","snapshot_observed_at":"2026-08-14T11:20:24.291725Z","title":"Note on generalized gravitational entropy in Lovelock gravity","venue":"hep-th","work_id":"dfc77126-e6ad-466a-93cf-ad9485b0d64c","year":2013},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.974049Z"},"links":{"cited_paper":"/paper/1305.6767","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:7750788466c10c15166a0049e8f68f5f8a703ad35cf76ad54894ac5cd656592a","observation_id":"507b9dde-2bee-4be5-893a-968b8537a5dd","resolution":{"observed_at":"2026-08-14T11:20:24.297326Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1310.5713","last_updated":"2014-01-15T02:17:53Z","snapshot_observed_at":"2026-08-14T23:58:11.362416Z","submitted_at":"2013-10-21T20:01:26Z","title":"Holographic Entanglement Entropy for General Higher Derivative Gravity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.5713","snapshot_observed_at":"2026-08-14T11:20:23.978707Z","title":"Dong, Holographic Entanglement Entropy for General Higher Derivative Gravity, JHEP 1401, 044 (2014) [arXiv:1310.5713 [hep-th]]","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.978707Z"},"links":{"cited_paper":"/paper/1310.5713","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:7aa7b750aef97a3bb25ec99af45db5148f76603e2fae7b232e5c81bfc0fe9a43","observation_id":"b8716a7a-9ef7-4973-9531-e690e660e40c","resolution":{"observed_at":"2026-08-14T11:20:23.978707Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.07870","last_updated":"2018-01-29T04:54:28Z","snapshot_observed_at":"2026-08-14T23:26:21.508287Z","submitted_at":"2018-01-24T06:18:59Z","title":"Note on Noether charge and holographic transports","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.07870","snapshot_observed_at":"2026-08-14T11:20:23.983261Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.983261Z"},"links":{"cited_paper":"/paper/1801.07870","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:363898e0eddaa6bfbbf733b0f80f6faee59c40558f1f7f434168b10ccbdf4349","observation_id":"917a20ce-405f-4a9c-a449-8d6e91419218","resolution":{"observed_at":"2026-08-14T11:20:23.983261Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0109133","last_updated":"2002-01-12T03:57:23Z","snapshot_observed_at":"2026-07-07T04:41:09.659939Z","submitted_at":"2001-09-18T08:43:03Z","title":"Gauss-Bonnet Black Holes in AdS Spaces","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0109133","snapshot_observed_at":"2026-08-14T11:20:23.987946Z","title":null,"venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.987946Z"},"links":{"cited_paper":"/paper/hep-th/0109133","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:53e6f02a8ef3abc8b64b4b3d5cde1fc49ad14ba8869c2a0a84f5f67ed5af3b9a","observation_id":"2695c3cd-0b89-4452-bf23-c5f0464178c5","resolution":{"observed_at":"2026-08-14T11:20:23.987946Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0109122","last_updated":"2002-07-18T05:25:13Z","snapshot_observed_at":"2026-07-07T04:41:09.659939Z","submitted_at":"2001-09-15T12:16:36Z","title":"Anti-de Sitter Black Hole Thermodynamics in Higher Derivative Gravity and New Confining-Deconfining Phases in dual CFT","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0109122","snapshot_observed_at":"2026-08-14T11:20:23.993050Z","title":"Nojiri and S","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.993050Z"},"links":{"cited_paper":"/paper/hep-th/0109122","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:a4e5d7fd66ab4121879a35dd6016b25f3d0b63b65409165cf58699a6f2efce46","observation_id":"33c83cb4-39fa-49bc-aea2-49374c17dcc0","resolution":{"observed_at":"2026-08-14T11:20:23.993050Z","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":"2026-08-14T11:20:23.997829Z","title":null,"venue":null,"work_id":null,"year":1988},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:23.997829Z"},"links":{"citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:59c7dacf4b901f757157a7ab7c12a8bd89972dbab12d1d358c366067c3e1fa5a","observation_id":"c0a6eb53-f7b1-40a7-b940-e0c9f2601f20","resolution":{"observed_at":"2026-08-14T11:20:23.997829Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0311240","last_updated":"2004-01-15T02:18:25Z","snapshot_observed_at":"2026-07-07T04:48:57.112351Z","submitted_at":"2003-11-25T13:34:14Z","title":"A Note on Thermodynamics of Black Holes in Lovelock Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0311240","snapshot_observed_at":"2026-08-14T11:20:24.002367Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.002367Z"},"links":{"cited_paper":"/paper/hep-th/0311240","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:22d505f7caf73ba7fdd84d63e6365b089f6a9604da241571fa58d674c04ee81c","observation_id":"c0b129d3-2c1e-4f91-a380-35262edf85aa","resolution":{"observed_at":"2026-08-14T11:20:24.002367Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.4260","last_updated":"2009-03-25T08:37:56Z","snapshot_observed_at":"2026-07-06T01:51:41.413596Z","submitted_at":"2009-03-25T08:37:56Z","title":"Thermodynamic Instability of Black Holes of Third Order Lovelock Gravity","version":1},"cited_work":{"arxiv_id":"0903.4260","doi":null,"metadata_source":"pith","pith_arxiv_id":"0903.4260","snapshot_observed_at":"2026-08-14T11:20:24.195467Z","title":"Thermodynamic Instability of Black Holes of Third Order Lovelock Gravity","venue":"gr-qc","work_id":"2b220f4d-1737-4882-b4ef-7e005b5cca4f","year":2009},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.009144Z"},"links":{"cited_paper":"/paper/0903.4260","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:40285d76e26f1c2e5d6634d059dfb42a163a57fb68d6f23a86a8d92102a9c071","observation_id":"cea16b53-eb8e-4749-bb57-082507b006ef","resolution":{"observed_at":"2026-08-14T11:20:24.202727Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9307038","last_updated":"1993-07-29T16:37:13Z","snapshot_observed_at":"2026-07-07T03:24:21.295752Z","submitted_at":"1993-07-29T16:37:13Z","title":"Black Hole Entropy is Noether Charge","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9307038","snapshot_observed_at":"2026-08-14T11:20:24.013586Z","title":"Wald, Black hole entropy is the Noether charge , Phys","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.013586Z"},"links":{"cited_paper":"/paper/gr-qc/9307038","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:d8b5abd00319f577071dcabe3af86f33997182b98bcf2403eebeaa3a1697a4f9","observation_id":"bffdb455-97b0-4f09-b761-a67e33a41afc","resolution":{"observed_at":"2026-08-14T11:20:24.013586Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9403028","last_updated":"1994-03-15T18:18:00Z","snapshot_observed_at":"2026-08-08T08:03:16.411862Z","submitted_at":"1994-03-15T18:18:00Z","title":"Some Properties of Noether Charge and a Proposal for Dynamical Black Hole Entropy","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9403028","snapshot_observed_at":"2026-08-14T11:20:24.017769Z","title":"Iyer and R.M","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.017769Z"},"links":{"cited_paper":"/paper/gr-qc/9403028","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:4a88a4ba7b9d77f32592902d1ddd53e161cd1b18e1e97af9b3c9063ef521e785","observation_id":"552f9e57-24a4-443c-a1f4-b75840f4f7c6","resolution":{"observed_at":"2026-08-14T11:20:24.017769Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9305016","last_updated":"1993-05-06T01:16:00Z","snapshot_observed_at":"2026-07-07T05:03:04.481102Z","submitted_at":"1993-05-06T01:16:00Z","title":"Entropy of Lovelock Black Holes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9305016","snapshot_observed_at":"2026-08-14T11:20:24.021802Z","title":"Jacobson and R","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.021802Z"},"links":{"cited_paper":"/paper/hep-th/9305016","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:e5952993d6a0f0f05bc9eb69976e9262bce9b4f3a5f64abae2fc573e8074e7db","observation_id":"947c9ca8-4b7e-418f-81c7-00d078c178fa","resolution":{"observed_at":"2026-08-14T11:20:24.021802Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0908.0679","last_updated":"2009-08-05T17:40:30Z","snapshot_observed_at":"2026-08-13T10:51:07.234195Z","submitted_at":"2009-08-05T17:40:30Z","title":"Hamiltonian formulation of f(Riemann) theories of gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0908.0679","snapshot_observed_at":"2026-08-14T11:20:24.026618Z","title":"Deruelle, M","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.026618Z"},"links":{"cited_paper":"/paper/0908.0679","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:1e00cf1b2c9d9ec8dcca7b098587ac8ce32f3f4d72595155d2fffe056488f70a","observation_id":"b83de697-57bb-499c-8938-64bd3de9eb4f","resolution":{"observed_at":"2026-08-14T11:20:24.026618Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.00172","last_updated":"2018-10-08T10:39:00Z","snapshot_observed_at":"2026-08-14T19:40:51.745043Z","submitted_at":"2018-03-01T02:27:45Z","title":"Lovelock action with nonsmooth boundaries","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.00172","snapshot_observed_at":"2026-08-14T11:20:24.031507Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.031507Z"},"links":{"cited_paper":"/paper/1803.00172","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:d823c5de49eaed1a02977bb9bd56a211d0bbd61aa22ee0671190334c88234a9d","observation_id":"7daa222f-7bbb-44f6-bdee-a667d46b17fd","resolution":{"observed_at":"2026-08-14T11:20:24.031507Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1501.00006","last_updated":"2015-02-13T02:21:24Z","snapshot_observed_at":"2026-08-14T23:05:39.382764Z","submitted_at":"2014-12-30T21:00:11Z","title":"Thermodynamical First Laws of Black Holes in Quadratically-Extended Gravities","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1501.00006","snapshot_observed_at":"2026-08-14T11:20:24.036157Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.036157Z"},"links":{"cited_paper":"/paper/1501.00006","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:52c12b7d144db4f37daa64c52fc27975df3ce5c85b462108ebaead38524a87b8","observation_id":"b4e0763d-2d8c-4639-8d15-7d4544e01953","resolution":{"observed_at":"2026-08-14T11:20:24.036157Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.08282","last_updated":"2016-09-14T01:39:42Z","snapshot_observed_at":"2026-08-14T23:25:16.198110Z","submitted_at":"2016-04-28T01:41:16Z","title":"AdS and Lifshitz Scalar Hairy Black Holes in Gauss-Bonnet Gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.08282","snapshot_observed_at":"2026-08-14T11:20:24.041012Z","title":null,"venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.041012Z"},"links":{"cited_paper":"/paper/1604.08282","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:169edfc96a3f7423b0f715c372d97212ff359475f18c683472bfa9f98e292a50","observation_id":"ef539fc8-1862-4690-ad92-6e476c0fb730","resolution":{"observed_at":"2026-08-14T11:20:24.041012Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0208205","last_updated":"2002-12-18T14:28:13Z","snapshot_observed_at":"2026-08-06T16:06:21.788403Z","submitted_at":"2002-08-28T13:31:14Z","title":"Generalised Israel Junction Conditions for a Gauss-Bonnet Brane World","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0208205","snapshot_observed_at":"2026-08-14T11:20:24.045473Z","title":null,"venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes","version":3},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-14T11:20:24.045473Z"},"links":{"cited_paper":"/paper/hep-th/0208205","citing_paper":"/paper/1908.09310"},"observation_digest":"sha256:505868bc4a2a8f6f31ae47b01036b7159f3f1936226099415aa699cb44d8c70f","observation_id":"4443c43e-6763-4d2b-b597-6395e511e372","resolution":{"observed_at":"2026-08-14T11:20:24.045473Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1908.09310","last_updated":"2019-10-24T13:41:21Z","latest_version":3,"primary_category":"hep-th","snapshot_observed_at":"2026-08-14T23:36:25.713385Z","submitted_at":"2019-08-25T12:06:12Z","title":"Time dependence of complexity for Lovelock black holes"},"reference_resolution":{"displayed":90,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":71,"verified_exact":19,"verified_fuzzy":0},"total_outbound_references":90},"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":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 90 of 90 outbound references and 0 inbound Pith citation observations for arXiv:1908.09310."}