{"as_of":"2026-08-09T19:21:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:0c0249734c70dce8ce449da3746ff66a67ee19b70dc3b9a696e9c7578c7d79ed","coverage":[{"denominator":60,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":60,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T10:52:09.642538Z","state":"measured"},{"denominator":60,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":60,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-09T06:31:02.800959+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/2510.08258/citation-record","integrity":"/paper/2510.08258/integrity","json":"/paper/2510.08258/citation-record.json","paper":"/paper/2510.08258"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T10:52:03.456789Z","title":"The largeNlimit of superconformal field theories and supergravity","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:03.456789Z"},"links":{"citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:4f97ce71bea98aeec9955db932b7d3ac003ceb17be65c01106a1ecc6afd4cb17","observation_id":"2d467f07-b618-4c27-9ef2-dfceac6fcf07","resolution":{"observed_at":"2026-08-04T10:52:03.456789Z","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":"2026-08-04T10:52:03.517304Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:03.517304Z"},"links":{"citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:198c2ea4f7194d13486bfc4204b66b999483c68aed2a85ccc682896fb5906f18","observation_id":"2fd62017-6119-4705-be1b-ddcfc8eb3fec","resolution":{"observed_at":"2026-08-04T10:52:03.517304Z","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":"2026-08-04T10:52:03.569583Z","title":"Anti De Sitter Space and holography","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:03.569583Z"},"links":{"citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:ccc2f511528dafa7faf6a017a5723c93a102b8e1296553442c787f9173057818","observation_id":"59b43ef4-b780-4bab-8195-fbb0f271fff4","resolution":{"observed_at":"2026-08-04T10:52:03.569583Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.08900","last_updated":"2019-09-12T12:09:04Z","snapshot_observed_at":"2026-08-07T14:27:38.340435Z","submitted_at":"2019-06-21T00:54:10Z","title":"Consistent KK truncations for M5-branes wrapped on Riemann surfaces","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.08900","snapshot_observed_at":"2026-08-04T10:52:03.682078Z","title":"Consistent KK truncations for M5-branes wrapped on Riemann surfaces","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:03.682078Z"},"links":{"cited_paper":"/paper/1906.08900","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:0801084b45a6803d7fc9b6ff037c42c9d2cedac02835807e5f19493928c71238","observation_id":"ad841a56-f30b-4279-bebe-0d0dbe048622","resolution":{"observed_at":"2026-08-04T10:52:03.682078Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9905075","last_updated":"1999-11-16T20:02:04Z","snapshot_observed_at":"2026-07-07T05:19:52.660207Z","submitted_at":"1999-05-11T16:47:01Z","title":"Consistent nonlinear KK reduction of 11d supergravity on $AdS_7\\times S_4$ and self-duality in odd dimensions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9905075","snapshot_observed_at":"2026-08-04T10:52:03.737814Z","title":"Consistent nonlinear KK reduction of 11-d supergravity onAdS 7 ×S 4 and selfduality in odd dimensions","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:03.737814Z"},"links":{"cited_paper":"/paper/hep-th/9905075","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:e901acbaed75cbeb861c53f6a061e83a8d4f388be96366f94fae8e5eb627d52e","observation_id":"ffbef233-eca4-48fb-804b-5823256fa376","resolution":{"observed_at":"2026-08-04T10:52:03.737814Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9911238","last_updated":"2000-02-03T20:54:43Z","snapshot_observed_at":"2026-07-07T05:21:30.904101Z","submitted_at":"1999-11-29T23:32:37Z","title":"Consistency of the $AdS_7\\times S_4$ reduction and the origin of self-duality in odd dimensions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9911238","snapshot_observed_at":"2026-08-04T10:52:03.844957Z","title":"Consistency of the AdS7 ×S 4 reduction and the origin of selfduality in odd dimensions","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:03.844957Z"},"links":{"cited_paper":"/paper/hep-th/9911238","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:7bc7e1d4964487ed3059b7280fe4b2304da09aa3f1deb054db496c2f3b3a771a","observation_id":"6ffe8c88-8690-4dd2-adc4-aca6ff292504","resolution":{"observed_at":"2026-08-04T10:52:03.844957Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.15601","last_updated":"2020-12-31T13:28:17Z","snapshot_observed_at":"2026-08-04T23:34:11.853955Z","submitted_at":"2020-12-31T13:28:17Z","title":"Consistent truncations around half-maximal AdS$_5$ vacua of 11-dimensional supergravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.15601","snapshot_observed_at":"2026-08-04T10:52:03.889566Z","title":"Consistent truncations around half-maximal AdS5 vacua of 11-dimensional supergravity","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:03.889566Z"},"links":{"cited_paper":"/paper/2012.15601","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:9510791b5590c29f5a5bbff4b3d3862d666f9e1faa559b743aeced27004089f5","observation_id":"b9a1eaf1-7662-4a2e-af2f-8dbd2ee6b407","resolution":{"observed_at":"2026-08-04T10:52:03.889566Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9810126","last_updated":"1999-02-25T16:16:03Z","snapshot_observed_at":"2026-07-07T05:17:58.862598Z","submitted_at":"1998-10-16T13:27:53Z","title":"Novel Local CFT and Exact Results on Perturbations of N=4 Super Yang Mills from AdS Dynamics","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9810126","snapshot_observed_at":"2026-08-04T10:52:04.029885Z","title":"Girardello, M","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:04.029885Z"},"links":{"cited_paper":"/paper/hep-th/9810126","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:4366bd9560d80d4c8d4d55e00d231dc7f9c4f8a68e01a555533f6e47b86aab04","observation_id":"9ebca7a7-fdd5-4c95-8b54-f9ed8f91a9d8","resolution":{"observed_at":"2026-08-04T10:52:04.029885Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9904017","last_updated":"1999-05-07T15:01:38Z","snapshot_observed_at":"2026-07-07T05:19:35.192917Z","submitted_at":"1999-04-03T00:44:58Z","title":"Renormalization Group Flows from Holography--Supersymmetry and a c-Theorem","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9904017","snapshot_observed_at":"2026-08-04T10:52:04.078755Z","title":"Renormalization group flows from holography supersymmetry and a c theorem","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:04.078755Z"},"links":{"cited_paper":"/paper/hep-th/9904017","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:f534da6d051eba08858435455623c5390777df3bd5016946b45da6d4a90cae36","observation_id":"5a953c06-7778-4b0c-b254-d23450df873d","resolution":{"observed_at":"2026-08-04T10:52:04.078755Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0009159","last_updated":"2000-10-07T22:17:30Z","snapshot_observed_at":"2026-07-07T04:37:47.632480Z","submitted_at":"2000-09-20T23:15:29Z","title":"A Class of N=1 Supersymmetric RG Flows from Five-dimensional N = 8 Supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0009159","snapshot_observed_at":"2026-08-04T10:52:04.190707Z","title":"A Class ofN= 1 Supersymmetric RG Flows from Five-dimensionalN= 8 Supergravity","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:04.190707Z"},"links":{"cited_paper":"/paper/hep-th/0009159","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:f813f9ad74dde21946f8961bb710e693bf90fb3355f0f4a1ae5e08624674e3cf","observation_id":"213571ae-64df-45ee-bbac-6c9f4b171948","resolution":{"observed_at":"2026-08-04T10:52:04.190707Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0004063","last_updated":"2000-06-09T22:13:37Z","snapshot_observed_at":"2026-07-07T04:36:26.761021Z","submitted_at":"2000-04-10T22:58:02Z","title":"N=2 Supersymmetric RG Flows and the IIB Dilaton","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0004063","snapshot_observed_at":"2026-08-04T10:52:04.351993Z","title":"N= 2 Supersymmetric RG Flows and the IIB Dilaton","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:04.351993Z"},"links":{"cited_paper":"/paper/hep-th/0004063","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:aff82218526116a696c9ff97eef3968fad82564f9a38f2ac9418dd666a82dd19","observation_id":"97ce8645-0e99-44bb-9adb-d4be29bf5b41","resolution":{"observed_at":"2026-08-04T10:52:04.351993Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0006048","last_updated":"2000-06-06T18:34:48Z","snapshot_observed_at":"2026-07-07T04:36:55.674582Z","submitted_at":"2000-06-06T18:34:48Z","title":"AdS RG-Flow and the Super-Yang-Mills Cascade","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0006048","snapshot_observed_at":"2026-08-04T10:52:04.462409Z","title":"AdS RG-Flow and the Super-Yang-Mills Cas- cade","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:04.462409Z"},"links":{"cited_paper":"/paper/hep-th/0006048","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:6516034ad3f034d3dea60fe98f88fe27452d1bfb7fba26a3cfe7e254354e0a37","observation_id":"5dc4c304-b0be-4b19-8536-7937c1d708e9","resolution":{"observed_at":"2026-08-04T10:52:04.462409Z","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":"2026-08-04T10:52:04.571408Z","title":"Domain walls ofD= 5 supergravity and fixed points of N= 1 Super Yang Mills","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:04.571408Z"},"links":{"citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:e3ed932ce28fcc51a4a24c1ac451f637c7810fbbb4a9969c0b80749bb5991afd","observation_id":"5e23acc8-0d0c-472c-8a6c-4b45ee893b39","resolution":{"observed_at":"2026-08-04T10:52:04.571408Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.03276","last_updated":"2018-06-20T10:32:32Z","snapshot_observed_at":"2026-08-02T20:01:01.923690Z","submitted_at":"2018-04-09T23:58:13Z","title":"Holographic RG Flows for Four-dimensional $\\mathcal{N}=2$ SCFTs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.03276","snapshot_observed_at":"2026-08-04T10:52:04.690741Z","title":"Holographic RG Flows for Four- dimensionalN= 2 SCFTs","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:04.690741Z"},"links":{"cited_paper":"/paper/1804.03276","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:bca3c0ded851e1a80d0aef66ecb0f6cd9c49d527aa9da6e4b7eaf78eec450b98","observation_id":"f34ca548-f6d2-4722-ba98-bb6ee846603f","resolution":{"observed_at":"2026-08-04T10:52:04.690741Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1210.8125","last_updated":"2013-03-21T22:34:55Z","snapshot_observed_at":"2026-07-06T02:58:50.042191Z","submitted_at":"2012-10-30T19:11:40Z","title":"BPS domain walls in N=4 supergravity and dual flows","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1210.8125","snapshot_observed_at":"2026-08-04T10:52:04.919181Z","title":"BPS domain walls inN= 4 supergravity and dual flows","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:04.919181Z"},"links":{"cited_paper":"/paper/1210.8125","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:9766d3512fa0689b7552079fba4af052e18b7394799698bd74f18e25a701502b","observation_id":"def8cdf8-e1a7-45c6-a868-36695b2e29ba","resolution":{"observed_at":"2026-08-04T10:52:04.919181Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0104056","last_updated":"2004-11-02T16:57:41Z","snapshot_observed_at":"2026-08-06T21:06:23.346347Z","submitted_at":"2001-04-05T20:03:04Z","title":"Hypermultiplets, domain walls and supersymmetric attractors","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0104056","snapshot_observed_at":"2026-08-04T10:52:05.050959Z","title":"Hypermulti- plets, domain walls and supersymmetric attractors","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.050959Z"},"links":{"cited_paper":"/paper/hep-th/0104056","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:d23d10c3a2008d4bd7db5278893ecb64931f0d697896b29394e6bf230896abc1","observation_id":"7a4fde3f-fffc-468b-a24c-1cf1edebb9e5","resolution":{"observed_at":"2026-08-04T10:52:05.050959Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.13516","last_updated":"2020-03-14T08:37:49Z","snapshot_observed_at":"2026-08-08T23:21:03.876676Z","submitted_at":"2019-12-31T18:59:28Z","title":"Consistent truncations of supergravity and $\\frac{1}{2}$-BPS RG flows in $4d$ SCFTs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.13516","snapshot_observed_at":"2026-08-04T10:52:05.113262Z","title":"Consistent truncations of supergravity and 1 2 -BPS RG flows in 4dSCFTs","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.113262Z"},"links":{"cited_paper":"/paper/1912.13516","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:71740d9338e5498b798cd284b5e0df879b4304a499c0b4e0071c19458705e7e3","observation_id":"bdaaf192-5a40-44a9-84ac-631d0c57a8e3","resolution":{"observed_at":"2026-08-04T10:52:05.113262Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.05270","last_updated":"2023-02-21T13:35:30Z","snapshot_observed_at":"2026-08-02T22:21:06.995913Z","submitted_at":"2022-09-12T14:25:45Z","title":"AdS5 vacua and holographic RG flows from 5D N=4 gauged supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.05270","snapshot_observed_at":"2026-08-04T10:52:05.191581Z","title":"AdS 5 vacua and holographic RG flows from 5DN= 4 gauged supergravity","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.191581Z"},"links":{"cited_paper":"/paper/2209.05270","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:675bda1fd0f258f135fecc0d46a6efc61985e95b02a9f1e59cb395a1fae0f9aa","observation_id":"a56ff29b-2cf9-423e-ad39-cf84479cbbc9","resolution":{"observed_at":"2026-08-04T10:52:05.191581Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0304129","last_updated":"2003-06-04T01:47:46Z","snapshot_observed_at":"2026-07-07T04:46:49.004180Z","submitted_at":"2003-04-15T04:09:53Z","title":"A Dilatonic Deformation of AdS_5 and its Field Theory Dual","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0304129","snapshot_observed_at":"2026-08-04T10:52:05.299454Z","title":"A Dilatonic Deformation ofAdS 5 and its Field Theory Dual","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.299454Z"},"links":{"cited_paper":"/paper/hep-th/0304129","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:2f7c6f5ad0b1f07735e8f398a766cf31aa6ba34b0c5ead99548a71b55b001f7b","observation_id":"eaa5d188-db4e-47cb-b1a8-3ac475cdc87f","resolution":{"observed_at":"2026-08-04T10:52:05.299454Z","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":"2026-08-04T10:52:05.370683Z","title":"Super Janus","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.370683Z"},"links":{"citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:e3e50c9ccfa5a96c15e8a53d4645d38bedb80bc27a1833fa233300a9a3e8fadb","observation_id":"679c07cf-51d9-4e20-ad76-b246c643aee1","resolution":{"observed_at":"2026-08-04T10:52:05.370683Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0407073","last_updated":"2004-12-28T22:51:32Z","snapshot_observed_at":"2026-07-07T04:51:10.690015Z","submitted_at":"2004-07-09T19:49:52Z","title":"The dual of Janus -:- an interface CFT","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0407073","snapshot_observed_at":"2026-08-04T10:52:05.416155Z","title":"Dual of the Janus solution: An interface conformal field theory","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.416155Z"},"links":{"cited_paper":"/paper/hep-th/0407073","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:f5c96aa21d1db965d50b32bc74ea3a7563720fd029dc094cc40074fa32945da1","observation_id":"29ce19b4-db2f-4d95-8a0d-4319cd0483cf","resolution":{"observed_at":"2026-08-04T10:52:05.416155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0603013","last_updated":"2006-03-02T17:22:52Z","snapshot_observed_at":"2026-08-06T14:19:57.075045Z","submitted_at":"2006-03-02T17:22:52Z","title":"Interface Yang-Mills, Supersymmetry, and Janus","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0603013","snapshot_observed_at":"2026-08-04T10:52:05.523486Z","title":"Interface Yang-Mills, supersymme- try, and Janus","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.523486Z"},"links":{"cited_paper":"/paper/hep-th/0603013","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:a4f3c7e94cf4f9576e421c183ebe8b555f76914ffcf114cd725d20ec18516de9","observation_id":"d8c6a252-836d-479c-bba8-69ed238babee","resolution":{"observed_at":"2026-08-04T10:52:05.523486Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1107.2796","last_updated":"2011-09-28T06:46:35Z","snapshot_observed_at":"2026-07-06T02:30:52.928718Z","submitted_at":"2011-07-14T12:05:24Z","title":"Supersymmetric Janus solutions in five and ten dimensions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.2796","snapshot_observed_at":"2026-08-04T10:52:05.573892Z","title":"Supersymmetric Janus solutions in five and ten dimensions","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.573892Z"},"links":{"cited_paper":"/paper/1107.2796","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:bd01df8e20899ca09968ae05e22f22bc06150e24711a826e8a22f62323dae48d","observation_id":"8990c059-7476-49d0-8f3d-9b0e850af04a","resolution":{"observed_at":"2026-08-04T10:52:05.573892Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.11132","last_updated":"2019-07-25T15:16:58Z","snapshot_observed_at":"2026-08-03T11:23:03.479636Z","submitted_at":"2019-07-25T15:16:58Z","title":"Janus and J-fold Solutions from Sasaki-Einstein Manifolds","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.11132","snapshot_observed_at":"2026-08-04T10:52:05.620050Z","title":"Janus and J-fold Solutions from Sasaki-Einstein Manifolds","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.620050Z"},"links":{"cited_paper":"/paper/1907.11132","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:4754901b2b132601c69252977dab46b261f56bafc2497615e8be1f9e84cb3c63","observation_id":"005d893e-ef5b-4324-8a9d-2fb0940a2a1b","resolution":{"observed_at":"2026-08-04T10:52:05.620050Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2003.09154","last_updated":"2020-03-20T08:59:01Z","snapshot_observed_at":"2026-08-06T13:51:24.083586Z","submitted_at":"2020-03-20T08:59:01Z","title":"Holographic Interfaces in N=4 SYM: Janus and J-folds","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2003.09154","snapshot_observed_at":"2026-08-04T10:52:05.679043Z","title":"Holographic Interfaces inN= 4 SYM: Janus and J-folds","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.679043Z"},"links":{"cited_paper":"/paper/2003.09154","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:9f875b50846b39d9732600730be051d123f140f45aaf06f0b311e3aad6a21184","observation_id":"c4226e7a-4f78-4934-bb28-5958b2f01e5f","resolution":{"observed_at":"2026-08-04T10:52:05.679043Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.06704","last_updated":"2025-07-29T03:45:21Z","snapshot_observed_at":"2026-08-07T17:18:43.153945Z","submitted_at":"2025-03-09T17:41:28Z","title":"Janus and RG-flow interfaces from 5D N=4 gauged supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.06704","snapshot_observed_at":"2026-08-04T10:52:05.761861Z","title":"Janus and RG-flow interfaces from 5D N= 4 gauged super- gravity","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.761861Z"},"links":{"cited_paper":"/paper/2503.06704","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:cfaeafaca28737ae3d934cf133b87c96c1f6cc47763ef243b229d46478f7a4ac","observation_id":"da9a574b-a740-4738-bd61-d9a89e5ca305","resolution":{"observed_at":"2026-08-04T10:52:05.761861Z","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":"2026-08-04T10:52:05.881412Z","title":"Topological Quantum Field Theory","venue":null,"work_id":null,"year":1988},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.881412Z"},"links":{"citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:61ccfe0f681de485eb925ae3c9a6a67b82336780eba746224d055ef3267f945d","observation_id":"d45672ee-ec59-46cc-96c6-dd28c1c11384","resolution":{"observed_at":"2026-08-04T10:52:05.881412Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0007018","last_updated":"2000-07-08T18:31:09Z","snapshot_observed_at":"2026-07-07T04:37:07.123786Z","submitted_at":"2000-07-03T19:38:24Z","title":"Supergravity description of field theories on curved manifolds and a no go theorem","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0007018","snapshot_observed_at":"2026-08-04T10:52:05.988056Z","title":"Supergravity description of field theories on curved manifolds and a no go theorem","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:05.988056Z"},"links":{"cited_paper":"/paper/hep-th/0007018","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:2445c1c204b31f979cd199735cfecccf7f368d4848e26e051915c30c41e48a63","observation_id":"63a77ee0-159d-498e-8a49-2084b6ed55cd","resolution":{"observed_at":"2026-08-04T10:52:05.988056Z","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":"2026-08-04T10:52:06.148279Z","title":"Supersymmetry of black strings ind= 5 gauged supergravities","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:06.148279Z"},"links":{"citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:7d5843acb0aedb714fb0f84fc0d932de7523f71d3156d11b00c266cf9b2f0d87","observation_id":"cb21313e-7719-4ecc-a0f3-761a478bbfb1","resolution":{"observed_at":"2026-08-04T10:52:06.148279Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0302218","last_updated":"2003-03-21T12:32:35Z","snapshot_observed_at":"2026-07-07T04:46:24.743002Z","submitted_at":"2003-02-27T18:10:39Z","title":"Supersymmetric Domain Walls and Strings in D=5 gauged Supergravity coupled to Vector Multiplets","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0302218","snapshot_observed_at":"2026-08-04T10:52:06.232690Z","title":"Supersymmetric domain walls and strings ind= 5 gauged supergravity coupled to vector multiplets","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:06.232690Z"},"links":{"cited_paper":"/paper/hep-th/0302218","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:67cfd97af80b16c163ada0009961182c4c382bf1577b48e06cb8412ebaa1e2b9","observation_id":"23985b5f-da55-46fc-819d-65289a39bc24","resolution":{"observed_at":"2026-08-04T10:52:06.232690Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0708.2402","last_updated":"2008-01-10T15:41:41Z","snapshot_observed_at":"2026-07-06T01:29:47.793956Z","submitted_at":"2007-08-17T17:30:53Z","title":"Black strings in AdS_5","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0708.2402","snapshot_observed_at":"2026-08-04T10:52:06.352990Z","title":"Black strings inAdS 5","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:06.352990Z"},"links":{"cited_paper":"/paper/0708.2402","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:fe1b36d764c15f49cb2568fda52a61f1b0f667b43bc6cb35c9795257073fd9cf","observation_id":"1318be75-924f-4aa2-bf12-25e7ef243da7","resolution":{"observed_at":"2026-08-04T10:52:06.352990Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1302.4451","last_updated":"2013-03-25T19:24:20Z","snapshot_observed_at":"2026-08-04T03:19:44.889082Z","submitted_at":"2013-02-18T21:00:14Z","title":"Two-dimensional SCFTs from wrapped branes and c-extremization","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1302.4451","snapshot_observed_at":"2026-08-04T10:52:06.467855Z","title":"Two-dimensional SCFTs from wrapped branes and c-extremization","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:06.467855Z"},"links":{"cited_paper":"/paper/1302.4451","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:a55d0091868db3e6b5839abca4f0a3f993a6e4960ba2de68988c45f426b2d2b5","observation_id":"ea3a8864-4fcf-4c44-ad32-6211cb667d4b","resolution":{"observed_at":"2026-08-04T10:52:06.467855Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.2086","last_updated":"2013-09-27T18:50:26Z","snapshot_observed_at":"2026-08-06T10:10:55.953030Z","submitted_at":"2013-07-08T13:31:36Z","title":"3D Supergravity from wrapped D3-branes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.2086","snapshot_observed_at":"2026-08-04T10:52:06.607622Z","title":"3D Supergravity from wrapped D3- branes","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:06.607622Z"},"links":{"cited_paper":"/paper/1307.2086","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:da6215e79fa81172d837d8a50f23a27e1fd137cf34daae98d5b6f454e093800e","observation_id":"5d7cdeaf-e88d-4831-af29-95d55ad10bf8","resolution":{"observed_at":"2026-08-04T10:52:06.607622Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.7131","last_updated":"2014-03-27T16:51:05Z","snapshot_observed_at":"2026-07-06T03:39:39.812144Z","submitted_at":"2014-03-27T16:51:05Z","title":"(0,2) SCFTs from the Leigh-Strassler Fixed Point","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.7131","snapshot_observed_at":"2026-08-04T10:52:06.735173Z","title":"(0,2) SCFTs from the Leigh-Strassler fixed point","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:06.735173Z"},"links":{"cited_paper":"/paper/1403.7131","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:9af0317bcb5306bc4a531468b00dc2667b0013d3f198c6c6c4cf124021634009","observation_id":"5f513e5f-131f-4778-85de-a09d5fdbdfaa","resolution":{"observed_at":"2026-08-04T10:52:06.735173Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.09462","last_updated":"2016-05-09T15:49:24Z","snapshot_observed_at":"2026-08-07T02:58:51.157905Z","submitted_at":"2015-11-30T20:40:11Z","title":"Two-dimensional SCFTs from D3-branes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.09462","snapshot_observed_at":"2026-08-04T10:52:06.836741Z","title":"Two-dimensional SCFTs from D3-branes","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:06.836741Z"},"links":{"cited_paper":"/paper/1511.09462","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:a65b7bc9d997638a1cc2fb984a42816dfec969a2bad75019b2d026854b413e1b","observation_id":"6bda3a87-35ce-4e02-b6f4-1cf3397af5be","resolution":{"observed_at":"2026-08-04T10:52:06.836741Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.07367","last_updated":"2017-01-16T10:41:22Z","snapshot_observed_at":"2026-07-06T05:15:44.489379Z","submitted_at":"2016-10-24T11:33:29Z","title":"Black string first order flow in N=2, d=5 abelian gauged supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.07367","snapshot_observed_at":"2026-08-04T10:52:06.943075Z","title":"Black string first order flow in N= 2,d= 5 abelian gauged supergravity","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:06.943075Z"},"links":{"cited_paper":"/paper/1610.07367","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:f73724ef5ef63bd210a3151c845c60d75f25ca04596c93b6a1bb6c5b85c87996","observation_id":"9ba1ec36-e7cb-4da4-9f3f-67c2f492fa3e","resolution":{"observed_at":"2026-08-04T10:52:06.943075Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.05052","last_updated":"2017-08-23T21:34:17Z","snapshot_observed_at":"2026-08-09T17:28:59.842292Z","submitted_at":"2017-08-16T19:57:50Z","title":"Universal RG Flows Across Dimensions and Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.05052","snapshot_observed_at":"2026-08-04T10:52:07.057178Z","title":"Universal RG Flows Across Dimensions and Holography","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:07.057178Z"},"links":{"cited_paper":"/paper/1708.05052","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:3fbe65ec5a03647c54b7fc3f280b9022e22d72cd5793652bf70a8de9a71fa1a4","observation_id":"4bdc52cb-703d-49a8-b75d-d5d11ee39fd5","resolution":{"observed_at":"2026-08-04T10:52:07.057178Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.03570","last_updated":"2018-10-01T09:40:50Z","snapshot_observed_at":"2026-08-06T09:56:47.875609Z","submitted_at":"2018-03-09T15:42:00Z","title":"AdS$_5$ black strings in the stu model of FI-gauged $N=2$ supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.03570","snapshot_observed_at":"2026-08-04T10:52:07.186339Z","title":"AdS 5 black strings in the stu model of FI-gaugedN= 2 supergravity","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:07.186339Z"},"links":{"cited_paper":"/paper/1803.03570","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:f2681a4de02fd62228b2e973b4f4090413342f63f5ae549cce80c30b98d504f4","observation_id":"c59436fb-d6de-4c7a-b815-e486a3947870","resolution":{"observed_at":"2026-08-04T10:52:07.186339Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.08858","last_updated":"2017-06-07T20:11:11Z","snapshot_observed_at":"2026-07-30T21:21:46.825917Z","submitted_at":"2016-10-27T15:56:43Z","title":"Betti multiplets, flows across dimensions and c-extremization","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.08858","snapshot_observed_at":"2026-08-04T10:52:07.341514Z","title":"Betti multiplets, flows across dimensions and c-extremization","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:07.341514Z"},"links":{"cited_paper":"/paper/1610.08858","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:cf900578d42de3db4460d11a75dbb52a368aa32217fc5c75ea97e642776c610b","observation_id":"d688fa76-9c69-4c55-9742-9299dec2ca20","resolution":{"observed_at":"2026-08-04T10:52:07.341514Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.01608","last_updated":"2019-02-06T17:09:34Z","snapshot_observed_at":"2026-07-06T07:12:36.518166Z","submitted_at":"2018-11-05T10:57:23Z","title":"Holographic RG flows and $AdS_5$ black strings from 5D half-maximal gauged supergravity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.01608","snapshot_observed_at":"2026-08-04T10:52:07.509228Z","title":"Holographic RG flows andAdS 5 black strings from 5D half-maximal gauged supergravity","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:07.509228Z"},"links":{"cited_paper":"/paper/1811.01608","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:c9c598c22a33a084cf541f95e1ac273874784b5fca45cf0e522541c3fb13ae6b","observation_id":"0842a484-6324-44fc-9141-c6485b3d6705","resolution":{"observed_at":"2026-08-04T10:52:07.509228Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.10122","last_updated":"2019-03-12T14:10:15Z","snapshot_observed_at":"2026-07-06T07:23:23.471740Z","submitted_at":"2018-12-25T15:30:47Z","title":"Supersymmetric $AdS_5$ black holes and strings from 5D $N=4$ gauged supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.10122","snapshot_observed_at":"2026-08-04T10:52:07.633494Z","title":"Supersymmetric black holes and strings from 5D gauged supergravity","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:07.633494Z"},"links":{"cited_paper":"/paper/1812.10122","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:dec424dc07fdf81427018b0fdc19e2fed12eef2b792e07de8a3811f1be34e7b9","observation_id":"ec3d78ed-3757-4504-8ca8-8e94ec62ff3d","resolution":{"observed_at":"2026-08-04T10:52:07.633494Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.07456","last_updated":"2023-05-22T15:24:36Z","snapshot_observed_at":"2026-08-05T18:07:04.398762Z","submitted_at":"2022-11-14T15:32:21Z","title":"New supersymmetric $AdS_5$ black strings from 5D $N=4$ gauged supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.07456","snapshot_observed_at":"2026-08-04T10:52:07.775864Z","title":"New supersymmetricAdS 5 black strings from 5DN= 4 gauged supergravity","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:07.775864Z"},"links":{"cited_paper":"/paper/2211.07456","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:715068fbe2067eb7394a2d9d7ea5a675a7ae5c068e0e9b1e681d97579a660b6f","observation_id":"587c5ad4-2f9a-40a6-98fb-d54f5e857f9c","resolution":{"observed_at":"2026-08-04T10:52:07.775864Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0602024","last_updated":"2008-12-13T03:47:05Z","snapshot_observed_at":"2026-07-07T04:56:30.478178Z","submitted_at":"2006-02-02T18:05:26Z","title":"Gauged N=4 supergravities","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0602024","snapshot_observed_at":"2026-08-04T10:52:07.900210Z","title":"GaugedN= 4 supergravities","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:07.900210Z"},"links":{"cited_paper":"/paper/hep-th/0602024","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:e641783742cd7f9c8e2525fc47302d080e2ab4304f62c580cb2d189033f620d0","observation_id":"26af5052-e9c9-48b0-9399-f3bbace1bb9f","resolution":{"observed_at":"2026-08-04T10:52:07.900210Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0103106","last_updated":"2001-08-30T09:44:18Z","snapshot_observed_at":"2026-07-07T04:39:24.857155Z","submitted_at":"2001-03-14T13:25:11Z","title":"General Matter Coupled N=4 Gauged Supergravity in Five Dimensions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0103106","snapshot_observed_at":"2026-08-04T10:52:08.064662Z","title":"General matter coupled N= 4 gauged supergravity in five-dimensions","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.064662Z"},"links":{"cited_paper":"/paper/hep-th/0103106","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:3e4fbb3e95130bda4fbc96915150428e824ee290e9fbcb504694c26e832fcd80","observation_id":"020584bd-0eb4-4d0d-b4fb-48b7d204fb9c","resolution":{"observed_at":"2026-08-04T10:52:08.064662Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.01623","last_updated":"2015-11-04T12:13:45Z","snapshot_observed_at":"2026-07-06T04:23:01.876801Z","submitted_at":"2015-07-06T20:57:37Z","title":"N=4 Supersymmetric AdS5 Vacua and their Moduli Spaces","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.01623","snapshot_observed_at":"2026-08-04T10:52:08.142350Z","title":"N= 4 supersymmetricAdS 5 vacua and their moduli spaces","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.142350Z"},"links":{"cited_paper":"/paper/1507.01623","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:2eeea6717855c4cb24bb0500713ddc32bc68c064d8d6401feaee9c24c178f547","observation_id":"d366613b-06ee-4c23-ace4-8e7d52c2b5ca","resolution":{"observed_at":"2026-08-04T10:52:08.142350Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0002160","last_updated":"2000-02-18T23:58:46Z","snapshot_observed_at":"2026-07-07T04:35:53.698820Z","submitted_at":"2000-02-18T23:58:46Z","title":"Curvature Singularities: the Good, the Bad, and the Naked","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0002160","snapshot_observed_at":"2026-08-04T10:52:08.267126Z","title":"Curvature singularities: the good, the bad and the naked,","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.267126Z"},"links":{"cited_paper":"/paper/hep-th/0002160","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:72a7d5c75290fc52e16a463f295c0f3cd48d518ab9351114c2af3c32bbb92c01","observation_id":"9499f8c1-ab52-4af9-a793-c13fa2b03575","resolution":{"observed_at":"2026-08-04T10:52:08.267126Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.09204","last_updated":"2017-10-18T16:12:29Z","snapshot_observed_at":"2026-08-04T15:26:30.429531Z","submitted_at":"2017-09-26T18:15:17Z","title":"Janus solutions in six-dimensional gauged supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.09204","snapshot_observed_at":"2026-08-04T10:52:08.382636Z","title":"Janus solutions in six-dimensional gauged supergravity","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.382636Z"},"links":{"cited_paper":"/paper/1709.09204","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:c0163d52b5b87d0ba1bb75b5207d598e07a5ebbaed9b41a4913806ec174da91e","observation_id":"295262ca-e3c6-4a62-9e25-0ce7d87df7d2","resolution":{"observed_at":"2026-08-04T10:52:08.382636Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.00041","last_updated":"2018-04-20T16:26:09Z","snapshot_observed_at":"2026-07-06T06:25:56.759173Z","submitted_at":"2018-02-28T19:24:51Z","title":"Supersymmetric Janus solutions of dyonic $ISO(7)$-gauged $\\mathcal{N}\\,=\\,8$ supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.00041","snapshot_observed_at":"2026-08-04T10:52:08.515895Z","title":"Supersymmetric Janus solutions of dyonicISO(7)-gaugedN= 8 supergravity","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.515895Z"},"links":{"cited_paper":"/paper/1803.00041","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:3e267bd7fa9c7640abc4576b3ef5dc6f7703b6c814705dac794874515499a331","observation_id":"1a8d0558-4d9c-4bfd-be03-c85f2e79fb4a","resolution":{"observed_at":"2026-08-04T10:52:08.515895Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.13398","last_updated":"2021-11-15T16:51:57Z","snapshot_observed_at":"2026-08-06T03:51:49.754039Z","submitted_at":"2021-08-30T17:43:15Z","title":"Janus solutions from dyonic ISO(7) maximal gauged supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.13398","snapshot_observed_at":"2026-08-04T10:52:08.664238Z","title":"Janus solutions from dyonicISO(7) max- imal gauged supergravity","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.664238Z"},"links":{"cited_paper":"/paper/2108.13398","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:d4cbce6d8d31d1db3ce7eae77e24d94242058103db0a798c0d0d67f0ff19a905","observation_id":"5afb53be-bb7b-4de4-a41e-bf60bd424a26","resolution":{"observed_at":"2026-08-04T10:52:08.664238Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1207.7325","last_updated":"2012-07-31T17:27:54Z","snapshot_observed_at":"2026-07-06T02:52:54.937210Z","submitted_at":"2012-07-31T17:27:54Z","title":"Holographic RG-flows and Boundary CFTs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1207.7325","snapshot_observed_at":"2026-08-04T10:52:08.778451Z","title":"Holographic RG-flows and Boundary CFTs","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.778451Z"},"links":{"cited_paper":"/paper/1207.7325","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:46da0ab05cf266da80c790267e3150e5d17333efe09b7abd61f5fddabd126166","observation_id":"d7cd4d3a-b4d2-4225-8a19-be2222fb1b8c","resolution":{"observed_at":"2026-08-04T10:52:08.778451Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.07983","last_updated":"2017-03-02T10:47:36Z","snapshot_observed_at":"2026-07-06T05:15:59.221126Z","submitted_at":"2016-10-25T17:46:39Z","title":"Supersymmetric deformations of 3D SCFTs from tri-sasakian truncation","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.07983","snapshot_observed_at":"2026-08-04T10:52:08.868388Z","title":"Supersymmetric deformations of 3D SCFTs from tri- sasakian truncation","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.868388Z"},"links":{"cited_paper":"/paper/1610.07983","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:8c74f9d344d4ccb951f91a6f2343171598abd3e56be9d25d3a8be5726818345d","observation_id":"37a1e6f6-e630-4a82-b43a-d88313a029c9","resolution":{"observed_at":"2026-08-04T10:52:08.868388Z","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":"2026-08-04T10:52:08.957880Z","title":"GaugedN= 4 supergravities in five dimensions and their magnetovac backgrounds","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:08.957880Z"},"links":{"citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:cfe7c062f25415be59acdca59c34cba084ff99fb77e656178955fd678f9c16ae","observation_id":"3083ed46-8178-4b3f-bbe3-eb19a8a746cc","resolution":{"observed_at":"2026-08-04T10:52:08.957880Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0712.3560","last_updated":"2008-02-22T10:30:49Z","snapshot_observed_at":"2026-07-06T01:36:40.238730Z","submitted_at":"2007-12-20T20:31:39Z","title":"D=5 SU(2)xU(1) Gauged Supergravity from D=11 Supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0712.3560","snapshot_observed_at":"2026-08-04T10:52:09.055131Z","title":"D= 5SU(2)×U(1) gauged supergravity fromD= 11 supergravity","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:09.055131Z"},"links":{"cited_paper":"/paper/0712.3560","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:ca0e29918066589ed4bba476e63a4f0bbd3e4359365c24ba166d10b176eb17ac","observation_id":"fdd0e3d6-a34e-4e56-985f-264f2eeffc8b","resolution":{"observed_at":"2026-08-04T10:52:09.055131Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0011288","last_updated":"2000-12-13T14:38:47Z","snapshot_observed_at":"2026-07-07T04:38:33.980959Z","submitted_at":"2000-11-30T16:47:30Z","title":"Supergravity and D-branes Wrapping Supersymmetric 3-Cycles","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0011288","snapshot_observed_at":"2026-08-04T10:52:09.153306Z","title":"Supergravity and D-branes Wrapping Supersymmetric 3-Cycles","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:09.153306Z"},"links":{"cited_paper":"/paper/hep-th/0011288","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:20966a5f7a52cc799f4e0f72a370f6f08da419a3a33315b93d48ea6254f29d72","observation_id":"ea0822d5-63b4-410b-8fd0-b95747fad76b","resolution":{"observed_at":"2026-08-04T10:52:09.153306Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.17923","last_updated":"2025-07-10T05:54:50Z","snapshot_observed_at":"2026-08-05T12:37:41.145070Z","submitted_at":"2025-01-29T19:00:02Z","title":"Defects in 4d SCFTs from supergravity and holographic renormalization","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.17923","snapshot_observed_at":"2026-08-04T10:52:09.219443Z","title":"Defects in 4d SCFTs from supergravity and holographic renormalization","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:09.219443Z"},"links":{"cited_paper":"/paper/2501.17923","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:611152fb169b95b4b81216d7ae0e72f2c5c0fccda440813b1bf2fb3e1d1d1fd4","observation_id":"506f23db-552a-4e6d-a0d8-a083e27e2742","resolution":{"observed_at":"2026-08-04T10:52:09.219443Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.10579","last_updated":"2021-03-03T08:08:22Z","snapshot_observed_at":"2026-08-08T01:45:30.531626Z","submitted_at":"2020-11-20T19:00:01Z","title":"D3-branes wrapped on a spindle","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.10579","snapshot_observed_at":"2026-08-04T10:52:09.302366Z","title":"D3-Branes Wrapped on a Spindle","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:09.302366Z"},"links":{"cited_paper":"/paper/2011.10579","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:10e152e36874b36ddd67aeb94f072658535d883bd708cff08bc026fb413d2bd1","observation_id":"4fda7042-7e14-46eb-ac98-8509b0817d4a","resolution":{"observed_at":"2026-08-04T10:52:09.302366Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.01105","last_updated":"2022-03-10T14:15:14Z","snapshot_observed_at":"2026-08-09T11:55:17.016836Z","submitted_at":"2021-08-02T18:03:39Z","title":"D3-branes and M5-branes wrapped on a topological disc","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.01105","snapshot_observed_at":"2026-08-04T10:52:09.413237Z","title":"D3-branes and M5-branes wrapped on a topological disc","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:09.413237Z"},"links":{"cited_paper":"/paper/2108.01105","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:69f7890828abd592c6a3ea9c4e48963441913306b97cfb19cb0d5aa85a7e60e0","observation_id":"61c84b6b-fab4-4512-ad8f-6d6bf8627102","resolution":{"observed_at":"2026-08-04T10:52:09.413237Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.03698","last_updated":"2015-10-28T10:54:54Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2015-04-14T20:01:53Z","title":"A topologically twisted index for three-dimensional supersymmetric theories","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.03698","snapshot_observed_at":"2026-08-04T10:52:09.485475Z","title":"A topologically twisted index for three- dimensional supersymmetric theories","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:09.485475Z"},"links":{"cited_paper":"/paper/1504.03698","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:6c8355ca60906fa58b35cc379df99e3d14d675214800c90ba846bebfa2aae0a6","observation_id":"99360620-bebb-4be0-ada6-a6cfe4602be1","resolution":{"observed_at":"2026-08-04T10:52:09.485475Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.04085","last_updated":"2016-02-17T15:25:18Z","snapshot_observed_at":"2026-08-02T02:37:08.100067Z","submitted_at":"2015-11-12T21:00:08Z","title":"Black hole microstates in AdS$_4$ from supersymmetric localization","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.04085","snapshot_observed_at":"2026-08-04T10:52:09.572583Z","title":"Black hole microstates in AdS4 from supersymmetric localization","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:09.572583Z"},"links":{"cited_paper":"/paper/1511.04085","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:5683f2a57fe0c9fb0dc166d6a872d221669d0841f554d82d13130c9300a7dacd","observation_id":"ab9cb20b-3c04-4629-8f2b-eec28ce03b81","resolution":{"observed_at":"2026-08-04T10:52:09.572583Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1608.07294","last_updated":"2016-08-25T20:00:09Z","snapshot_observed_at":"2026-08-08T23:20:19.978725Z","submitted_at":"2016-08-25T20:00:09Z","title":"Exact microstate counting for dyonic black holes in AdS4","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1608.07294","snapshot_observed_at":"2026-08-04T10:52:09.642538Z","title":"Exact microstate counting for dyonic black holes in AdS4","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity","version":3},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-04T10:52:09.642538Z"},"links":{"cited_paper":"/paper/1608.07294","citing_paper":"/paper/2510.08258"},"observation_digest":"sha256:a6a79e934cebc10f014e738322e144c1db18745d6a641b15386fc26ad3514262","observation_id":"52b846f4-b450-4289-9c59-d6083b7a4dcf","resolution":{"observed_at":"2026-08-04T10:52:09.642538Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2510.08258","last_updated":"2026-06-29T04:20:26Z","latest_version":3,"primary_category":"hep-th","snapshot_observed_at":"2026-08-08T19:08:17.824033Z","submitted_at":"2025-10-09T14:16:00Z","title":"Holographic solutions from 5D $SO(2)\\times ISO(3)$ $N=4$ gauged supergravity"},"reference_resolution":{"displayed":60,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":60,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":60},"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":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"thesis":"As of 9 August 2026, this Paper Citation Record lists 60 of 60 outbound references and 0 inbound Pith citation observations for arXiv:2510.08258."}