{"as_of":"2026-08-10T07:03:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:3742935bbdb5600abbc3815f5cbd0307888d107acd4d24ea2a2cd316c4e6db3b","coverage":[{"denominator":16,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":16,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T18:57:05.956909Z","state":"measured"},{"denominator":16,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":16,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+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/2507.06845/citation-record","integrity":"/paper/2507.06845/integrity","json":"/paper/2507.06845/citation-record.json","paper":"/paper/2507.06845"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"hep-th/9711200","last_updated":"1998-01-22T15:42:41Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"1997-11-27T23:53:13Z","title":"The Large N Limit of Superconformal Field Theories and Supergravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9711200","snapshot_observed_at":"2026-08-06T18:57:05.902728Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.902728Z"},"links":{"cited_paper":"/paper/hep-th/9711200","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:7ada3a206ff6f4dd6a54b334848b9319949d368e8ca5c8f5b09f7adb2a5d4d53","observation_id":"aaf4286b-64a6-4039-825a-2168c7640af8","resolution":{"observed_at":"2026-08-06T18:57:05.902728Z","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":"2026-08-06T18:57:05.906803Z","title":"Aharony, S","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.906803Z"},"links":{"citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:5f35160aae4b3117d07df6ad6a1c82b5664437684f0e413633e27a84b6d0794a","observation_id":"dadf7dbb-9420-4d20-9791-6c09844ce85c","resolution":{"observed_at":"2026-08-06T18:57:05.906803Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9805156","last_updated":"1998-09-09T18:11:10Z","snapshot_observed_at":"2026-08-03T03:50:23.202838Z","submitted_at":"1998-05-25T00:43:37Z","title":"Coupling Constant Dependence in the Thermodynamics of N=4 Supersymmetric Yang-Mills Theory","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9805156","snapshot_observed_at":"2026-08-06T18:57:05.910900Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.910900Z"},"links":{"cited_paper":"/paper/hep-th/9805156","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:d664cb99dab44a05cb2d6cf1e3ef4964896adbd97128a1b0324628c1603ae502","observation_id":"3306ec94-cbb6-4057-b9c0-87077263d5c4","resolution":{"observed_at":"2026-08-06T18:57:05.910900Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0406264","last_updated":"2007-07-11T17:49:39Z","snapshot_observed_at":"2026-07-07T04:51:05.067173Z","submitted_at":"2004-06-29T11:20:15Z","title":"Coupling constant dependence of the shear viscosity in N=4 supersymmetric Yang-Mills theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0406264","snapshot_observed_at":"2026-08-06T18:57:05.915243Z","title":"Buchel, J","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.915243Z"},"links":{"cited_paper":"/paper/hep-th/0406264","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:c524c0abb4653fce1708b5ab4037b04c1d18b1a6391723ed027e48aa54bbee8d","observation_id":"dc680a69-6c1c-4e51-9902-517e802a3059","resolution":{"observed_at":"2026-08-06T18:57:05.915243Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.02983","last_updated":"2015-11-09T18:03:59Z","snapshot_observed_at":"2026-07-06T04:29:24.362640Z","submitted_at":"2015-09-10T01:55:18Z","title":"Finite coupling corrections to holographic predictions for hot QCD","version":3},"cited_work":{"arxiv_id":"1509.02983","doi":null,"metadata_source":"pith","pith_arxiv_id":"1509.02983","snapshot_observed_at":"2026-08-06T18:57:06.098611Z","title":"Finite coupling corrections to holographic predictions for hot QCD","venue":"hep-th","work_id":"bf197022-9d7c-4637-b88c-e7de57b1af3e","year":2015},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.919068Z"},"links":{"cited_paper":"/paper/1509.02983","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:f7e8b18be243cc1429a2ce5f79b496a6ee3709c94b413f1828194c915e75ef02","observation_id":"a998706c-09a3-4bef-858e-570f2a39cb39","resolution":{"observed_at":"2026-08-06T18:57:06.102009Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1210.5187","last_updated":"2012-12-04T12:47:35Z","snapshot_observed_at":"2026-07-06T02:57:59.705351Z","submitted_at":"2012-10-18T16:57:04Z","title":"The finite 't Hooft coupling correction on the jet quenching parameter in a $\\mathcal N=4$ Super Yang-Mills Plasma","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1210.5187","snapshot_observed_at":"2026-08-06T18:57:05.922596Z","title":"Zhang, D.-f","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.922596Z"},"links":{"cited_paper":"/paper/1210.5187","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:e8ea26738ab9050b02fea36610a1923acc383b327d3c39ce7d535b42d39db3e8","observation_id":"46c3fb55-086f-449c-8c64-418cf7354757","resolution":{"observed_at":"2026-08-06T18:57:05.922596Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.12160","last_updated":"2022-01-06T17:35:49Z","snapshot_observed_at":"2026-07-06T12:11:34.830889Z","submitted_at":"2021-11-23T21:31:57Z","title":"${\\cal N}=4$ supersymmetric Yang-Mills thermodynamics from effective field theory","version":2},"cited_work":{"arxiv_id":"2111.12160","doi":null,"metadata_source":"pith","pith_arxiv_id":"2111.12160","snapshot_observed_at":"2026-08-06T18:57:06.078630Z","title":"${\\cal N}=4$ supersymmetric Yang-Mills thermodynamics from effective field theory","venue":"hep-th","work_id":"9316e601-de3f-4ae4-a9de-f2ab5a1aa60a","year":2021},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.926301Z"},"links":{"cited_paper":"/paper/2111.12160","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:f6b53e64bcb59fb905bbb48776f73107ea2ff6ecb034fc23aeff28d2094ef082","observation_id":"5c549dfe-3fe5-46ba-bee8-638d522bba44","resolution":{"observed_at":"2026-08-06T18:57:06.082256Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0605199","last_updated":"2006-06-19T21:32:05Z","snapshot_observed_at":"2026-07-07T04:11:03.005981Z","submitted_at":"2006-05-17T19:55:12Z","title":"Heavy Quark Diffusion in Strongly Coupled $\\N=4$ Yang Mills","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0605199","snapshot_observed_at":"2026-08-06T18:57:05.929510Z","title":"Casalderrey-Solana and D","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.929510Z"},"links":{"cited_paper":"/paper/hep-ph/0605199","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:e8e06125b15c70e07561d11410fe835f06ca131415ff08015e00b3e865fb09df","observation_id":"f14ab783-fbd4-453d-b6d0-bafa17b5f5a3","resolution":{"observed_at":"2026-08-06T18:57:05.929510Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0606245","last_updated":"2006-07-03T17:05:45Z","snapshot_observed_at":"2026-07-07T04:11:23.949703Z","submitted_at":"2006-06-22T19:31:46Z","title":"Jet quenching at finite `t Hooft coupling and chemical potential from AdS/CFT","version":3},"cited_work":{"arxiv_id":"hep-ph/0606245","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0606245","snapshot_observed_at":"2026-08-06T18:57:06.057974Z","title":"Jet quenching at finite `t Hooft coupling and chemical potential from AdS/CFT","venue":"hep-ph","work_id":"e6abdd3b-e7df-4cd7-b9c9-85bba24c106b","year":2006},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.932755Z"},"links":{"cited_paper":"/paper/hep-ph/0606245","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:97f42ac320c3d1954ab66f4ee01aa1ca6e5ce1ad04c2da10b6e29bcba6b9c925","observation_id":"754ccfb7-0324-4317-aacc-b955fd231022","resolution":{"observed_at":"2026-08-06T18:57:06.061563Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0801.2173","last_updated":"2008-01-14T22:30:36Z","snapshot_observed_at":"2026-08-07T02:48:37.517598Z","submitted_at":"2008-01-14T22:30:36Z","title":"Heavy quark diffusion in QCD and N=4 SYM at next-to-leading order","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0801.2173","snapshot_observed_at":"2026-08-06T18:57:05.936098Z","title":"Caron-Huot and G","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.936098Z"},"links":{"cited_paper":"/paper/0801.2173","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:b299d113e16b3808075cacc41c802413193f27fa30453e30337a539b2017432a","observation_id":"25ef52a8-650e-4a16-bccf-4733a51cdf2d","resolution":{"observed_at":"2026-08-06T18:57:05.936098Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.09535","last_updated":"2018-02-26T19:00:02Z","snapshot_observed_at":"2026-07-06T06:25:29.112809Z","submitted_at":"2018-02-26T19:00:02Z","title":"QCD Shear Viscosity at (almost) NLO","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.09535","snapshot_observed_at":"2026-08-06T18:57:05.939366Z","title":"Ghiglieri, G","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.939366Z"},"links":{"cited_paper":"/paper/1802.09535","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:7aa0e43609ae12eec4994409529a00d935eea7167cebdcc8ec121b1192cf80b6","observation_id":"47b79351-7110-4ee9-b3cc-c8badfb0354a","resolution":{"observed_at":"2026-08-06T18:57:05.939366Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0608062","last_updated":"2006-08-30T20:12:23Z","snapshot_observed_at":"2026-07-07T04:11:51.935750Z","submitted_at":"2006-08-04T17:41:35Z","title":"Shear viscosity in weakly coupled ${\\cal N} {=} 4$ Super Yang-Mills theory compared to QCD","version":2},"cited_work":{"arxiv_id":"hep-ph/0608062","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0608062","snapshot_observed_at":"2026-08-06T18:57:06.031688Z","title":"Shear viscosity in weakly coupled ${\\cal N} {=} 4$ Super Yang-Mills theory compared to QCD","venue":"hep-ph","work_id":"cd2988ed-5c86-48b8-b62b-71ceaffd9a81","year":2006},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.942888Z"},"links":{"cited_paper":"/paper/hep-ph/0608062","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:9aef8ddb2a5d7c5872c64a08b6e9418529a30e2e2ab100ad07ca6739ecab4658","observation_id":"b93bc2fc-88fe-4472-a742-20cb36611ebe","resolution":{"observed_at":"2026-08-06T18:57:06.035032Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0703082","last_updated":"2007-06-14T01:44:54Z","snapshot_observed_at":"2026-07-07T04:14:01.315574Z","submitted_at":"2007-03-07T17:40:20Z","title":"Small Shear Viscosity of a Quark-Gluon Plasma Implies Strong Jet Quenching","version":3},"cited_work":{"arxiv_id":"hep-ph/0703082","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0703082","snapshot_observed_at":"2026-08-06T18:57:06.020079Z","title":"Small Shear Viscosity of a Quark-Gluon Plasma Implies Strong Jet Quenching","venue":"hep-ph","work_id":"4f6140ca-1fb6-4119-bded-843559df7336","year":2007},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.946188Z"},"links":{"cited_paper":"/paper/hep-ph/0703082","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:2f2564453271d4a37cbf0a317e9e8b7b339f628426c3facf66030984bbf88db7","observation_id":"52eb979e-f969-4906-8ed0-3a71e85d5dd0","resolution":{"observed_at":"2026-08-06T18:57:06.023623Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2107.14775","last_updated":"2021-08-03T17:57:59Z","snapshot_observed_at":"2026-08-09T09:22:15.972534Z","submitted_at":"2021-07-30T17:27:47Z","title":"$\\eta/s-\\hat{q}/T^3$ Relation at Next-to-Leading Order in QCD","version":2},"cited_work":{"arxiv_id":"2107.14775","doi":null,"metadata_source":"pith","pith_arxiv_id":"2107.14775","snapshot_observed_at":"2026-08-06T18:57:06.007064Z","title":"$\\eta/s-\\hat{q}/T^3$ Relation at Next-to-Leading Order in QCD","venue":"hep-ph","work_id":"9b7615ba-5086-4436-b76d-1cce5d2f62ab","year":2021},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.949240Z"},"links":{"cited_paper":"/paper/2107.14775","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:73315f2fe791a45fae4da65748e09d83f8cfed9dbb7070eb06e9088014fb6bb2","observation_id":"aecd7cca-543d-4c02-96df-d029ecdfa151","resolution":{"observed_at":"2026-08-06T18:57:06.011480Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1809.01349","last_updated":"2018-12-10T12:30:21Z","snapshot_observed_at":"2026-07-06T06:59:15.592729Z","submitted_at":"2018-09-05T06:42:08Z","title":"Transverse momentum broadening and collinear radiation at NLO in the $\\mathcal{N}=4$ SYM plasma","version":2},"cited_work":{"arxiv_id":"1809.01349","doi":null,"metadata_source":"pith","pith_arxiv_id":"1809.01349","snapshot_observed_at":"2026-08-06T18:57:05.991955Z","title":"Transverse momentum broadening and collinear radiation at NLO in the $\\mathcal{N}=4$ SYM plasma","venue":"hep-ph","work_id":"e4ab335d-986c-4bef-8bb2-a4b2a945d94e","year":2018},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.952860Z"},"links":{"cited_paper":"/paper/1809.01349","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:b9d9100efa15913da134974cb933ed6971277c42e3be724adf327ffdc89f5394","observation_id":"9c4d02d5-19af-465c-b7a0-2a0257d9474f","resolution":{"observed_at":"2026-08-06T18:57:05.997839Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0805.2683","last_updated":"2008-05-17T16:15:18Z","snapshot_observed_at":"2026-08-03T01:53:39.552835Z","submitted_at":"2008-05-17T16:15:18Z","title":"Resolving disagreement for eta/s in a CFT plasma at finite coupling","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0805.2683","snapshot_observed_at":"2026-08-06T18:57:05.956909Z","title":"Buchel, Nucl","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-06T18:57:05.956909Z"},"links":{"cited_paper":"/paper/0805.2683","citing_paper":"/paper/2507.06845"},"observation_digest":"sha256:9657c6ac3a78da45c0ae7b3bb1ef724883f5920cbd3efc90ec6041850954ab29","observation_id":"f87b377f-4e6f-4d6f-8a4e-683ecea2985e","resolution":{"observed_at":"2026-08-06T18:57:05.956909Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2507.06845","last_updated":"2025-07-21T15:33:14Z","latest_version":2,"primary_category":"hep-th","snapshot_observed_at":"2026-08-08T20:37:28.039595Z","submitted_at":"2025-07-09T13:48:33Z","title":"Transition from weak to strong coupling in thermal gauge theories: Lessons from ${\\cal N}=4$ SYM Theory"},"reference_resolution":{"displayed":16,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":9,"verified_exact":7,"verified_fuzzy":0},"total_outbound_references":16},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 16 of 16 outbound references and 0 inbound Pith citation observations for arXiv:2507.06845."}