{"as_of":"2026-08-12T08:42:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:64d47bb78b833d04dbb15ca5963ca6dbd350636d187ed276394ce391e46ea036","coverage":[{"denominator":59,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":59,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-10T13:22:42.007750Z","state":"measured"},{"denominator":62,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":62,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-12T06:34:41.77262+00:00","state":"measured"},{"denominator":3,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":3,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-10T11:06:21.977258Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-13T03:07:08.898498Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"cited_work":{"arxiv_id":"2501.16441","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2501.16441","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Frangi and S","venue":null,"work_id":"99a3e24e-7adc-4535-9312-8328cdd645e3","year":2025},"citing_paper":{"arxiv_id":"2605.11096","last_updated":"2026-07-15T14:19:58Z","snapshot_observed_at":"2026-08-08T18:13:53.829263Z","submitted_at":"2026-05-11T18:02:46Z","title":"Stochastic inflation from a non-equilibrium renormalization group","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-05-13T03:04:25.590965Z"},"links":{"cited_paper":"/paper/2501.16441","citing_paper":"/paper/2605.11096"},"observation_digest":"sha256:d93483c869d5b8caca79eec71ad5688eeb2dbf201f284876546aaba72a335d56","observation_id":"afa17847-5d51-42a7-b096-70680d80da8c","resolution":{"observed_at":"2026-05-13T03:07:08.900065Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.16441","snapshot_observed_at":"2026-08-02T14:25:56.901455Z","title":"Frangi and S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2605.11096","last_updated":"2026-07-15T14:19:58Z","snapshot_observed_at":"2026-08-08T18:13:53.829263Z","submitted_at":"2026-05-11T18:02:46Z","title":"Stochastic inflation from a non-equilibrium renormalization group","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-02T14:25:56.901455Z"},"links":{"cited_paper":"/paper/2501.16441","citing_paper":"/paper/2605.11096"},"observation_digest":"sha256:45c7b4683a1bdf31f14b48e36a56edb9367a7b74ba12bea5f872d32aaabbedca","observation_id":"c8c3be71-0091-4fc2-b2f4-8f3a79b37dd6","resolution":{"observed_at":"2026-08-02T14:25:56.901455Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.16441","snapshot_observed_at":"2026-08-10T11:06:21.977258Z","title":"Frangi and S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.07292","last_updated":"2026-08-07T14:48:52Z","snapshot_observed_at":"2026-08-12T08:11:57.420989Z","submitted_at":"2026-08-07T14:48:52Z","title":"Critical dynamics of a scalar field near four spatial dimensions","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-10T11:06:21.977258Z"},"links":{"cited_paper":"/paper/2501.16441","citing_paper":"/paper/2608.07292"},"observation_digest":"sha256:cd62303853fba8d7d2371f47071e70a9c6c5136ab51dfea86675ca1bc60f1d8f","observation_id":"aa97d955-2c19-456f-8c2f-974360fe8223","resolution":{"observed_at":"2026-08-10T11:06:21.977258Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2501.16441/citation-record","integrity":"/paper/2501.16441/integrity","json":"/paper/2501.16441/citation-record.json","paper":"/paper/2501.16441"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.165428Z","title":null,"venue":null,"work_id":"0168b2c8-5412-431e-b0c9-176c575688db","year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.735752Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:329a77f99cd62e6b755da1ba5fdba75d67b41e8de43ee7ba41f1eb9d8fb2533e","observation_id":"a75004ef-f830-4879-beb9-bacdbac2d03d","resolution":{"observed_at":"2026-08-10T13:22:43.169662Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.149383Z","title":null,"venue":null,"work_id":"93ccd93e-858b-40e2-8580-1a83d2b0c157","year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.741307Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:a4fa97544ec9ddbd0a9311c61081bcfa3becf3bd371db3a418e2f9978e40fe54","observation_id":"e6e5b4d9-2b85-4018-94a1-5892d34ad0b3","resolution":{"observed_at":"2026-08-10T13:22:43.153927Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.134075Z","title":"In terms of the path integral, the effective action is then given by eiSeff [ϕ<] ≡ eiS0[ϕ<] Z Dϕ>eiS0[ϕ>]eiSint[ϕ<,ϕ>]","venue":null,"work_id":"aef88aa0-7142-457c-a44d-eecaca7fdecf","year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.745946Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:3fd97355acdc9c4d24574eb24babebe151cd61c0d4ffe475a415721ebc2b0ae2","observation_id":"528895dd-7ada-4c4a-880d-d2c873279995","resolution":{"observed_at":"2026-08-10T13:22:43.138539Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.072760Z","title":"Calzetta and B","venue":null,"work_id":"17571fda-ed5e-48fb-b155-0135b42a9c99","year":2008},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.769275Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:1b4cdcb0a986b3e7f2370a1fd7b533e4af9a9f6ce79fbeee6b0053da804522b9","observation_id":"ef38321a-f438-4947-8eae-662e7e80ee6b","resolution":{"observed_at":"2026-08-10T13:22:43.077307Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9210046","last_updated":"1999-06-08T16:24:03Z","snapshot_observed_at":"2026-07-07T05:01:51.679446Z","submitted_at":"1992-10-08T18:06:00Z","title":"Effective Field Theory and the Fermi Surface","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9210046","snapshot_observed_at":"2026-08-10T13:22:41.756296Z","title":"Polchinski, Effective field theory and the fermi surface (1999), arXiv:hep-th/9210046 [hep-th]","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.756296Z"},"links":{"cited_paper":"/paper/hep-th/9210046","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:a804a6e96026d12eff48fbe1afe958f679f2f2afe0ba7bf7eca5847a49c69589","observation_id":"6b2585b6-5725-4e6a-9a3b-7c7ad2607f28","resolution":{"observed_at":"2026-08-10T13:22:41.756296Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.103149Z","title":null,"venue":null,"work_id":"8e5a4fe4-bbc7-4fa5-9696-873bc86cb2f9","year":1987},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.760707Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:2535e6be7616fb8ce059bea4689f8fc380d7905fee1d7c0bc6ee7c75f52b1c9a","observation_id":"ac0b59ee-3fb3-4fdc-b1e0-cb4170358889","resolution":{"observed_at":"2026-08-10T13:22:43.108029Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.087859Z","title":null,"venue":null,"work_id":"51acc0c5-b5e7-4fe3-9132-ceae940ca552","year":1997},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.765058Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:8610c3b7b03456a835c8cc41922f1547e1d2fdec5f4a7b30ed9870070b61ad09","observation_id":"084f74db-e741-4374-94ee-2883b114252d","resolution":{"observed_at":"2026-08-10T13:22:43.092534Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1305.3670","last_updated":"2015-05-08T17:04:40Z","snapshot_observed_at":"2026-07-06T03:13:29.286484Z","submitted_at":"2013-05-16T02:13:09Z","title":"Viscosity and dissipative hydrodynamics from effective field theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1305.3670","snapshot_observed_at":"2026-08-10T13:22:41.787327Z","title":"Grozdanov and J","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.787327Z"},"links":{"cited_paper":"/paper/1305.3670","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:34ee23fb119a0ecd01b06979c537d51113ce1435cbd3c65f9506b169baffad31","observation_id":"ff5e4762-f710-485d-b2da-00731f5c6c42","resolution":{"observed_at":"2026-08-10T13:22:41.787327Z","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":"2026-08-10T13:22:41.773379Z","title":"Kamenev, Field Theory of Non-Equilibrium Systems (Cambridge University Press, 2011)","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.773379Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:150ee844f72b841b61e7b49f120a26b9a65d32f2bf2bf8b13a8c804e03e30245","observation_id":"05af9448-8c24-435c-b6fc-c11e0d689922","resolution":{"observed_at":"2026-08-10T13:22:41.773379Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.09331","last_updated":"2018-05-23T18:00:01Z","snapshot_observed_at":"2026-08-09T05:11:38.762832Z","submitted_at":"2018-05-23T18:00:01Z","title":"Lectures on non-equilibrium effective field theories and fluctuating hydrodynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.09331","snapshot_observed_at":"2026-08-10T13:22:41.777596Z","title":"Liu and P","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.777596Z"},"links":{"cited_paper":"/paper/1805.09331","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:9013cedb1d73506588c34515ad929057d15561afdffedfe1bd3a8e15506f3e4d","observation_id":"2261aa69-80bb-48b6-b0df-5825bb8ead23","resolution":{"observed_at":"2026-08-10T13:22:41.777596Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.02739","last_updated":"2025-01-27T23:49:48Z","snapshot_observed_at":"2026-08-11T23:07:06.814189Z","submitted_at":"2024-12-03T19:00:00Z","title":"Effective Field Theory and In-In Correlators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.02739","snapshot_observed_at":"2026-08-10T13:22:41.782498Z","title":"Green and G","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.782498Z"},"links":{"cited_paper":"/paper/2412.02739","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:ebd6ad6c0a1fcb9b5a2fc01a7c0023bc644ee6bf457681e96b769b41453f1ac6","observation_id":"913c455c-bee9-4592-94e8-17d3a270d38b","resolution":{"observed_at":"2026-08-10T13:22:41.782498Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.07817","last_updated":"2017-02-24T02:23:40Z","snapshot_observed_at":"2026-07-06T05:27:43.025754Z","submitted_at":"2017-01-26T18:52:23Z","title":"Effective field theory for dissipative fluids (II): classical limit, dynamical KMS symmetry and entropy current","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.07817","snapshot_observed_at":"2026-08-10T13:22:41.806413Z","title":"Glorioso, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.806413Z"},"links":{"cited_paper":"/paper/1701.07817","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:41be3522b85881f23ae6f31f4c3bf545d0252a87ae8f4b99b7d5c2eea890c1a5","observation_id":"30a08299-ae4e-4ea4-8854-bfe4b4b56b42","resolution":{"observed_at":"2026-08-10T13:22:41.806413Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1604.05291","last_updated":"2016-11-01T16:17:51Z","snapshot_observed_at":"2026-07-06T04:53:16.872546Z","submitted_at":"2016-04-18T19:47:17Z","title":"A Lagrangian formulation of relativistic Israel-Stewart hydrodynamics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1604.05291","snapshot_observed_at":"2026-08-10T13:22:41.792138Z","title":"Montenegro and G","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.792138Z"},"links":{"cited_paper":"/paper/1604.05291","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:a7ff149fc5198c1c4fadbb16e45c8c79c7aa1835b295ce975543ac0c2b9d23d8","observation_id":"397fd185-90ee-4bf5-bdf3-fd104ec18e0e","resolution":{"observed_at":"2026-08-10T13:22:41.792138Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1511.03646","last_updated":"2017-01-27T18:07:19Z","snapshot_observed_at":"2026-08-05T19:13:07.994343Z","submitted_at":"2015-11-11T20:32:34Z","title":"Effective field theory of dissipative fluids","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.03646","snapshot_observed_at":"2026-08-10T13:22:41.797081Z","title":"Crossley, P","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.797081Z"},"links":{"cited_paper":"/paper/1511.03646","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:d5bfb47b42af8a7f3067cb5bd8e657f0ec76137a7cf5ba5685d25f617a2a7fad","observation_id":"c470c477-c2d6-426e-9bc7-2accdf97c89f","resolution":{"observed_at":"2026-08-10T13:22:41.797081Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.07705","last_updated":"2017-02-17T14:09:30Z","snapshot_observed_at":"2026-08-10T09:10:18.596945Z","submitted_at":"2016-12-22T17:11:00Z","title":"The second law of thermodynamics from symmetry and unitarity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.07705","snapshot_observed_at":"2026-08-10T13:22:41.801821Z","title":"Glorioso and H","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.801821Z"},"links":{"cited_paper":"/paper/1612.07705","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:1ba3cc3f54d644ffb47239f94100a258422c20a3f2502809f7eed8e7bf856c10","observation_id":"3e19d600-7f19-4c10-ab26-98af9b9b8340","resolution":{"observed_at":"2026-08-10T13:22:41.801821Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.12540","last_updated":"2019-12-22T09:19:36Z","snapshot_observed_at":"2026-08-10T00:07:48.262357Z","submitted_at":"2018-11-29T23:47:45Z","title":"Theory of diffusive fluctuations","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.12540","snapshot_observed_at":"2026-08-10T13:22:41.825829Z","title":"Chen-Lin, L","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.825829Z"},"links":{"cited_paper":"/paper/1811.12540","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:f246792d1c662bb89e21eee6bc9909a707eda606e7b54a97184f465b046b9a6b","observation_id":"2848882a-d0c9-4c58-b920-be59b89da85d","resolution":{"observed_at":"2026-08-10T13:22:41.825829Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1312.0610","last_updated":"2014-03-14T13:22:29Z","snapshot_observed_at":"2026-07-06T03:29:45.941536Z","submitted_at":"2013-12-02T21:00:08Z","title":"Effective actions for anomalous hydrodynamics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1312.0610","snapshot_observed_at":"2026-08-10T13:22:41.811710Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.811710Z"},"links":{"cited_paper":"/paper/1312.0610","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:57fc1a5729a3d9f07fe4d5c06fd9253875a13d172351c05f6b5f86a0f3198fae","observation_id":"20b9b9de-6971-4187-a680-3e6f3ef80d50","resolution":{"observed_at":"2026-08-10T13:22:41.811710Z","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":"10.1007/jhep01(2016)184","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:42.057960Z","title":null,"venue":null,"work_id":"c693654e-689b-463c-af10-ed09a9097ce3","year":2016},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.816604Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:c7197792b1ad1de1ae58d40229fec3f031871cce68cac00ac46fc2d21b4562b3","observation_id":"7db6602d-9d93-43ae-9d5e-a5cbac633a91","resolution":{"observed_at":"2026-08-10T13:22:42.062828Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1511.07809","last_updated":"2017-01-31T04:30:53Z","snapshot_observed_at":"2026-07-06T04:37:39.055441Z","submitted_at":"2015-11-24T17:10:23Z","title":"Topological sigma models & dissipative hydrodynamics","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1511.07809","snapshot_observed_at":"2026-08-10T13:22:41.821177Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.821177Z"},"links":{"cited_paper":"/paper/1511.07809","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:d4505d80357417fcfeb7b0dca65e9b60129a1f8c16c1c565c03989e14e7ad871","observation_id":"7854cd2d-d94c-4d55-92c3-26364d180320","resolution":{"observed_at":"2026-08-10T13:22:41.821177Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.12868","last_updated":"2025-05-26T06:26:26Z","snapshot_observed_at":"2026-07-06T19:04:57.203125Z","submitted_at":"2024-08-23T06:55:53Z","title":"Effective field theories of dissipative fluids with one-form symmetries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.12868","snapshot_observed_at":"2026-08-10T13:22:41.845183Z","title":"Vardhan, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.845183Z"},"links":{"cited_paper":"/paper/2408.12868","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:a8e117f1899cd7d94e6ea2bb05f27c9a045cc4c27c7eebb6154d966b2f4e6817","observation_id":"274db9db-a16f-4cea-b8ae-4d5edb8cd9d5","resolution":{"observed_at":"2026-08-10T13:22:41.845183Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.07436","last_updated":"2018-06-24T13:58:03Z","snapshot_observed_at":"2026-08-10T12:31:24.072904Z","submitted_at":"2017-01-25T19:00:01Z","title":"Dissipative hydrodynamics in superspace","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.07436","snapshot_observed_at":"2026-08-10T13:22:41.830604Z","title":"Jensen, N","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.830604Z"},"links":{"cited_paper":"/paper/1701.07436","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:95db09621e42cdf69126bbd9dbe89c1b0e0e1249ad8d8b6262d8a804d01e23a4","observation_id":"19013700-a442-4d7b-b107-1a92c82915cc","resolution":{"observed_at":"2026-08-10T13:22:41.830604Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.04654","last_updated":"2018-11-06T22:18:39Z","snapshot_observed_at":"2026-07-06T06:33:11.138971Z","submitted_at":"2018-04-12T17:59:58Z","title":"A panoply of Schwinger-Keldysh transport","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.04654","snapshot_observed_at":"2026-08-10T13:22:41.835316Z","title":"Jensen, R","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.835316Z"},"links":{"cited_paper":"/paper/1804.04654","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:2e69d3b0b8451a73ddca48c6759ac1dd3df97602a7f45d4a215dccf470d27cc3","observation_id":"eaf2f586-0e02-4ddc-80b8-ed558ceae26e","resolution":{"observed_at":"2026-08-10T13:22:41.835316Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.01636","last_updated":"2024-12-09T10:56:45Z","snapshot_observed_at":"2026-07-06T13:27:42.434055Z","submitted_at":"2022-07-04T18:00:03Z","title":"Strong-field magnetohydrodynamics for neutron stars","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.01636","snapshot_observed_at":"2026-08-10T13:22:41.840152Z","title":"Vardhan, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.840152Z"},"links":{"cited_paper":"/paper/2207.01636","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:e3e5649ccebf8b03e3ad2b818eaca6d4747971670a779e10a37a5fc45e2b811b","observation_id":"a87b49f8-60d0-41ef-a428-0c1f388e4c8a","resolution":{"observed_at":"2026-08-10T13:22:41.840152Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.01436","last_updated":"2022-03-11T21:59:18Z","snapshot_observed_at":"2026-07-06T10:20:03.494822Z","submitted_at":"2020-12-02T19:00:01Z","title":"Hydrodynamic Theory of the Connected Spectral Form Factor","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.01436","snapshot_observed_at":"2026-08-10T13:22:41.863369Z","title":"Winer and B","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.863369Z"},"links":{"cited_paper":"/paper/2012.01436","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:7e89ac4b72c3d55da068f8a3db85065bbdb3085d719ed51a72374aa3ab90b498","observation_id":"22db15dd-69e3-48c8-bbec-395a40ea2641","resolution":{"observed_at":"2026-08-10T13:22:41.863369Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.00010","last_updated":"2018-10-15T15:49:48Z","snapshot_observed_at":"2026-07-31T02:33:31.092655Z","submitted_at":"2017-12-29T19:00:04Z","title":"A quantum hydrodynamical description for scrambling and many-body chaos","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.00010","snapshot_observed_at":"2026-08-10T13:22:41.850024Z","title":"Blake, H","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.850024Z"},"links":{"cited_paper":"/paper/1801.00010","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:79018798d14b5e66585fee205bb2d1b96c1383d3fca9a2c50b5ac7e1fa474ce8","observation_id":"3324a2b7-f90a-49d1-8acc-e465b1caf849","resolution":{"observed_at":"2026-08-10T13:22:41.850024Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.11294","last_updated":"2021-06-01T11:58:09Z","snapshot_observed_at":"2026-08-09T15:33:38.718822Z","submitted_at":"2021-02-22T19:00:09Z","title":"On systems of maximal quantum chaos","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.11294","snapshot_observed_at":"2026-08-10T13:22:41.854855Z","title":"Blake and H","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.854855Z"},"links":{"cited_paper":"/paper/2102.11294","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:44b92f232c57772b24b985d1b38890f1ebe494fd8f4a4343e3328a845e7ac463","observation_id":"407f5bbf-3be6-4cc8-a893-0e4593bc0184","resolution":{"observed_at":"2026-08-10T13:22:41.854855Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2301.05256","last_updated":"2023-08-15T15:15:15Z","snapshot_observed_at":"2026-08-10T11:59:29.992867Z","submitted_at":"2023-01-12T19:10:09Z","title":"An effective field theory for non-maximal quantum chaos","version":2},"cited_work":{"arxiv_id":"2301.05256","doi":null,"metadata_source":"pith","pith_arxiv_id":"2301.05256","snapshot_observed_at":"2026-08-10T13:22:42.643339Z","title":"An effective field theory for non-maximal quantum chaos","venue":"hep-th","work_id":"6041dde4-54a0-43d2-a853-efd74b85da2e","year":2023},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.859119Z"},"links":{"cited_paper":"/paper/2301.05256","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:cf8a8dfe9a27e8f8d697a8be929424df6e8c203371c2aef5f4a2cb4a2267963c","observation_id":"920ab2a0-c339-49c2-9303-d3ca73e1aaf0","resolution":{"observed_at":"2026-08-10T13:22:42.648024Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2306.17232","last_updated":"2024-05-31T19:09:00Z","snapshot_observed_at":"2026-08-10T05:16:48.374291Z","submitted_at":"2023-06-29T18:01:08Z","title":"The Schwinger-Keldysh Coset Construction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.17232","snapshot_observed_at":"2026-08-10T13:22:41.882276Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.882276Z"},"links":{"cited_paper":"/paper/2306.17232","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:b75fc681de2d07a5d8bcdf18319ced33dc64e3ff314f0bc6be2818046742223b","observation_id":"92ca2b9e-2c82-436c-9059-b47310078e25","resolution":{"observed_at":"2026-08-10T13:22:41.882276Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.01356","last_updated":"2020-09-02T21:38:10Z","snapshot_observed_at":"2026-08-09T10:32:15.317442Z","submitted_at":"2020-09-02T21:38:10Z","title":"Non-universality of hydrodynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.01356","snapshot_observed_at":"2026-08-10T13:22:41.868083Z","title":"Jain and P","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.868083Z"},"links":{"cited_paper":"/paper/2009.01356","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:0bbd2c7eb956a69385ca420dc1785edd2e1abd53f4816df097552e4ede5acb14","observation_id":"2de55711-44d0-44ed-8adb-bd794e5762d3","resolution":{"observed_at":"2026-08-10T13:22:41.868083Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.07929","last_updated":"2025-04-28T08:17:11Z","snapshot_observed_at":"2026-08-12T02:08:41.779026Z","submitted_at":"2024-10-10T13:57:02Z","title":"Three-point functions from a Schwinger-Keldysh effective action, resummed in derivatives","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.07929","snapshot_observed_at":"2026-08-10T13:22:41.872891Z","title":"Abbasi and D","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.872891Z"},"links":{"cited_paper":"/paper/2410.07929","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:fd66af680237317915f0b200737e65813c6991eeec078ab612c5fc541be002b7","observation_id":"f4916c76-0e99-4936-8987-9f660c29f9a0","resolution":{"observed_at":"2026-08-10T13:22:41.872891Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.08263","last_updated":"2017-08-27T23:31:01Z","snapshot_observed_at":"2026-07-06T05:27:54.149181Z","submitted_at":"2017-01-28T07:36:16Z","title":"The ideal relativistic fluid limit for a medium with polarization","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.08263","snapshot_observed_at":"2026-08-10T13:22:41.877693Z","title":"Montenegro, L","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.877693Z"},"links":{"cited_paper":"/paper/1701.08263","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:b3cec6702a93b26131e53401290863da90e2a9a9655cad64e464f6262903d33e","observation_id":"189bcc85-333a-402e-ad22-b0865d061db5","resolution":{"observed_at":"2026-08-10T13:22:41.877693Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.00511","last_updated":"2023-09-01T14:59:05Z","snapshot_observed_at":"2026-08-10T01:49:31.980721Z","submitted_at":"2023-09-01T14:59:05Z","title":"Schwinger-Keldysh effective field theory for stable and causal relativistic hydrodynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.00511","snapshot_observed_at":"2026-08-10T13:22:41.901001Z","title":"Jain and P","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.901001Z"},"links":{"cited_paper":"/paper/2309.00511","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:aeb3df12d95e76862e2778a9c82a74989e0c71961e87ff1a0bed890f29dc331c","observation_id":"9b69d588-3121-4988-8b64-5ea4a8828921","resolution":{"observed_at":"2026-08-10T13:22:41.901001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.14173","last_updated":"2023-08-27T22:33:36Z","snapshot_observed_at":"2026-07-06T15:20:45.845539Z","submitted_at":"2023-04-27T13:21:15Z","title":"U(1) quasi-hydrodynamics: Schwinger-Keldysh effective field theory and holography","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.14173","snapshot_observed_at":"2026-08-10T13:22:41.887080Z","title":"Baggioli, Y","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.887080Z"},"links":{"cited_paper":"/paper/2304.14173","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:62c2e546a64681b63fc6bb4a43fffeaf3aee91798a41021dc6dd268a48897c27","observation_id":"6f9fb38e-7666-4411-b5d0-d3a9c2ae811c","resolution":{"observed_at":"2026-08-10T13:22:41.887080Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.08016","last_updated":"2024-11-12T18:49:03Z","snapshot_observed_at":"2026-08-08T20:07:37.557684Z","submitted_at":"2024-11-12T18:49:03Z","title":"Schwinger-Keldysh effective action for hydrodynamics with approximate symmetries","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.08016","snapshot_observed_at":"2026-08-10T13:22:41.892096Z","title":"Hongo, N","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.892096Z"},"links":{"cited_paper":"/paper/2411.08016","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:8d8bb71c204ccfeb2112fe71bee475057e339e3bae306bed4ddd54ebea6c210c","observation_id":"ebfac654-4422-4c7f-9714-e6b636177f06","resolution":{"observed_at":"2026-08-10T13:22:41.892096Z","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":"2026-08-10T13:22:41.896606Z","title":"Armas, A","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.896606Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:52b0bdb8b18ffe0487c977d2377c3ccae028b110a6ab1bd9762350f79121c2b3","observation_id":"ddce5d1e-b55a-40b4-bd92-0d25560e09cd","resolution":{"observed_at":"2026-08-10T13:22:41.896606Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9210227","last_updated":"1992-10-10T00:27:16Z","snapshot_observed_at":"2026-07-07T04:14:41.385429Z","submitted_at":"1992-10-10T00:27:16Z","title":"Computing Spectral Densities in Finite Temperature Field Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9210227","snapshot_observed_at":"2026-08-10T13:22:41.920153Z","title":"Jeon, Computing spectral densities in finite tem- perature field theory, Phys","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.920153Z"},"links":{"cited_paper":"/paper/hep-ph/9210227","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:d82aab903054a45329b74ee88254ec826e45c341b3af4717dfd4ade2531865d0","observation_id":"d0701f12-7687-4241-a34b-680a2a7364ad","resolution":{"observed_at":"2026-08-10T13:22:41.920153Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.13550","last_updated":"2024-07-18T14:24:29Z","snapshot_observed_at":"2026-07-06T18:48:29.372633Z","submitted_at":"2024-07-18T14:24:29Z","title":"Analytic structure of diffusive correlation functions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.13550","snapshot_observed_at":"2026-08-10T13:22:41.905780Z","title":"Grozdanov, T","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.905780Z"},"links":{"cited_paper":"/paper/2407.13550","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:7f8209001e8c845af69c3aaaed8d547c1f21be74c1e48dfeee59abd1dbb51aab","observation_id":"240a6154-4fd4-49b1-ba5f-25259f002054","resolution":{"observed_at":"2026-08-10T13:22:41.905780Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.13811","last_updated":"2022-02-15T18:30:05Z","snapshot_observed_at":"2026-07-06T10:27:57.301891Z","submitted_at":"2020-12-26T21:08:46Z","title":"Renormalizing open quantum field theories","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.13811","snapshot_observed_at":"2026-08-10T13:22:41.910293Z","title":"Nagy and J","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.910293Z"},"links":{"cited_paper":"/paper/2012.13811","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:cacef1990bc29fa71e0c851e852c4eff6b6b446aa2f2650ec330b68acd324dcf","observation_id":"83c56390-c724-4377-9ac8-61d82188aaa9","resolution":{"observed_at":"2026-08-10T13:22:41.910293Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.15763","last_updated":"2023-10-24T12:10:10Z","snapshot_observed_at":"2026-08-04T00:35:39.027827Z","submitted_at":"2023-10-24T12:10:10Z","title":"Nonequilibrium thermodynamics perspectives for the monotonicity of the renormalization group flow","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.15763","snapshot_observed_at":"2026-08-10T13:22:41.915235Z","title":"Kim and S","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.915235Z"},"links":{"cited_paper":"/paper/2310.15763","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:c08d5473d335b598f3fefd365c7bf7b96a887b80b4c2e2539fcd171fb6d4c003","observation_id":"0c9bf387-81c0-448a-924d-4fff109b7c54","resolution":{"observed_at":"2026-08-10T13:22:41.915235Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.09292","last_updated":"2018-12-14T12:04:08Z","snapshot_observed_at":"2026-07-06T06:30:05.047391Z","submitted_at":"2018-03-25T16:42:16Z","title":"Boost invariant regulator for field theories","version":2},"cited_work":{"arxiv_id":"1803.09292","doi":null,"metadata_source":"pith","pith_arxiv_id":"1803.09292","snapshot_observed_at":"2026-08-10T13:22:42.208983Z","title":"Boost invariant regulator for field theories","venue":"hep-th","work_id":"675c18c3-b702-4c1b-b765-babb60c156b0","year":2018},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.938838Z"},"links":{"cited_paper":"/paper/1803.09292","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:8f389f45e53d323568a9641668ad39c5eafe77148facc629d9ddcec7c3f2f22c","observation_id":"98288168-9ae7-40b5-9369-d69d9f688e42","resolution":{"observed_at":"2026-08-10T13:22:42.214467Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.046836Z","title":"Jeon, Hydrodynamic transport coefficients in relativis- tic scalar field theory, Phys","venue":null,"work_id":"7ef67b43-6dde-4b68-ab40-4c823e8bb084","year":1995},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.924999Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:26bf7ebff1ce964739cf064321bd23a826dfca3123dacdb6b86eb5da718e9ea9","observation_id":"786bbda5-6e08-4532-bc4b-09b55f2c264c","resolution":{"observed_at":"2026-08-10T13:22:43.051781Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0201116","last_updated":"2002-05-16T16:47:42Z","snapshot_observed_at":"2026-07-07T04:42:21.260275Z","submitted_at":"2002-01-16T03:19:09Z","title":"Shear viscosity of hot scalar field theory in the real-time formalism","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0201116","snapshot_observed_at":"2026-08-10T13:22:41.929494Z","title":"Wang and U","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.929494Z"},"links":{"cited_paper":"/paper/hep-th/0201116","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:b9242ba1d3698b0e6dde4242ea86d4cc0bde4890006dffe42ff5cdfc853fb72b","observation_id":"b7b214c5-2264-4d2a-8d05-a081688362d4","resolution":{"observed_at":"2026-08-10T13:22:41.929494Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.031256Z","title":"Arnold, G","venue":null,"work_id":"eea8c8e3-afa0-433b-97f9-74f1354cef37","year":2000},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.934305Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:ac1a69d03d75ad6489e12528395a23c41ce05e97ca51f4c6970cf85e9f9c8bc7","observation_id":"e42c229d-5f7b-496b-8a04-0c3b4526a253","resolution":{"observed_at":"2026-08-10T13:22:43.035988Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.000457Z","title":null,"venue":null,"work_id":"94b3f9ac-7720-44e2-b14b-5c8771d5f51d","year":1984},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.957240Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:307f45336d8c808b42dd670f8241c3a11c5ba3dfdf15c5f228e13720fdff8555","observation_id":"b1080734-2101-438e-85e1-f65c25bec371","resolution":{"observed_at":"2026-08-10T13:22:43.005729Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1908.11311","last_updated":"2020-11-21T19:30:48Z","snapshot_observed_at":"2026-07-06T08:17:44.489058Z","submitted_at":"2019-08-29T15:52:14Z","title":"Renormalization in Minkowski space-time","version":2},"cited_work":{"arxiv_id":"1908.11311","doi":null,"metadata_source":"pith","pith_arxiv_id":"1908.11311","snapshot_observed_at":"2026-08-10T13:22:42.187996Z","title":"Renormalization in Minkowski space-time","venue":"hep-th","work_id":"084668f4-2045-4bfc-b636-72ab73392e89","year":2019},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.943398Z"},"links":{"cited_paper":"/paper/1908.11311","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:05905b10810658b331542dbe0ddd84b15833dfe081e75510c58ba1208afb0af4","observation_id":"13bba2d3-d418-471d-8c0a-75366bbe652f","resolution":{"observed_at":"2026-08-10T13:22:42.192910Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.016246Z","title":"Ojima, Lorentz Invariance Versus Temperature in QFT, Lett","venue":null,"work_id":"abc6237d-79df-43f3-9a5c-aba55f53703d","year":1986},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.948121Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:bb2bb231c0bd49879efaacee2372d99f2eb7f70c3de3472d43c5cfae85c924ab","observation_id":"a40b4d4a-6576-4071-a877-499f7a1f336b","resolution":{"observed_at":"2026-08-10T13:22:43.021004Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9408254","last_updated":"1994-08-09T09:01:46Z","snapshot_observed_at":"2026-08-12T07:13:31.599329Z","submitted_at":"1994-08-09T09:01:46Z","title":"The Thermal Beta-Function in Yang-Mills Theory","version":1},"cited_work":{"arxiv_id":"hep-ph/9408254","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9408254","snapshot_observed_at":"2026-08-10T13:22:42.166477Z","title":"The Thermal Beta-Function in Yang-Mills Theory","venue":"hep-ph","work_id":"c282c8a2-4242-4bd3-b092-f68e555d8c4d","year":1994},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.952457Z"},"links":{"cited_paper":"/paper/hep-ph/9408254","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:4f079c75452fdca421e087212753df75455cb4f080af6f91328b2aff5fd1862e","observation_id":"6ccbcd54-f102-41a7-bfa4-25c4b70ad772","resolution":{"observed_at":"2026-08-10T13:22:42.171768Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:43.119194Z","title":"[49, 50]","venue":null,"work_id":"6cc18471-d41e-4b0c-a696-171853b2ffa9","year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.752104Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:33802b03126261f1e49f8dc3a8f9ca747c0d833c0981accfe6fb64c8c8a9fe94","observation_id":"db19fea1-60ce-459d-981b-dfa277da5b23","resolution":{"observed_at":"2026-08-10T13:22:43.124106Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/jhep10(2016)009","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:42.039954Z","title":"Stanford, Many-body chaos at weak coupling, Journal of High Energy Physics 2016, 10.1007/jhep10(2016)009 (2016)","venue":null,"work_id":"e1e7f750-272e-4f21-a9ff-734420a556e2","year":2016},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.961788Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:cd36844dad87b5bc7b6ee9a2c1dedc1eb9f58449c99af298a0291834160ec9da","observation_id":"46fa32cb-b36e-4400-9d66-cf589a8c9b0f","resolution":{"observed_at":"2026-08-10T13:22:42.047133Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:42.984452Z","title":"Dolan and R","venue":null,"work_id":"02750318-afc8-4f4f-8d8f-0c57492ea4ea","year":1974},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.966025Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:dd68aa2157b70a6639508899ec25d520f62c6aa903491004fff267733bff0a29","observation_id":"29133e70-074d-49cf-9e60-d429bb1606a6","resolution":{"observed_at":"2026-08-10T13:22:42.989024Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0110026","last_updated":"2003-01-10T17:49:52Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2001-10-02T13:39:48Z","title":"Lectures on the functional renormalization group method","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0110026","snapshot_observed_at":"2026-08-10T13:22:41.970373Z","title":"Polonyi, Lectures on the functional renormalization group method, Central Eur","venue":null,"work_id":null,"year":2003},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.970373Z"},"links":{"cited_paper":"/paper/hep-th/0110026","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:a017ba3481c143e2456caaa2fa4e4c5a1bd88d399f0db746881667f6be8f66f3","observation_id":"8c8929a2-fd14-4ab0-8475-2a5a646a97aa","resolution":{"observed_at":"2026-08-10T13:22:41.970373Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:42.969331Z","title":null,"venue":null,"work_id":"d343642b-f623-46da-819e-fdaaf868c174","year":1986},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.974551Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:6ad176bf0daebc0bf532529dc2ccfd163482e4cb9d77fd6f3bba79e395bbd5bc","observation_id":"1f15667e-94d3-4b54-9937-5a71ea1b3d2b","resolution":{"observed_at":"2026-08-10T13:22:42.974002Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2010.15133","last_updated":"2021-04-29T17:36:38Z","snapshot_observed_at":"2026-07-06T10:09:30.922063Z","submitted_at":"2020-10-28T18:00:03Z","title":"RG Limit Cycles and Unconventional Fixed Points in Perturbative QFT","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.15133","snapshot_observed_at":"2026-08-10T13:22:41.979057Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.979057Z"},"links":{"cited_paper":"/paper/2010.15133","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:fbf17bae76fa281eb4dbd720b8c04210289209445788f52fd0801cbc584a07c5","observation_id":"0544db27-22d7-4e8e-a0b0-6e2874a48eaa","resolution":{"observed_at":"2026-08-10T13:22:41.979057Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.01625","last_updated":"2021-05-24T16:16:46Z","snapshot_observed_at":"2026-07-06T11:06:15.569040Z","submitted_at":"2021-05-04T17:02:10Z","title":"Homoclinic RG flows, or when relevant operators become irrelevant","version":2},"cited_work":{"arxiv_id":"2105.01625","doi":null,"metadata_source":"pith","pith_arxiv_id":"2105.01625","snapshot_observed_at":"2026-08-10T13:22:42.113115Z","title":"Homoclinic RG flows, or when relevant operators become irrelevant","venue":"hep-th","work_id":"a4dc200b-204c-4be1-ac5b-c9528825b872","year":2021},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.983717Z"},"links":{"cited_paper":"/paper/2105.01625","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:62a2b09ea8fe83b3aa4902316d31186d2efec90134bd8c5ad7970e2593cd2c95","observation_id":"1dcdc072-c612-4f1f-a441-942377b8d051","resolution":{"observed_at":"2026-08-10T13:22:42.118831Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:42.953715Z","title":"Nauenberg, Scaling representation for critical phe- nomena, Journal of Physics A: Mathematical and Gen- eral 8, 925 (1975)","venue":null,"work_id":"b1c07a0c-94d0-4888-bc5b-316d073add0f","year":1975},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.988524Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:e710a3758231b4e76d9bcc3451f2ea824a10c25804f84820cbf5d64b00133cdc","observation_id":"52f5e1b4-252a-432b-a992-264b9fddb585","resolution":{"observed_at":"2026-08-10T13:22:42.958475Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:42.939240Z","title":"Sornette and C","venue":null,"work_id":"422c3251-6c94-4db9-a5e1-0eb178c79950","year":1995},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.992957Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:aac42bc30cab34d906f45aab1a84c85df8d11e6f77ec05e19aa858b5b8f5b72a","observation_id":"e64d80ad-1209-48cd-b28e-1c9030c2509f","resolution":{"observed_at":"2026-08-10T13:22:42.943745Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2004.02888","last_updated":"2020-07-29T18:41:15Z","snapshot_observed_at":"2026-08-05T15:06:35.821023Z","submitted_at":"2020-04-06T18:00:01Z","title":"Open quantum systems and Schwinger-Keldysh holograms","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2004.02888","snapshot_observed_at":"2026-08-10T13:22:41.997409Z","title":null,"venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:41.997409Z"},"links":{"cited_paper":"/paper/2004.02888","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:d1e1a3cd55e8a5336520c88e3c81917addbe058be55b7af7b6f0743499acd945","observation_id":"e97ad0ec-5ae8-4236-b0c0-f34b97d27117","resolution":{"observed_at":"2026-08-10T13:22:41.997409Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.07683","last_updated":"2023-04-14T21:28:01Z","snapshot_observed_at":"2026-08-10T22:59:12.274702Z","submitted_at":"2022-11-14T19:01:10Z","title":"Holographic open quantum systems: Toy models and analytic properties of thermal correlators","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.07683","snapshot_observed_at":"2026-08-10T13:22:42.002893Z","title":"Loganayagam, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:42.002893Z"},"links":{"cited_paper":"/paper/2211.07683","citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:fd61f4c7acb8c616e0a03aa960754064c22753b64ba9169a1c0de97ffe8e4eaf","observation_id":"f2f32861-cd50-450b-b943-e41813da1331","resolution":{"observed_at":"2026-08-10T13:22:42.002893Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-10T13:22:42.924820Z","title":null,"venue":null,"work_id":"6ebc5028-2796-4142-8efa-d55029a90f6d","year":1966},"citing_paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-10T13:22:42.007750Z"},"links":{"citing_paper":"/paper/2501.16441"},"observation_digest":"sha256:8e9bd5a2ffb4c6ca1d9b84a9f893df701a180116c5029b326d8d1bc4b6cc099d","observation_id":"7428f1d3-68b8-4796-bd0f-4adaefefc796","resolution":{"observed_at":"2026-08-10T13:22:42.929201Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2501.16441","last_updated":"2025-01-30T00:03:39Z","latest_version":2,"primary_category":"hep-th","snapshot_observed_at":"2026-08-10T22:07:26.246686Z","submitted_at":"2025-01-27T19:03:01Z","title":"Wilsonian renormalisation group and thermal field theory in the Schwinger-Keldysh closed-time-path formalism"},"reference_resolution":{"displayed":59,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":43,"verified_exact":7,"verified_fuzzy":9},"total_outbound_references":59},"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":"2026-08-12T06:34:41.77262+00:00","source":"crossref"},{"observed_at":"2026-08-12T06:34:36.333875+00:00","source":"retraction_watch"}],"thesis":"As of 12 August 2026, this Paper Citation Record lists 59 of 59 outbound references and 3 inbound Pith citation observations for arXiv:2501.16441."}