{"as_of":"2026-08-08T19:35:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6bf69e995a1cec67f6d4152a8ae4f3d5d88965147539df2d3d3509995f9a4cc6","coverage":[{"denominator":38,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":38,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T11:38:10.190091Z","state":"measured"},{"denominator":39,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":39,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-08T06:32:00.761636+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T17:14:13.767856Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"pith","source_observed_at":"2026-08-06T17:14:16.948671Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"cited_work":{"arxiv_id":"2502.07879","doi":null,"metadata_source":"pith","pith_arxiv_id":"2502.07879","snapshot_observed_at":"2026-08-06T17:14:16.948671Z","title":"Phase transitions in an expanding medium -- hot remnants","venue":"hep-th","work_id":"38cc5a5c-5205-4ccb-91a8-c0ccad2a128d","year":2025},"citing_paper":{"arxiv_id":"2507.11622","last_updated":"2026-07-03T07:50:04Z","snapshot_observed_at":"2026-08-06T19:19:02.311579Z","submitted_at":"2025-07-15T18:01:37Z","title":"Testing the effective action approach to bubble nucleation in holography","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T17:14:13.767856Z"},"links":{"cited_paper":"/paper/2502.07879","citing_paper":"/paper/2507.11622"},"observation_digest":"sha256:9112b6aa2c85f76095dc52b75066989c0c5222c7cc79109df1bb414d6a3c0efd","observation_id":"b3de8db3-253a-4a7c-b505-c0db048a13c5","resolution":{"observed_at":"2026-08-06T17:14:16.955001Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2502.07879/citation-record","integrity":"/paper/2502.07879/integrity","json":"/paper/2502.07879/citation-record.json","paper":"/paper/2502.07879"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2106.02642","last_updated":"2021-06-23T12:42:15Z","snapshot_observed_at":"2026-07-06T11:16:06.357384Z","submitted_at":"2021-06-04T18:00:00Z","title":"A simple description of holographic domain walls in confining theories -- extended hydrodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.02642","snapshot_observed_at":"2026-08-08T11:38:10.020983Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.020983Z"},"links":{"cited_paper":"/paper/2106.02642","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:548aefa8abccc8ce6e7f0fcd3d20e87f5015df25602f651177e92c0707b9bd45","observation_id":"4b33c233-0164-4592-a8d2-ac6a2944447b","resolution":{"observed_at":"2026-08-08T11:38:10.020983Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9803131","last_updated":"1998-04-07T18:29:30Z","snapshot_observed_at":"2026-07-07T05:16:12.441340Z","submitted_at":"1998-03-16T22:35:39Z","title":"Anti-de Sitter Space, Thermal Phase Transition, And Confinement In Gauge Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9803131","snapshot_observed_at":"2026-08-08T11:38:10.027027Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.027027Z"},"links":{"cited_paper":"/paper/hep-th/9803131","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:eb12c4263846b9b6770badd6d17f60719234ec7a13381f0240e12635be28e75a","observation_id":"cf1f940d-e654-4ece-8bab-516835a69091","resolution":{"observed_at":"2026-08-08T11:38:10.027027Z","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":"2026-08-08T11:38:10.753129Z","title":"high energy","venue":null,"work_id":"d9e330e5-88c8-42cd-8a4f-6dc12c65c1b2","year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.008318Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:2d2268b9a5966e6333c6132d3f0f94ad18f82913f134d501535aaf9d9d0df4c8","observation_id":"43a687af-1d8c-420b-8c27-b93b59a7d0bd","resolution":{"observed_at":"2026-08-08T11:38:10.757563Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0507219","last_updated":"2005-10-20T17:32:59Z","snapshot_observed_at":"2026-08-03T01:11:09.109102Z","submitted_at":"2005-07-22T07:45:37Z","title":"Plasma-balls in large N gauge theories and localized black holes","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0507219","snapshot_observed_at":"2026-08-08T11:38:10.032000Z","title":"Aharony, S","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.032000Z"},"links":{"cited_paper":"/paper/hep-th/0507219","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:74ad48d2315948bc2830740a7582bfbb85c61513580133c29ae7c5d959e5f60e","observation_id":"4a1eaaa6-2903-401f-9a2d-e6c7b47cd170","resolution":{"observed_at":"2026-08-08T11:38:10.032000Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0604161","last_updated":"2006-06-07T07:15:05Z","snapshot_observed_at":"2026-07-07T04:57:17.922142Z","submitted_at":"2006-04-24T15:16:08Z","title":"A holographic model of deconfinement and chiral symmetry restoration","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0604161","snapshot_observed_at":"2026-08-08T11:38:10.037030Z","title":"Aharony, J","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.037030Z"},"links":{"cited_paper":"/paper/hep-th/0604161","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:5a145aee44aa2df85ab6e23eb71acd5355859603cfd73b2f52bc0c641fbdab55","observation_id":"d94f010c-7a24-433a-b0c6-4aa2eb606fd3","resolution":{"observed_at":"2026-08-08T11:38:10.037030Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0804.0899","last_updated":"2008-10-25T08:52:55Z","snapshot_observed_at":"2026-08-05T19:57:11.895023Z","submitted_at":"2008-04-07T17:25:24Z","title":"Deconfinement and Gluon Plasma Dynamics in Improved Holographic QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0804.0899","snapshot_observed_at":"2026-08-08T11:38:10.042038Z","title":"Gursoy, E","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.042038Z"},"links":{"cited_paper":"/paper/0804.0899","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:9e5c740be0b2f6ca7cf03bdd520718e28ceed73e55ab88b6f8c19531e48dc698","observation_id":"8435d125-fd24-421f-a803-8bcdf9a80a54","resolution":{"observed_at":"2026-08-08T11:38:10.042038Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0812.0792","last_updated":"2009-05-08T21:54:12Z","snapshot_observed_at":"2026-07-06T01:48:49.072219Z","submitted_at":"2008-12-03T20:11:42Z","title":"Holography and Thermodynamics of 5D Dilaton-gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0812.0792","snapshot_observed_at":"2026-08-08T11:38:10.047086Z","title":"Gursoy, E","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.047086Z"},"links":{"cited_paper":"/paper/0812.0792","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:84e78fa0c55ad5f79fdd143d9e0507390d4ad31789ad4ac6ae0c34766a9f8c60","observation_id":"2038fbb8-a369-415f-bf6e-28ccf3e0b268","resolution":{"observed_at":"2026-08-08T11:38:10.047086Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1501.06379","last_updated":"2015-03-26T11:12:44Z","snapshot_observed_at":"2026-07-06T04:07:15.490023Z","submitted_at":"2015-01-26T13:14:25Z","title":"Quantum and stringy corrections to the equation of state of holographic QCD matter and the nature of the chiral transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1501.06379","snapshot_observed_at":"2026-08-08T11:38:10.051987Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.051987Z"},"links":{"cited_paper":"/paper/1501.06379","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:c437a92e0d131fdb4fa5a3000d89882f1fdfa21fd4486e6220ad53ec9972a716","observation_id":"306928f2-32e5-4b85-bee1-89fd1b593e9d","resolution":{"observed_at":"2026-08-08T11:38:10.051987Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.05652","last_updated":"2018-05-14T17:03:13Z","snapshot_observed_at":"2026-08-05T09:04:34.862824Z","submitted_at":"2018-02-15T16:44:55Z","title":"Holographic Anisotropic Background with Confinement-Deconfinement Phase Transition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.05652","snapshot_observed_at":"2026-08-08T11:38:10.057024Z","title":"Aref’eva and K","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.057024Z"},"links":{"cited_paper":"/paper/1802.05652","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:24783958b85b30a6863282a8c65deb990a800a30a107f04523d2f802474d7a7a","observation_id":"b9a04ac7-84e9-40c7-8f33-367892d19f0b","resolution":{"observed_at":"2026-08-08T11:38:10.057024Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.05708","last_updated":"2022-03-17T20:18:50Z","snapshot_observed_at":"2026-08-05T23:50:42.603880Z","submitted_at":"2021-04-12T17:59:46Z","title":"Bubble Wall Velocity from Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.05708","snapshot_observed_at":"2026-08-08T11:38:10.061818Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.061818Z"},"links":{"cited_paper":"/paper/2104.05708","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:6178a537052df5c579c498050ddfbc115e072c754f96c4919dd6795f45fd668d","observation_id":"10b99e84-e2eb-4203-bc29-e79834b9dea2","resolution":{"observed_at":"2026-08-08T11:38:10.061818Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.05476","last_updated":"2020-05-12T16:42:23Z","snapshot_observed_at":"2026-08-07T14:12:06.502882Z","submitted_at":"2020-01-15T18:40:50Z","title":"Real-time Dynamics of Plasma Balls from Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.05476","snapshot_observed_at":"2026-08-08T11:38:10.067051Z","title":"Bantilan, P","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.067051Z"},"links":{"cited_paper":"/paper/2001.05476","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:555c13382fb9a6c5938ef3a008022df6b32eca0520ea4f3fa8784d7ea39a6c8c","observation_id":"ee31dcd0-2f36-41e8-b2a8-d072f7c3f6af","resolution":{"observed_at":"2026-08-08T11:38:10.067051Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.02579","last_updated":"2020-08-06T11:18:08Z","snapshot_observed_at":"2026-07-06T09:45:01.182512Z","submitted_at":"2020-08-06T11:18:08Z","title":"Fate of false vacua in holographic first-order phase transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.02579","snapshot_observed_at":"2026-08-08T11:38:10.071789Z","title":"Bigazzi, A","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.071789Z"},"links":{"cited_paper":"/paper/2008.02579","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:4a5dd292319552f400996b9d6fa8ef25e32802e62f1420dfc29a2742031a3276","observation_id":"ba1ab656-361f-4d57-923a-b34abfd5c170","resolution":{"observed_at":"2026-08-08T11:38:10.071789Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.08757","last_updated":"2021-01-22T16:12:43Z","snapshot_observed_at":"2026-08-06T01:55:03.958697Z","submitted_at":"2020-11-17T16:35:49Z","title":"Dark Holograms and Gravitational Waves","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.08757","snapshot_observed_at":"2026-08-08T11:38:10.076345Z","title":"Bigazzi, A","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.076345Z"},"links":{"cited_paper":"/paper/2011.08757","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:f365e28f3dff839c84a911b4af8f4ecc8691d9145e2d2d70bc68abd56379f3fe","observation_id":"6538e041-09d1-4097-b858-8b38dd8eb6ae","resolution":{"observed_at":"2026-08-08T11:38:10.076345Z","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":"2026-08-08T11:38:10.080839Z","title":null,"venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.080839Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:ab4744aa6760fb7ede3e44729a744dc436d0262e8bbe1c2f61863ace736257ad","observation_id":"4c003943-bcad-4c5b-8b2f-2ecd58a6dd02","resolution":{"observed_at":"2026-08-08T11:38:10.080839Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9309059","last_updated":"1993-09-30T14:11:07Z","snapshot_observed_at":"2026-08-03T23:24:29.621657Z","submitted_at":"1993-09-30T14:11:07Z","title":"The Growth of Bubbles in Cosmological Phase Transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9309059","snapshot_observed_at":"2026-08-08T11:38:10.085285Z","title":"Ignatius, K","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.085285Z"},"links":{"cited_paper":"/paper/astro-ph/9309059","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:63b740ea6ce1a3f981f2b1291198fa99baa277df6d2722cdaad37129740017b9","observation_id":"fa36a79a-0738-416d-bb2a-2a0df3b8aa11","resolution":{"observed_at":"2026-08-08T11:38:10.085285Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.03291","last_updated":"2016-01-07T12:36:12Z","snapshot_observed_at":"2026-08-04T03:47:54.114346Z","submitted_at":"2015-04-13T18:45:28Z","title":"Numerical simulations of acoustically generated gravitational waves at a first order phase transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.03291","snapshot_observed_at":"2026-08-08T11:38:10.089919Z","title":"Hindmarsh, S","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.089919Z"},"links":{"cited_paper":"/paper/1504.03291","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:571a3e49dce3eb2cd78a408ad978a38676f8417408a6334edb4c0e15bcc641e4","observation_id":"38519c61-224c-4fba-8bbf-7323603f81f7","resolution":{"observed_at":"2026-08-08T11:38:10.089919Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.06274","last_updated":"2022-05-12T18:00:01Z","snapshot_observed_at":"2026-07-06T13:09:25.356940Z","submitted_at":"2022-05-12T18:00:01Z","title":"A perfect fluid hydrodynamic picture of domain wall velocities at strong coupling","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.06274","snapshot_observed_at":"2026-08-08T11:38:10.094321Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.094321Z"},"links":{"cited_paper":"/paper/2205.06274","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:85a8fa62fb1dc6756c152c3c934ecf3954efb7cb3d98f594f12b2db6fc612cf1","observation_id":"9b9ca03d-5e3e-4a14-8545-624a890c3ff9","resolution":{"observed_at":"2026-08-08T11:38:10.094321Z","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":"2026-08-08T11:38:10.098736Z","title":null,"venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.098736Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:1ec0aea03344af9d98d42cfbd791ec7e0711a6408d412253e31bb85f571068c6","observation_id":"58ecf530-c7c0-4e12-ac9e-bd41c2d1be2c","resolution":{"observed_at":"2026-08-08T11:38:10.098736Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0512162","last_updated":"2005-12-20T16:06:23Z","snapshot_observed_at":"2026-07-07T04:56:09.320065Z","submitted_at":"2005-12-14T14:56:22Z","title":"Asymptotic perfect fluid dynamics as a consequence of AdS/CFT","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0512162","snapshot_observed_at":"2026-08-08T11:38:10.103065Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.103065Z"},"links":{"cited_paper":"/paper/hep-th/0512162","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:28c817851011c175ba10a68ea12a8b9895908bbbdd303a1c56e90c556d6d29c1","observation_id":"818a8845-b3d2-49d5-ae34-6dfc29e0bedf","resolution":{"observed_at":"2026-08-08T11:38:10.103065Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0906.4426","last_updated":"2009-07-20T23:05:51Z","snapshot_observed_at":"2026-08-03T17:51:55.246189Z","submitted_at":"2009-06-24T08:28:42Z","title":"Boost invariant flow, black hole formation, and far-from-equilibrium dynamics in N = 4 supersymmetric Yang-Mills theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0906.4426","snapshot_observed_at":"2026-08-08T11:38:10.107624Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.107624Z"},"links":{"cited_paper":"/paper/0906.4426","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:21505f534aa68bea8bed112db076f0632fa1df9a66025c8237905c0432aca24a","observation_id":"5f34bd98-08e1-41fd-9d76-9ba29a1a6877","resolution":{"observed_at":"2026-08-08T11:38:10.107624Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1103.3452","last_updated":"2012-06-12T08:38:47Z","snapshot_observed_at":"2026-07-06T02:24:59.568746Z","submitted_at":"2011-03-17T16:25:06Z","title":"The characteristics of thermalization of boost-invariant plasma from holography","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1103.3452","snapshot_observed_at":"2026-08-08T11:38:10.112006Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.112006Z"},"links":{"cited_paper":"/paper/1103.3452","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:44ea6a32a68a9f57594fd2c21107dac705a83e88a7784d27fe7fabdaa61e95c3","observation_id":"afc24430-1bb6-4677-bcdf-b5e435eb6fca","resolution":{"observed_at":"2026-08-08T11:38:10.112006Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1302.0697","last_updated":"2013-05-24T09:25:26Z","snapshot_observed_at":"2026-07-06T03:05:35.277694Z","submitted_at":"2013-02-04T14:16:27Z","title":"Hydrodynamic gradient expansion in gauge theory plasmas","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1302.0697","snapshot_observed_at":"2026-08-08T11:38:10.116284Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.116284Z"},"links":{"cited_paper":"/paper/1302.0697","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:3110a8d0b62459a62a884ad35bc7b29c4fbac5857f9d0cf76d9450823ba6595e","observation_id":"d66afd47-5b9b-44a5-a413-235b26265b7c","resolution":{"observed_at":"2026-08-08T11:38:10.116284Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.08628","last_updated":"2015-07-30T18:58:02Z","snapshot_observed_at":"2026-07-06T04:25:24.625762Z","submitted_at":"2015-07-30T18:58:02Z","title":"Late time behavior of non-conformal plasmas","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.08628","snapshot_observed_at":"2026-08-08T11:38:10.120871Z","title":"Gursoy, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.120871Z"},"links":{"cited_paper":"/paper/1507.08628","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:a198cf80da55eadd768e40782c5fb8d460e9160528b8972f9aaac91b04a35bb2","observation_id":"62f6f53c-04e9-40c9-ace2-06ef900fe46f","resolution":{"observed_at":"2026-08-08T11:38:10.120871Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.17806","last_updated":"2025-01-09T15:00:43Z","snapshot_observed_at":"2026-07-06T19:57:33.013839Z","submitted_at":"2024-11-26T19:00:01Z","title":"Cosmic censorship in a (dual) collider","version":2},"cited_work":{"arxiv_id":"2411.17806","doi":null,"metadata_source":"pith","pith_arxiv_id":"2411.17806","snapshot_observed_at":"2026-08-08T11:38:10.334078Z","title":"Cosmic censorship in a (dual) collider","venue":"hep-th","work_id":"6cdcd716-d098-4a04-9fd5-bc173ded9bfd","year":2024},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.125585Z"},"links":{"cited_paper":"/paper/2411.17806","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:96a84f71b85e7dcc40a3a52dfee5e33696293b92664733c13fba58ea6fad4491","observation_id":"22f254cd-307d-40b2-8ca8-753547998558","resolution":{"observed_at":"2026-08-08T11:38:10.339869Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2302.10042","last_updated":"2023-11-13T14:30:31Z","snapshot_observed_at":"2026-07-06T14:53:42.192162Z","submitted_at":"2023-02-20T15:45:06Z","title":"Bubble expansion at strong coupling","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.10042","snapshot_observed_at":"2026-08-08T11:38:10.130300Z","title":"Li, S.-J","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.130300Z"},"links":{"cited_paper":"/paper/2302.10042","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:69a5cc83d866671c8e8115ad68c11e1a773f6b20df85f5fda68d795c18b9e209","observation_id":"c46ea9f2-c0dc-4ab5-9132-6416efab04c6","resolution":{"observed_at":"2026-08-08T11:38:10.130300Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.07347","last_updated":"2024-05-11T16:26:11Z","snapshot_observed_at":"2026-07-06T16:46:34.235227Z","submitted_at":"2023-11-13T14:05:20Z","title":"General bubble expansion at strong coupling","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.07347","snapshot_observed_at":"2026-08-08T11:38:10.134790Z","title":"Wang, Z.-Y","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.134790Z"},"links":{"cited_paper":"/paper/2311.07347","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:008adab4c8814b4c603cce50fe694802591fe912c9fa33ce9284a8a0b08d46b2","observation_id":"3d622be3-6d7b-40bc-9048-3e5fecb57718","resolution":{"observed_at":"2026-08-08T11:38:10.134790Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.13420","last_updated":"2021-10-04T16:24:08Z","snapshot_observed_at":"2026-08-07T00:30:38.648517Z","submitted_at":"2021-04-27T18:35:23Z","title":"Continuity equations for general matter: applications in numerical relativity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.13420","snapshot_observed_at":"2026-08-08T11:38:10.139832Z","title":"Clough, Continuity equations for general matter: ap- plications in numerical relativity, Class","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.139832Z"},"links":{"cited_paper":"/paper/2104.13420","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:50fae2dcb80a7cc4219d5f408e225630dcb0bb21d88c29528df900b4070a1c4d","observation_id":"a730da96-7497-461a-8ced-c705661a5652","resolution":{"observed_at":"2026-08-08T11:38:10.139832Z","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":"10.1103/physrevlett.130.251001","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T11:38:10.218765Z","title":"Ecker, E","venue":null,"work_id":"50652375-35d5-4599-97c6-8cea6654201d","year":2023},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.144392Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:43cbc5c686b0a886bee56a087db4fa1fee01dd957b18ab07408b2827124ef4cf","observation_id":"d0e5d757-3806-49c6-84fa-66d7ea17b801","resolution":{"observed_at":"2026-08-08T11:38:10.224862Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1906.00480","last_updated":"2020-07-19T13:26:57Z","snapshot_observed_at":"2026-08-08T03:35:10.249210Z","submitted_at":"2019-06-02T20:44:40Z","title":"Vorticity, kinetic energy, and suppressed gravitational wave production in strong first order phase transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.00480","snapshot_observed_at":"2026-08-08T11:38:10.148963Z","title":"Cutting, M","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.148963Z"},"links":{"cited_paper":"/paper/1906.00480","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:49c1bade9c1fd11703fb2f9b89851f030b87486287aa5a079f85497d95fab888","observation_id":"f70c5979-2a09-4538-9dc7-b2df58803785","resolution":{"observed_at":"2026-08-08T11:38:10.148963Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.03396","last_updated":"2023-01-03T07:20:23Z","snapshot_observed_at":"2026-07-06T12:57:51.108636Z","submitted_at":"2022-04-07T12:33:22Z","title":"Droplet collapse during strongly supercooled transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.03396","snapshot_observed_at":"2026-08-08T11:38:10.153605Z","title":"Cutting, E","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.153605Z"},"links":{"cited_paper":"/paper/2204.03396","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:2b86eb9a6e1e6aee4d7654a5b0925e41a6ae455646072e46520e58abd4364001","observation_id":"29e04bbe-635f-48e0-8a16-5b7934dfb5ed","resolution":{"observed_at":"2026-08-08T11:38:10.153605Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.09136","last_updated":"2021-05-25T10:45:23Z","snapshot_observed_at":"2026-08-04T15:40:04.004736Z","submitted_at":"2020-08-20T18:01:05Z","title":"Phase transitions in the early universe","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.09136","snapshot_observed_at":"2026-08-08T11:38:10.158270Z","title":"domain wall","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.158270Z"},"links":{"cited_paper":"/paper/2008.09136","citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:6bf87fdf2733c5f4716586dcf05dee7c43bd6f53704edd19e39289c7a26a149e","observation_id":"272ff8a5-dc1a-4436-a582-b27ccce54215","resolution":{"observed_at":"2026-08-08T11:38:10.158270Z","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":"2026-08-08T11:38:10.728725Z","title":"We replaced factors of1/(1 − γ) in the equations of motion by(1−γ)/[(1−γ)2 +εγ]","venue":null,"work_id":"e2d02942-0095-4f33-9944-f22692e24744","year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.163357Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:03665c5080c0f79f317b580dee8e05f4b45fab9ee7d4a4dca1c9b77fee75b082","observation_id":"e50d10a0-e0e6-4e12-a45c-a069c72e375e","resolution":{"observed_at":"2026-08-08T11:38:10.733474Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-08T11:38:10.712519Z","title":"We replaced non-integer powers of Ts by regulated expressions, e.g.,T f (γ) s by (T 2 s + εT )f (γ)/2","venue":null,"work_id":"fbc9efb4-0325-4ccd-8f82-5cdf083f5a34","year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.168261Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:ea69845b86f081d301e44dc75a1524b98cad61f81b5523ca1b9e645586c7b1bb","observation_id":"219b81c6-1be6-48a2-b338-0cf92a0113be","resolution":{"observed_at":"2026-08-08T11:38:10.718155Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-08T11:38:10.697186Z","title":"We replaced factors of1/J by J/(J 2 + εJ )","venue":null,"work_id":"36f9f2d7-4236-4e92-9289-5d1b68c980fb","year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.172511Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:64adb916ad60d4b6a03c69716c2e365c9d2bc714c0255ef63e4f351f4224c6cf","observation_id":"d6c8482a-6d43-4137-b10d-dca7753c3d9a","resolution":{"observed_at":"2026-08-08T11:38:10.701717Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-08T11:38:10.682407Z","title":"The velocity and the time derivative ofγ were set to zero initially","venue":null,"work_id":"8d0438e1-7487-4f06-8c6f-6323a1fecb0c","year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.177079Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:7be792cc7dadc152091408d20774e5319a9e32096d9327fb5c4ef6bf5348fcdd","observation_id":"a3d30f9e-4e97-48cc-9f98-29804a3d235e","resolution":{"observed_at":"2026-08-08T11:38:10.687243Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-08T11:38:10.666812Z","title":"That is, γ was chosen to be nonzero only for|x| ≲ 30, with the blob limited by smooth tanh steps hav- ing widths equal to one","venue":null,"work_id":"8f5773ae-51c0-4c60-bd46-67016bd6b1f1","year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.181412Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:41248ebc982113293c51639cd13017990188a428537e0c96b8f80ce1bc2dfb02","observation_id":"eaff40b6-dfde-431a-85c4-f665600bd90a","resolution":{"observed_at":"2026-08-08T11:38:10.671707Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-08T11:38:10.651389Z","title":"Profiles were chosen similarly to the second simulation, but we added also an initial velocity profile (i.e.,θ) corre- sponding to a uniformly shrinking blob","venue":null,"work_id":"fd010ea7-cdeb-4bc4-be2f-ebaee89b4988","year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.185587Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:c9fdd6be907c2169183aae0a93759ba2d41e7e820085a2ee740fc7d95adfcf30","observation_id":"36c937d0-eb5e-463f-abfb-274731052fcb","resolution":{"observed_at":"2026-08-08T11:38:10.656386Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+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":"2026-08-08T11:38:10.636043Z","title":"This width was chosen to see better the effect of the decaying γ profile","venue":null,"work_id":"66f6b4d7-0f3b-40a4-abb9-379bfec4c6e3","year":null},"citing_paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-08T11:38:10.190091Z"},"links":{"citing_paper":"/paper/2502.07879"},"observation_digest":"sha256:46edd46f2044a5e3a3aab746e6c426137b7d90f7438a6f710e566ba831a9e46e","observation_id":"687272b8-bc9c-445f-b373-851ee6a7b075","resolution":{"observed_at":"2026-08-08T11:38:10.640921Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2502.07879","last_updated":"2025-03-06T15:25:23Z","latest_version":2,"primary_category":"hep-th","snapshot_observed_at":"2026-08-08T11:30:07.761453Z","submitted_at":"2025-02-11T19:00:01Z","title":"Phase transitions in an expanding medium -- hot remnants"},"reference_resolution":{"displayed":38,"state_counts":{"malformed_identifier":0,"metadata_mismatch":1,"parse_uncertain":0,"unresolved":28,"verified_exact":1,"verified_fuzzy":8},"total_outbound_references":38},"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":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"thesis":"As of 8 August 2026, this Paper Citation Record lists 38 of 38 outbound references and 1 inbound Pith citation observation for arXiv:2502.07879."}