{"as_of":"2026-08-10T09:10:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:db37d06de506b47f161cb059d85ec72ca2d376008725f8da16ae27c8fb11bf67","coverage":[{"denominator":62,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":62,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T19:04:10.557956Z","state":"measured"},{"denominator":65,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":65,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+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":"2026-08-03T19:46:45.123973Z","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":"2026-07-04T01:59:25.916628Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.07755","snapshot_observed_at":"2026-08-03T19:46:45.123973Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2511.22711","last_updated":"2026-06-18T09:41:07Z","snapshot_observed_at":"2026-08-08T04:43:52.552973Z","submitted_at":"2025-11-27T19:00:01Z","title":"Bubble velocities in local equilibrium from a pseudopotential","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-03T19:46:45.123973Z"},"links":{"cited_paper":"/paper/2507.07755","citing_paper":"/paper/2511.22711"},"observation_digest":"sha256:8881a67e64188f11cfb1cd2cc39f5291c7ca8c7bc5a06adc11cb9aabc3f9f56b","observation_id":"e253a521-8bb6-46e7-a1bf-da2272248f12","resolution":{"observed_at":"2026-08-03T19:46:45.123973Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"cited_work":{"arxiv_id":"2507.07755","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2507.07755","snapshot_observed_at":"2026-07-04T01:59:25.916628Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations,","venue":null,"work_id":"2bd58825-d292-4a7f-a468-0b129f55e2f6","year":2025},"citing_paper":{"arxiv_id":"2606.19425","last_updated":"2026-06-17T18:00:00Z","snapshot_observed_at":"2026-08-01T15:31:44.453480Z","submitted_at":"2026-06-17T18:00:00Z","title":"LeWRON: Agentic Analysis of Electroweak Phase Transitions","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-06-26T20:06:49.568135Z"},"links":{"cited_paper":"/paper/2507.07755","citing_paper":"/paper/2606.19425"},"observation_digest":"sha256:95e23a3ace286b77471c600dad6dbfd9ec69d295cbe0bb4f39f44c37367b6972","observation_id":"54991513-6a85-4a6c-8cc4-a90622f6dce1","resolution":{"observed_at":"2026-07-04T01:59:25.919925Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"cited_work":{"arxiv_id":"2507.07755","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2507.07755","snapshot_observed_at":"2026-07-04T01:59:25.916628Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations,","venue":null,"work_id":"2bd58825-d292-4a7f-a468-0b129f55e2f6","year":2025},"citing_paper":{"arxiv_id":"2607.02505","last_updated":"2026-07-02T17:58:57Z","snapshot_observed_at":"2026-08-09T21:23:34.341335Z","submitted_at":"2026-07-02T17:58:57Z","title":"A critical look at low-scale cosmological phase transitions in the PTA era","version":1},"reference_index":154,"source":"pdf_text","source_observed_at":"2026-07-03T09:23:17.300830Z"},"links":{"cited_paper":"/paper/2507.07755","citing_paper":"/paper/2607.02505"},"observation_digest":"sha256:eb89914274616f4ebd927705c0b13f60b25501fb2b9de080f6a9b1237ee3c29c","observation_id":"abd52c54-9cc5-43cb-92f1-86c329b0157b","resolution":{"observed_at":"2026-07-03T09:27:48.622224Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/2507.07755/citation-record","integrity":"/paper/2507.07755/integrity","json":"/paper/2507.07755/citation-record.json","paper":"/paper/2507.07755"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"1910.13125","last_updated":"2021-01-12T09:42:19Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2019-10-29T07:58:57Z","title":"Detecting gravitational waves from cosmological phase transitions with LISA: an update","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.13125","snapshot_observed_at":"2026-08-06T19:04:02.086902Z","title":"Caprini et al, Detecting gravitational waves from cosmological phase tra nsitions with LISA: an update, JCAP 03 (2020) 024 [1910.13125]","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:02.086902Z"},"links":{"cited_paper":"/paper/1910.13125","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:df6b6411993b6075f87a43b9588d32024f552440849c0c60ca0bbbbf69dae530","observation_id":"f9f82877-f5a5-48f8-bd65-33b79b8bd43b","resolution":{"observed_at":"2026-08-06T19:04:02.086902Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.07294","last_updated":"2021-11-05T19:24:43Z","snapshot_observed_at":"2026-08-06T16:46:07.307400Z","submitted_at":"2020-09-15T18:00:07Z","title":"Baryogenesis from the weak scale to the grand unification scale","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.07294","snapshot_observed_at":"2026-08-06T19:04:02.194508Z","title":"B¨ odeker and W","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:02.194508Z"},"links":{"cited_paper":"/paper/2009.07294","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:b39b0d5124f4f19d42c13294b651cb7a8f19585193933a1fc79a5d4047327d71","observation_id":"5c8df582-ab18-4ec8-b77d-dd395fd48393","resolution":{"observed_at":"2026-08-06T19:04:02.194508Z","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":"2026-08-06T19:04:02.347721Z","title":"Hindmarsh, M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:02.347721Z"},"links":{"cited_paper":"/paper/2008.09136","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:b62db9a02557bb2ca910d2d8d522003d04ce9d7ea8b96849329dfe483de1f43f","observation_id":"11020215-73e5-469f-a5e8-9aaa51ada402","resolution":{"observed_at":"2026-08-06T19:04:02.347721Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9605288","last_updated":"1996-05-12T15:53:42Z","snapshot_observed_at":"2026-07-07T04:22:39.163372Z","submitted_at":"1996-05-12T15:53:42Z","title":"Is There a Hot Electroweak Phase Transition at $m_H\\gsim m_W$?","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9605288","snapshot_observed_at":"2026-08-06T19:04:02.477819Z","title":"Kajantie, M","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:02.477819Z"},"links":{"cited_paper":"/paper/hep-ph/9605288","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:b12a8e1d9895b2664c2bf4bb9404e919f84ead648f065fbc29e56dcd7b383e6a","observation_id":"d26f6f78-83fc-4042-9df8-9a6174b34a30","resolution":{"observed_at":"2026-08-06T19:04:02.477819Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9208227","last_updated":"1992-08-14T21:16:48Z","snapshot_observed_at":"2026-07-07T04:14:32.134799Z","submitted_at":"1992-08-14T21:16:48Z","title":"Two Stage Phase Transition in Two Higgs Models","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9208227","snapshot_observed_at":"2026-08-06T19:04:02.625095Z","title":"Land and E.D","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:02.625095Z"},"links":{"cited_paper":"/paper/hep-ph/9208227","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:7261b0634e4410c7f76f26fd17b5b18f0ed89616c475bc5565fd85e6e544047d","observation_id":"c3835a65-efba-4d53-92ab-789571d04726","resolution":{"observed_at":"2026-08-06T19:04:02.625095Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9612364","last_updated":"1996-12-15T13:06:28Z","snapshot_observed_at":"2026-07-07T04:24:34.027083Z","submitted_at":"1996-12-15T13:06:28Z","title":"The 2-loop MSSM finite temperature effective potential with stop condensation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9612364","snapshot_observed_at":"2026-08-06T19:04:02.762267Z","title":"B¨ odeker, P","venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:02.762267Z"},"links":{"cited_paper":"/paper/hep-ph/9612364","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:9ab006dfa8f3843fa9bafb4a1af2e0a8e18607b7f1f6b42e6aa3521a3c7166be","observation_id":"b8e54253-e5a8-4088-b921-404e99d403b2","resolution":{"observed_at":"2026-08-06T19:04:02.762267Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9902220","last_updated":"1999-03-11T22:28:34Z","snapshot_observed_at":"2026-07-07T04:32:03.911882Z","submitted_at":"1999-02-02T17:14:08Z","title":"Was the Electroweak Phase Transition Preceded by a Color-Broken Phase?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9902220","snapshot_observed_at":"2026-08-06T19:04:02.909088Z","title":"Cline, G.D","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:02.909088Z"},"links":{"cited_paper":"/paper/hep-ph/9902220","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:3fbdf2b78e06b1315b9a398ca75d56611a3006042d05c7e8c20889c20ffb799d","observation_id":"e17284ef-afd5-40f3-b467-5adaa811ad4d","resolution":{"observed_at":"2026-08-06T19:04:02.909088Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0705.2425","last_updated":"2007-08-23T23:21:48Z","snapshot_observed_at":"2026-07-06T01:28:00.990743Z","submitted_at":"2007-05-17T18:06:00Z","title":"Singlet Higgs Phenomenology and the Electroweak Phase Transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0705.2425","snapshot_observed_at":"2026-08-06T19:04:03.069318Z","title":"Profumo, M.J","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:03.069318Z"},"links":{"cited_paper":"/paper/0705.2425","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:67bf48b6cdca4a8ed3a52cbf9f0dfa3ea004d82594e39f42b7b1f92ec00f7343","observation_id":"8a4ab253-abcf-4059-8059-f502b403e5a2","resolution":{"observed_at":"2026-08-06T19:04:03.069318Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1107.5441","last_updated":"2011-07-27T11:09:25Z","snapshot_observed_at":"2026-08-10T07:30:48.827268Z","submitted_at":"2011-07-27T11:09:25Z","title":"Strong Electroweak Phase Transitions in the Standard Model with a Singlet","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.5441","snapshot_observed_at":"2026-08-06T19:04:03.218286Z","title":"Espinosa, T","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:03.218286Z"},"links":{"cited_paper":"/paper/1107.5441","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:143f03f43878ae983391693af7a3bf8118a4d1befe5b260edfa1bd9d7ccb9c1c","observation_id":"0c285893-9e83-4de6-ba4c-b0c5b362bfb9","resolution":{"observed_at":"2026-08-06T19:04:03.218286Z","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":"2026-08-06T19:04:14.905325Z","title":"Landau and E.M","venue":null,"work_id":"b8c47a4c-ade7-42f7-8838-e1ff2adb3332","year":null},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:03.383368Z"},"links":{"citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:a35716e50686c8918af649d82a56d6baa8e63b7a6e64206dbfe043e45e5b8f10","observation_id":"42052aa8-1369-400c-b295-b292e77bc3f6","resolution":{"observed_at":"2026-08-06T19:04:14.995920Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T19:04:14.613452Z","title":"Enqvist, J","venue":null,"work_id":"88ea08c2-6ba8-45ef-9a08-783dcef398c9","year":1992},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:03.541743Z"},"links":{"citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:840b2c376ddb4fc349c290c20ecd83595adf61b70325452e5dc95d5d26949b03","observation_id":"ebfdb3a9-34d8-4098-a492-efcab00556be","resolution":{"observed_at":"2026-08-06T19:04:14.736594Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T19:04:14.351340Z","title":"Landau and E.M","venue":null,"work_id":"ce286fb4-c211-4f47-9196-00c45224a641","year":null},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:03.680532Z"},"links":{"citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:c935dcff96bf0b4ac01aaa67ed99420e16349203cddce5ddf72e48f2cf4441c2","observation_id":"1a9220ca-9ffb-4d30-a937-3496396f6b97","resolution":{"observed_at":"2026-08-06T19:04:14.473364Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"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":"2026-08-06T19:04:03.817819Z","title":"Ignatius, K","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:03.817819Z"},"links":{"cited_paper":"/paper/astro-ph/9309059","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:fc4fdddb476137bcf91f3898bb45b343b3c2cf2d4d8d62ef787cd8d65d0e0c96","observation_id":"91127d5c-e7c7-4168-a496-131b669128f1","resolution":{"observed_at":"2026-08-06T19:04:03.817819Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.05871","last_updated":"2020-04-15T14:58:21Z","snapshot_observed_at":"2026-08-09T17:33:20.066113Z","submitted_at":"2017-04-19T18:08:03Z","title":"Shape of the acoustic gravitational wave power spectrum from a first order phase transition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.05871","snapshot_observed_at":"2026-08-06T19:04:03.945011Z","title":"Hindmarsh, S.J","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:03.945011Z"},"links":{"cited_paper":"/paper/1704.05871","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:eda628c26eacf58c343fd0fd35db6642822f0a2255b403b32f7b306d0eb70343","observation_id":"cef2bf20-20c5-4490-a5a8-3e49a8f3b898","resolution":{"observed_at":"2026-08-06T19:04:03.945011Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.05826","last_updated":"2024-11-13T13:22:52Z","snapshot_observed_at":"2026-07-06T18:42:56.281402Z","submitted_at":"2024-07-08T11:10:25Z","title":"Primordial acoustic turbulence: three-dimensional simulations and gravitational wave predictions","version":2},"cited_work":{"arxiv_id":"2407.05826","doi":null,"metadata_source":"pith","pith_arxiv_id":"2407.05826","snapshot_observed_at":"2026-08-06T19:04:12.874043Z","title":"Primordial acoustic turbulence: three-dimensional simulations and gravitational wave predictions","venue":"gr-qc","work_id":"be23773b-4d14-47cb-856a-53fdca208592","year":2024},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:04.125438Z"},"links":{"cited_paper":"/paper/2407.05826","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:6121e3472453a620b5f69ca149af79e71d64c020a000b9749f12551e6cb65af8","observation_id":"a63789d5-0e20-4247-bc08-7021a161459c","resolution":{"observed_at":"2026-08-06T19:04:13.009890Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9607382","last_updated":"1996-08-01T07:47:15Z","snapshot_observed_at":"2026-07-07T04:23:14.515335Z","submitted_at":"1996-07-22T03:59:11Z","title":"Real-Time History of the Cosmological Electroweak Phase Transition","version":2},"cited_work":{"arxiv_id":"hep-ph/9607382","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9607382","snapshot_observed_at":"2026-08-06T19:04:12.659765Z","title":"Real-Time History of the Cosmological Electroweak Phase Transition","venue":"hep-ph","work_id":"09309da0-1daa-440c-8cd7-b7cf85c2e720","year":1996},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:04.240202Z"},"links":{"cited_paper":"/paper/hep-ph/9607382","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:21965c3e71731a14c557c7f520b9eb8a1f51d17fcdbacd9682825cda01f957d5","observation_id":"ad873ad4-b281-48bb-9655-4cb91424749a","resolution":{"observed_at":"2026-08-06T19:04:12.777815Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T19:04:14.090159Z","title":"Kurki-Suonio, Deﬂagration bubbles in the quark-hadron phase transition, Nucl","venue":null,"work_id":"2e75a3dd-0926-40a0-b48c-411ee663197f","year":1985},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:04.345255Z"},"links":{"citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:506f0270a9156eb88fd8d207fe1b634f83c062f8ff56ebafc6cf01fccef07615","observation_id":"07b6fa50-3e10-4bfc-b0fc-726f1d73619a","resolution":{"observed_at":"2026-08-06T19:04:14.219636Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9309242","last_updated":"1993-09-08T05:03:22Z","snapshot_observed_at":"2026-07-07T04:16:01.492229Z","submitted_at":"1993-09-08T05:03:22Z","title":"Bubble Growth as a Detonation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9309242","snapshot_observed_at":"2026-08-06T19:04:04.460329Z","title":"Laine, Bubble growth as a detonation, Phys","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:04.460329Z"},"links":{"cited_paper":"/paper/hep-ph/9309242","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:6e5c11df2531db926a90637b272b22795d7b3f6bac3ec42bf1e19559a9750503","observation_id":"e2f6877a-8cf3-4e16-9503-caab12b9fa32","resolution":{"observed_at":"2026-08-06T19:04:04.460329Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9501216","last_updated":"1995-01-05T12:57:08Z","snapshot_observed_at":"2026-07-07T04:18:52.280884Z","submitted_at":"1995-01-05T12:57:08Z","title":"Supersonic Deflagrations in Cosmological Phase Transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9501216","snapshot_observed_at":"2026-08-06T19:04:04.593979Z","title":"Kurki-Suonio and M","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:04.593979Z"},"links":{"cited_paper":"/paper/hep-ph/9501216","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:39dd9e00ebed1421f2bc52194a6b2b60e235a64b5136b6c0bd92c02507ddde4b","observation_id":"f5658484-3eca-49bc-8a73-3a593aab5464","resolution":{"observed_at":"2026-08-06T19:04:04.593979Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.08215","last_updated":"2017-05-12T18:56:59Z","snapshot_observed_at":"2026-08-06T23:46:00.165669Z","submitted_at":"2017-03-23T19:51:47Z","title":"Electroweak Bubble Wall Speed Limit","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.08215","snapshot_observed_at":"2026-08-06T19:04:04.704601Z","title":"B¨ odeker and G.D","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:04.704601Z"},"links":{"cited_paper":"/paper/1703.08215","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:7138cb3decdd36acbdac2a2406273585cd837a941cfb35efacb863e2d541dbac","observation_id":"602ed4c1-1d92-45dc-8c17-784807e32eb7","resolution":{"observed_at":"2026-08-06T19:04:04.704601Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.10343","last_updated":"2021-03-16T10:03:22Z","snapshot_observed_at":"2026-08-09T14:32:56.911620Z","submitted_at":"2020-07-20T18:00:01Z","title":"Towards an all-orders calculation of the electroweak bubble wall velocity","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.10343","snapshot_observed_at":"2026-08-06T19:04:04.841042Z","title":"H¨ oche, J","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:04.841042Z"},"links":{"cited_paper":"/paper/2007.10343","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:1f023dce92f0216d8e43b5e7653b283e6cfeaa884215466affaa2b0ee079bb1c","observation_id":"a65cc6d8-3aed-4a50-8175-3f6fcaf8d33f","resolution":{"observed_at":"2026-08-06T19:04:04.841042Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.02590","last_updated":"2020-11-26T12:17:38Z","snapshot_observed_at":"2026-08-10T06:38:35.330029Z","submitted_at":"2020-10-06T10:00:44Z","title":"Bubble wall velocity: heavy physics effects","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.02590","snapshot_observed_at":"2026-08-06T19:04:04.954835Z","title":"Azatov and M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:04.954835Z"},"links":{"cited_paper":"/paper/2010.02590","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:2ab324ed6e8098c310c3613afacce3938c616d9e9289cad9ab471f9f7437db80","observation_id":"ed3309a7-a453-47ba-8280-5ec8211f7118","resolution":{"observed_at":"2026-08-06T19:04:04.954835Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.12903","last_updated":"2020-11-25T17:39:37Z","snapshot_observed_at":"2026-08-10T02:07:07.276740Z","submitted_at":"2020-11-25T17:39:37Z","title":"Bubble wall velocity beyond leading-log approximation in electroweak phase transition","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.12903","snapshot_observed_at":"2026-08-06T19:04:05.067450Z","title":"Wang, F.P","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:05.067450Z"},"links":{"cited_paper":"/paper/2011.12903","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:5a018c38943805c8d2f9f1b63440f8a6b0332f03a8aad4c0c440eaff40e61614","observation_id":"964a7e5e-5fbb-4682-9cfa-10c0292f63d3","resolution":{"observed_at":"2026-08-06T19:04:05.067450Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.07686","last_updated":"2022-07-14T14:04:23Z","snapshot_observed_at":"2026-08-09T21:56:10.195949Z","submitted_at":"2021-12-14T19:00:02Z","title":"Friction pressure on relativistic bubble walls","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.07686","snapshot_observed_at":"2026-08-06T19:04:05.185890Z","title":"Gouttenoire, R","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:05.185890Z"},"links":{"cited_paper":"/paper/2112.07686","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:710f1417dd0975849e5dbdef65f4b4d154694ac03a517b657862fdcdbada45d3","observation_id":"ebc1b436-bfac-4d02-8351-e2c0bc712cb0","resolution":{"observed_at":"2026-08-06T19:04:05.185890Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.13120","last_updated":"2022-04-27T18:00:01Z","snapshot_observed_at":"2026-08-07T04:23:35.530243Z","submitted_at":"2022-04-27T18:00:01Z","title":"First principles determination of bubble wall velocity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.13120","snapshot_observed_at":"2026-08-06T19:04:05.335969Z","title":"Laurent and J.M","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:05.335969Z"},"links":{"cited_paper":"/paper/2204.13120","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:4ae85ff719647989a45d1b419e5c3c242d5536f41c9524e4f2e0f55685ab6d57","observation_id":"de451042-7633-486c-943c-40ad5caf13ab","resolution":{"observed_at":"2026-08-06T19:04:05.335969Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.10679","last_updated":"2023-10-19T17:45:37Z","snapshot_observed_at":"2026-07-06T16:08:29.285279Z","submitted_at":"2023-08-21T12:26:18Z","title":"Logarithmically divergent friction on ultrarelativistic bubble walls","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.10679","snapshot_observed_at":"2026-08-06T19:04:05.465676Z","title":"Ai, Logarithmic divergent friction on ultrarelativistic bubb le walls, JCAP 10 (2023) 052 [2308.10679]","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:05.465676Z"},"links":{"cited_paper":"/paper/2308.10679","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:9f6f1d3cc4539ac584373eb59b2f97c31b9a463c539349e9414e37ae4570d2c5","observation_id":"4f5ecbfc-cb04-432b-9808-1df93e1f4b35","resolution":{"observed_at":"2026-08-06T19:04:05.465676Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.06972","last_updated":"2024-07-13T10:30:47Z","snapshot_observed_at":"2026-07-06T16:30:46.321160Z","submitted_at":"2023-10-10T19:51:43Z","title":"Quantisation Across Bubble Walls and Friction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.06972","snapshot_observed_at":"2026-08-06T19:04:05.600745Z","title":"Azatov, G","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:05.600745Z"},"links":{"cited_paper":"/paper/2310.06972","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:41a1114e05e967247f56d83c3d0cc982eeb3078ff35c40977d088de727f0ca17","observation_id":"dd902c36-c4c6-452e-8346-307f17931c10","resolution":{"observed_at":"2026-08-06T19:04:05.600745Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.13522","last_updated":"2024-01-24T15:18:22Z","snapshot_observed_at":"2026-07-06T17:19:56.099931Z","submitted_at":"2024-01-24T15:18:22Z","title":"Non-linearities in cosmological bubble wall dynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.13522","snapshot_observed_at":"2026-08-06T19:04:05.758974Z","title":"De Curtis, L","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:05.758974Z"},"links":{"cited_paper":"/paper/2401.13522","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:54d5e341552dbf163912f6d37ef6a8435a2da09544d1f61e9e36050d78ea0639","observation_id":"abacd337-2927-4063-8204-d47a714ff3d3","resolution":{"observed_at":"2026-08-06T19:04:05.758974Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.18196","last_updated":"2024-11-04T14:07:55Z","snapshot_observed_at":"2026-08-05T15:39:08.120494Z","submitted_at":"2024-07-25T16:59:38Z","title":"Thermal pressure on ultrarelativistic bubbles from a semiclassical formalism","version":2},"cited_work":{"arxiv_id":"2407.18196","doi":null,"metadata_source":"pith","pith_arxiv_id":"2407.18196","snapshot_observed_at":"2026-08-06T19:04:12.247039Z","title":"Thermal pressure on ultrarelativistic bubbles from a semiclassical formalism","venue":"hep-ph","work_id":"e60b24d7-5a90-40ef-a4f3-b5ce0c41a36b","year":2024},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:05.935947Z"},"links":{"cited_paper":"/paper/2407.18196","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:2266ea3d37d1e32c581b489de205635db65478ee2cc43a48c10bd41dd69875b4","observation_id":"aae8339b-4339-4f70-bb56-b5b118e63914","resolution":{"observed_at":"2026-08-06T19:04:12.334250Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.04970","last_updated":"2024-11-07T18:46:31Z","snapshot_observed_at":"2026-08-02T11:06:51.034205Z","submitted_at":"2024-11-07T18:46:31Z","title":"How fast does the WallGo? A package for computing wall velocities in first-order phase transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.04970","snapshot_observed_at":"2026-08-06T19:04:06.080318Z","title":"Ekstedt, O","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:06.080318Z"},"links":{"cited_paper":"/paper/2411.04970","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:26627fa632f59234c4ac47ed1984fccb33b320e36868931120fea88ae80d7e3f","observation_id":"c4c3cd27-3f44-4721-8bdf-c3f10bdaf0ef","resolution":{"observed_at":"2026-08-06T19:04:06.080318Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.13724","last_updated":"2026-06-01T05:43:16Z","snapshot_observed_at":"2026-08-07T16:01:06.473396Z","submitted_at":"2025-04-18T14:50:01Z","title":"Bubble wall velocity from Kadanoff-Baym equations: fluid dynamics and microscopic interactions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.13724","snapshot_observed_at":"2026-08-06T19:04:06.241213Z","title":"Ramsey-Musolf and J","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:06.241213Z"},"links":{"cited_paper":"/paper/2504.13724","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:fcaaf766b924a9c7fffc124e9a700c5ba4fef9c60ea153486b2a689d30c90c12","observation_id":"2edc3cb1-0906-44c5-afca-3bcf18241441","resolution":{"observed_at":"2026-08-06T19:04:06.241213Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-07T16:01:06.637971Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.13725","snapshot_observed_at":"2026-08-06T19:04:06.363253Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:06.363253Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:b217f99305679eed458bb16c4ed6e946d91b01ca6766ddc0d2539df830030cce","observation_id":"07541e47-1d06-4553-8ccf-091d4519ae5e","resolution":{"observed_at":"2026-08-06T19:04:06.363253Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1011.3735","last_updated":"2011-02-23T13:31:07Z","snapshot_observed_at":"2026-07-06T02:19:18.766120Z","submitted_at":"2010-11-16T15:42:20Z","title":"Hydrodynamic obstruction to bubble expansion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1011.3735","snapshot_observed_at":"2026-08-06T19:04:06.545218Z","title":"Konstandin and J.M","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:06.545218Z"},"links":{"cited_paper":"/paper/1011.3735","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:71fcf72371862eda533b9e2c2241c1aba98bedeaa32659f43910c4fc3f8224f3","observation_id":"7696fab7-7c53-4811-a7df-b8ac08468a92","resolution":{"observed_at":"2026-08-06T19:04:06.545218Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2005.10875","last_updated":"2021-01-12T09:32:30Z","snapshot_observed_at":"2026-08-03T14:48:11.309871Z","submitted_at":"2020-05-21T20:00:17Z","title":"Field-theoretic derivation of bubble-wall force","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2005.10875","snapshot_observed_at":"2026-08-06T19:04:06.677100Z","title":"Barroso Mancha, T","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:06.677100Z"},"links":{"cited_paper":"/paper/2005.10875","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:26eb4a99f1e24468c235d8b1888cdc7129f6e018ca0f3dd2344b073636cc2194","observation_id":"ffe32ec9-5c3d-417c-b73c-0eb92b88de86","resolution":{"observed_at":"2026-08-06T19:04:06.677100Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.08013","last_updated":"2021-03-18T19:28:43Z","snapshot_observed_at":"2026-08-10T07:33:16.261184Z","submitted_at":"2020-10-15T20:45:51Z","title":"Cosmological bubble friction in local equilibrium","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.08013","snapshot_observed_at":"2026-08-06T19:04:06.824685Z","title":"Balaji, M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:06.824685Z"},"links":{"cited_paper":"/paper/2010.08013","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:30ded503c0b94047d770768ba72ec0aa85abf821c56ceada7a4527b928eb4c25","observation_id":"92b1209f-80ab-418e-a9fb-06d3075ab35b","resolution":{"observed_at":"2026-08-06T19:04:06.824685Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.13710","last_updated":"2022-03-07T18:25:08Z","snapshot_observed_at":"2026-08-09T17:30:04.172217Z","submitted_at":"2021-09-28T13:29:16Z","title":"Bubble wall velocities in local equilibrium","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.13710","snapshot_observed_at":"2026-08-06T19:04:06.979514Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:06.979514Z"},"links":{"cited_paper":"/paper/2109.13710","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:3d2678e24c4ffc79131911adf05709c8d30cecad430785a78c85d9b295c8d1fb","observation_id":"36732501-1315-4e9a-be61-7a03510b5af2","resolution":{"observed_at":"2026-08-06T19:04:06.979514Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.02492","last_updated":"2023-01-30T01:48:26Z","snapshot_observed_at":"2026-08-09T03:00:34.381633Z","submitted_at":"2022-05-05T08:02:24Z","title":"Hydrodynamic backreaction force of cosmological bubble expansion","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.02492","snapshot_observed_at":"2026-08-06T19:04:07.071954Z","title":"Wang and Z.Y","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:07.071954Z"},"links":{"cited_paper":"/paper/2205.02492","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:55aa4e030687d0f4ce8a2f61dd99e3639d56e658d6ba16816b340950fdc213b9","observation_id":"2ae4fbf5-927a-4259-b8ce-5d992857947e","resolution":{"observed_at":"2026-08-06T19:04:07.071954Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.10171","last_updated":"2023-07-04T15:43:07Z","snapshot_observed_at":"2026-08-10T06:22:17.579002Z","submitted_at":"2023-03-17T17:59:58Z","title":"Model-independent bubble wall velocities in local thermal equilibrium","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.10171","snapshot_observed_at":"2026-08-06T19:04:07.168723Z","title":null,"venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:07.168723Z"},"links":{"cited_paper":"/paper/2303.10171","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:1e45e9c283f7b310060e685a8a978576d1e0527bfe8406c8530a962b8cb3dc23","observation_id":"9a48b2e2-f243-4ec3-b8c8-1fafd3d8d6b5","resolution":{"observed_at":"2026-08-06T19:04:07.168723Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.18216","last_updated":"2024-02-26T10:17:06Z","snapshot_observed_at":"2026-07-06T15:10:37.557445Z","submitted_at":"2023-03-31T17:16:40Z","title":"Hydrodynamical constraints on bubble wall velocity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.18216","snapshot_observed_at":"2026-08-06T19:04:07.271313Z","title":"Krajewski, M","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:07.271313Z"},"links":{"cited_paper":"/paper/2303.18216","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:a2d1b65ee0c76a3697c67fc805c090fa83870a77842abcfa0a396103b0603132","observation_id":"5c0852fa-06ef-4f6b-9d25-3af3243e548e","resolution":{"observed_at":"2026-08-06T19:04:07.271313Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.05911","last_updated":"2024-03-13T19:04:55Z","snapshot_observed_at":"2026-07-06T17:14:19.624035Z","submitted_at":"2024-01-11T13:41:46Z","title":"Criterion for ultra-fast bubble walls: the impact of hydrodynamic obstruction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.05911","snapshot_observed_at":"2026-08-06T19:04:07.354880Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:07.354880Z"},"links":{"cited_paper":"/paper/2401.05911","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:72c910dc22a34e0d14fa6eb185726cd3515d9a0fdc9f699d6e4f303f553e7601","observation_id":"3edabc27-4ef7-4cc4-a1b5-302a6d4a2a7c","resolution":{"observed_at":"2026-08-06T19:04:07.354880Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.13641","last_updated":"2025-02-24T16:06:40Z","snapshot_observed_at":"2026-08-10T01:22:35.786562Z","submitted_at":"2024-11-20T19:00:00Z","title":"Bounds on the bubble wall velocity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.13641","snapshot_observed_at":"2026-08-06T19:04:07.531208Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:07.531208Z"},"links":{"cited_paper":"/paper/2411.13641","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:80819ac03c7f234bf3df44682d225fe69499e87ca1cfdbee9a3284d830f9e7db","observation_id":"8cba5f88-bfc4-43c9-b6a7-9f50c6d81aed","resolution":{"observed_at":"2026-08-06T19:04:07.531208Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.16580","last_updated":"2025-07-28T11:17:17Z","snapshot_observed_at":"2026-07-06T19:56:39.115630Z","submitted_at":"2024-11-25T17:12:09Z","title":"Steady-state bubbles beyond local thermal equilibrium","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.16580","snapshot_observed_at":"2026-08-06T19:04:07.684602Z","title":"Krajewski, M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:07.684602Z"},"links":{"cited_paper":"/paper/2411.16580","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:30c0ec29338d948b3a274f94f17d39f13e10b0c40c0d9e8c93bca107f1282ed7","observation_id":"f6369e74-f75e-41cd-8ea1-b0a520461a90","resolution":{"observed_at":"2026-08-06T19:04:07.684602Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.17841","last_updated":"2025-08-16T20:16:35Z","snapshot_observed_at":"2026-08-07T22:10:09.566160Z","submitted_at":"2025-04-24T18:00:00Z","title":"The Discriminant Power of Bubble Wall Velocities: Gravitational Waves and Electroweak Baryogenesis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.17841","snapshot_observed_at":"2026-08-06T19:04:07.823834Z","title":"Carena, A","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:07.823834Z"},"links":{"cited_paper":"/paper/2504.17841","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:406a06c7257f6f41953f405674f76ce17f99c7d21d894e41ba20c780c33a3e34","observation_id":"9e594e08-febd-4cfe-9101-e73ec8359c81","resolution":{"observed_at":"2026-08-06T19:04:07.823834Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.21213","last_updated":"2025-08-06T10:43:05Z","snapshot_observed_at":"2026-08-07T15:58:01.534749Z","submitted_at":"2025-04-29T22:48:13Z","title":"Electroweak Phase Transition and Bubble Wall Velocity in Local Thermal Equilibrium","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.21213","snapshot_observed_at":"2026-08-06T19:04:07.950966Z","title":"Branchina, A","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:07.950966Z"},"links":{"cited_paper":"/paper/2504.21213","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:038931361a20802e692604a2ec602d9b8df676fc9d6e0db09bd2aed61114a139","observation_id":"a368f03a-b596-4a86-8dd4-0a50b534aeca","resolution":{"observed_at":"2026-08-06T19:04:07.950966Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.19584","last_updated":"2025-09-04T02:09:36Z","snapshot_observed_at":"2026-08-09T15:33:57.402808Z","submitted_at":"2025-05-26T06:56:24Z","title":"The Bubble Wall Velocity in Local Thermal Equilibrium and Energy Budget with Full Effective Potential","version":2},"cited_work":{"arxiv_id":"2505.19584","doi":null,"metadata_source":"pith","pith_arxiv_id":"2505.19584","snapshot_observed_at":"2026-08-06T19:04:11.858726Z","title":"The Bubble Wall Velocity in Local Thermal Equilibrium and Energy Budget with Full Effective Potential","venue":"hep-ph","work_id":"a4eeea4b-d734-4dee-9933-0e69547a11f0","year":2025},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:08.120508Z"},"links":{"cited_paper":"/paper/2505.19584","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:ba59702860f512a153e2616f0a958ac4c0ec8dd828f0e72187aba15f2130aa7b","observation_id":"1c3d44da-7d1e-4bcf-98ca-390f2d278d1d","resolution":{"observed_at":"2026-08-06T19:04:11.957228Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T19:04:13.772207Z","title":"Lifshitz and L.P","venue":null,"work_id":"79a68b44-d211-402d-ac11-c908fb4d4e0c","year":null},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:08.233630Z"},"links":{"citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:3a596dee3aa233dcc9a1a14d459b0e9ba942edae0b8e4db4ab71608969cb3b85","observation_id":"992cfad3-ee2e-4c78-8a27-7aa8d753e11d","resolution":{"observed_at":"2026-08-06T19:04:13.959297Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1803.01871","last_updated":"2018-04-26T13:01:51Z","snapshot_observed_at":"2026-07-06T06:26:44.471172Z","submitted_at":"2018-03-05T19:00:27Z","title":"Hydrodynamic fluctuations from a weakly coupled scalar field","version":2},"cited_work":{"arxiv_id":"1803.01871","doi":null,"metadata_source":"pith","pith_arxiv_id":"1803.01871","snapshot_observed_at":"2026-08-06T19:04:11.604515Z","title":"Hydrodynamic fluctuations from a weakly coupled scalar field","venue":"hep-ph","work_id":"5f63eb4e-39e8-43bd-9c13-8555e7ca10b3","year":2018},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:08.423274Z"},"links":{"cited_paper":"/paper/1803.01871","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:187580b34d15e53d5f2c024ff85978b9b27b6a4ec698d40e10b0111481cdd4ab","observation_id":"31309a88-8bad-47fc-a3da-ff50d1e00849","resolution":{"observed_at":"2026-08-06T19:04:11.734757Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1104.1586","last_updated":"2011-04-08T14:36:40Z","snapshot_observed_at":"2026-07-06T02:26:03.723768Z","submitted_at":"2011-04-08T14:36:40Z","title":"The stickiness of sound: An absolute lower limit on viscosity and the breakdown of second order relativistic hydrodynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1104.1586","snapshot_observed_at":"2026-08-06T19:04:08.583197Z","title":"Kovtun, G.D","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:08.583197Z"},"links":{"cited_paper":"/paper/1104.1586","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:e74ddc6c0e093dbb39d10863874b975f22fbd8c4936052c0d86c8560d04ae255","observation_id":"a3962e6a-d336-4d79-9c4c-65092cbf820b","resolution":{"observed_at":"2026-08-06T19:04:08.583197Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9212224","last_updated":"1992-12-10T23:33:20Z","snapshot_observed_at":"2026-07-07T04:14:51.399626Z","submitted_at":"1992-12-05T00:57:10Z","title":"Hydrodynamic Stability Analysis of Burning Bubbles in Electroweak Theory and in QCD","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9212224","snapshot_observed_at":"2026-08-06T19:04:08.717866Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:08.717866Z"},"links":{"cited_paper":"/paper/hep-ph/9212224","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:0835994ea97ea01805038be3efd9e0ecd46b94ddfde1da7cfe5317d3b13d14ae","observation_id":"6d6e03be-0aaa-426f-9ae3-5d4a01912604","resolution":{"observed_at":"2026-08-06T19:04:08.717866Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.07331","last_updated":"2022-09-30T08:02:27Z","snapshot_observed_at":"2026-08-09T14:41:21.076481Z","submitted_at":"2022-01-18T21:54:26Z","title":"Bubble Nucleation to All Orders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.07331","snapshot_observed_at":"2026-08-06T19:04:08.823929Z","title":"Ekstedt, Bubble nucleation to all orders, JHEP 08 (2022) 115 [2201.07331]","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:08.823929Z"},"links":{"cited_paper":"/paper/2201.07331","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:c1bbd49bfbb6a384b001663164214391c7efc58d3307403c5e71a3e21ab81431","observation_id":"3b45e3a1-5829-46d4-95a0-4b5e0e9b618e","resolution":{"observed_at":"2026-08-06T19:04:08.823929Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.05075","last_updated":"2024-11-07T19:00:14Z","snapshot_observed_at":"2026-07-06T19:47:03.132530Z","submitted_at":"2024-11-07T19:00:14Z","title":"Bubble-wall speed with loop corrections","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.05075","snapshot_observed_at":"2026-08-06T19:04:08.946225Z","title":"Dashko and A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:08.946225Z"},"links":{"cited_paper":"/paper/2411.05075","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:59a1e6d8abfb0f0ccc3efae930e207d1911566b2a7961c6a74066aaa52ab396c","observation_id":"0501721f-f9fd-4f64-b405-4a9302c860d9","resolution":{"observed_at":"2026-08-06T19:04:08.946225Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.17074","last_updated":"2024-10-17T05:48:26Z","snapshot_observed_at":"2026-08-09T16:27:06.601135Z","submitted_at":"2024-07-24T08:03:43Z","title":"Evolution of coupled scalar perturbations through smooth reheating. I. Dissipative regime","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.17074","snapshot_observed_at":"2026-08-06T19:04:09.109157Z","title":"Laine, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:09.109157Z"},"links":{"cited_paper":"/paper/2407.17074","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:b541351032b6284593e6c053865c16d1d20764a293301f51a40cdb63bbb0f393","observation_id":"2b9ff095-f24c-412a-905d-4d748ab0b64d","resolution":{"observed_at":"2026-08-06T19:04:09.109157Z","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":"2026-08-06T19:04:13.520531Z","title":"Carrington, Eﬀective potential at ﬁnite temperature in the Standard Mod el, Phys","venue":null,"work_id":"a04d843b-bfa9-4c27-a757-aa9a0f94acd1","year":1992},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:09.286157Z"},"links":{"citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:278b591c9aa93e9b071ae2f28d1a809d8c99057db75f8585f33849086673cc07","observation_id":"ede68814-a59a-4251-903a-ff9aabddb05a","resolution":{"observed_at":"2026-08-06T19:04:13.628889Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9204228","last_updated":"1992-04-23T00:17:51Z","snapshot_observed_at":"2026-07-07T04:14:16.305741Z","submitted_at":"1992-04-23T00:17:51Z","title":"Phase Transition Temperatures at Next-to-Leading Order","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9204228","snapshot_observed_at":"2026-08-06T19:04:09.427362Z","title":"Arnold, Phase transition temperatures at next-to-leading order, Phys","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:09.427362Z"},"links":{"cited_paper":"/paper/hep-ph/9204228","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:681a5cb9f27a0d63d23450d12c7ac7bd451b5a36dc8c731eb423d1b2afa817ad","observation_id":"8fd43dbf-9194-45bd-a1cb-449af20676c9","resolution":{"observed_at":"2026-08-06T19:04:09.427362Z","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":"2026-08-06T19:04:13.272967Z","title":"Linde, Infrared problem in thermodynamics of the Yang-Mills gas, Phys","venue":null,"work_id":"652c63b6-5217-4cbc-b207-156388faa2a2","year":1980},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:09.531490Z"},"links":{"citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:08923e5b4ce446a88dafb53631e23b93688fafe8b87a186cbae0ca707fdf47b1","observation_id":"47b29991-b234-4cde-8351-d48975685afc","resolution":{"observed_at":"2026-08-06T19:04:13.361000Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0512177","last_updated":"2006-03-14T10:05:42Z","snapshot_observed_at":"2026-07-07T04:09:41.622044Z","submitted_at":"2005-12-14T09:46:01Z","title":"Pressure of the Standard Model Near the Electroweak Phase Transition","version":2},"cited_work":{"arxiv_id":"hep-ph/0512177","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0512177","snapshot_observed_at":"2026-08-06T19:04:11.320653Z","title":"Pressure of the Standard Model Near the Electroweak Phase Transition","venue":"hep-ph","work_id":"d29d714c-c627-4536-85da-fe5f415b6c41","year":2005},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:09.676988Z"},"links":{"cited_paper":"/paper/hep-ph/0512177","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:816edcbd525ab5853d5f55eb4a5846ef8735c6ab1ed3af30f75534999763c931","observation_id":"52fc1670-fb98-4f69-ac64-2b464bb39274","resolution":{"observed_at":"2026-08-06T19:04:11.417324Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1503.04935","last_updated":"2015-07-23T12:35:10Z","snapshot_observed_at":"2026-07-06T04:12:14.505853Z","submitted_at":"2015-03-17T06:37:44Z","title":"Standard Model thermodynamics across the electroweak crossover","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.04935","snapshot_observed_at":"2026-08-06T19:04:09.788632Z","title":"Laine and M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:09.788632Z"},"links":{"cited_paper":"/paper/1503.04935","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:8073ae6d3b8fefd2874952ea1c5c3e1118944d01339cad3e5af7f0d76ea71163","observation_id":"6133e981-3d95-468a-9dd3-dd4da7fb8926","resolution":{"observed_at":"2026-08-06T19:04:09.788632Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.01672","last_updated":"2023-09-04T15:35:50Z","snapshot_observed_at":"2026-08-06T01:49:20.256519Z","submitted_at":"2023-09-04T15:35:50Z","title":"Perturbative effective field theory expansions for cosmological phase transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.01672","snapshot_observed_at":"2026-08-06T19:04:09.960142Z","title":"Gould and T.V.I","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:09.960142Z"},"links":{"cited_paper":"/paper/2309.01672","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:17d135a3a033d5de4620e9628e3c160ec28adf89f8436431959da58ed8115567","observation_id":"368eb95e-a3c0-45e0-ac9e-748195214ab6","resolution":{"observed_at":"2026-08-06T19:04:09.960142Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9603339","last_updated":"1996-03-19T09:17:36Z","snapshot_observed_at":"2026-07-07T04:22:15.203297Z","submitted_at":"1996-03-19T09:17:36Z","title":"Damping Rate and Lyapunov Exponent of a Higgs Field at High Temperature","version":1},"cited_work":{"arxiv_id":"hep-ph/9603339","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9603339","snapshot_observed_at":"2026-08-06T19:04:10.984810Z","title":"Damping Rate and Lyapunov Exponent of a Higgs Field at High Temperature","venue":"hep-ph","work_id":"2219eb68-c797-4d2b-880d-9e7b58ccf9a7","year":1996},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:10.110461Z"},"links":{"cited_paper":"/paper/hep-ph/9603339","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:3627428ffb58253a7de453694993e42a3f38ce803b198928c51f020d2e077f70","observation_id":"b0cd70bc-87a5-4c3e-a1e1-96d8309e4711","resolution":{"observed_at":"2026-08-06T19:04:11.139128Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2404.06116","last_updated":"2024-06-14T11:18:23Z","snapshot_observed_at":"2026-07-06T17:57:40.022710Z","submitted_at":"2024-04-09T08:38:54Z","title":"Soft contributions to the thermal Higgs width across an electroweak phase transition","version":2},"cited_work":{"arxiv_id":"2404.06116","doi":null,"metadata_source":"pith","pith_arxiv_id":"2404.06116","snapshot_observed_at":"2026-08-06T19:04:10.716023Z","title":"Soft contributions to the thermal Higgs width across an electroweak phase transition","venue":"hep-ph","work_id":"e9350b8e-2d74-4b66-917e-7a4f391a26f6","year":2024},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:10.244165Z"},"links":{"cited_paper":"/paper/2404.06116","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:ef5e02569fb4b9bfe2352f6b2e725fb56b3f1d3c5e53ab11360ff9cc3160bf01","observation_id":"892b3656-7e9f-4a47-b219-3efe87ad6f96","resolution":{"observed_at":"2026-08-06T19:04:10.844074Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2210.11710","last_updated":"2022-12-13T16:29:16Z","snapshot_observed_at":"2026-08-06T18:09:22.440455Z","submitted_at":"2022-10-21T03:40:36Z","title":"Gravitational wave background from vacuum and thermal fluctuations during axion-like inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.11710","snapshot_observed_at":"2026-08-06T19:04:10.375843Z","title":"Klose, M","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:10.375843Z"},"links":{"cited_paper":"/paper/2210.11710","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:33f4b994b0944596e14f6ef1266c2e6d4048c120e02119f8215786019e547642","observation_id":"0a14bd8c-a846-4bfb-91c7-3e319545180e","resolution":{"observed_at":"2026-08-06T19:04:10.375843Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.4099","last_updated":"2009-07-31T13:52:44Z","snapshot_observed_at":"2026-08-03T06:27:01.579261Z","submitted_at":"2009-03-24T15:24:24Z","title":"Can electroweak bubble walls run away?","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.4099","snapshot_observed_at":"2026-08-06T19:04:10.557956Z","title":"B¨ odeker and G.D","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-06T19:04:10.557956Z"},"links":{"cited_paper":"/paper/0903.4099","citing_paper":"/paper/2507.07755"},"observation_digest":"sha256:25c7501fe16292f07778c02d522cb83ae5904a9a7df6ff648c2036a6ed2f0cdf","observation_id":"a6d488f5-3250-4cef-b771-5e1f072f405c","resolution":{"observed_at":"2026-08-06T19:04:10.557956Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2507.07755","last_updated":"2025-09-11T08:01:09Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-09T04:48:42.490522Z","submitted_at":"2025-07-10T13:34:05Z","title":"Entropy production at electroweak bubble walls from scalar field fluctuations"},"reference_resolution":{"displayed":62,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":47,"verified_exact":8,"verified_fuzzy":7},"total_outbound_references":62},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 62 of 62 outbound references and 3 inbound Pith citation observations for arXiv:2507.07755."}