{"as_of":"2026-08-20T21:32:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:f85203315ef3fee96b6721682aeada7cbda3bfb6f75bd5b8662d1123b5c592ba","coverage":[{"denominator":138,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-16T12:08:29.226088Z","state":"measured"},{"denominator":112,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":112,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-20T06:33:59.587034+00:00","state":"measured"},{"denominator":12,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":12,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-16T05:18:13.446696Z","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":"2026-07-04T01:59:25.531352Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","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":"2026-08-16T05:18:13.446696Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.21213","last_updated":"2025-08-06T10:43:05Z","snapshot_observed_at":"2026-08-16T16:55:45.877645Z","submitted_at":"2025-04-29T22:48:13Z","title":"Electroweak Phase Transition and Bubble Wall Velocity in Local Thermal Equilibrium","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-16T05:18:13.446696Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2504.21213"},"observation_digest":"sha256:e8d6112b76fda35e862646778b16b9b023a1ee35fe1dfc52b61bc31ef931507e","observation_id":"b4bb2f70-e08c-40da-aa07-f1a4a61cd3b6","resolution":{"observed_at":"2026-08-16T05:18:13.446696Z","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":"2026-08-17T21:27:10.939039Z","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":"2026-08-07T14:18:45.865266Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.19584","last_updated":"2025-09-04T02:09:36Z","snapshot_observed_at":"2026-08-17T23:20:15.636640Z","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},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-07T14:18:45.865266Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2505.19584"},"observation_digest":"sha256:db4680f9a217923fbb1018d431dc936445c60e514d4064eae589c6c2a2c14cea","observation_id":"27b37cf5-e628-4f58-9659-67d76d5ad3e4","resolution":{"observed_at":"2026-08-07T14:18:45.865266Z","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":"2026-08-17T21:27:10.939039Z","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":"2026-08-06T19:51:30.632376Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.04799","last_updated":"2025-07-07T09:18:46Z","snapshot_observed_at":"2026-08-13T22:27:30.254762Z","submitted_at":"2025-07-07T09:18:46Z","title":"The Domain Wall String's Anti-Stokes Scattering Cross Section","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-06T19:51:30.632376Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2507.04799"},"observation_digest":"sha256:5dd222921a6b708068cada7238014cc9e8593714eed52187f252d0f12ec6a1b9","observation_id":"f2fe6984-efb7-4685-aa8e-432c3c3ca1f2","resolution":{"observed_at":"2026-08-06T19:51:30.632376Z","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":"2026-08-17T21:27:10.939039Z","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":"2026-08-13T06:02:05.874493Z","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":"sha256:3dd8338730c49d6d46d023f1fb187620b22fa005b4a18e8ab809a7a68138c424","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":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","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":"2026-08-03T19:46:45.167810Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2511.22711","last_updated":"2026-06-18T09:41:07Z","snapshot_observed_at":"2026-08-17T07:06:04.559453Z","submitted_at":"2025-11-27T19:00:01Z","title":"Bubble velocities in local equilibrium from a pseudopotential","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-03T19:46:45.167810Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2511.22711"},"observation_digest":"sha256:4a232d6bdfeee600f873924b13661ca0cd680501e976d229c3ae4180f48eb499","observation_id":"4c989591-cd2e-4779-a672-e0a440db50aa","resolution":{"observed_at":"2026-08-03T19:46:45.167810Z","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":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"cited_work":{"arxiv_id":"2504.13725","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2504.13725","snapshot_observed_at":"2026-07-04T01:59:25.531352Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory,","venue":null,"work_id":"dd299ad8-3ab6-4e69-9484-33e239c1cfb3","year":2025},"citing_paper":{"arxiv_id":"2604.17383","last_updated":"2026-04-19T11:17:31Z","snapshot_observed_at":"2026-08-08T19:39:54.799925Z","submitted_at":"2026-04-19T11:17:31Z","title":"Hydrodynamics of Filtered Dark Matter: A Two-Component Approach","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-05-10T05:50:48.902560Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2604.17383"},"observation_digest":"sha256:7033627f3215bb3282d29a5f2e0a0ec4aa19d3e9a7bfda203aed15498eb4610c","observation_id":"24b6d773-7646-4280-80c0-5418a2048c2d","resolution":{"observed_at":"2026-05-10T05:51:09.700800Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-20T06:33:59.587034+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"cited_work":{"arxiv_id":"2504.13725","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2504.13725","snapshot_observed_at":"2026-07-04T01:59:25.531352Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory,","venue":null,"work_id":"dd299ad8-3ab6-4e69-9484-33e239c1cfb3","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":73,"source":"pdf_text","source_observed_at":"2026-06-26T20:06:49.568135Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2606.19425"},"observation_digest":"sha256:57b420df7ebb9585f5493a857dab9299d17300b8398ccdc83dcfec564608b605","observation_id":"23533079-7c22-4d4e-b5f4-c46272f08fa6","resolution":{"observed_at":"2026-07-04T01:59:25.533972Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-20T06:33:59.587034+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"cited_work":{"arxiv_id":"2504.13725","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2504.13725","snapshot_observed_at":"2026-07-04T01:59:25.531352Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory,","venue":null,"work_id":"dd299ad8-3ab6-4e69-9484-33e239c1cfb3","year":2025},"citing_paper":{"arxiv_id":"2606.30740","last_updated":"2026-06-29T18:00:07Z","snapshot_observed_at":"2026-07-07T00:04:34.491408Z","submitted_at":"2026-06-29T18:00:07Z","title":"Dynamical evolution of the pressure on the bubble wall","version":1},"reference_index":129,"source":"pdf_text","source_observed_at":"2026-07-01T02:04:55.907846Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2606.30740"},"observation_digest":"sha256:d84622f7046c3195c43294bbbdaecc3b48e1f2cacbdac83bf6018554fe5ee60b","observation_id":"9237b9c0-5bd6-412f-ab75-dad96786e91e","resolution":{"observed_at":"2026-07-01T12:25:43.965772Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-20T06:33:59.587034+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","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":"2026-08-02T00:54:44.284872Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.14867","last_updated":"2026-07-16T11:41:51Z","snapshot_observed_at":"2026-08-16T16:56:27.562097Z","submitted_at":"2026-07-16T11:41:51Z","title":"Thermal Masses and Bubble-Wall Friction in Cosmological Phase Transitions","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-02T00:54:44.284872Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2607.14867"},"observation_digest":"sha256:2d33238f808cb327e83cee797474b27370712574b40119c6ecb49a7b9a819339","observation_id":"1fc259d7-46b0-41ca-967b-6bf25d26c457","resolution":{"observed_at":"2026-08-02T00:54:44.284872Z","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":"2026-08-17T21:27:10.939039Z","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":"2026-08-01T12:45:38.589335Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.19469","last_updated":"2026-07-21T18:00:02Z","snapshot_observed_at":"2026-08-20T00:52:51.933600Z","submitted_at":"2026-07-21T18:00:02Z","title":"Can the universe be matter-dominated after a supercooled first-order phase transition?","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-01T12:45:38.589335Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2607.19469"},"observation_digest":"sha256:49dd77fb4287225143d06277b102194742c58f006fab45d542627a19b9094747","observation_id":"027f2343-1a4e-4da1-9da1-28109bf0a294","resolution":{"observed_at":"2026-08-01T12:45:38.589335Z","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":"2026-08-17T21:27:10.939039Z","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":"2026-07-31T23:22:07.587367Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.24026","last_updated":"2026-07-27T05:53:12Z","snapshot_observed_at":"2026-08-17T17:40:23.402769Z","submitted_at":"2026-07-27T05:53:12Z","title":"Electroweak Baryogenesis: Advances in Sphaleron Rate Calculations and Implications of Thermal Phase Transitions","version":1},"reference_index":185,"source":"pdf_text","source_observed_at":"2026-07-31T23:22:07.587367Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2607.24026"},"observation_digest":"sha256:60caa1661fff476b5cef240f517c71c31bf5eb82da632f75040363656304d9f1","observation_id":"656bbba5-f7ec-41f6-8869-9bd72f838544","resolution":{"observed_at":"2026-07-31T23:22:07.587367Z","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":"2026-08-17T21:27:10.939039Z","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":"2026-08-16T00:27:41.510275Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.12736","last_updated":"2026-08-13T02:34:47Z","snapshot_observed_at":"2026-08-18T21:34:06.649818Z","submitted_at":"2026-08-13T02:34:47Z","title":"Cosmological Vacuum Decays from Schwinger-Keldysh Formalism","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-16T00:27:41.510275Z"},"links":{"cited_paper":"/paper/2504.13725","citing_paper":"/paper/2608.12736"},"observation_digest":"sha256:7811c0a147b1926c491366cfd04b2f09907d1926d9625a02c3867f2e476afa20","observation_id":"4da7dedd-4405-41f8-9a99-aaa52102a93d","resolution":{"observed_at":"2026-08-16T00:27:41.510275Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2504.13725/citation-record","integrity":"/paper/2504.13725/integrity","json":"/paper/2504.13725/citation-record.json","paper":"/paper/2504.13725"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-16T12:08:26.100784Z","title":"Cosmic Separation of Phases,","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.100784Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:7959fd1bb7c1d3e1a065f5e8313f6e8640c787472a435a32a8dd15160d22aeca","observation_id":"d962500d-a1cd-4392-b68f-b390b75866d7","resolution":{"observed_at":"2026-08-16T12:08:26.100784Z","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":"2026-08-16T12:08:26.138062Z","title":"Gravitational radiation from cosmological phase transitions,","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.138062Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:0c33f2efc7aa8f5b343261933f82290a04de18aa8d9cad81b9be0223c9a1dc25","observation_id":"58ad2509-1495-4a55-bdb8-3f28f7f2ef4e","resolution":{"observed_at":"2026-08-16T12:08:26.138062Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9211004","last_updated":"1992-11-07T20:57:32Z","snapshot_observed_at":"2026-08-13T12:43:41.315812Z","submitted_at":"1992-11-07T20:57:32Z","title":"Gravitational Radiation from Colliding Vacuum Bubbles: Envelope Approximation to Many-Bubble Collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9211004","snapshot_observed_at":"2026-08-16T12:08:26.144631Z","title":"Gravitational radiation from colliding vacuum bubbles: envelope approximation to many bubble collisions,","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.144631Z"},"links":{"cited_paper":"/paper/astro-ph/9211004","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:31119fa0eb6b2e714314a6c5ff45f5e265ddec01172bb0953ddc0db15b43e342","observation_id":"f34db77a-746c-4317-b17e-5d824c0c1b00","resolution":{"observed_at":"2026-08-16T12:08:26.144631Z","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":"2026-08-16T12:08:26.151046Z","title":"Gravitational waves from first order cosmological phase transitions,","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.151046Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:3ec5493dd089df7bf14446cebbe76de3b24b604d8c589e9a900508ddae89e196","observation_id":"33f4831f-bd4b-439a-b55b-ca9d9aa1cb49","resolution":{"observed_at":"2026-08-16T12:08:26.151046Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/9310044","last_updated":"1993-10-25T23:39:35Z","snapshot_observed_at":"2026-07-07T01:09:02.298352Z","submitted_at":"1993-10-25T23:39:35Z","title":"Gravitational Radiation from First-Order Phase Transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/9310044","snapshot_observed_at":"2026-08-16T12:08:26.225470Z","title":"Gravitational radiation from first order phase transitions,","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.225470Z"},"links":{"cited_paper":"/paper/astro-ph/9310044","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:15022a9f24dc0a8536a97c44187f0b29fa775788dcc8a59000b04e629a024fc7","observation_id":"3aeaeb2f-2594-441f-87e5-c7c7980148a8","resolution":{"observed_at":"2026-08-16T12:08:26.225470Z","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":"2026-08-16T12:08:26.233846Z","title":"On the Anomalous Electroweak Baryon Number Nonconservation in the Early Universe,","venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.233846Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:d31926ac788e4053b8a89da83d14e8c5dae7df78abb510a4a8f653855d555087","observation_id":"77de48d7-3a87-4a5b-8e72-fcd1e1301354","resolution":{"observed_at":"2026-08-16T12:08:26.233846Z","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":"2026-08-16T12:08:26.345912Z","title":"Possible Appearance of the Baryon Asymmetry of the Universe in an Electroweak Theory,","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.345912Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:15f6455e86e85a5e2aac8ace9d7ae3a9017b94bccaa2f510db8088c430564073","observation_id":"7580fd1c-a629-4031-862e-6d64bef84b56","resolution":{"observed_at":"2026-08-16T12:08:26.345912Z","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":"2026-08-16T12:08:26.477015Z","title":"Why there is something rather than nothing: Matter from weak interactions,","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.477015Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:4113b23dec2c692c7fa325e2da600efdef1c37b16493adf423cd985a59d1324d","observation_id":"97480f3e-6fc4-443b-8b30-d204a6cc66d1","resolution":{"observed_at":"2026-08-16T12:08:26.477015Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9603420","last_updated":"1996-03-26T21:31:46Z","snapshot_observed_at":"2026-08-06T13:09:37.412157Z","submitted_at":"1996-03-26T21:31:46Z","title":"Opening the Window for Electroweak Baryogenesis","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9603420","snapshot_observed_at":"2026-08-16T12:08:26.484530Z","title":"Opening the window for electroweak baryogenesis,","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.484530Z"},"links":{"cited_paper":"/paper/hep-ph/9603420","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:c71b59c0c0148fcfee20d2ad27c3b20e8b19399e0ad6fa6c113043127cc596a5","observation_id":"9afc4d47-44e2-4b45-a042-f9194035cf44","resolution":{"observed_at":"2026-08-16T12:08:26.484530Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.04902","last_updated":"2017-03-15T03:07:52Z","snapshot_observed_at":"2026-08-19T03:18:44.628030Z","submitted_at":"2017-03-15T03:07:52Z","title":"Baryogenesis at a Lepton-Number-Breaking Phase Transition","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.04902","snapshot_observed_at":"2026-08-16T12:08:26.494146Z","title":"Baryogenesis at a Lepton-Number-Breaking Phase Transition,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.494146Z"},"links":{"cited_paper":"/paper/1703.04902","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:9a3d3feaffd124420add0b014dd6c5ad0a6c983cdc36fd3defd4fd3143df15a8","observation_id":"98a2a61a-b90b-4ece-a588-69257f9a2976","resolution":{"observed_at":"2026-08-16T12:08:26.494146Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1804.07314","last_updated":"2018-12-07T20:24:41Z","snapshot_observed_at":"2026-08-14T19:24:08.604741Z","submitted_at":"2018-04-19T18:01:11Z","title":"Electroweak Phase Transition and Baryogenesis in Composite Higgs Models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1804.07314","snapshot_observed_at":"2026-08-16T12:08:26.505711Z","title":"Electroweak Phase Transition and Baryogenesis in Composite Higgs Models,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.505711Z"},"links":{"cited_paper":"/paper/1804.07314","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:395f462bbc796fc3151bc8bdd9c1f8702daa4eeb6905165d831d65b03c0c8495","observation_id":"ec9ffbec-8223-477c-a8c6-45a106d3e503","resolution":{"observed_at":"2026-08-16T12:08:26.505711Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.08546","last_updated":"2018-08-30T13:10:08Z","snapshot_observed_at":"2026-08-14T19:33:24.118623Z","submitted_at":"2018-03-22T19:01:08Z","title":"The Baryon Asymmetry from a Composite Higgs","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.08546","snapshot_observed_at":"2026-08-16T12:08:26.590858Z","title":"Baryon Asymmetry from a Composite Higgs Boson,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.590858Z"},"links":{"cited_paper":"/paper/1803.08546","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:9c0785a3bd26b91c8f783666c1ce483967d612244703a82ee76e21b5d37ec5de","observation_id":"6304bb6d-4553-4c06-b079-39c0686e5dcd","resolution":{"observed_at":"2026-08-16T12:08:26.590858Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1206.2942","last_updated":"2012-06-13T21:09:14Z","snapshot_observed_at":"2026-08-15T00:56:56.720619Z","submitted_at":"2012-06-13T21:09:14Z","title":"Electroweak baryogenesis","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.2942","snapshot_observed_at":"2026-08-16T12:08:26.626014Z","title":"Electroweak baryogenesis,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.626014Z"},"links":{"cited_paper":"/paper/1206.2942","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:f25e5ed0b6b3dff5633ff7dcdd89c5224269fee8e103c70370d8be7c8b2fb602","observation_id":"3c1f8e12-a2b1-45bf-ba69-347820687017","resolution":{"observed_at":"2026-08-16T12:08:26.626014Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.14913","last_updated":"2021-09-15T08:54:13Z","snapshot_observed_at":"2026-08-19T10:17:19.576491Z","submitted_at":"2021-06-28T18:00:49Z","title":"Baryogenesis via relativistic bubble walls","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.14913","snapshot_observed_at":"2026-08-16T12:08:26.632645Z","title":"Baryogenesis via relativistic bubble walls,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.632645Z"},"links":{"cited_paper":"/paper/2106.14913","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:b83fda7f1fabaf91be22966926d4e064652257ef17a3b565931a8035296d7a15","observation_id":"5ad1cf47-8b6f-4f18-a5e7-f3b37bad7d90","resolution":{"observed_at":"2026-08-16T12:08:26.632645Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.15602","last_updated":"2021-12-01T08:59:06Z","snapshot_observed_at":"2026-08-19T10:17:22.180009Z","submitted_at":"2021-06-29T17:44:11Z","title":"Baryogenesis via relativistic bubble expansion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.15602","snapshot_observed_at":"2026-08-16T12:08:26.643074Z","title":"Baryogenesis via relativistic bubble expansion,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.643074Z"},"links":{"cited_paper":"/paper/2106.15602","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:8db3543a434507610c149da155d37bbab73252632b680beec85fb5c72a811e54","observation_id":"e160d3b0-492f-41c6-bcae-cb5815bb937f","resolution":{"observed_at":"2026-08-16T12:08:26.643074Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.04691","last_updated":"2022-08-26T02:25:10Z","snapshot_observed_at":"2026-08-19T10:17:26.296436Z","submitted_at":"2022-06-09T18:00:00Z","title":"Leptogenesis triggered by a first-order phase transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.04691","snapshot_observed_at":"2026-08-16T12:08:26.700694Z","title":"Leptogenesis triggered by a first-order phase transition,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.700694Z"},"links":{"cited_paper":"/paper/2206.04691","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:9734c09bc30bbacb18e6158e52e5ffc704c20e4e032625f0ea7c7e538dbed738","observation_id":"17c2829b-f8c9-4ae4-b823-be09ae36f96b","resolution":{"observed_at":"2026-08-16T12:08:26.700694Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.10759","last_updated":"2023-09-14T15:17:35Z","snapshot_observed_at":"2026-08-18T03:58:11.372824Z","submitted_at":"2023-05-18T06:58:01Z","title":"Bubble-assisted Leptogenesis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.10759","snapshot_observed_at":"2026-08-16T12:08:26.706920Z","title":"Bubble-assisted leptogenesis,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.706920Z"},"links":{"cited_paper":"/paper/2305.10759","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:2d7e6e676b040413d08295be18af4f20b627ad302a38cc4b15dde63bdee4ce5c","observation_id":"68adc6d2-22f6-444c-b692-5999b64af521","resolution":{"observed_at":"2026-08-16T12:08:26.706920Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.09282","last_updated":"2024-01-23T21:06:19Z","snapshot_observed_at":"2026-08-16T14:34:38.229679Z","submitted_at":"2023-12-14T19:00:03Z","title":"Baryogenesis and Leptogenesis from Supercooled Confinement","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.09282","snapshot_observed_at":"2026-08-16T12:08:26.713531Z","title":"Baryogenesis and leptogenesis from supercooled confinement,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.713531Z"},"links":{"cited_paper":"/paper/2312.09282","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:f78edbe2032cb8c695bd6e5ef27c21d55a0d5e06197d07c19b65d0abe5776281","observation_id":"2fd4340e-b041-4695-b962-e394f230fabe","resolution":{"observed_at":"2026-08-16T12:08:26.713531Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.16747","last_updated":"2024-12-04T13:13:08Z","snapshot_observed_at":"2026-08-16T13:31:40.008402Z","submitted_at":"2024-07-23T18:00:01Z","title":"Leptogenesis via Bubble Collisions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.16747","snapshot_observed_at":"2026-08-16T12:08:26.760184Z","title":"Leptogenesis via bubble collisions,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.760184Z"},"links":{"cited_paper":"/paper/2407.16747","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:08cfc777e3d3fdf558444e00ca897c43c4107528aa51e6e8ca1a4bd66317a6a4","observation_id":"58b41afc-e408-4f1c-8da1-2019b298d8bb","resolution":{"observed_at":"2026-08-16T12:08:26.760184Z","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":"2026-08-16T12:08:26.820775Z","title":"Magnetic fields from cosmological phase transitions,","venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.820775Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:ebeec8ff1ed26ea474ad50225115d06c941ed8b5f50be01cac84f44473e17122","observation_id":"fb2fb664-07f4-46df-8de3-12c50c957e1e","resolution":{"observed_at":"2026-08-16T12:08:26.820775Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9704334","last_updated":"1997-04-16T14:15:28Z","snapshot_observed_at":"2026-08-08T02:56:18.346587Z","submitted_at":"1997-04-16T14:15:28Z","title":"Magnetic field generation in first order phase transition bubble collisions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9704334","snapshot_observed_at":"2026-08-16T12:08:26.830038Z","title":"Magnetic field generation in first order phase transition bubble collisions,","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.830038Z"},"links":{"cited_paper":"/paper/hep-ph/9704334","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:fd4472fc89baca2c2898e1cd1ed819b8049da6aac5ee5235cadf50bccc53cc69","observation_id":"1ecadf2a-4320-4fb2-b368-75a335dbbd0f","resolution":{"observed_at":"2026-08-16T12:08:26.830038Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"astro-ph/0101261","last_updated":"2001-11-01T18:39:26Z","snapshot_observed_at":"2026-07-07T00:15:19.403306Z","submitted_at":"2001-01-16T11:02:27Z","title":"Estimate of the primordial magnetic field helicity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"astro-ph/0101261","snapshot_observed_at":"2026-08-16T12:08:26.838223Z","title":"Estimate of the primordial magnetic field helicity,","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.838223Z"},"links":{"cited_paper":"/paper/astro-ph/0101261","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:c307dface9807b6871f1a1a679a5d5b3d052c6e9e47daf5317b70d1240540d0f","observation_id":"58571453-f3dd-4d8f-970d-16fb89cae149","resolution":{"observed_at":"2026-08-16T12:08:26.838223Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1907.04315","last_updated":"2019-10-07T10:48:34Z","snapshot_observed_at":"2026-08-17T09:52:00.459066Z","submitted_at":"2019-07-09T17:58:05Z","title":"Intergalactic Magnetic Fields from First-Order Phase Transitions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.04315","snapshot_observed_at":"2026-08-16T12:08:26.911411Z","title":"Intergalactic Magnetic Fields from First-Order Phase Transitions,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.911411Z"},"links":{"cited_paper":"/paper/1907.04315","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:9ece7a7be5a9ef42de1d171b92b61a54da0e7badc7505c693e7f62190061a9ae","observation_id":"f5e969f7-980e-4af0-a74d-3227408c89ff","resolution":{"observed_at":"2026-08-16T12:08:26.911411Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2012.15625","last_updated":"2021-08-22T09:03:10Z","snapshot_observed_at":"2026-08-20T17:50:39.566515Z","submitted_at":"2020-12-31T14:27:46Z","title":"Magnetic field and gravitational waves from the first-order Phase Transition","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2012.15625","snapshot_observed_at":"2026-08-16T12:08:26.982683Z","title":"Magnetic Field and Gravitational Waves from the First-Order Phase Transition,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:26.982683Z"},"links":{"cited_paper":"/paper/2012.15625","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:a8930d6551bfd0c999bf6a8717fcfb69e89757d85133bd70941d2d602cea48a8","observation_id":"224b6755-604c-4066-b995-f1e56d4d719a","resolution":{"observed_at":"2026-08-16T12:08:26.982683Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.19948","last_updated":"2024-05-06T08:57:56Z","snapshot_observed_at":"2026-08-16T14:47:28.706113Z","submitted_at":"2023-10-30T19:00:22Z","title":"Primordial Magnetogenesis in the Two-Higgs-doublet Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.19948","snapshot_observed_at":"2026-08-16T12:08:27.064820Z","title":"Primordial magnetogenesis in the two-Higgs-doublet model,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.064820Z"},"links":{"cited_paper":"/paper/2310.19948","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:9b7e1ca46ab4a8071c6c93ae5d035cdde2b098f258327d4d39bcb78a8797ace2","observation_id":"c7af3642-9236-4cab-af4c-8ca81655caad","resolution":{"observed_at":"2026-08-16T12:08:27.064820Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.05179","last_updated":"2025-03-20T20:18:54Z","snapshot_observed_at":"2026-08-20T14:01:58.212931Z","submitted_at":"2024-02-07T19:00:04Z","title":"Magnetogenesis with gravitational waves and primordial black hole dark matter","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.05179","snapshot_observed_at":"2026-08-16T12:08:27.112495Z","title":"Magnetogenesis with gravitational waves and primordial black hole dark matter,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.112495Z"},"links":{"cited_paper":"/paper/2402.05179","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:f5fe8b51bd5f0356f48aff2440af45d5a4f5f84cea80daf4600b2f32f7d88b3f","observation_id":"88bfcd04-734c-4b79-8784-dc8c2503091d","resolution":{"observed_at":"2026-08-16T12:08:27.112495Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1211.5615","last_updated":"2012-11-23T21:39:44Z","snapshot_observed_at":"2026-08-20T20:26:06.825787Z","submitted_at":"2012-11-23T21:39:44Z","title":"Non-thermal Dark Matter Production from the Electroweak Phase Transition: Multi-TeV WIMPs and \"Baby-Zillas\"","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1211.5615","snapshot_observed_at":"2026-08-16T12:08:27.120258Z","title":"Non-thermal Dark Matter Production from the Electroweak Phase Transition: Multi-TeV WIMPs and ’Baby-Zillas’,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.120258Z"},"links":{"cited_paper":"/paper/1211.5615","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:7679e20169df9a6b0c718d5d16c9c70f6a1d02333a8360c998effdb6a31b716b","observation_id":"27012ab2-6567-401c-881c-5b93bd38790e","resolution":{"observed_at":"2026-08-16T12:08:27.120258Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.08440","last_updated":"2021-05-03T10:23:35Z","snapshot_observed_at":"2026-08-09T11:28:04.109486Z","submitted_at":"2020-07-16T16:25:29Z","title":"String Fragmentation in Supercooled Confinement and Implications for Dark Matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.08440","snapshot_observed_at":"2026-08-16T12:08:27.127269Z","title":"String Fragmentation in Supercooled Confinement and Implications for Dark Matter,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.127269Z"},"links":{"cited_paper":"/paper/2007.08440","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:27be5182ea69f99906e40e5072c3772f16c6f63432318bdfc76641a035bb91da","observation_id":"791a2627-2f0a-468e-9fbb-5431e1479a20","resolution":{"observed_at":"2026-08-16T12:08:27.127269Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.04430","last_updated":"2020-10-15T06:47:11Z","snapshot_observed_at":"2026-08-15T00:54:48.174146Z","submitted_at":"2020-08-10T21:54:08Z","title":"Fermi-ball dark matter from a first-order phase transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.04430","snapshot_observed_at":"2026-08-16T12:08:27.189528Z","title":"Fermi-ball dark matter from a first-order phase transition,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.189528Z"},"links":{"cited_paper":"/paper/2008.04430","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:0021b73379947256692d8a15ffbd450e256a22c50f19e5252d9d63870d1c41f5","observation_id":"29b5f730-c7e5-4205-9bdb-5e011f54c807","resolution":{"observed_at":"2026-08-16T12:08:27.189528Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.05721","last_updated":"2021-01-14T16:55:29Z","snapshot_observed_at":"2026-08-20T21:17:28.774514Z","submitted_at":"2021-01-14T16:55:29Z","title":"Dark Matter production from relativistic bubble walls","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.05721","snapshot_observed_at":"2026-08-16T12:08:27.196542Z","title":"Dark Matter production from relativistic bubble walls,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.196542Z"},"links":{"cited_paper":"/paper/2101.05721","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:ef80137f84eeac5455fdefb626ea3c25c3a92ea85f78b0fe4114c6300b0dc826","observation_id":"03b49b44-5a3a-4d38-b598-bf2be5f8f327","resolution":{"observed_at":"2026-08-16T12:08:27.196542Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.13926","last_updated":"2022-07-13T19:56:13Z","snapshot_observed_at":"2026-08-16T17:46:21.496361Z","submitted_at":"2021-10-26T18:00:02Z","title":"Supercool Composite Dark Matter Beyond 100 TeV","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.13926","snapshot_observed_at":"2026-08-16T12:08:27.203212Z","title":"Supercool composite Dark Matter beyond 100 TeV,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.203212Z"},"links":{"cited_paper":"/paper/2110.13926","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:866f00ea018a7125cc7d907ca42e012aac8dc11157d9ac3d60966a23bd0d73d4","observation_id":"30ce4409-1d6d-424d-a3c9-f8df3e8e68cc","resolution":{"observed_at":"2026-08-16T12:08:27.203212Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.09827","last_updated":"2022-04-18T15:38:09Z","snapshot_observed_at":"2026-08-16T18:38:11.935594Z","submitted_at":"2021-03-17T18:00:01Z","title":"Thermal Squeezeout of Dark Matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.09827","snapshot_observed_at":"2026-08-16T12:08:27.237543Z","title":"Thermal squeezeout of dark matter,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.237543Z"},"links":{"cited_paper":"/paper/2103.09827","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:2f689603249437ece76aba5542f9bf4fcd9dc495a16eb2ab58e8922b288fcf12","observation_id":"8902cee8-edec-42ea-b8ff-6d04e1272722","resolution":{"observed_at":"2026-08-16T12:08:27.237543Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.05096","last_updated":"2022-12-05T16:30:56Z","snapshot_observed_at":"2026-08-19T17:25:51.305695Z","submitted_at":"2022-07-11T18:00:03Z","title":"Hot and heavy dark matter from a weak scale phase transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.05096","snapshot_observed_at":"2026-08-16T12:08:27.290372Z","title":"Hot and heavy dark matter from a weak scale phase transition,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.290372Z"},"links":{"cited_paper":"/paper/2207.05096","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:c50d1f4d84c4b21cdbe2087af9376079752988b9b66f4d35d2f186b5616d166a","observation_id":"d88b4451-87a5-4c9e-a4ed-f2d561bddcc0","resolution":{"observed_at":"2026-08-16T12:08:27.290372Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.02230","last_updated":"2022-07-05T18:00:06Z","snapshot_observed_at":"2026-08-19T10:17:27.510388Z","submitted_at":"2022-07-05T18:00:06Z","title":"Ultra-relativistic bubbles from the simplest Higgs portal and their cosmological consequences","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.02230","snapshot_observed_at":"2026-08-16T12:08:27.297257Z","title":"Ultra-relativistic bubbles from the simplest Higgs portal and their cosmological consequences,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.297257Z"},"links":{"cited_paper":"/paper/2207.02230","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:05d4433f1513f4ed64eddacf82f3f0f3fa8543329f467dcfe3a8089cb30dccc3","observation_id":"5a1aa80e-b35b-4257-a56c-15ae79833d6e","resolution":{"observed_at":"2026-08-16T12:08:27.297257Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.15555","last_updated":"2025-02-18T13:50:47Z","snapshot_observed_at":"2026-08-16T15:20:42.362385Z","submitted_at":"2023-06-27T15:25:50Z","title":"Bubbletrons: Ultrahigh-Energy Particle Collisions and Heavy Dark Matter at Phase Transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.15555","snapshot_observed_at":"2026-08-16T12:08:27.359558Z","title":"Ultrahigh-Energy Particle Collisions and Heavy Dark Matter at Phase Transitions,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.359558Z"},"links":{"cited_paper":"/paper/2306.15555","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:31687d90845f845ae68a4f3a1d56a58e2a90b89676ff933422d55adcb9563da8","observation_id":"3be75b7e-4af0-4f98-8d14-7bdee2c1fc66","resolution":{"observed_at":"2026-08-16T12:08:27.359558Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.07075","last_updated":"2023-03-02T11:14:09Z","snapshot_observed_at":"2026-08-16T16:24:27.950747Z","submitted_at":"2022-10-13T15:01:14Z","title":"Conformal model for gravitational waves and dark matter: A status update","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.07075","snapshot_observed_at":"2026-08-16T12:08:27.457474Z","title":"Conformal model for gravitational waves and dark matter: a status update,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.457474Z"},"links":{"cited_paper":"/paper/2210.07075","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:6d0e1b0929d8a46a0f2c97b5f086778ab867508e03e381ae2699de1a748351b8","observation_id":"2c382336-707f-4fe9-8c30-58c674b38e51","resolution":{"observed_at":"2026-08-16T12:08:27.457474Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.08526","last_updated":"2024-03-20T20:31:33Z","snapshot_observed_at":"2026-08-18T16:39:35.712347Z","submitted_at":"2023-10-12T17:19:09Z","title":"Recycled Dark Matter","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.08526","snapshot_observed_at":"2026-08-16T12:08:27.466273Z","title":"Recycled dark matter,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.466273Z"},"links":{"cited_paper":"/paper/2310.08526","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:8c83fc6d726e298b0a7046a66e2e03aa0085449b1e603da3148200596ebe4de3","observation_id":"1fc1557b-8412-4085-90b3-c5f4fb80f436","resolution":{"observed_at":"2026-08-16T12:08:27.466273Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.03252","last_updated":"2025-01-09T15:09:17Z","snapshot_observed_at":"2026-08-19T17:35:01.084519Z","submitted_at":"2024-03-05T19:00:02Z","title":"Nonthermal Heavy Dark Matter from a First-Order Phase Transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.03252","snapshot_observed_at":"2026-08-16T12:08:27.544996Z","title":"Nonthermal heavy dark matter from a first-order phase transition,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.544996Z"},"links":{"cited_paper":"/paper/2403.03252","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:b032ea4216dda18d35e739993e882658026618d5129c8b505a855aa2a72f6ffb","observation_id":"7baba452-134f-43e5-9e0a-16387a0da94e","resolution":{"observed_at":"2026-08-16T12:08:27.544996Z","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":"2026-08-16T12:08:27.551288Z","title":"Non-thermal production of heavy vector dark matter from relativistic bubble walls,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.551288Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:cac237babfd2fc076e4ad821e05f5b388a41967743c65723839ea84b3317e1be","observation_id":"1c1376a6-85e2-4263-ac65-33dfd97cd964","resolution":{"observed_at":"2026-08-16T12:08:27.551288Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.14592","last_updated":"2025-04-02T18:00:01Z","snapshot_observed_at":"2026-08-16T13:32:37.251564Z","submitted_at":"2024-07-19T18:00:01Z","title":"Scalar Dark Matter Production through the Bubble Expansion Mechanism:The Role of the Lorentz factor and Non-Renormalizable Interactions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.14592","snapshot_observed_at":"2026-08-16T12:08:27.559719Z","title":"Scalar dark matter production through the bubble expansion mechanism: the role of the Lorentz factor and non-renormalizable interactions,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.559719Z"},"links":{"cited_paper":"/paper/2407.14592","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:57cb0f38371c54847988fc10ad59b561240ae28f0c07a229a8ce2e66c002b416","observation_id":"3fdff9bc-bb9a-45c5-971d-c1e9b0d4e16b","resolution":{"observed_at":"2026-08-16T12:08:27.559719Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2504.10593","last_updated":"2025-04-14T18:00:11Z","snapshot_observed_at":"2026-08-20T07:41:51.007784Z","submitted_at":"2025-04-14T18:00:11Z","title":"Dark matter phase-in: producing feebly-interacting particles after a first-order phase transition","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2504.10593","snapshot_observed_at":"2026-08-16T12:08:27.566090Z","title":"Dark matter phase-in: producing feebly-interacting particles after a first-order phase transition,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.566090Z"},"links":{"cited_paper":"/paper/2504.10593","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:155f0b5186f2748a74aefc6d6023bf1e31c74c7dccb36d0fed0c8aaa10f1e8e3","observation_id":"b22d4b25-eea2-47b0-af16-c86b6f59cc1c","resolution":{"observed_at":"2026-08-16T12:08:27.566090Z","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":"2026-08-16T12:08:27.620622Z","title":"Abundance of Primordial Holes Produced by Cosmological First Order Phase Transition,","venue":null,"work_id":null,"year":1982},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.620622Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:80937aeb7d96e111c34f0f84fcbcc61a43ae93014c3fd461f300a7d5cc4f663d","observation_id":"fc4ebdec-e0a1-4b2f-8e76-ce6478547f65","resolution":{"observed_at":"2026-08-16T12:08:27.620622Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.00111","last_updated":"2021-11-21T23:38:00Z","snapshot_observed_at":"2026-08-19T03:18:48.396117Z","submitted_at":"2021-05-31T21:36:22Z","title":"Primordial black holes from a cosmic phase transition: The collapse of Fermi-balls","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.00111","snapshot_observed_at":"2026-08-16T12:08:27.651261Z","title":"Primordial black holes from a cosmic phase transition: The collapse of Fermi-balls,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.651261Z"},"links":{"cited_paper":"/paper/2106.00111","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:dc962ebd2148b73de438abf2c742818ab6adc0c000eb50bb7bed3087f85c681c","observation_id":"d24900a8-dad6-405f-adc6-a65ce9e494d5","resolution":{"observed_at":"2026-08-16T12:08:27.651261Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.05637","last_updated":"2022-01-14T11:58:31Z","snapshot_observed_at":"2026-08-19T03:18:04.200890Z","submitted_at":"2021-06-10T10:20:25Z","title":"Primordial black hole production during first-order phase transitions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.05637","snapshot_observed_at":"2026-08-16T12:08:27.657398Z","title":"Primordial black hole production during first-order phase transitions,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.657398Z"},"links":{"cited_paper":"/paper/2106.05637","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:c6daee6d07c35b38838c12f05de059f37e556656309062a009ecbd3e0c2c35ff","observation_id":"78e9c1a4-9b50-42ce-9b72-2444b9eaf4ac","resolution":{"observed_at":"2026-08-16T12:08:27.657398Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.04271","last_updated":"2024-11-19T12:21:30Z","snapshot_observed_at":"2026-08-17T08:48:17.268597Z","submitted_at":"2021-10-08T17:33:54Z","title":"Primordial black holes from bubble collisions during a first-order phase transition","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.04271","snapshot_observed_at":"2026-08-16T12:08:27.663276Z","title":"Primordial black holes from bubble collisions during a first-order phase transition,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.663276Z"},"links":{"cited_paper":"/paper/2110.04271","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:5e9bab431daef1d229006509731713208f7a2bc8ed8e39d74f08513cc0925269","observation_id":"97e88261-dd99-4244-850c-227f435c1620","resolution":{"observed_at":"2026-08-16T12:08:27.663276Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.04942","last_updated":"2025-03-03T19:22:02Z","snapshot_observed_at":"2026-08-20T16:59:31.535518Z","submitted_at":"2023-05-08T18:00:00Z","title":"Primordial Black Holes from Supercooled Phase Transitions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.04942","snapshot_observed_at":"2026-08-16T12:08:27.668729Z","title":"Primordial black holes from supercooled phase transitions,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.668729Z"},"links":{"cited_paper":"/paper/2305.04942","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:68b6ca18a2849219ab6db3a75a7a0c702b041c96db591c63c43504698b59e444","observation_id":"a79233b1-a1e1-4573-820f-f1d462134900","resolution":{"observed_at":"2026-08-16T12:08:27.668729Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.04158","last_updated":"2024-10-31T11:51:17Z","snapshot_observed_at":"2026-08-16T14:20:56.751756Z","submitted_at":"2024-02-06T17:15:33Z","title":"Black holes and gravitational waves from slow phase transitions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.04158","snapshot_observed_at":"2026-08-16T12:08:27.675041Z","title":"Black Holes and Gravitational Waves from Slow First-Order Phase Transitions,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.675041Z"},"links":{"cited_paper":"/paper/2402.04158","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:d05f081401120f57fc33275d99314c35579a908ec8def9c6a1657e3007ba2ebf","observation_id":"9cd97afe-b1ca-4e78-b9f9-1572f6f99c11","resolution":{"observed_at":"2026-08-16T12:08:27.675041Z","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":"2026-08-16T12:08:27.681568Z","title":"Primordial black holes from an interrupted phase transition,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.681568Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:a1fb613eb64518041087efcb130e015a6986cf8f8a00fa657ab4db35155cd29d","observation_id":"fde21b77-a4b6-4b04-b02b-17759a0731bb","resolution":{"observed_at":"2026-08-16T12:08:27.681568Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.02291","last_updated":"2025-07-10T02:47:30Z","snapshot_observed_at":"2026-08-15T23:08:50.377919Z","submitted_at":"2025-02-04T12:59:54Z","title":"Primordial Black Hole Formation via Inverted Bubble Collapse","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.02291","snapshot_observed_at":"2026-08-16T12:08:27.812590Z","title":"Primordial Black Hole Formation via Inverted Bubble Collapse,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.812590Z"},"links":{"cited_paper":"/paper/2502.02291","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:4b94f89fe7e4c890c358008c032b48d0b1eaa241903e748c226a926aab991ec3","observation_id":"8131d76b-e841-4ef5-8d41-51efcc86b8ae","resolution":{"observed_at":"2026-08-16T12:08:27.812590Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2106.05984","last_updated":"2021-06-10T18:00:30Z","snapshot_observed_at":"2026-08-16T18:17:59.655911Z","submitted_at":"2021-06-10T18:00:30Z","title":"Observational prospects for phase transitions at LISA: Fisher matrix analysis","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2106.05984","snapshot_observed_at":"2026-08-16T12:08:27.819712Z","title":"Observational prospects for phase transitions at LISA: Fisher matrix analysis,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.819712Z"},"links":{"cited_paper":"/paper/2106.05984","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:6894dd751c19ca46c52583ec6a9ab53b95b5e6b0a3b9e21c8801cb9503a0f2a7","observation_id":"d7ee017a-4d38-429b-8dec-f69e8312608a","resolution":{"observed_at":"2026-08-16T12:08:27.819712Z","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":"2026-08-16T18:32:09.122865Z","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":"2026-08-16T12:08:27.826393Z","title":"Bubble wall velocity from holography,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.826393Z"},"links":{"cited_paper":"/paper/2104.05708","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:5aa013faa8034a8bb20ab0853ee2836ac2b86989404d76e182906b5b510f3544","observation_id":"e9f6549a-2285-476c-baef-1920f7af559f","resolution":{"observed_at":"2026-08-16T12:08:27.826393Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2104.12817","last_updated":"2021-10-05T13:59:28Z","snapshot_observed_at":"2026-08-16T18:28:57.222698Z","submitted_at":"2021-04-26T18:50:52Z","title":"Bubble Wall Velocity at Strong Coupling","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.12817","snapshot_observed_at":"2026-08-16T12:08:27.917245Z","title":"Bubble wall velocity at strong coupling,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.917245Z"},"links":{"cited_paper":"/paper/2104.12817","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:5d00801093ea08eaea6aabcd1a405c28672ccddd40c480c3efe495585d2002a2","observation_id":"05569310-f013-4c0a-8c88-938bc5cce729","resolution":{"observed_at":"2026-08-16T12:08:27.917245Z","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":"2026-08-16T17:00:42.364931Z","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":"2026-08-16T12:08:27.959849Z","title":"Perfect Fluid Hydrodynamic Picture of Domain Wall Velocities at Strong Coupling,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.959849Z"},"links":{"cited_paper":"/paper/2205.06274","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:0657154e06d4cb03659a35578e1a96dd6f42715e23aca3546b8b4ea667a327f5","observation_id":"938f705a-f193-4c2a-acbf-d920e5660b7b","resolution":{"observed_at":"2026-08-16T12:08:27.959849Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.10042","last_updated":"2023-11-13T14:30:31Z","snapshot_observed_at":"2026-08-20T16:58:43.418557Z","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":"2026-08-16T12:08:27.966677Z","title":"Bubble expansion at strong coupling,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.966677Z"},"links":{"cited_paper":"/paper/2302.10042","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:37045090f50c50a3c8392dc35a1c4a075892bf9b0ea550a26faa45275d5b5d30","observation_id":"256f772c-8a60-4cef-b5ed-d1297890c248","resolution":{"observed_at":"2026-08-16T12:08:27.966677Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.09588","last_updated":"2024-12-12T18:55:58Z","snapshot_observed_at":"2026-08-14T14:15:22.610497Z","submitted_at":"2024-12-12T18:55:58Z","title":"Bubble dynamics in a QCD-like phase diagram","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.09588","snapshot_observed_at":"2026-08-16T12:08:27.973714Z","title":"Bubble dynamics in a QCD-like phase diagram,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:27.973714Z"},"links":{"cited_paper":"/paper/2412.09588","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:785834e7de03639a694ed50512afc13de77bb24c8525cff12e6e6ac8b5d54aaa","observation_id":"c60805cf-9416-4513-8600-328fd9ad4abf","resolution":{"observed_at":"2026-08-16T12:08:27.973714Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9503296","last_updated":"1995-03-10T21:52:30Z","snapshot_observed_at":"2026-07-07T04:19:22.926961Z","submitted_at":"1995-03-10T21:52:30Z","title":"Bubble Wall Velocity at the Electroweak Phase Transition","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9503296","snapshot_observed_at":"2026-08-16T12:08:28.080955Z","title":"Bubble wall velocity in a first order electroweak phase transition,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.080955Z"},"links":{"cited_paper":"/paper/hep-ph/9503296","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:b3787225f468997ebee1f65fe8c13bac72bf4c9c66caf94d4040e214ea43f65a","observation_id":"616e8072-8cf1-4c98-93ba-a2cbe61acd5c","resolution":{"observed_at":"2026-08-16T12:08:28.080955Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9506475","last_updated":"1995-08-02T01:46:55Z","snapshot_observed_at":"2026-08-19T21:04:55.136752Z","submitted_at":"1995-06-30T21:47:58Z","title":"How fast can the wall move? A study of the electroweak phase transition dynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9506475","snapshot_observed_at":"2026-08-16T12:08:28.123825Z","title":"How fast can the wall move? A Study of the electroweak phase transition dynamics,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.123825Z"},"links":{"cited_paper":"/paper/hep-ph/9506475","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:86345f970920ece360e9c369288fb34a8527d39c2340318dd971ccac38f128c0","observation_id":"90460900-e404-45d9-8246-80e744348ee9","resolution":{"observed_at":"2026-08-16T12:08:28.123825Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1004.4187","last_updated":"2010-04-23T17:30:24Z","snapshot_observed_at":"2026-08-19T15:25:18.345201Z","submitted_at":"2010-04-23T17:30:24Z","title":"Energy Budget of Cosmological First-order Phase Transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1004.4187","snapshot_observed_at":"2026-08-16T12:08:28.130048Z","title":"Energy Budget of Cosmological First-order Phase Transitions,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.130048Z"},"links":{"cited_paper":"/paper/1004.4187","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:57105c07d12f0f8e373562f021bc54ddbf56a15fb2bff618497d9e1984248152","observation_id":"10e8f9a1-4df1-434b-8248-9e02d2cfb8aa","resolution":{"observed_at":"2026-08-16T12:08:28.130048Z","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":"2026-08-16T12:08:28.135738Z","title":"Bubble nucleation and growth at a baryon number producing electroweak phase transition,","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.135738Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:55ff38a2cafd1e51cd3257aec04b35e1cdaa94562eb50108f0706d178744095b","observation_id":"10cff8df-82bf-40fb-9711-4efacb6fa50a","resolution":{"observed_at":"2026-08-16T12:08:28.135738Z","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":"2026-08-19T15:25:17.955865Z","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":"2026-08-16T12:08:28.171710Z","title":"Hydrodynamic obstruction to bubble expansion,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.171710Z"},"links":{"cited_paper":"/paper/1011.3735","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:be98454e7c2ebb119ad2addb550569e9679ee1fbcd42ac02c199037ad73ecee6","observation_id":"35b75313-6cf9-4817-98cb-0dd89d77e75c","resolution":{"observed_at":"2026-08-16T12:08:28.171710Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.1888","last_updated":"2011-12-08T17:25:58Z","snapshot_observed_at":"2026-08-15T04:26:24.401360Z","submitted_at":"2011-12-08T17:25:58Z","title":"The bubble wall velocity in the minimal supersymmetric light stop scenario","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1112.1888","snapshot_observed_at":"2026-08-16T12:08:28.215718Z","title":"The bubble wall velocity in the minimal supersymmetric light stop scenario,","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.215718Z"},"links":{"cited_paper":"/paper/1112.1888","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:9d336eafea8857029b8e30048a0161eac4992180cb12b9b31e820d0af28e9ad1","observation_id":"e9d3cbaa-1b28-47b4-bc60-ad99af43f6ea","resolution":{"observed_at":"2026-08-16T12:08:28.215718Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1506.04741","last_updated":"2015-11-11T21:56:02Z","snapshot_observed_at":"2026-08-19T04:44:43.378789Z","submitted_at":"2015-06-15T20:00:24Z","title":"Bubble Expansion and the Viability of Singlet-Driven Electroweak Baryogenesis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1506.04741","snapshot_observed_at":"2026-08-16T12:08:28.223558Z","title":"Bubble Expansion and the Viability of Singlet-Driven Electroweak Baryogenesis,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.223558Z"},"links":{"cited_paper":"/paper/1506.04741","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:683253c418ac92561e65fdbbac120f08ca0f3fc25bd8485a084d38334b29300c","observation_id":"4bec858d-4d87-45f4-b58c-db26d1388c45","resolution":{"observed_at":"2026-08-16T12:08:28.223558Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1809.04907","last_updated":"2018-09-13T12:16:26Z","snapshot_observed_at":"2026-08-14T18:28:54.948530Z","submitted_at":"2018-09-13T12:16:26Z","title":"Bubble wall velocities in the Standard Model and beyond","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1809.04907","snapshot_observed_at":"2026-08-16T12:08:28.230954Z","title":"Bubble wall velocities in the Standard 58 Model and beyond,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.230954Z"},"links":{"cited_paper":"/paper/1809.04907","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:b16f428f9548b834071d2eb48cc0d602d2e4d87aac2f20ec8e174ec9d59a0fa7","observation_id":"1d20b64c-db7c-4fdb-a6fe-f10639534005","resolution":{"observed_at":"2026-08-16T12:08:28.230954Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.14295","last_updated":"2021-02-28T17:36:09Z","snapshot_observed_at":"2026-08-20T04:59:44.455850Z","submitted_at":"2020-09-29T20:36:01Z","title":"Wall speed and shape in singlet-assisted strong electroweak phase transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.14295","snapshot_observed_at":"2026-08-16T12:08:28.248156Z","title":"Wall speed and shape in singlet-assisted strong electroweak phase transitions,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.248156Z"},"links":{"cited_paper":"/paper/2009.14295","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:a4a3309f3b33da2a9c343d89b7f3d87aa8c1f649dbf9b15bd8e9401a9a79510e","observation_id":"9d1fd7db-9151-4071-97c1-f8e50dc93692","resolution":{"observed_at":"2026-08-16T12:08:28.248156Z","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":"2026-08-19T15:30:49.569376Z","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":"2026-08-16T12:08:28.301174Z","title":"Cosmological bubble friction in local equilibrium,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.301174Z"},"links":{"cited_paper":"/paper/2010.08013","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:eaf30ef7c9556910da5832af494366001182f202cfde0e6966f093ac680bd4b2","observation_id":"56990651-3a82-4edb-a81e-dae15047bd03","resolution":{"observed_at":"2026-08-16T12:08:28.301174Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.12490","last_updated":"2021-03-05T16:56:23Z","snapshot_observed_at":"2026-08-20T05:01:07.906604Z","submitted_at":"2021-02-24T19:00:01Z","title":"Baryogenesis and gravity waves from a UV-completed electroweak phase transition","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.12490","snapshot_observed_at":"2026-08-16T12:08:28.374075Z","title":"Baryogenesis and gravity waves from a UV-completed electroweak phase transition,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.374075Z"},"links":{"cited_paper":"/paper/2102.12490","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:22ba5856084f267ac0fa52cae18353dd29a0d0f6a423309203771875c52b2e97","observation_id":"e77470c8-7766-4b06-ad62-5c6bac227ffd","resolution":{"observed_at":"2026-08-16T12:08:28.374075Z","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":"2026-08-19T15:30:46.483985Z","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":"2026-08-16T12:08:28.393512Z","title":"Bubble wall velocities in local equilibrium,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.393512Z"},"links":{"cited_paper":"/paper/2109.13710","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:066f27ce1ce24b6e5c3c662cab76ac0fdf2b20c29fa3a877c0e8fafc89e3739f","observation_id":"e8d569d1-0826-4af7-83bc-397d8aff7322","resolution":{"observed_at":"2026-08-16T12:08:28.393512Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.02393","last_updated":"2021-11-03T17:58:29Z","snapshot_observed_at":"2026-08-18T01:39:35.771359Z","submitted_at":"2021-11-03T17:58:29Z","title":"Electroweak bubble wall expansion: gravitational waves and baryogenesis in Standard Model-like thermal plasma","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.02393","snapshot_observed_at":"2026-08-16T12:08:28.401758Z","title":"Electroweak bubble wall expansion: gravitational waves and baryogenesis in Standard Model-like thermal plasma,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.401758Z"},"links":{"cited_paper":"/paper/2111.02393","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:00aafb8ead395becea3d1f73b88872fa435758a06dd78b0269072c0058b37dfc","observation_id":"c0188533-202e-4aa4-9904-e35054c8ecca","resolution":{"observed_at":"2026-08-16T12:08:28.401758Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.12548","last_updated":"2022-02-15T12:48:21Z","snapshot_observed_at":"2026-08-16T17:32:54.567762Z","submitted_at":"2021-12-21T17:33:30Z","title":"A sonic boom in bubble wall friction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.12548","snapshot_observed_at":"2026-08-16T12:08:28.408153Z","title":"A sonic boom in bubble wall friction,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.408153Z"},"links":{"cited_paper":"/paper/2112.12548","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:1faf7db740ecf16785e8515e2018974dca304062e36126caea75f662332e8d26","observation_id":"4dd92036-40f3-43c4-929c-cf729be0244b","resolution":{"observed_at":"2026-08-16T12:08:28.408153Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.13142","last_updated":"2023-05-03T14:48:59Z","snapshot_observed_at":"2026-08-19T16:50:53.570148Z","submitted_at":"2022-11-23T17:17:51Z","title":"Bubble wall velocity during electroweak phase transition in the inert doublet model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.13142","snapshot_observed_at":"2026-08-16T12:08:28.490857Z","title":"Bubble wall velocity during electroweak phase transition in the inert doublet model,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.490857Z"},"links":{"cited_paper":"/paper/2211.13142","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:44ce25501e16d68a2cd240ad83d7aaff0de0f04cfe78b40599c7f48ad4c478f2","observation_id":"4da594e8-531a-4480-854f-2b2714bbba88","resolution":{"observed_at":"2026-08-16T12:08:28.490857Z","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":"2026-08-19T15:26:54.857377Z","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":"2026-08-16T12:08:28.548624Z","title":"First principles determination of bubble wall velocity,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.548624Z"},"links":{"cited_paper":"/paper/2204.13120","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:11f44e2b5164d624fb22f0a4095a7b7d2db3551708ffa3958b3856dd23a6f536","observation_id":"704d2847-dea5-4378-a55b-b520226eab66","resolution":{"observed_at":"2026-08-16T12:08:28.548624Z","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":"2026-08-16T17:02:27.405505Z","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":"2026-08-16T12:08:28.555230Z","title":"Hydrodynamic backreaction force of cosmological bubble expansion,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.555230Z"},"links":{"cited_paper":"/paper/2205.02492","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:62a67f3788795c7e8a82d83cda230ef2beee395200fad4ee6e00e81785065837","observation_id":"ea38af10-e4f5-49f0-8083-d1dd80f5376d","resolution":{"observed_at":"2026-08-16T12:08:28.555230Z","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":"2026-08-19T15:30:49.985762Z","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":"2026-08-16T12:08:28.562083Z","title":"Model-independent bubble wall velocities in local thermal equilibrium,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.562083Z"},"links":{"cited_paper":"/paper/2303.10171","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:0655bd09fa6f10f49cbf3e1ffaece9f319db9d497a16b29090afd08abee293ac","observation_id":"a88f70b6-25dd-4f12-9727-734d77a9d64d","resolution":{"observed_at":"2026-08-16T12:08:28.562083Z","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":"2026-08-19T15:26:50.086500Z","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":"2026-08-16T12:08:28.637766Z","title":"Hydrodynamical constraints on the bubble wall velocity,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.637766Z"},"links":{"cited_paper":"/paper/2303.18216","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:8ea2cd37a163dc37cec268b44611b1adefac389fd508fdd094025f418af49078","observation_id":"26648d59-ed5b-4274-84b9-ffc4c6b42174","resolution":{"observed_at":"2026-08-16T12:08:28.637766Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.07691","last_updated":"2024-07-31T14:28:27Z","snapshot_observed_at":"2026-08-16T14:52:58.595459Z","submitted_at":"2023-10-11T17:37:24Z","title":"General backreaction force of cosmological bubble expansion","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.07691","snapshot_observed_at":"2026-08-16T12:08:28.670126Z","title":"General backreaction force of cosmological bubble expansion,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.670126Z"},"links":{"cited_paper":"/paper/2310.07691","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:a4359caab9b1800c67ec4080116ce93735191401c48a2495db7a232f7c6d6f85","observation_id":"7e8edaf3-728c-4c23-8b79-df7846fad31f","resolution":{"observed_at":"2026-08-16T12:08:28.670126Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.02354","last_updated":"2023-12-04T21:34:26Z","snapshot_observed_at":"2026-08-20T12:55:28.821337Z","submitted_at":"2023-12-04T21:34:26Z","title":"Bubble wall velocities with an extended fluid Ansatz","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.02354","snapshot_observed_at":"2026-08-16T12:08:28.676204Z","title":"Bubble wall velocities with an extended fluid Ansatz,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.676204Z"},"links":{"cited_paper":"/paper/2312.02354","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:f317598b915644988d5a80340c158787e2d8ed7979a3736f9bbb1d2f64b66119","observation_id":"46e33bee-c163-4e74-8256-4903b314db3a","resolution":{"observed_at":"2026-08-16T12:08:28.676204Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.03849","last_updated":"2025-01-02T02:53:32Z","snapshot_observed_at":"2026-08-16T14:29:08.499218Z","submitted_at":"2024-01-08T12:23:36Z","title":"Confinement Bubble Wall Velocity via Quasiparticle Determination","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.03849","snapshot_observed_at":"2026-08-16T12:08:28.683884Z","title":"Confinement Bubble Wall Velocity via Quasiparticle Determination,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.683884Z"},"links":{"cited_paper":"/paper/2401.03849","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:8ee638b2daac9f21bb1434acde8901cfc3b3df56479f26d905b76c4a8503c02c","observation_id":"da0ff3c6-fd2d-4614-a916-941f8bcac3a4","resolution":{"observed_at":"2026-08-16T12:08:28.683884Z","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":"2026-08-19T15:30:44.846589Z","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":"2026-08-16T12:08:28.690596Z","title":"Criterion for ultra-fast bubble walls: the impact of hydrodynamic obstruction,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.690596Z"},"links":{"cited_paper":"/paper/2401.05911","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:ee879cc7f2ca11555dfd223592667d033c1ef2f5342fd6260f8084fb473a0461","observation_id":"4124daf0-24ab-4af4-a040-c4a520a19bc0","resolution":{"observed_at":"2026-08-16T12:08:28.690596Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.15408","last_updated":"2024-05-07T08:39:12Z","snapshot_observed_at":"2026-08-19T15:31:22.518101Z","submitted_at":"2024-02-23T16:13:57Z","title":"Bubble-wall velocity in local thermal equilibrium: hydrodynamical simulations vs analytical treatment","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.15408","snapshot_observed_at":"2026-08-16T12:08:28.733172Z","title":"Bubble-wall velocity in local thermal equilibrium: hydrodynamical simulations vs analytical treatment,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.733172Z"},"links":{"cited_paper":"/paper/2402.15408","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:02d304ed3ace187edb0681313abb7d6fb9972447170739570b769200b62fbad1","observation_id":"316889a7-9169-4d77-8e40-aaa67f52317b","resolution":{"observed_at":"2026-08-16T12:08:28.733172Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.01949","last_updated":"2024-05-06T17:42:48Z","snapshot_observed_at":"2026-08-16T13:55:42.271640Z","submitted_at":"2024-05-03T09:22:20Z","title":"Bubble wall velocity and gravitational wave in the minimal left-right symmetric model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.01949","snapshot_observed_at":"2026-08-16T12:08:28.795367Z","title":"Bubble wall velocity and gravitational wave in the minimal left-right symmetric model,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.795367Z"},"links":{"cited_paper":"/paper/2405.01949","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:0755e46af6f281420ea0db761a12ea34ea8330177ad3127825e41bbc434da08d","observation_id":"678172cc-61a0-43eb-8023-fdfd59637c01","resolution":{"observed_at":"2026-08-16T12:08:28.795367Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.01596","last_updated":"2024-10-22T09:49:09Z","snapshot_observed_at":"2026-08-16T13:46:36.035490Z","submitted_at":"2024-06-03T17:59:57Z","title":"The hydrodynamics of inverse phase transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.01596","snapshot_observed_at":"2026-08-16T12:08:28.825710Z","title":"The hydrodynamics of inverse phase transitions,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.825710Z"},"links":{"cited_paper":"/paper/2406.01596","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:2af2d86e27d506dc01fec140771640cda549f7485f505fc5b700f567adcb852a","observation_id":"d1cd0bbf-46ee-4b45-a047-ccaf82004056","resolution":{"observed_at":"2026-08-16T12:08:28.825710Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.04970","last_updated":"2024-11-07T18:46:31Z","snapshot_observed_at":"2026-08-19T15:29:52.504312Z","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":"2026-08-16T12:08:28.832446Z","title":"How fast does the WallGo? A package for computing wall velocities in first-order phase transitions,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.832446Z"},"links":{"cited_paper":"/paper/2411.04970","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:7a4fa69d441c6e5e0ca150ae2b3b7bf5c1c7d9f30b951cc8885d7de6894e5a3d","observation_id":"54953340-5536-4444-a2fb-c5966a1ac19a","resolution":{"observed_at":"2026-08-16T12:08:28.832446Z","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":"2026-08-15T17:38:12.700184Z","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":"2026-08-16T12:08:28.838250Z","title":"Bounds on the bubble wall velocity,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.838250Z"},"links":{"cited_paper":"/paper/2411.13641","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:0ef84f2cde4d1297e57a2e38e70c177993f32947ced2498a7cba1036919a8542","observation_id":"e186614d-9a60-4d3d-9ee7-639d6a7cf2ab","resolution":{"observed_at":"2026-08-16T12:08:28.838250Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.15094","last_updated":"2024-11-22T17:49:39Z","snapshot_observed_at":"2026-08-18T19:46:56.659284Z","submitted_at":"2024-11-22T17:49:39Z","title":"Thermalization effects on the dynamics of growing vacuum bubbles","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.15094","snapshot_observed_at":"2026-08-16T12:08:28.844530Z","title":"Thermalization effects on the dynamics of growing vacuum bubbles,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.844530Z"},"links":{"cited_paper":"/paper/2411.15094","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:06d4fe089307b1391867561b082bd5e806a6c9b6189290083d1865dc133e2aca","observation_id":"51e3d995-0404-4907-94db-80818f89d7c0","resolution":{"observed_at":"2026-08-16T12:08:28.844530Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.09266","last_updated":"2024-12-12T13:23:17Z","snapshot_observed_at":"2026-08-19T15:26:11.622794Z","submitted_at":"2024-12-12T13:23:17Z","title":"Non-singular solutions to the Boltzmann equation with a fluid Ansatz","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.09266","snapshot_observed_at":"2026-08-16T12:08:28.931559Z","title":"Non-singular solutions to the Boltzmann equation with a fluid Ansatz,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.931559Z"},"links":{"cited_paper":"/paper/2412.09266","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:6c5d60381aaf35c55e586afb550b16de7c0a923bcbf390a7417fcf4647917928","observation_id":"d5ba533d-ae67-4a21-a345-be278e7b7704","resolution":{"observed_at":"2026-08-16T12:08:28.931559Z","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":"2026-08-19T04:00:16.857903Z","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":"2026-08-16T12:08:28.940203Z","title":"The Discriminant Power of Bubble Wall Velocities: Gravitational Waves and Electroweak Baryogenesis,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.940203Z"},"links":{"cited_paper":"/paper/2504.17841","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:341821108e2b4abc47e73ee62424838b58e550ffeff9b99777d7de3f1721095a","observation_id":"44e0d5ad-d0e1-457d-9dac-8aeb5f65e3ec","resolution":{"observed_at":"2026-08-16T12:08:28.940203Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9203203","last_updated":"1992-03-03T16:32:33Z","snapshot_observed_at":"2026-08-08T00:16:24.653051Z","submitted_at":"1992-03-03T16:32:33Z","title":"Towards the Theory of Cosmological Phase Transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9203203","snapshot_observed_at":"2026-08-16T12:08:28.946244Z","title":"Towards the theory of the electroweak phase transition,","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.946244Z"},"links":{"cited_paper":"/paper/hep-ph/9203203","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:d9b70856bf8878ff7add0f77b24f8cd163037db7a1f97cbc618bdfeda851f5f6","observation_id":"f6d088df-29b2-469d-a1e2-765b6b8d8eb7","resolution":{"observed_at":"2026-08-16T12:08:28.946244Z","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":"2026-08-15T05:52:16.940439Z","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":"2026-08-16T12:08:28.954391Z","title":"Can electroweak bubble walls run away?,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.954391Z"},"links":{"cited_paper":"/paper/0903.4099","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:4e2a98652bb2c5ac124934bf0d28894090903837a3f05224f8613a7ed4f8e0ce","observation_id":"ad62fe46-3189-4cc3-bb03-c420923ce186","resolution":{"observed_at":"2026-08-16T12:08:28.954391Z","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":"2026-08-14T21:10:18.041698Z","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":"2026-08-16T12:08:28.962033Z","title":"Electroweak Bubble Wall Speed Limit,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:28.962033Z"},"links":{"cited_paper":"/paper/1703.08215","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:7af49e0bafc852d6ecb99d332fde53225256060f9b2f1972bea7586908f0fa9c","observation_id":"016020c0-af99-4d61-ab1c-2889b84fd189","resolution":{"observed_at":"2026-08-16T12:08:28.962033Z","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":"2026-08-19T15:25:40.958352Z","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":"2026-08-16T12:08:29.021267Z","title":"Field-theoretic derivation of bubble-wall force,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.021267Z"},"links":{"cited_paper":"/paper/2005.10875","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:93674255a71ece25e461f4354c5def7d3f8615d8adc7616270ecebc23e9d7b6e","observation_id":"093972d6-b169-4b76-9564-7fcb67f5968c","resolution":{"observed_at":"2026-08-16T12:08:29.021267Z","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":"2026-08-14T21:10:44.517931Z","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":"2026-08-16T12:08:29.063000Z","title":"Towards an all-orders calculation of the electroweak bubble wall velocity,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.063000Z"},"links":{"cited_paper":"/paper/2007.10343","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:49717f84bf5368c465d5169f95923cc01233e0d55b45704745f76759416ca66a","observation_id":"b14713dd-ce47-4172-9e57-56d721f6ad9c","resolution":{"observed_at":"2026-08-16T12:08:29.063000Z","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":"2026-08-19T17:24:09.508044Z","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":"2026-08-16T12:08:29.068777Z","title":"Bubble wall velocity: heavy physics effects,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.068777Z"},"links":{"cited_paper":"/paper/2010.02590","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:873dd62411962477fe6368f241cb398d1dbb6b7df1296a53e50c7e992fc8f104","observation_id":"9e352f46-444b-4efb-b494-14efcb2afe26","resolution":{"observed_at":"2026-08-16T12:08:29.068777Z","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":"2026-08-16T17:34:38.941038Z","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":"2026-08-16T12:08:29.075002Z","title":"Friction pressure on relativistic bubble walls,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.075002Z"},"links":{"cited_paper":"/paper/2112.07686","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:7b48415d1c5bf854d99f17a29e3020637ec16db27a97da089436d46c3366a9d3","observation_id":"44c57687-b1db-41da-951e-50fe8a141c7f","resolution":{"observed_at":"2026-08-16T12:08:29.075002Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.10572","last_updated":"2022-12-20T19:00:00Z","snapshot_observed_at":"2026-08-16T16:07:11.274483Z","submitted_at":"2022-12-20T19:00:00Z","title":"Reflections on Bubble Walls","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.10572","snapshot_observed_at":"2026-08-16T12:08:29.081280Z","title":"Reflections on Bubble Walls,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.081280Z"},"links":{"cited_paper":"/paper/2212.10572","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:f5b288fc3f2d5d078105645a416b61c6c9dd911a57d7d1ed0cbeb5a1bca6159a","observation_id":"03e834b0-ae25-44b4-9fbb-3bb55c9b0670","resolution":{"observed_at":"2026-08-16T12:08:29.081280Z","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":"2026-08-18T00:57:57.325057Z","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":"2026-08-16T12:08:29.086833Z","title":"Logarithmically divergent friction on ultrarelativistic bubble walls,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.086833Z"},"links":{"cited_paper":"/paper/2308.10679","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:32d931938a9404df0635f8176df736d400c5cd85d83a4f26d058a48423274b27","observation_id":"cb8474e2-21cc-4b36-9c37-bcfa13949510","resolution":{"observed_at":"2026-08-16T12:08:29.086833Z","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":"2026-08-18T14:00:26.954050Z","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":"2026-08-16T12:08:29.163728Z","title":"Quantisation across bubble walls and friction,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.163728Z"},"links":{"cited_paper":"/paper/2310.06972","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:19696f4d501ebd42dbb5b1ddb2e810abac562576662ab0f2ee5c82aa4cfd13b7","observation_id":"be7078cb-f940-4381-b295-7aff489bbbd1","resolution":{"observed_at":"2026-08-16T12:08:29.163728Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.05615","last_updated":"2024-05-21T09:30:40Z","snapshot_observed_at":"2026-08-17T02:01:15.356358Z","submitted_at":"2024-03-08T19:00:00Z","title":"Particle shells from relativistic bubble walls","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.05615","snapshot_observed_at":"2026-08-16T12:08:29.209444Z","title":"Particle shells from relativistic bubble walls,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.209444Z"},"links":{"cited_paper":"/paper/2403.05615","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:8652319b4165f49d08cb4bdf8e3669c794b632324e037a0e441ff0253eca0bba","observation_id":"0fe64839-db06-4642-a880-2c69287d1f5f","resolution":{"observed_at":"2026-08-16T12:08:29.209444Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.19447","last_updated":"2024-05-29T18:47:24Z","snapshot_observed_at":"2026-08-20T06:34:03.884988Z","submitted_at":"2024-05-29T18:47:24Z","title":"NLO friction in symmetry restoring phase transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.19447","snapshot_observed_at":"2026-08-16T12:08:29.214985Z","title":"NLO friction in symmetry restoring phase transitions,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.214985Z"},"links":{"cited_paper":"/paper/2405.19447","citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:657ed6cb9dd22e39c3def661d4506482f58365f586f3f99e528b3c1ee888890c","observation_id":"554b228e-6f36-4e21-90b1-659a590500db","resolution":{"observed_at":"2026-08-16T12:08:29.214985Z","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":"2026-08-16T12:08:29.220980Z","title":"Brownian motion of a quantum oscillator,","venue":null,"work_id":null,"year":1961},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.220980Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:5102d1c216c0a32957f8530526f21aa4b4510e076398c77c5214c34c3445fb4b","observation_id":"7caf3b07-cae5-46a3-8d30-b464e578cc34","resolution":{"observed_at":"2026-08-16T12:08:29.220980Z","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":"2026-08-16T12:08:29.226088Z","title":"Diagram technique for nonequilibrium processes,","venue":null,"work_id":null,"year":1965},"citing_paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory","version":2},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-16T12:08:29.226088Z"},"links":{"citing_paper":"/paper/2504.13725"},"observation_digest":"sha256:4a0c03b7864faf001cad2d50c0db560ab8fbc0b16e444f8b9d7a1ff3aa13ed9a","observation_id":"c7978070-59f9-48dc-b076-29678d276d65","resolution":{"observed_at":"2026-08-16T12:08:29.226088Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2504.13725","last_updated":"2025-08-12T19:54:01Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-17T21:27:10.939039Z","submitted_at":"2025-04-18T14:50:03Z","title":"Bubble wall dynamics from nonequilibrium quantum field theory"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":100,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":138},"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":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"thesis":"As of 20 August 2026, this Paper Citation Record lists 100 of 138 outbound references and 12 inbound Pith citation observations for arXiv:2504.13725."}