{"as_of":"2026-08-03T12:18:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6889adc99ffd04c4f51a48a0fb7fbec33b94d6db5c5fedfb1bed51aa74bec3b9","coverage":[{"denominator":113,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-05-09T22:00:42.126071Z","state":"measured"},{"denominator":101,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":101,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-03T06:30:56.289259+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-01T14:27:25.955223Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.21492","snapshot_observed_at":"2026-08-01T14:27:25.955223Z","title":"Choudhury, J","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.18803","last_updated":"2026-07-21T07:30:45Z","snapshot_observed_at":"2026-08-01T14:27:10.337287Z","submitted_at":"2026-07-21T07:30:45Z","title":"A Non-Holomorphic Modular $A_4$ Framework for Resonant Leptogenesis with Gravitational Wave Signatures","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-01T14:27:25.955223Z"},"links":{"cited_paper":"/paper/2604.21492","citing_paper":"/paper/2607.18803"},"observation_digest":"sha256:838fa9e85571b682d03755ac2479ba21c21f25bff6d098bfe40dd23c8e896949","observation_id":"3d9d44cf-681d-4d55-8b4a-9e38e8f5aca7","resolution":{"observed_at":"2026-08-01T14:27:25.955223Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2604.21492/citation-record","integrity":"/paper/2604.21492/integrity","json":"/paper/2604.21492/citation-record.json","paper":"/paper/2604.21492"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Sakharov,Violation of cp invariance, c asymmetry, and baryon asymmetry of the universe,Soviet Physics Uspekhi34(1991) 392","venue":null,"work_id":"dc2c9a46-f654-43e1-b10c-97ffdf883d83","year":1991},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:7a5490a0eb4c37ff9903e6c89f0855d99ee165e5cbf824f2ed0d43e20671862f","observation_id":"94fd27f9-4337-49fc-97dc-1ebe3ddad3bb","resolution":{"observed_at":"2026-05-23T15:15:42.392158Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0404175","last_updated":"2004-08-13T15:46:27Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2004-04-21T13:12:59Z","title":"Particle Dark Matter: Evidence, Candidates and Constraints","version":2},"cited_work":{"arxiv_id":"hep-ph/0404175","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0404175","snapshot_observed_at":"2026-07-10T14:47:14.453944Z","title":"Particle Dark Matter: Evidence, Candidates and Constraints","venue":"hep-ph","work_id":"9f1f415a-e524-408a-8b8d-07c41bbab6c3","year":2004},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/0404175","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:9b22a1af687c89b18ebe8c32f8b82346f7e12f69b36e8e2a56d6c960cbddd2a8","observation_id":"22e7f5cf-fb34-4942-802a-663bf547eb1b","resolution":{"observed_at":"2026-05-11T14:21:05.650232Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9605288","last_updated":"1996-05-12T15:53:42Z","snapshot_observed_at":"2026-07-07T04:22:39.163372Z","submitted_at":"1996-05-12T15:53:42Z","title":"Is There a Hot Electroweak Phase Transition at $m_H\\gsim m_W$?","version":1},"cited_work":{"arxiv_id":"hep-ph/9605288","doi":"10.1103/physrevlett.77.2887","metadata_source":"pith","pith_arxiv_id":"hep-ph/9605288","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Is There a Hot Electroweak Phase Transition at $m_H\\gsim m_W$?","venue":"hep-ph","work_id":"37be07d8-d732-4d01-9390-cea888dd3492","year":1996},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9605288","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:66a76ad64f37cdb046dc070802445df1ae9388c157af9d016aac69bdafb3059b","observation_id":"4da2aff0-3262-40e1-9ca8-9bb81861f8fe","resolution":{"observed_at":"2026-05-11T14:21:05.677659Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-05-24T15:26:12.638354+00:00","source":"crossref_status_cache"},{"observed_at":"2026-05-24T15:26:12.638354+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9809291","last_updated":"1998-09-07T18:07:10Z","snapshot_observed_at":"2026-07-07T04:30:37.815561Z","submitted_at":"1998-09-07T18:07:10Z","title":"Endpoint of the hot electroweak phase transition","version":1},"cited_work":{"arxiv_id":"hep-ph/9809291","doi":"10.1103/physrevlett.82.21","metadata_source":"pith","pith_arxiv_id":"hep-ph/9809291","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Endpoint of the hot electroweak phase transition","venue":"hep-ph","work_id":"7d9ad881-9192-417f-943c-723e209d3af2","year":1998},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9809291","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:ab49051904c430ea7a629f7871f8ba92a0528a02ba006c7d553f598bb5074cee","observation_id":"b4bc2ba2-9ae8-4962-b8ff-034ae72c6ff5","resolution":{"observed_at":"2026-05-11T14:21:05.626434Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1508.07161","last_updated":"2015-08-28T10:42:18Z","snapshot_observed_at":"2026-07-06T04:27:58.649660Z","submitted_at":"2015-08-28T10:42:18Z","title":"The Standard Model cross-over on the lattice","version":1},"cited_work":{"arxiv_id":"1508.07161","doi":null,"metadata_source":"pith","pith_arxiv_id":"1508.07161","snapshot_observed_at":"2026-07-03T09:27:48.852037Z","title":"The Standard Model cross-over on the lattice","venue":"hep-ph","work_id":"68fecdf3-9f96-44ff-9e42-20f34a5d5103","year":2015},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1508.07161","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:971987e3fd6cb15962e9e73c4b29e9bfd78cc7db05d52bd6ed1f560fcb741efd","observation_id":"8b949543-dc1c-472c-b230-2e5b81be17bd","resolution":{"observed_at":"2026-05-11T14:21:05.718432Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0706.4311","last_updated":"2007-06-28T20:06:11Z","snapshot_observed_at":"2026-07-06T01:31:38.875888Z","submitted_at":"2007-06-28T20:06:11Z","title":"LHC Phenomenology of an Extended Standard Model with a Real Scalar Singlet","version":1},"cited_work":{"arxiv_id":"0706.4311","doi":null,"metadata_source":"pith","pith_arxiv_id":"0706.4311","snapshot_observed_at":"2026-07-03T15:48:35.541845Z","title":"LHC Phenomenology of an Extended Standard Model with a Real Scalar Singlet","venue":"hep-ph","work_id":"54938c2b-7242-4a22-91bd-95a9e488e62b","year":2007},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/0706.4311","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:12c498fca6b0ca4b8be8100d61b7098af3a1ca2654b0edc81e1b4583bdf5427a","observation_id":"5e391fd4-b788-43fc-8cf0-61845c0a9a0e","resolution":{"observed_at":"2026-05-11T14:21:05.614161Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1107.5441","last_updated":"2011-07-27T11:09:25Z","snapshot_observed_at":"2026-07-06T02:31:32.394007Z","submitted_at":"2011-07-27T11:09:25Z","title":"Strong Electroweak Phase Transitions in the Standard Model with a Singlet","version":1},"cited_work":{"arxiv_id":"1107.5441","doi":null,"metadata_source":"pith","pith_arxiv_id":"1107.5441","snapshot_observed_at":"2026-07-03T15:48:35.584307Z","title":"Strong Electroweak Phase Transitions in the Standard Model with a Singlet","venue":"hep-ph","work_id":"1cbe2cf4-d7df-4ed4-9434-f239005483fd","year":2011},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1107.5441","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:5b712d66fce316d2c533d9605e77f3e4230ff10376c39c110d70c9f946aa5bfd","observation_id":"12fac02a-91b5-4c9f-baf2-9b622343c150","resolution":{"observed_at":"2026-05-11T14:21:05.635065Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0711.3018","last_updated":"2008-06-11T17:21:02Z","snapshot_observed_at":"2026-07-06T01:35:46.153755Z","submitted_at":"2007-11-20T19:33:28Z","title":"Higgs Self-Coupling as a Probe of Electroweak Phase Transition","version":3},"cited_work":{"arxiv_id":"0711.3018","doi":null,"metadata_source":"pith","pith_arxiv_id":"0711.3018","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Higgs Self-Coupling as a Probe of Electroweak Phase Transition","venue":"hep-ph","work_id":"81df47d0-0f29-40c1-89b3-634c77746749","year":2007},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/0711.3018","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:754958d13af90f16a1dacb79a6f7e4349fae79cfe5dfad36c76037fcfc1fe584","observation_id":"04a96942-da37-47d7-9a6e-123fff924286","resolution":{"observed_at":"2026-05-11T14:21:05.688056Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1210.4196","last_updated":"2013-06-07T09:01:47Z","snapshot_observed_at":"2026-07-06T02:57:42.468624Z","submitted_at":"2012-10-15T21:21:52Z","title":"Electroweak baryogenesis and dark matter from a singlet Higgs","version":3},"cited_work":{"arxiv_id":"1210.4196","doi":null,"metadata_source":"pith","pith_arxiv_id":"1210.4196","snapshot_observed_at":"2026-07-03T15:48:35.610722Z","title":"Cline and K","venue":"hep-ph","work_id":"56f11de4-66b2-4451-b701-4232c9841e81","year":2012},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1210.4196","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:ead0d3d466065aa8629e29a66b39a6b589ad4b7010f8f48630e4920209e17982","observation_id":"70a0760a-aa55-4c4d-8069-449d8c42a31a","resolution":{"observed_at":"2026-05-11T14:21:05.834792Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1407.0688","last_updated":"2015-07-14T10:03:53Z","snapshot_observed_at":"2026-08-01T19:45:28.163250Z","submitted_at":"2014-07-02T19:33:22Z","title":"Strong phase transition, dark matter and vacuum stability from simple hidden sectors","version":2},"cited_work":{"arxiv_id":"1407.0688","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1407.0688","snapshot_observed_at":"2026-07-04T20:28:31.350830Z","title":"Alanne, K","venue":null,"work_id":"b99193cb-b7c1-4942-816e-620abfd314d8","year":2014},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1407.0688","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:aeadf2da372f5f7dcab4b62f22a3cf6a9e954dd131750e43355268a90ee6b76d","observation_id":"96b8cd32-60e1-4286-8ed9-dc420b439c0b","resolution":{"observed_at":"2026-07-04T20:28:31.350830Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1306.4710","last_updated":"2015-08-05T21:47:00Z","snapshot_observed_at":"2026-07-06T03:16:20.483507Z","submitted_at":"2013-06-19T22:22:50Z","title":"Update on scalar singlet dark matter","version":5},"cited_work":{"arxiv_id":"1306.4710","doi":"10.1103/physrevd.88.055025","metadata_source":"pith","pith_arxiv_id":"1306.4710","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Update on scalar singlet dark matter","venue":"hep-ph","work_id":"62f5cd9f-4a77-4ab8-b53a-2d9372b87fd9","year":2013},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1306.4710","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:fcdd91ebcfe6f0bf845f67a7f6178f18ad776a48e2f1e25d7b88bb4f2f79b304","observation_id":"28d2b5c4-6d11-4815-9d5f-7b22777b2e4c","resolution":{"observed_at":"2026-05-11T14:21:05.702738Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1912.12634","last_updated":"2020-07-17T00:05:05Z","snapshot_observed_at":"2026-07-06T08:47:28.564867Z","submitted_at":"2019-12-29T11:22:31Z","title":"First-order electroweak phase transition in a complex singlet model with $\\mathbb{Z}_3$ symmetry","version":2},"cited_work":{"arxiv_id":"1912.12634","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1912.12634","snapshot_observed_at":"2026-07-03T15:48:35.549509Z","title":"Chiang and B.-Q","venue":null,"work_id":"c04a18a9-18f3-404f-8862-0c90442f59ac","year":2020},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1912.12634","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:3980457781ddaf51f4e212bf4724f1bd801ae59709a1ec77e2380cbabedecad0","observation_id":"c0ace2fd-9c5b-4264-bff1-d229e22c04df","resolution":{"observed_at":"2026-05-11T14:21:06.128887Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.13136","last_updated":"2019-08-07T09:22:36Z","snapshot_observed_at":"2026-07-06T08:11:17.778786Z","submitted_at":"2019-07-30T18:00:01Z","title":"Gravitational Wave Signals of Pseudo-Goldstone Dark Matter in the $\\mathbb{Z}_{3}$ Complex Singlet Model","version":2},"cited_work":{"arxiv_id":"1907.13136","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1907.13136","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Kannike, K","venue":null,"work_id":"0b9f4152-ea5f-40c8-b386-26d1bc6b6db8","year":2020},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1907.13136","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:43b158f04c40b7c250be3394deae48599224b6dfa7ce4f9c60e50f757a541269","observation_id":"f12af695-8119-4292-9060-96b89b15eeef","resolution":{"observed_at":"2026-05-11T14:21:05.824789Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2507.05917","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-03T15:48:35.642192Z","title":"Srivastava, J","venue":null,"work_id":"51b4a47e-6d01-4049-982a-6a86639beb36","year":2026},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:3e7a12086f05e18e1108bd9cbcbfec77610bf76b1852292aaf8fa6afbda1b196","observation_id":"865afed5-30ed-416b-b1a8-99941987db91","resolution":{"observed_at":"2026-05-11T14:21:06.216101Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2206.08699","last_updated":"2022-08-05T12:06:43Z","snapshot_observed_at":"2026-07-06T13:21:57.238438Z","submitted_at":"2022-06-17T11:32:16Z","title":"Study of entropy production due to electroweak phase transition in $Z_2$ symmetric extension of the Standard Model","version":2},"cited_work":{"arxiv_id":"2206.08699","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2206.08699","snapshot_observed_at":"2026-07-03T15:48:35.566166Z","title":"Chaudhuri and J","venue":null,"work_id":"75182cf4-ccda-4851-9b1c-ad281c3be3b0","year":2022},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2206.08699","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:46a3b75c440ffec1a4daf2006854cee28ddeaafceddede4be74f7b7a319174e8","observation_id":"d2823f4e-5d5c-4cdc-be41-8fe421f650f4","resolution":{"observed_at":"2026-05-11T14:21:05.762346Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2601.13147","last_updated":"2026-06-05T19:03:55Z","snapshot_observed_at":"2026-08-03T09:44:49.273216Z","submitted_at":"2026-01-19T15:30:02Z","title":"Revisiting Singlet Fermion Dark Matter with a Scalar Portal: Connecting Higgs Phenomenology and Strong Electroweak Phase Transition","version":4},"cited_work":{"arxiv_id":"2601.13147","doi":null,"metadata_source":"pith","pith_arxiv_id":"2601.13147","snapshot_observed_at":"2026-07-03T15:48:35.644670Z","title":"Revisiting Singlet Fermion Dark Matter with a Scalar Portal: Connecting Higgs Phenomenology and Strong Electroweak Phase Transition","venue":"hep-ph","work_id":"896ee673-750f-44ff-82c9-d992fe45f394","year":2026},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2601.13147","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:73b3adf4e683c5964d22558ebe30b326aebe7e36ca03fffae5eba8cf14ccd3b1","observation_id":"5167671e-b92d-42e6-adac-aa7ca5ccd23c","resolution":{"observed_at":"2026-06-09T02:05:23.339076Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2212.09659","last_updated":"2022-12-19T17:40:21Z","snapshot_observed_at":"2026-07-06T14:32:33.541029Z","submitted_at":"2022-12-19T17:40:21Z","title":"Single-step first order phase transition and gravitational waves in a SIMP dark matter scenario","version":1},"cited_work":{"arxiv_id":"2212.09659","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2212.09659","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Chakrabarty, H","venue":null,"work_id":"339d862d-7eb1-4b15-957c-deffa52843a9","year":2024},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2212.09659","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:b0bcf77265f912fa61a68eff75e7b9cace2cc342df981b8cb21961cb09bbe422","observation_id":"d953182b-d9ee-4bed-8fc1-03d97b627e1f","resolution":{"observed_at":"2026-05-11T14:21:05.844046Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2103.14022","last_updated":"2021-10-14T11:54:12Z","snapshot_observed_at":"2026-07-06T10:53:28.085825Z","submitted_at":"2021-03-25T17:58:40Z","title":"A new perspective on the electroweak phase transition in the Standard Model Effective Field Theory","version":3},"cited_work":{"arxiv_id":"2103.14022","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2103.14022","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Camargo-Molina, R","venue":null,"work_id":"4540eda4-d341-48e8-a96c-0d2004a97148","year":2021},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2103.14022","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:e1d82af966ffdd7b8b1ff12fb8b2138b46e94255ccb0f3f8ce795a7db2d7359a","observation_id":"28ff752a-fe23-4294-a6e7-35a523f6e69b","resolution":{"observed_at":"2026-05-11T14:21:06.118521Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2210.11241","last_updated":"2025-09-10T11:34:15Z","snapshot_observed_at":"2026-07-06T14:08:10.679611Z","submitted_at":"2022-10-20T13:13:14Z","title":"SMEFT effects on gravitational wave spectrum from electroweak phase transition","version":3},"cited_work":{"arxiv_id":"2210.11241","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2210.11241","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Hashino and D","venue":null,"work_id":"cbe60cc9-a4a9-4a3c-9e40-ad8404b85103","year":2023},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2210.11241","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:c8407859ec25a244e5e24dd6c1b09b0c6f643bac438bbd5c3f5d8583dbe01793","observation_id":"40139a0b-8912-4a12-89b3-962d2937d73f","resolution":{"observed_at":"2026-05-11T14:21:05.866859Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2403.01591","last_updated":"2024-05-23T20:13:51Z","snapshot_observed_at":"2026-07-06T17:38:51.653737Z","submitted_at":"2024-03-03T19:09:46Z","title":"Electroweak Phase Transition in Singlet Extensions of The Standard Model with Dimension-Six Operators","version":2},"cited_work":{"arxiv_id":"2403.01591","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2403.01591","snapshot_observed_at":"2026-07-03T15:48:35.590195Z","title":"Oikonomou and A","venue":null,"work_id":"58963da4-09cb-47ce-9b29-87e1f93809f1","year":2024},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2403.01591","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:a6cd58ce40e19a2c5a033f62e4aebeef835e482b49a86950d962bde9de145a8b","observation_id":"8e9cc200-4b11-4d16-9734-03cc9955ee73","resolution":{"observed_at":"2026-05-11T14:21:05.792624Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Anderson and L.J","venue":null,"work_id":"945ec824-81e6-4a63-b39b-aef94b20d38b","year":1992},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:0f5a7592eefe1dcc40c659d6c6cde8022b5403dc418a7edf3871536741006363","observation_id":"0cde54b8-a618-415f-84d8-b76dacf9dbee","resolution":{"observed_at":"2026-05-23T15:15:42.388449Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9301277","last_updated":"1993-01-26T18:24:00Z","snapshot_observed_at":"2026-07-07T04:15:01.181188Z","submitted_at":"1993-01-26T18:24:00Z","title":"Operator Analysis for the Higgs Potential and Cosmological Bound on the Higgs-Boson Mass","version":1},"cited_work":{"arxiv_id":"hep-ph/9301277","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9301277","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Operator Analysis for the Higgs Potential and Cosmological Bound on the Higgs-Boson Mass","venue":"hep-ph","work_id":"aabbff99-0f4e-4e51-b490-1079b8cdbee2","year":1993},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9301277","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:9fe17c7d4eb7a5a2badecfc514509a22881ecbaf869915012e6c101086c291b1","observation_id":"b66aaa88-c85e-4359-bb7e-f9b6517b3b4d","resolution":{"observed_at":"2026-05-11T14:21:05.951220Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-08T18:35:27.409414Z","title":"Fukugita and T","venue":null,"work_id":"4a7d0a61-decb-45b2-9a3d-378f72f1cdec","year":1986},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:ee78a35cad988cc72adc0d79f581aa54f27675f2d096d058cd422dd8e319ba49","observation_id":"653e37d7-d3ad-4f70-a60f-ed704056a98d","resolution":{"observed_at":"2026-05-23T15:15:42.374501Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9707235","last_updated":"1997-07-03T12:07:40Z","snapshot_observed_at":"2026-07-07T04:26:14.581072Z","submitted_at":"1997-07-03T12:07:40Z","title":"CP Violation and Baryogenesis due to Heavy Majorana Neutrinos","version":1},"cited_work":{"arxiv_id":"hep-ph/9707235","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9707235","snapshot_observed_at":"2026-07-04T20:20:08.089752Z","title":"CP Violation and Baryogenesis due to Heavy Majorana Neutrinos","venue":"hep-ph","work_id":"0e7bf87c-0933-4055-96a0-a7ca00b45fce","year":1997},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9707235","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:817595944ba43e7bab56bfd2aea3dd89d74d636e94297d0d21f78c108033b49b","observation_id":"70526dea-72ae-4566-9f65-57d6604bf75f","resolution":{"observed_at":"2026-05-11T14:21:06.158298Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0502169","last_updated":"2006-03-08T16:45:06Z","snapshot_observed_at":"2026-07-07T04:06:42.047196Z","submitted_at":"2005-02-18T16:01:12Z","title":"Leptogenesis as the origin of matter","version":2},"cited_work":{"arxiv_id":"hep-ph/0502169","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0502169","snapshot_observed_at":"2026-07-04T16:59:59.057005Z","title":"Leptogenesis as the origin of matter","venue":"hep-ph","work_id":"78131fa8-d3a4-434d-a16d-f85686ac72bd","year":2005},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/0502169","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:869e2935570419f3238dac1d99a47d2f2bdf4ae22c3a4d33779b05a4f4221ea2","observation_id":"46f2399b-f935-48da-b7bf-b16a5649e844","resolution":{"observed_at":"2026-05-11T14:21:05.997708Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0802.2962","last_updated":"2008-06-06T18:05:54Z","snapshot_observed_at":"2026-07-06T01:35:41.376119Z","submitted_at":"2008-02-20T23:35:35Z","title":"Leptogenesis","version":3},"cited_work":{"arxiv_id":"0802.2962","doi":null,"metadata_source":"pith","pith_arxiv_id":"0802.2962","snapshot_observed_at":"2026-07-04T17:09:58.350984Z","title":"Leptogenesis","venue":"hep-ph","work_id":"7aa9783c-57f0-409f-96ac-75e49833a0f8","year":2008},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/0802.2962","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:4f03464a7a1df4d916eb88cdebf18874b36d1c918a1c6c54a2042e4b202ca213","observation_id":"ffd3f880-f42b-480b-b0f6-cb6c9b6672ad","resolution":{"observed_at":"2026-05-11T14:21:06.111972Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2206.07037","last_updated":"2022-06-14T17:55:04Z","snapshot_observed_at":"2026-07-06T13:20:47.902165Z","submitted_at":"2022-06-14T17:55:04Z","title":"Searches for heavy neutrinos at multi-TeV muon collider : a resonant leptogenesis perspective","version":1},"cited_work":{"arxiv_id":"2206.07037","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2206.07037","snapshot_observed_at":"2026-07-04T04:09:33.815091Z","title":"Chakraborty, H","venue":null,"work_id":"c3971986-ceff-4af7-b271-ad31314ff48d","year":2023},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2206.07037","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:466b8ffeb25ff7d3a5485cc0c3c8d1d96ce5514bdd11ff0cf4ef3d0684ea6127","observation_id":"83260085-049b-487b-9560-ae13f344718e","resolution":{"observed_at":"2026-05-11T14:21:05.936903Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1908.00909","last_updated":"2019-08-02T15:30:26Z","snapshot_observed_at":"2026-07-06T08:12:02.357580Z","submitted_at":"2019-08-02T15:30:26Z","title":"MeV scale model of SIMP dark matter, neutrino mass and leptogenesis","version":1},"cited_work":{"arxiv_id":"1908.00909","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1908.00909","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Mohanty, A","venue":null,"work_id":"f7a962b1-3a40-40ac-922c-1ea1da47a3dc","year":2020},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1908.00909","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:897f8e7c20bbed29b6b2cfe1d78572dc90fcaec0d375b3272f0273e23e89d59c","observation_id":"2d3880ca-1c54-4499-a375-a9b9f1f1de8d","resolution":{"observed_at":"2026-05-11T14:21:06.016142Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2312.15053","last_updated":"2024-06-14T17:46:46Z","snapshot_observed_at":"2026-07-06T17:07:23.809593Z","submitted_at":"2023-12-22T20:32:25Z","title":"Leptogenesis, Dark Matter and Gravitational Waves from Discrete Symmetry Breaking","version":2},"cited_work":{"arxiv_id":"2312.15053","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2312.15053","snapshot_observed_at":"2026-07-04T11:29:51.237575Z","title":"Bhattacharya, N","venue":null,"work_id":"de8e8530-d90d-46d5-8c31-d81153523e2d","year":2024},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2312.15053","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:da7b1d4a5ad1de79f7c4400f29ac7f18a4f45ece297eae1aabf68956fed253db","observation_id":"e51a0b29-5cc7-4196-933e-9927760b06dc","resolution":{"observed_at":"2026-05-11T14:21:06.323976Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2504.03837","last_updated":"2026-04-12T10:02:55Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-04-04T18:00:02Z","title":"Exploring Leptogenesis in the Era of First Order Electroweak Phase Transition","version":2},"cited_work":{"arxiv_id":"2504.03837","doi":null,"metadata_source":"pith","pith_arxiv_id":"2504.03837","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Exploring Leptogenesis in the Era of First Order Electroweak Phase Transition","venue":"hep-ph","work_id":"c6bf1d65-eaa5-48ba-95b9-ac3c612a47a7","year":2025},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2504.03837","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:1edae430ddc5c9cbe0f5c7b559cf4dfe3b5d1d287c1fdd3eb1e56111f27c841d","observation_id":"babc7324-0e13-44da-9735-9e37f6e7aa21","resolution":{"observed_at":"2026-05-11T14:21:05.727464Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9603208","last_updated":"1996-04-10T13:31:09Z","snapshot_observed_at":"2026-08-01T15:54:39.239374Z","submitted_at":"1996-03-01T17:54:47Z","title":"Electroweak Baryon Number Non-Conservation in the Early Universe and in High Energy Collisions","version":2},"cited_work":{"arxiv_id":"hep-ph/9603208","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9603208","snapshot_observed_at":"2026-07-04T17:09:58.305762Z","title":"Rubakov and M.E","venue":"hep-ph","work_id":"499c3c1e-2c84-4221-8e3b-0e8612a31ce0","year":1996},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9603208","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:c480fc9a0afcd86722bdf685c42fc1a3fcded9a8d0560182f7147d8a514ab913","observation_id":"0929ff98-0e5e-4d13-9cfa-1fa90e9b0898","resolution":{"observed_at":"2026-05-11T14:21:05.815507Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Klinkhamer and N.S","venue":null,"work_id":"53fe1bb0-113a-49ed-befe-216b9028ea12","year":1984},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:f89556208347796997370c05aaef7ab0d2f35ef580fa08b19ee8cfeb4f890f22","observation_id":"51a01141-55ac-42a4-9a53-e53d685f924e","resolution":{"observed_at":"2026-05-23T15:15:42.377006Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Manton,Topology in the Weinberg-Salam Theory,Phys","venue":null,"work_id":"93cc0ce4-eef6-46a6-813c-aa8713dea5f5","year":1983},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:b72ff87342bd71af605a51926c52680cce2b3cc1ad040ae41130765262a0a3ae","observation_id":"68bfeec0-0f65-4705-9bb9-0ef9a72b8a85","resolution":{"observed_at":"2026-05-23T15:15:42.382406Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2007.14792","last_updated":"2020-07-27T18:00:02Z","snapshot_observed_at":"2026-07-06T09:42:46.838901Z","submitted_at":"2020-07-27T18:00:02Z","title":"The fate of hints: updated global analysis of three-flavor neutrino oscillations","version":1},"cited_work":{"arxiv_id":"2007.14792","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2007.14792","snapshot_observed_at":"2026-07-04T10:49:46.018050Z","title":"Esteban, M","venue":null,"work_id":"084f39cb-6d45-4459-9ca0-5d3b13e0113a","year":2020},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2007.14792","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:a4dce076b2f145feadbfd6e16333cf325e7f5b0bee01385dab8a50605dc35751","observation_id":"d6d47ea9-a67d-4435-af0a-b7b27985aaa3","resolution":{"observed_at":"2026-05-11T14:21:06.282607Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"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":"astro-ph/9310044","doi":null,"metadata_source":"pith","pith_arxiv_id":"astro-ph/9310044","snapshot_observed_at":"2026-07-04T01:59:25.494969Z","title":"Gravitational Radiation from First-Order Phase Transitions","venue":"astro-ph","work_id":"97dbea29-8566-49b2-b259-f414042bb63c","year":1993},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/astro-ph/9310044","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:8294f31b4724f6930153e0ac13db18abf33683349f9aa15abeac7fdf49e197ae","observation_id":"f3c3897f-b19f-432c-acaf-2f58dcd3f0f9","resolution":{"observed_at":"2026-05-11T14:21:06.150086Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1809.08242","last_updated":"2019-04-02T16:56:31Z","snapshot_observed_at":"2026-07-06T07:03:35.666378Z","submitted_at":"2018-09-21T18:00:01Z","title":"On the Maximal Strength of a First-Order Electroweak Phase Transition and its Gravitational Wave Signal","version":2},"cited_work":{"arxiv_id":"1809.08242","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1809.08242","snapshot_observed_at":"2026-07-04T04:59:35.181447Z","title":"Ellis, M","venue":null,"work_id":"bf0934bc-344d-4667-9b8a-2ac3b35b7d43","year":2019},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1809.08242","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:4a24f784a2d2f9ec508a031c5d1be93352593abae6e5d6e2a6e3e317b322ca16","observation_id":"355c4e0e-5e92-4789-80ba-43aacaaed091","resolution":{"observed_at":"2026-05-11T14:21:05.810204Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1809.01441","last_updated":"2019-07-15T09:16:20Z","snapshot_observed_at":"2026-07-06T06:59:18.703646Z","submitted_at":"2018-09-05T11:33:54Z","title":"Planck Mass Charged Gravitino Dark Matter","version":3},"cited_work":{"arxiv_id":"1809.01441","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1809.01441","snapshot_observed_at":"2026-07-03T18:18:50.182376Z","title":"Croon et al.,Gravitational waves from strongly coupled phase transitions,JHEP01 (2019) 081 [1809.01441]","venue":null,"work_id":"a4aa77d5-20b0-43e9-82a3-6ae57d5b07ac","year":2019},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1809.01441","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:2295a51fe14871658070c0999b8b59cfa9f3aecb667b397aa6ee6d40dc89a088","observation_id":"deec894b-6c5d-4dd3-a873-8e486f1dbb0e","resolution":{"observed_at":"2026-05-11T14:21:05.890960Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1803.03264","last_updated":"2019-02-14T17:52:40Z","snapshot_observed_at":"2026-07-06T06:27:21.963345Z","submitted_at":"2018-03-08T19:00:01Z","title":"Search for Boosted Dark Matter at ProtoDUNE","version":2},"cited_work":{"arxiv_id":"1803.03264","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1803.03264","snapshot_observed_at":"2026-07-04T23:23:26.716639Z","title":"Beniwal et al.,Gravitational waves from electroweak phase transitions,JHEP02(2019) 183 [1803.03264]","venue":null,"work_id":"cd319ef3-484a-481a-87bc-07efc6103d20","year":2019},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1803.03264","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:c021ea883a8c9685f28cf9f097fd5d75c54a909ce34464cb3698476847b1dd57","observation_id":"805a7c4d-3614-40ba-b2b3-a75799363186","resolution":{"observed_at":"2026-07-04T23:23:26.716639Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1709.04843","last_updated":"2019-09-18T00:29:45Z","snapshot_observed_at":"2026-07-06T05:59:39.997438Z","submitted_at":"2017-09-14T15:40:39Z","title":"Multivariate reciprocal inverse Gaussian distributions from the Sabot -Tarr\\`es -Zeng integral","version":2},"cited_work":{"arxiv_id":"1709.04843","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1709.04843","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Huang et al.,Cosmological phase transition and gravitational wave signals,Phys","venue":null,"work_id":"ac364355-ae02-442e-aaa7-dab8057e3344","year":2018},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1709.04843","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:d2d5b2ebbbc1d33cef3499f36b7be5dfec5d89a5809f74545a7967cd57c759e1","observation_id":"4fa52967-b2c4-47f3-b296-02f5400e61c6","resolution":{"observed_at":"2026-05-11T14:21:05.786915Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1809.04994","last_updated":"2018-09-13T14:45:02Z","snapshot_observed_at":"2026-07-06T07:01:59.869677Z","submitted_at":"2018-09-13T14:45:02Z","title":"Fingerprinting models of first-order phase transitions by the synergy between collider and gravitational-wave experiments","version":1},"cited_work":{"arxiv_id":"1809.04994","doi":null,"metadata_source":"pith","pith_arxiv_id":"1809.04994","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Fingerprinting models of first-order phase transitions by the synergy between collider and gravitational-wave experiments","venue":"hep-ph","work_id":"9cdb5068-69cc-4ce2-86a0-fced061cf367","year":2018},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1809.04994","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:a819d637d57ea511e511787244a73bc2c9fdca8a69bd341878ba3294a99085da","observation_id":"4c14b5f4-7f2a-4ce8-929a-29dbaac513e5","resolution":{"observed_at":"2026-05-11T14:21:06.005009Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1712.00087","last_updated":"2018-12-11T08:30:36Z","snapshot_observed_at":"2026-07-06T06:12:09.658727Z","submitted_at":"2017-11-30T21:21:53Z","title":"Gravitational waves from phase transition in split NMSSM","version":2},"cited_work":{"arxiv_id":"1712.00087","doi":null,"metadata_source":"pith","pith_arxiv_id":"1712.00087","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Gravitational waves from phase transition in split NMSSM","venue":"hep-ph","work_id":"335c7986-805d-4621-a030-e9d475b008ea","year":2017},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1712.00087","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:9b01a63117bca66b2d60504a535a6e6b51d7293e09d1e06e98096ba9521543c2","observation_id":"efc65419-64e6-4b77-ace2-d430374c4e64","resolution":{"observed_at":"2026-05-11T14:21:05.804968Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1811.01948","last_updated":"2019-12-18T20:09:18Z","snapshot_observed_at":"2026-07-06T07:12:46.946899Z","submitted_at":"2018-11-05T19:00:00Z","title":"Cosmic phase transitions: their applications and experimental signatures","version":3},"cited_work":{"arxiv_id":"1811.01948","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1811.01948","snapshot_observed_at":"2026-07-03T11:28:03.867896Z","title":"Mazumdar and G","venue":null,"work_id":"abd8e2da-64b4-4cc6-9f6e-c45245420986","year":2019},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1811.01948","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:8496bc3c981ecb553a82edb66889f0939c351ea82d90772028cb939ca52f87e7","observation_id":"6fdcafa3-472f-4f76-95b3-2f880fde04d9","resolution":{"observed_at":"2026-05-11T14:21:05.829479Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1607.06363","last_updated":"2016-11-30T15:25:07Z","snapshot_observed_at":"2026-07-06T05:04:27.576161Z","submitted_at":"2016-07-21T15:27:31Z","title":"Search for heavy resonances decaying to a $Z$ boson and a photon in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","version":2},"cited_work":{"arxiv_id":"1607.06363","doi":"10.1016/j.physletb.2016.11.005","metadata_source":"pith","pith_arxiv_id":"1607.06363","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Search for heavy resonances decaying to a $Z$ boson and a photon in $pp$ collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","venue":"hep-ex","work_id":"f93e91c5-8188-47c7-a085-61bd29379ea0","year":2016},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1607.06363","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:fc6858e589a22ee829f600fb31e68c6f864bbec429a70cdb226483fe4425a303","observation_id":"e0de0709-bb37-432e-aa10-c561107f8f42","resolution":{"observed_at":"2026-05-11T14:21:05.871944Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1712.06552","last_updated":"2017-12-18T17:51:26Z","snapshot_observed_at":"2026-07-06T06:14:56.693337Z","submitted_at":"2017-12-18T17:51:26Z","title":"Spectroscopy and thermal modelling of the first interstellar object 1I/2017 U1 'Oumuamua","version":1},"cited_work":{"arxiv_id":"1712.06552","doi":null,"metadata_source":"pith","pith_arxiv_id":"1712.06552","snapshot_observed_at":"2026-06-28T16:12:22.350800Z","title":"Spectroscopy and thermal modelling of the first interstellar object 1I/2017 U1 'Oumuamua","venue":"astro-ph.EP","work_id":"cb118f9e-af01-4eb9-8bec-d98ba1f5ac0b","year":2017},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1712.06552","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:2bebb46924a885d9113fac65cd4ec5f4a7da955681e8e4c666a7097ecf3f86f7","observation_id":"62b71d5b-7988-496d-8e7e-c13cc7902365","resolution":{"observed_at":"2026-05-11T14:21:06.243621Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1608.00991","last_updated":"2016-08-02T20:27:01Z","snapshot_observed_at":"2026-07-06T05:05:47.694853Z","submitted_at":"2016-08-02T20:27:01Z","title":"Character degrees of extensions of the Suzuki groups $^2B_2(q^2)$","version":1},"cited_work":{"arxiv_id":"1608.00991","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1608.00991","snapshot_observed_at":"2026-07-04T21:10:20.613501Z","title":"Dev et al.,Electroweak baryogenesis and gravitational waves,Phys","venue":null,"work_id":"9ece6304-0519-4986-a514-a931805858ae","year":2016},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1608.00991","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:58967844744e2b0b27d0c9fcc4f3a643176406c3e71333ab804e785d8c0a57ae","observation_id":"46958076-0d45-43d8-983b-bc9f09170469","resolution":{"observed_at":"2026-07-04T21:10:20.613501Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Kawamura et al.,The Japanese space gravitational wave antenna: DECIGO,Class","venue":null,"work_id":"8e1996c1-86b5-4ac5-b816-d0581ce1df56","year":2011},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:2efe0c469f26ae20f3ad6a8804c8450b1e71f5bf320004c49c64f74fcccdd8ad","observation_id":"d4a4453f-c30a-4210-922c-3ab28976fdb3","resolution":{"observed_at":"2026-05-23T15:15:42.371646Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0512039","last_updated":"2005-12-06T18:41:06Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2005-12-06T18:41:06Z","title":"Detecting the Cosmic Gravitational Wave Background with the Big Bang Observer","version":1},"cited_work":{"arxiv_id":"gr-qc/0512039","doi":"10.1088/0264-9381/23/7/014","metadata_source":"pith","pith_arxiv_id":"gr-qc/0512039","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Detecting the Cosmic Gravitational Wave Background with the Big Bang Observer","venue":"gr-qc","work_id":"1701a34f-bcc1-4e4f-a0af-3ef0e44104c1","year":2005},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/gr-qc/0512039","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:a5aa1a5a7c3dd464b7e44cc72b24fb9c1b00a943ec3ed21ebf08fc715a7af1d8","observation_id":"fe479f5a-4750-4f79-b8de-3b8527d69ade","resolution":{"observed_at":"2026-05-11T14:21:06.200039Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-07-13T10:49:43.445588+00:00","source":"crossref_status_cache"},{"observed_at":"2026-07-13T10:49:43.445588+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1410.7296","last_updated":"2014-11-28T14:41:08Z","snapshot_observed_at":"2026-07-06T03:58:36.745695Z","submitted_at":"2014-10-22T08:48:08Z","title":"Descope of the ALIA mission","version":2},"cited_work":{"arxiv_id":"1410.7296","doi":null,"metadata_source":"pith","pith_arxiv_id":"1410.7296","snapshot_observed_at":"2026-07-03T12:38:08.149539Z","title":"Descope of the ALIA mission","venue":"gr-qc","work_id":"4af4bf2f-6ee2-46c7-8ee8-3f817ab1317a","year":2014},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1410.7296","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:b1da68a543ece473c49ef089beee37f363c74a25752f7dd0b41df129206b065a","observation_id":"da1cf628-5c2a-4ace-a05a-84f267f8b967","resolution":{"observed_at":"2026-05-11T14:21:05.917664Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1903.00006","last_updated":"2019-07-31T17:22:47Z","snapshot_observed_at":"2026-08-03T02:11:49.865388Z","submitted_at":"2019-02-28T19:00:00Z","title":"Neutrino Portals to Dark Matter","version":2},"cited_work":{"arxiv_id":"1903.00006","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1903.00006","snapshot_observed_at":"2026-07-02T17:37:14.212756Z","title":"Blennow, E","venue":null,"work_id":"556a63be-608f-4b97-b6bb-b495237a8e42","year":2019},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1903.00006","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:ea8e2dc0ca844a2dc1672b61d7dd826e75d67cdfd7831e5dbe0be76af45124bf","observation_id":"cc99bbeb-567b-49e2-917f-a36ae4c94769","resolution":{"observed_at":"2026-05-11T14:21:06.065001Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2206.05811","last_updated":"2022-06-12T18:28:24Z","snapshot_observed_at":"2026-07-06T13:19:58.934755Z","submitted_at":"2022-06-12T18:28:24Z","title":"Semi-Annihilation of Fermionic Dark Matter","version":1},"cited_work":{"arxiv_id":"2206.05811","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2206.05811","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Bandyopadhyay, D","venue":null,"work_id":"9c1ab778-a4ca-4c79-9b76-e0730f04242b","year":2023},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2206.05811","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:e1728ff692fff497dc2b847d1f89447719878c8480cc64706b3dd8772e5e9825","observation_id":"f6c5505e-e71f-429b-82ac-fbec4720bfd2","resolution":{"observed_at":"2026-05-11T14:21:06.098155Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2104.14443","last_updated":"2025-02-03T08:18:54Z","snapshot_observed_at":"2026-07-06T11:04:51.273466Z","submitted_at":"2021-04-29T16:02:59Z","title":"A complete effective field theory for dark matter","version":2},"cited_work":{"arxiv_id":"2104.14443","doi":null,"metadata_source":"pith","pith_arxiv_id":"2104.14443","snapshot_observed_at":"2026-07-10T14:47:14.419041Z","title":"Criado, A","venue":"hep-ph","work_id":"d9bf4faf-611c-4690-8865-1ecfe4cdf91e","year":2021},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2104.14443","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:5ebae7d13858bf546e3302693604b95a597ff87648bce5cb3dc22895d901c726","observation_id":"66ec0b06-bb67-4140-b13c-e8cf509b427f","resolution":{"observed_at":"2026-05-11T14:21:06.297946Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1407.1859","last_updated":"2014-10-02T08:59:47Z","snapshot_observed_at":"2026-07-06T03:48:17.300160Z","submitted_at":"2014-07-07T20:10:34Z","title":"Singlet Majorana fermion dark matter: a comprehensive analysis in effective field theory","version":2},"cited_work":{"arxiv_id":"1407.1859","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1407.1859","snapshot_observed_at":"2026-07-04T19:07:59.712295Z","title":"Matsumoto, S","venue":null,"work_id":"f93ad805-d238-45b8-b40c-6724ac458edc","year":2014},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1407.1859","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:9ad00d902ba81800a4578e54bae4e97bed9272e56ad74acc97ca7df0899f4f2d","observation_id":"1f8aa706-7d30-4e9d-adc8-898a2b1223a4","resolution":{"observed_at":"2026-07-04T19:07:59.712295Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1008.4884","last_updated":"2017-01-15T20:19:22Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2010-08-28T19:19:07Z","title":"Dimension-Six Terms in the Standard Model Lagrangian","version":3},"cited_work":{"arxiv_id":"1008.4884","doi":null,"metadata_source":"pith","pith_arxiv_id":"1008.4884","snapshot_observed_at":"2026-07-10T18:07:32.071514Z","title":"Dimension-Six Terms in the Standard Model Lagrangian","venue":"hep-ph","work_id":"57216ec9-7bc4-457b-9e8a-c10cbb3929a1","year":2010},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1008.4884","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:17f6540aebdbc47149e25f666a002bd7270cfc2face6bf980273103cb9f3b4ee","observation_id":"4de52807-96c7-443e-b5cc-7877434ea3ff","resolution":{"observed_at":"2026-05-14T00:12:49.669922Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2012.02779","last_updated":"2021-04-08T15:54:25Z","snapshot_observed_at":"2026-07-06T10:20:52.839902Z","submitted_at":"2020-12-04T18:56:23Z","title":"Top, Higgs, Diboson and Electroweak Fit to the Standard Model Effective Field Theory","version":3},"cited_work":{"arxiv_id":"2012.02779","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2012.02779","snapshot_observed_at":"2026-07-03T12:18:07.057500Z","title":"Ellis, M","venue":null,"work_id":"99c30498-e566-416f-9bb7-75bc04954a7f","year":2021},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2012.02779","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:9cc1a59bdf805745049b20fc1dc0ab91dbfecf722e2ae2180990363355a429f7","observation_id":"bdea8714-c20d-4189-9666-a33e0ba2ae5b","resolution":{"observed_at":"2026-05-11T14:21:06.223708Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Coleman and E.J","venue":null,"work_id":"0f70bca4-df18-4143-b323-889a4efc3a62","year":1973},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:44938088ebd1df0c6a951f0ea42420a68acf356592487d9dd89d893d7dd9bacd","observation_id":"ebebe9e0-0efd-4c1b-ac79-94649d33f187","resolution":{"observed_at":"2026-05-23T15:15:42.358940Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1109.4189","last_updated":"2011-09-19T23:50:00Z","snapshot_observed_at":"2026-07-06T02:34:17.812392Z","submitted_at":"2011-09-19T23:50:00Z","title":"CosmoTransitions: Computing Cosmological Phase Transition Temperatures and Bubble Profiles with Multiple Fields","version":1},"cited_work":{"arxiv_id":"1109.4189","doi":null,"metadata_source":"pith","pith_arxiv_id":"1109.4189","snapshot_observed_at":"2026-07-08T13:44:55.090581Z","title":"CosmoTransitions: Computing Cosmological Phase Transition Temperatures and Bubble Profiles with Multiple Fields","venue":"hep-ph","work_id":"285e1474-4ef5-44c7-99ae-f5270f7ca2f0","year":2011},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1109.4189","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:24734dbdac1c228dc054fd9bf10ef22fee41ecc1ad5ece57048ecaf745eb30cc","observation_id":"802d853e-1f6e-46a6-96f1-38c4c817c68a","resolution":{"observed_at":"2026-05-11T14:21:06.267880Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1504.05949","last_updated":"2015-07-21T17:22:58Z","snapshot_observed_at":"2026-07-06T04:15:47.306139Z","submitted_at":"2015-04-22T20:00:27Z","title":"The Electroweak Phase Transition in the Inert Doublet Model","version":3},"cited_work":{"arxiv_id":"1504.05949","doi":null,"metadata_source":"pith","pith_arxiv_id":"1504.05949","snapshot_observed_at":"2026-07-03T15:48:35.524523Z","title":"Blinov, S","venue":"hep-ph","work_id":"7c597b39-ad2e-4e6b-adff-2ef85df9129a","year":2015},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1504.05949","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:218d4acf8aca8758f3fc658d109c76db1342657753585c4be2406da34249f66b","observation_id":"f4b1bbe7-8086-416d-8a6c-6cae70baf916","resolution":{"observed_at":"2026-05-11T14:21:06.071337Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2106.03439","last_updated":"2022-06-15T09:16:38Z","snapshot_observed_at":"2026-07-06T11:16:37.233588Z","submitted_at":"2021-06-07T09:16:14Z","title":"Possibility of multi-step electroweak phase transition in the two Higgs doublet models","version":2},"cited_work":{"arxiv_id":"2106.03439","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2106.03439","snapshot_observed_at":"2026-07-03T15:48:35.549132Z","title":null,"venue":null,"work_id":"da29592f-7825-4309-a98a-fa9729dc21f5","year":2022},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2106.03439","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:ca56873270546be2f12b5f2f6bf2f5c4f8c3ea276ed861ed35dae1834200a659","observation_id":"7a5086e0-e975-4871-bff4-099b555c7b61","resolution":{"observed_at":"2026-05-11T14:21:06.290255Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1808.01098","last_updated":"2018-12-12T08:18:25Z","snapshot_observed_at":"2026-07-06T06:53:53.056912Z","submitted_at":"2018-08-03T06:46:00Z","title":"Revisiting electroweak phase transition in the standard model with a real singlet scalar","version":2},"cited_work":{"arxiv_id":"1808.01098","doi":"10.1016/j.physletb.2018.12.017","metadata_source":"pith","pith_arxiv_id":"1808.01098","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Revisiting electroweak phase transition in the standard model with a real singlet scalar","venue":"hep-ph","work_id":"68029d1b-86f3-4210-a185-68c7abda11c1","year":2018},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1808.01098","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:4fcf4abf2f52dfe31016386155f6af3e4ecb1185df8c77e6795e33175ff247ac","observation_id":"695210cf-8cf1-4589-9427-816c2c138889","resolution":{"observed_at":"2026-05-11T14:21:06.177821Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2208.01319","last_updated":"2023-04-19T02:58:50Z","snapshot_observed_at":"2026-07-06T13:37:50.559341Z","submitted_at":"2022-08-02T08:59:49Z","title":"How arbitrary are perturbative calculations of the electroweak phase transition?","version":4},"cited_work":{"arxiv_id":"2208.01319","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2208.01319","snapshot_observed_at":"2026-07-03T15:48:35.597799Z","title":"Athron, C","venue":null,"work_id":"2fd611dc-5472-4055-81ed-5b49f24133be","year":2023},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2208.01319","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:bcd1d5b64e02b9f4c2ebe505e4f1041a3a7fd6f5efbb2677c46fafccd4df02dd","observation_id":"44f1ec7f-b892-49e8-a5fc-f7fa0f70bbe6","resolution":{"observed_at":"2026-05-11T14:21:06.163857Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2009.10080","last_updated":"2021-04-13T09:24:16Z","snapshot_observed_at":"2026-07-06T09:57:33.351931Z","submitted_at":"2020-09-21T18:00:01Z","title":"Theoretical uncertainties for cosmological first-order phase transitions","version":2},"cited_work":{"arxiv_id":"2009.10080","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2009.10080","snapshot_observed_at":"2026-07-04T01:59:25.561071Z","title":"Croon, O","venue":null,"work_id":"7d27007d-0814-4e8e-bab5-6296e3fe80db","year":2021},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2009.10080","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:c73d4c8ee4654802cbe66a450385990e80c5d1d6a431f422badd10a58bd19db1","observation_id":"9ee10b25-de7f-4366-8d7d-7459d2e5b298","resolution":{"observed_at":"2026-05-11T14:21:05.898019Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2104.04399","last_updated":"2021-06-22T19:08:23Z","snapshot_observed_at":"2026-07-06T10:58:01.160301Z","submitted_at":"2021-04-09T14:36:06Z","title":"On the perturbative expansion at high temperature and implications for cosmological phase transitions","version":2},"cited_work":{"arxiv_id":"2104.04399","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2104.04399","snapshot_observed_at":"2026-07-04T06:59:38.522004Z","title":"Gould and T","venue":null,"work_id":"d4c58549-70d3-4ce1-9897-c61429d4720f","year":2021},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2104.04399","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:8c6daaa4c842267fac98649304d52737588db70796027e9c473780b344bddf6b","observation_id":"6d703b41-5548-465c-8ebb-930b10432873","resolution":{"observed_at":"2026-05-11T14:21:05.971680Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1408.0287","last_updated":"2014-08-01T20:00:14Z","snapshot_observed_at":"2026-07-06T03:50:44.144028Z","submitted_at":"2014-08-01T20:00:14Z","title":"Consistent Use of Effective Potentials","version":1},"cited_work":{"arxiv_id":"1408.0287","doi":null,"metadata_source":"pith","pith_arxiv_id":"1408.0287","snapshot_observed_at":"2026-06-26T01:48:53.818697Z","title":"Andreassen, W","venue":"hep-ph","work_id":"f5d70a7f-e1b1-472b-b2a7-b0d534b757a5","year":2014},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1408.0287","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:634616404b7c8a8b7b3f6a6fbc8f6ea9c6dfa679aebac2c104b8346f35eb3a9d","observation_id":"8a65f4ce-7fe4-403a-ba2b-c2225a13fb35","resolution":{"observed_at":"2026-05-11T14:21:06.051739Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1408.0292","last_updated":"2014-08-25T19:39:10Z","snapshot_observed_at":"2026-07-06T03:50:44.144028Z","submitted_at":"2014-08-01T20:01:27Z","title":"Consistent Use of the Standard Model Effective Potential","version":2},"cited_work":{"arxiv_id":"1408.0292","doi":"10.1103/physrevlett.113.241801","metadata_source":"pith","pith_arxiv_id":"1408.0292","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Andreassen, W","venue":"hep-ph","work_id":"b59200cd-311a-4e9a-bbe8-e102ccd57ae9","year":2014},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1408.0292","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:0bc481ad6314d643efd9efe389cf21f531fa27ece990b8162f8fdf2c47e5ea31","observation_id":"4c77c894-09dc-41e1-80cd-273be01715cb","resolution":{"observed_at":"2026-05-11T14:21:06.142227Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Carrington,The Effective potential at finite temperature in the Standard Model,Phys","venue":null,"work_id":"1824394b-379a-4fd0-863d-2327c1f11f56","year":1992},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:168089b33c956b172faa3bd86312021fdbabfcccd5dc10fe9542d495efc7d3a7","observation_id":"64c4349d-ec98-41d6-b770-deebaedf8f39","resolution":{"observed_at":"2026-05-23T15:15:42.355525Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9901312","last_updated":"1999-01-14T15:40:22Z","snapshot_observed_at":"2026-07-07T04:31:58.630431Z","submitted_at":"1999-01-14T15:40:22Z","title":"Finite temperature field theory and phase transitions","version":1},"cited_work":{"arxiv_id":"hep-ph/9901312","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9901312","snapshot_observed_at":"2026-07-09T15:16:18.103128Z","title":"Finite temperature field theory and phase transitions","venue":"hep-ph","work_id":"de1f32a7-b5e8-45e3-88e4-311458872728","year":1999},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9901312","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:f96f1b8cb86bf79a75c514f656186896ddc825d49327ef07dde6a44f6747b6c7","observation_id":"ab61f986-a910-41e9-ac21-e16229de4b01","resolution":{"observed_at":"2026-05-13T18:19:01.789654Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2204.06966","last_updated":"2022-04-14T13:48:38Z","snapshot_observed_at":"2026-07-06T13:00:23.460342Z","submitted_at":"2022-04-14T13:48:38Z","title":"Two Higgs doublets, Effective Interactions and a Strong First-Order Electroweak Phase Transition","version":1},"cited_work":{"arxiv_id":"2204.06966","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2204.06966","snapshot_observed_at":"2026-07-04T01:59:25.536328Z","title":"Biermann, C","venue":null,"work_id":"43cbbb24-ba1f-404e-a783-e168670179ee","year":2022},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2204.06966","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:6fba389500499ab736a380bbe294703a4746be663a8d9ed452e2fe6875e760dc","observation_id":"f2f3ef90-7e71-4a36-a8fb-4deeb8027eb3","resolution":{"observed_at":"2026-05-11T14:21:06.092340Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Dolan and R","venue":null,"work_id":"043a4bdb-5122-4eb8-a96c-fe755706c689","year":1974},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:1a6f3b70e0338c7056ec56d5adee03295fcc5aeb1ed3ad223881123415dc8860","observation_id":"d3866880-b53a-4885-86b7-ea39048c744c","resolution":{"observed_at":"2026-05-23T15:15:42.346688Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Weinberg,Gauge and Global Symmetries at High Temperature,Phys","venue":null,"work_id":"7c5a3fcf-0f12-440f-aeb9-2c1d9ce4c89d","year":1974},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:7f628388b70b7e25a08d4e8416be4690b5f0591781170fb7d4ecf1516587d650","observation_id":"89fada2c-605c-4876-a137-a3f1d09d7ee6","resolution":{"observed_at":"2026-05-23T15:15:42.349687Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2012.03953","last_updated":"2020-12-07T19:00:01Z","snapshot_observed_at":"2026-07-06T10:21:33.099775Z","submitted_at":"2020-12-07T19:00:01Z","title":"Cosmological phase transitions: is effective field theory just a toy?","version":1},"cited_work":{"arxiv_id":"2012.03953","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2012.03953","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Postma and G","venue":null,"work_id":"74e726b5-bba4-45ff-ab89-9493b4cd6c3a","year":2021},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2012.03953","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:e58f8ca2086d48974691ea968dc82e95b9bfd51fea5982e50aa20bcc2b6d62f7","observation_id":"a0fb2550-8a45-4f90-937a-1fb630929579","resolution":{"observed_at":"2026-05-11T14:21:06.316941Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Senaha,Symmetry Restoration and Breaking at Finite Temperature: An Introductory Review,Symmetry12(2020) 733","venue":null,"work_id":"1a7bd832-4dff-48a8-aa9c-975a7fa4fe29","year":2020},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:dc78077ea22b24196eeda40fd2f31c88d6478a8b7810bde8ff9bdfb04206dd67","observation_id":"7237ef78-e5b9-49f0-bc63-c5362df8bb0c","resolution":{"observed_at":"2026-05-23T15:15:42.352645Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1904.01329","last_updated":"2019-06-24T14:05:28Z","snapshot_observed_at":"2026-07-06T07:43:17.209715Z","submitted_at":"2019-04-02T10:48:49Z","title":"On the validity of perturbative studies of the electroweak phase transition in the Two Higgs Doublet model","version":2},"cited_work":{"arxiv_id":"1904.01329","doi":null,"metadata_source":"pith","pith_arxiv_id":"1904.01329","snapshot_observed_at":"2026-07-08T13:44:55.064482Z","title":"On the validity of perturbative studies of the electroweak phase transition in the Two Higgs Doublet model","venue":"hep-ph","work_id":"e79e3947-6c5f-421d-ba48-ca472470efd8","year":2019},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1904.01329","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:120bd914c1376555bf626ba0e941c848c77ddd51496ba4b99f902028f5102852","observation_id":"82b6dd33-0971-4d53-bc0f-e6ac58c8d7fe","resolution":{"observed_at":"2026-05-11T14:21:05.959012Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9212235","last_updated":"1992-12-10T22:19:39Z","snapshot_observed_at":"2026-07-07T04:14:51.399626Z","submitted_at":"1992-12-08T03:16:25Z","title":"The Effective Potential and First-Order Phase Transitions: Beyond Leading Order","version":2},"cited_work":{"arxiv_id":"hep-ph/9212235","doi":"10.1103/physrevd.47.3546","metadata_source":"pith","pith_arxiv_id":"hep-ph/9212235","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"The Effective Potential and First-Order Phase Transitions: Beyond Leading Order","venue":"hep-ph","work_id":"90c93a15-44c5-45ee-a1ea-b7731d3943f1","year":1992},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9212235","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:72f8914a6b8043061fc78b1ef8d8cf6165d87c3e01bf4c79d9697532272343a2","observation_id":"1cb8ac6a-935b-4d96-b197-2b10458813ce","resolution":{"observed_at":"2026-05-11T14:21:05.696870Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9204216","last_updated":"1992-04-10T04:03:55Z","snapshot_observed_at":"2026-07-07T04:14:16.305741Z","submitted_at":"1992-04-10T04:03:55Z","title":"Resummation in a Hot Scalar Field Theory","version":1},"cited_work":{"arxiv_id":"hep-ph/9204216","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9204216","snapshot_observed_at":"2026-07-04T01:59:25.935781Z","title":"Resummation in a Hot Scalar Field Theory","venue":"hep-ph","work_id":"8c7089be-80fd-4c10-8ad8-1d3b5238c85c","year":1992},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9204216","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:037662b5ec1e9d5064d192e1f0f2ea20d391b95921f9b559940b2feb0f9e9979","observation_id":"0ab7cc8f-a676-48e7-b689-4f59e535a105","resolution":{"observed_at":"2026-05-11T14:21:06.135148Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1609.04979","last_updated":"2017-01-26T14:09:24Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2016-09-16T10:11:12Z","title":"On Effective Degrees of Freedom in the Early Universe","version":3},"cited_work":{"arxiv_id":"1609.04979","doi":null,"metadata_source":"pith","pith_arxiv_id":"1609.04979","snapshot_observed_at":"2026-07-04T05:39:39.480975Z","title":"On Effective Degrees of Freedom in the Early Universe","venue":"astro-ph.CO","work_id":"10102067-901b-46ec-922a-05f92e5505a9","year":2016},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1609.04979","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:02c7d56f6e12141171318c2c5e1666540b5007db485c50af18bfe82012da14cd","observation_id":"0e784416-2546-48ec-981e-15a55da3c7b7","resolution":{"observed_at":"2026-05-11T14:21:05.751741Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0911.0687","last_updated":"2010-02-24T19:55:49Z","snapshot_observed_at":"2026-08-03T04:02:24.382776Z","submitted_at":"2009-11-03T21:03:14Z","title":"Semi-Analytic Calculation of the Gravitational Wave Signal From the Electroweak Phase Transition for General Quartic Scalar Effective Potentials","version":3},"cited_work":{"arxiv_id":"0911.0687","doi":null,"metadata_source":"pith","pith_arxiv_id":"0911.0687","snapshot_observed_at":"2026-07-03T19:48:53.496503Z","title":"Kehayias and S","venue":"hep-ph","work_id":"40031835-4d52-4577-b3a3-2f62a0c3c557","year":2009},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/0911.0687","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:7144cc726530a6b6f28f43f600863cecf1b4a6ac8bbcaf2f5432b49e29ba7147","observation_id":"f449f9f1-9cfc-4704-a534-72c3afb8c909","resolution":{"observed_at":"2026-05-11T14:21:06.026851Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1512.06239","last_updated":"2016-04-01T10:50:20Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2015-12-19T12:44:06Z","title":"Science with the space-based interferometer eLISA. II: Gravitational waves from cosmological phase transitions","version":2},"cited_work":{"arxiv_id":"1512.06239","doi":null,"metadata_source":"pith","pith_arxiv_id":"1512.06239","snapshot_observed_at":"2026-07-10T23:37:43.558451Z","title":"Science with the space-based interferometer eLISA. II: Gravitational waves from cosmological phase transitions","venue":"astro-ph.CO","work_id":"1984496d-cfc6-46a3-953f-6b8aab5d502d","year":2015},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1512.06239","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:a2f2164ad60a7804fc32d847e6d8c3faee6e981ed80973b006d08b62955227e8","observation_id":"53f801f6-4011-41cc-8dad-3d133d1f3db9","resolution":{"observed_at":"2026-05-11T14:21:06.309671Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1605.01403","last_updated":"2016-10-18T16:29:21Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2016-05-04T20:00:00Z","title":"Gravitational waves from bubble collisions: analytic derivation","version":2},"cited_work":{"arxiv_id":"1605.01403","doi":null,"metadata_source":"pith","pith_arxiv_id":"1605.01403","snapshot_observed_at":"2026-07-04T12:09:48.728116Z","title":"Gravitational waves from bubble collisions: analytic derivation","venue":"astro-ph.CO","work_id":"bfe4efaf-e5e4-4376-9f78-2d7b1c047dc4","year":2016},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1605.01403","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:ddd74c4040f646d8f43a96bec46dd10c0f08dec92e69b2c0e3468f6009d4c0ab","observation_id":"1d787e99-f00c-4043-abf3-6359bc587e09","resolution":{"observed_at":"2026-05-11T14:21:05.668351Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1304.2433","last_updated":"2014-01-29T15:44:48Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2013-04-08T23:42:59Z","title":"Gravitational waves from the sound of a first order phase transition","version":2},"cited_work":{"arxiv_id":"1304.2433","doi":null,"metadata_source":"pith","pith_arxiv_id":"1304.2433","snapshot_observed_at":"2026-07-04T06:59:38.415002Z","title":"Gravitational waves from the sound of a first order phase transition","venue":"hep-ph","work_id":"2e4aba8e-2e9b-43a1-ae53-22fe2f79868f","year":2013},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1304.2433","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:2bc52e2a25b11650ffab406b9a1330c01e83a4cbac0a541f28bd0da7cd1fecd0","observation_id":"bc26c11c-6fb0-4fd9-a12b-aed6e4416a7f","resolution":{"observed_at":"2026-05-11T14:21:06.205735Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1608.04735","last_updated":"2016-08-16T19:59:31Z","snapshot_observed_at":"2026-07-06T05:07:11.900140Z","submitted_at":"2016-08-16T19:59:31Z","title":"Sound shell model for acoustic gravitational wave production at a first-order phase transition in the early Universe","version":1},"cited_work":{"arxiv_id":"1608.04735","doi":"10.1103/physrevlett.120.071301","metadata_source":"pith","pith_arxiv_id":"1608.04735","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Sound shell model for acoustic gravitational wave production at a first-order phase transition in the early Universe","venue":"astro-ph.CO","work_id":"88d70d48-75ca-404b-9859-5263a7303553","year":2016},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1608.04735","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:e83955daab4274dcc7fa78de822973ccd8cc9fe79e40938fe6f284e250bb6933","observation_id":"9242cbb4-43de-47ba-9837-83eb50de30ee","resolution":{"observed_at":"2026-05-11T14:21:06.232211Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-05-24T15:26:38.958765+00:00","source":"crossref_status_cache"},{"observed_at":"2026-05-24T15:26:38.958765+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1704.05871","last_updated":"2020-04-15T14:58:21Z","snapshot_observed_at":"2026-07-06T05:38:27.260025Z","submitted_at":"2017-04-19T18:08:03Z","title":"Shape of the acoustic gravitational wave power spectrum from a first order phase transition","version":3},"cited_work":{"arxiv_id":"1704.05871","doi":null,"metadata_source":"pith","pith_arxiv_id":"1704.05871","snapshot_observed_at":"2026-07-08T13:44:55.053242Z","title":"Hindmarsh, S","venue":"astro-ph.CO","work_id":"6b446ffc-378d-474d-abcd-82c81c385e7f","year":2017},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1704.05871","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:70dbd9171a25907c03e51a1978ccf14aad3081c81d1cf2ff236aba0c5b5fe9d2","observation_id":"a39ba7d4-92a2-463b-bc70-aef09e1d6e42","resolution":{"observed_at":"2026-05-11T14:21:06.302963Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0909.0622","last_updated":"2009-12-10T10:51:39Z","snapshot_observed_at":"2026-08-02T02:06:05.383741Z","submitted_at":"2009-09-03T10:51:40Z","title":"The stochastic gravitational wave background from turbulence and magnetic fields generated by a first-order phase transition","version":2},"cited_work":{"arxiv_id":"0909.0622","doi":null,"metadata_source":"pith","pith_arxiv_id":"0909.0622","snapshot_observed_at":"2026-07-04T04:49:36.467979Z","title":"The stochastic gravitational wave background from turbulence and magnetic fields generated by a first-order phase transition","venue":"astro-ph.CO","work_id":"6d7867c0-966e-4ed4-9428-e0321b5918f9","year":2009},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/0909.0622","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:cde1194181ac91871f03b2244849d62a8a45e2375bfde91ab3037e054189ed0c","observation_id":"4ae34cc2-ef5b-4705-8870-771f419f1065","resolution":{"observed_at":"2026-05-11T14:21:06.046522Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1101.3940","last_updated":"2017-04-17T04:39:15Z","snapshot_observed_at":"2026-07-06T02:22:18.758348Z","submitted_at":"2011-01-20T16:03:13Z","title":"Detector configuration of DECIGO/BBO and identification of cosmological neutron-star binaries","version":2},"cited_work":{"arxiv_id":"1101.3940","doi":null,"metadata_source":"pith","pith_arxiv_id":"1101.3940","snapshot_observed_at":"2026-07-04T17:50:00.545530Z","title":"Detector configuration of DECIGO/BBO and identification of cosmological neutron-star binaries","venue":"astro-ph.CO","work_id":"c3046f8e-efee-4c9e-8076-6cd2603314e5","year":2011},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1101.3940","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:53096f22ec2098d05de1906c3353f81a8630e8e4d2a749df191c95de271a6fd9","observation_id":"b399f51a-e4d7-43af-8fd2-7eb8d7c58c68","resolution":{"observed_at":"2026-05-11T14:21:06.040896Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Punturo et al.,The Einstein Telescope: A third-generation gravitational wave observatory,Class","venue":null,"work_id":"06e9ea0e-cd5a-4f35-a971-a04910b6e050","year":2010},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:956dd3017932a199843ce4d742dde2b74e2bf2dfab9f9780eb95f130be3a768d","observation_id":"ff3875ee-dec2-4dc4-9385-693cee89ecef","resolution":{"observed_at":"2026-05-23T15:15:42.363169Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1907.04833","last_updated":"2019-07-10T17:27:49Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2019-07-10T17:27:49Z","title":"Cosmic Explorer: The U.S. Contribution to Gravitational-Wave Astronomy beyond LIGO","version":1},"cited_work":{"arxiv_id":"1907.04833","doi":"10.48550/arxiv.1907.04833","metadata_source":"pith","pith_arxiv_id":"1907.04833","snapshot_observed_at":"2026-07-10T15:07:19.491442Z","title":"Cosmic Explorer: The U.S. Contribution to Gravitational-Wave Astronomy beyond LIGO","venue":"astro-ph.IM","work_id":"de7f174c-dbb7-4870-b03c-7faf70dce4e9","year":2019},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1907.04833","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:1e0172d8dc9e213bdc7cd85ed6fb3144016739733c464a941131b2040cda4ff1","observation_id":"5c5067ae-77cf-4413-a1ad-0ae6f0ac78a7","resolution":{"observed_at":"2026-05-11T14:21:06.104043Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-07-13T22:50:53.600025+00:00","source":"crossref_status_cache"},{"observed_at":"2026-07-13T22:50:53.600025+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0910.0715","last_updated":"2009-10-05T10:28:39Z","snapshot_observed_at":"2026-07-06T01:58:41.536473Z","submitted_at":"2009-10-05T10:28:39Z","title":"Gravitational Wave Background and Non-Gaussianity as a Probe of the Curvaton Scenario","version":1},"cited_work":{"arxiv_id":"0910.0715","doi":"10.1088/1475-7516/2010/","metadata_source":"pith","pith_arxiv_id":"0910.0715","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Gravitational Wave Background and Non-Gaussianity as a Probe of the Curvaton Scenario","venue":"astro-ph.CO","work_id":"6165c433-50c9-41c1-8817-a1619e6a6055","year":2009},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/0910.0715","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:895b1ec373df6db64a8828ad5d99b75b107b76a9bacf57f96d94d456bf6750d9","observation_id":"c250201f-94f9-4806-924f-07abf3405b31","resolution":{"observed_at":"2026-05-11T14:21:05.987344Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0103065","last_updated":"2001-11-07T15:56:59Z","snapshot_observed_at":"2026-07-07T03:51:41.576227Z","submitted_at":"2001-03-06T20:19:15Z","title":"Oscillating neutrinos and mu --> e, gamma","version":2},"cited_work":{"arxiv_id":"hep-ph/0103065","doi":"10.1016/s0550-3213(01)00475-8","metadata_source":"pith","pith_arxiv_id":"hep-ph/0103065","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Oscillating neutrinos and mu --> e, gamma","venue":"hep-ph","work_id":"71f351c1-bb52-4500-8a4f-29d0afa01bf6","year":2001},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/0103065","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:136e7e517d744a14cc141d1dd7a71ad5164bef5549232ca452888e0db4a520d8","observation_id":"85d32c80-9db3-4174-a40e-34d0bd05ca29","resolution":{"observed_at":"2026-05-11T14:21:06.009854Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-07-13T09:50:18.969738+00:00","source":"crossref_status_cache"},{"observed_at":"2026-07-13T09:50:18.969738+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2012.09845","last_updated":"2021-04-30T08:41:40Z","snapshot_observed_at":"2026-07-06T10:25:35.721396Z","submitted_at":"2020-12-17T18:58:17Z","title":"Searching for Lepton Flavour (Universality) Violation and Collider Signals from a Singly-Charged Scalar Singlet","version":3},"cited_work":{"arxiv_id":"2012.09845","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2012.09845","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Crivellin, F","venue":null,"work_id":"726cb73a-da93-4378-9b11-51bd555a8e75","year":2021},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2012.09845","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:d7175f105597d0f9d0b2a8cbbeccf3196e182ecf4913f2b4d247e8633c3ee22b","observation_id":"823bf5e2-3945-4907-893a-72ac7fb09491","resolution":{"observed_at":"2026-05-11T14:21:06.248921Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2005.13542","last_updated":"2021-01-28T12:57:54Z","snapshot_observed_at":"2026-07-06T09:23:52.102423Z","submitted_at":"2020-05-27T18:00:00Z","title":"Explaining $b\\to s\\ell^+\\ell^-$ and the Cabibbo Angle Anomaly with a Vector Triplet","version":3},"cited_work":{"arxiv_id":"2005.13542","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2005.13542","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Capdevila, A","venue":null,"work_id":"04f3352f-82cb-4271-b3b4-dd19d9219616","year":2021},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2005.13542","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:88f2d03a666d9430617bc3d6ccf2b704476b3dfabf4073d81a086e5df828b260","observation_id":"37f0963c-6387-4867-a5c2-88084ca597c5","resolution":{"observed_at":"2026-05-11T14:21:05.733196Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Pilaftsis,Advances in Leptogenesis,J","venue":null,"work_id":"6ce30b33-f9e4-48db-8d87-db1b57b82aa0","year":2013},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:6791786694c4c08364a441f1e9755e91a9837c13c9cd8e672152ff7ff744744c","observation_id":"2b7fdeca-bd09-401e-9284-7d0e56fa91d0","resolution":{"observed_at":"2026-05-23T15:15:42.368555Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0310123","last_updated":"2026-04-16T10:31:58Z","snapshot_observed_at":"2026-07-07T04:01:31.058013Z","submitted_at":"2003-10-10T15:55:22Z","title":"Towards a complete theory of thermal leptogenesis in the SM and MSSM","version":3},"cited_work":{"arxiv_id":"hep-ph/0310123","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0310123","snapshot_observed_at":"2026-07-10T03:46:44.713037Z","title":"Towards a complete theory of thermal leptogenesis in the SM and MSSM","venue":"hep-ph","work_id":"c2d39e81-d759-4cb4-ae10-ae003867c362","year":2003},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/0310123","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:70511f2a223e23c342495020f0cf54ae121523dd6d1bc061bb37630b84c1bdbf","observation_id":"4857e30a-e97a-4d2a-aae9-664b74ccddb9","resolution":{"observed_at":"2026-05-11T14:21:06.076901Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Weldon,Effective Fermion Masses of Order gT in High Temperature Gauge Theories with Exact Chiral Invariance,Phys","venue":null,"work_id":"3e9ec8ca-0e76-4943-bd01-d55b878f12e8","year":1982},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:5d8bd138c163207f3c9f3e464d12502d8aaeec6226a25c955e93f7d88418958b","observation_id":"f781d20c-b89e-4b2f-9e1b-9da691b277b9","resolution":{"observed_at":"2026-05-23T15:15:42.385481Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9704366","last_updated":"1997-04-21T12:04:29Z","snapshot_observed_at":"2026-07-07T04:25:34.862416Z","submitted_at":"1997-04-21T12:04:29Z","title":"Finite temperature effects on CP violating asymmetries","version":1},"cited_work":{"arxiv_id":"hep-ph/9704366","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"hep-ph/9704366","snapshot_observed_at":"2026-07-04T16:04:56.350897Z","title":null,"venue":null,"work_id":"cfa0c5ca-0ea4-4073-85cf-64f133b63904","year":1998},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/hep-ph/9704366","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:5490e8a7891e20499b825a9647cb088fd71d0870c68c840e46afee7f61f0028c","observation_id":"1eb3a5a6-9545-4711-bfaf-fe3b9ecbfc40","resolution":{"observed_at":"2026-07-04T16:04:56.350897Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0909.1559","last_updated":"2010-01-05T10:50:19Z","snapshot_observed_at":"2026-07-06T02:01:48.296130Z","submitted_at":"2009-09-09T12:44:17Z","title":"Systematic approach to leptogenesis in nonequilibrium QFT: vertex contribution to the CP-violating parameter","version":2},"cited_work":{"arxiv_id":"0909.1559","doi":"10.1103/physrevd.80.125027","metadata_source":"pith","pith_arxiv_id":"0909.1559","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Systematic approach to leptogenesis in nonequilibrium QFT: vertex contribution to the CP-violating parameter","venue":"hep-ph","work_id":"49eea83d-785b-4587-baad-a5123f766440","year":2009},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/0909.1559","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:e4febe1b9f411845b3f82c699196194b6623d303c6036d79687fa56733727a72","observation_id":"4390a958-5dd7-4e22-b52e-79869ba17827","resolution":{"observed_at":"2026-05-11T14:21:05.941150Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-05-24T05:23:35.002996+00:00","source":"crossref_status_cache"},{"observed_at":"2026-05-24T05:23:35.002996+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1002.0331","last_updated":"2010-05-03T10:12:50Z","snapshot_observed_at":"2026-07-06T02:08:11.293394Z","submitted_at":"2010-02-02T10:18:36Z","title":"Medium corrections to the CP-violating parameter in leptogenesis","version":2},"cited_work":{"arxiv_id":"1002.0331","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1002.0331","snapshot_observed_at":"2026-07-04T17:28:17.452116Z","title":"Garny, A","venue":null,"work_id":"e41a11b9-4745-4822-8615-98c48c23f379","year":2010},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1002.0331","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:68369cd1f2d7916ad5b1da361e9707a5eab630b109019072ce7bca1077abb690","observation_id":"2458fcbf-905f-4698-9177-c2ce27a2da2b","resolution":{"observed_at":"2026-07-04T17:28:17.452116Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.07180","last_updated":"2025-06-12T15:41:32Z","snapshot_observed_at":"2026-07-06T19:13:42.074230Z","submitted_at":"2024-09-11T10:43:29Z","title":"CP violation at finite temperature","version":2},"cited_work":{"arxiv_id":"2409.07180","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2409.07180","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Seller, Z","venue":null,"work_id":"b6c053e8-73ea-4171-885e-23d9e989c016","year":2025},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/2409.07180","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:ed31b454b958e6140f1a47e4f3d38078a6ccb27053bae679c497360e25180c2d","observation_id":"7594a71c-8423-4d52-b266-a0463291c32d","resolution":{"observed_at":"2026-05-11T14:21:05.744958Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0911.4122","last_updated":"2010-05-01T21:46:01Z","snapshot_observed_at":"2026-07-06T01:59:50.632502Z","submitted_at":"2009-11-23T10:53:42Z","title":"Systematic approach to leptogenesis in nonequilibrium QFT: self-energy contribution to the CP-violating parameter","version":2},"cited_work":{"arxiv_id":"0911.4122","doi":null,"metadata_source":"pith","pith_arxiv_id":"0911.4122","snapshot_observed_at":"2026-07-01T23:56:22.876199Z","title":"Garny, A","venue":"hep-ph","work_id":"446ef740-567f-4c90-b7e3-b80dec4cf6ca","year":2009},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/0911.4122","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:85ba4eaac402b61da2c3255b0c3f5fc8a7721c9a1de2a37fddbec09e8b635973","observation_id":"475b139d-f8ee-4589-b88d-f0a6df891bd3","resolution":{"observed_at":"2026-05-11T14:21:05.712006Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Kadanoff and G","venue":null,"work_id":"4525f5d5-2e2c-4d7d-8f24-bdbbded87bd5","year":1962},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:d832f5a6970461a32bbd99c39340a33e026aa461b7b2901f45101a6f3d0d5ae7","observation_id":"3634a287-1607-445a-994b-eff2c039be86","resolution":{"observed_at":"2026-05-23T15:15:42.338495Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1012.5821","last_updated":"2013-11-01T14:00:12Z","snapshot_observed_at":"2026-07-06T02:21:20.431425Z","submitted_at":"2010-12-28T19:18:57Z","title":"Quantum Leptogenesis I","version":3},"cited_work":{"arxiv_id":"1012.5821","doi":null,"metadata_source":"pith","pith_arxiv_id":"1012.5821","snapshot_observed_at":"2026-07-01T23:56:22.892779Z","title":"Anisimov, W","venue":"hep-ph","work_id":"bc3a0c0f-3404-4d4b-a133-4c036335755d","year":2010},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1012.5821","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:d23f6675649f14f81c17a64e79c2bb28f62a952294fe3e0c1e3a879009eabe85","observation_id":"31d88640-2d9a-4423-b17f-9ce4f87a5fd7","resolution":{"observed_at":"2026-05-11T14:21:06.021773Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1711.02861","last_updated":"2018-03-07T12:47:52Z","snapshot_observed_at":"2026-07-06T06:08:21.709024Z","submitted_at":"2017-11-08T08:15:04Z","title":"Flavor effects in leptogenesis","version":2},"cited_work":{"arxiv_id":"1711.02861","doi":null,"metadata_source":"pith","pith_arxiv_id":"1711.02861","snapshot_observed_at":"2026-07-04T03:59:33.260661Z","title":"Flavor effects in leptogenesis","venue":"hep-ph","work_id":"9b0fdbc2-7943-4ee8-9916-3b530c1a7604","year":2017},"citing_paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-05-09T22:00:42.126071Z"},"links":{"cited_paper":"/paper/1711.02861","citing_paper":"/paper/2604.21492"},"observation_digest":"sha256:807b8c730e271af2887ffcd3b08531784288e50da4727821176db5afa7d67458","observation_id":"83835961-03d0-4335-a45c-0675c42740f1","resolution":{"observed_at":"2026-05-11T14:21:06.256635Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2604.21492","last_updated":"2026-04-23T09:53:27Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-07-06T23:08:05.568089Z","submitted_at":"2026-04-23T09:53:27Z","title":"Solving Cosmological Puzzles using Finite Temperature $\\nu$SMEFT"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":2,"parse_uncertain":0,"unresolved":0,"verified_exact":83,"verified_fuzzy":15},"total_outbound_references":113},"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":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"thesis":"As of 3 August 2026, this Paper Citation Record lists 100 of 113 outbound references and 1 inbound Pith citation observation for arXiv:2604.21492."}