{"as_of":"2026-08-08T16:41:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:2c3e3a03a4a4cda88d32018e24a8711c28802852e79544cb39b0f1997b90862d","coverage":[{"denominator":134,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T00:43:57.092370Z","state":"measured"},{"denominator":100,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":100,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-08T06:32:00.761636+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"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":[],"links":{"evidence":"/evidence","html":"/paper/2608.04102/citation-record","integrity":"/paper/2608.04102/integrity","json":"/paper/2608.04102/citation-record.json","paper":"/paper/2608.04102"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.674244Z","title":"Kuzmin, V.A","venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.674244Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:c53a75dde607b641441615f0b889c1f7d0b0478514e93c5808e02ebc650af9ef","observation_id":"e6c08fe0-fd12-4194-92a3-21127acff9a2","resolution":{"observed_at":"2026-08-08T00:43:56.674244Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1206.2942","last_updated":"2012-06-13T21:09:14Z","snapshot_observed_at":"2026-08-08T01:42:38.357720Z","submitted_at":"2012-06-13T21:09:14Z","title":"Electroweak baryogenesis","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1206.2942","snapshot_observed_at":"2026-08-08T00:43:56.678141Z","title":"Morrissey and M.J","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.678141Z"},"links":{"cited_paper":"/paper/1206.2942","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:19233e824c48479774bde523dbc6b16c197bff61a2960964f4cc45800a98a0bd","observation_id":"6f264bff-aac4-4404-be29-6f4ba5a9b078","resolution":{"observed_at":"2026-08-08T00:43:56.678141Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.682228Z","title":"Sakharov,Violation of CP Invariance, C asymmetry, and baryon asymmetry of the universe,Pisma Zh","venue":null,"work_id":null,"year":1967},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.682228Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:e91a18d03de8e31f5c84762d91b2cd7f0d630abac529a71e2fb020da1ebb2d7a","observation_id":"2a4a6424-53bc-4033-a415-a6dc8b822400","resolution":{"observed_at":"2026-08-08T00:43:56.682228Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.00786","last_updated":"2017-02-23T05:33:01Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2017-02-02T07:06:53Z","title":"Laser Interferometer Space Antenna","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.00786","snapshot_observed_at":"2026-08-08T00:43:56.685601Z","title":"Hogan,Gravitational radiation from cosmological phase transitions,Mon","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.685601Z"},"links":{"cited_paper":"/paper/1702.00786","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:a8c08b3f531bc165f243d0a6268558b1beb10ae65dbb1c77cb4b4c5ecc450062","observation_id":"7233133c-73af-4de0-87ba-e208f7f7a4a1","resolution":{"observed_at":"2026-08-08T00:43:56.685601Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1907.04833","snapshot_observed_at":"2026-08-08T00:43:56.689592Z","title":"Reitze et al.,Cosmic Explorer: The U.S","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.689592Z"},"links":{"cited_paper":"/paper/1907.04833","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:135a2f6b30ca18ef9aefe7d54acfd2d0d4a65448de8d2861b436cc9a182fdfe0","observation_id":"35cc9b7a-8030-4447-966d-14ecc8403f15","resolution":{"observed_at":"2026-08-08T00:43:56.689592Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0506015","last_updated":"2005-10-17T19:04:42Z","snapshot_observed_at":"2026-08-05T12:28:13.758896Z","submitted_at":"2005-06-03T16:46:52Z","title":"Beyond LISA: Exploring Future Gravitational Wave Missions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0506015","snapshot_observed_at":"2026-08-08T00:43:56.692968Z","title":"Crowder and N.J","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.692968Z"},"links":{"cited_paper":"/paper/gr-qc/0506015","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:122cfbb2c53297f9b7415e98742de57d982ac1dc82cd2a7a1b63d2097f5e0673","observation_id":"252cd9bf-e170-489d-ad62-09d3a4163d9e","resolution":{"observed_at":"2026-08-08T00:43:56.692968Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0512039","snapshot_observed_at":"2026-08-08T00:43:56.696852Z","title":"Corbin and N.J","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.696852Z"},"links":{"cited_paper":"/paper/gr-qc/0512039","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:5d0c429317a4beac031113fc464fe4b1310116789ab8be718dccc6a409cdcd71","observation_id":"06791adf-007c-4c1e-9b82-ab05e2602062","resolution":{"observed_at":"2026-08-08T00:43:56.696852Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.700608Z","title":"Harry, P","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.700608Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:24bd078ee39481b49618f1ab9d695c21c907855086b50116943e63415126ceac","observation_id":"8874bfb0-8d88-4b8d-9b9c-bf3d76e7d781","resolution":{"observed_at":"2026-08-08T00:43:56.700608Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.03980","last_updated":"2022-01-11T14:50:51Z","snapshot_observed_at":"2026-08-02T19:37:58.755279Z","submitted_at":"2022-01-11T14:50:51Z","title":"The International Pulsar Timing Array second data release: Search for an isotropic Gravitational Wave Background","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.03980","snapshot_observed_at":"2026-08-08T00:43:56.703610Z","title":"Antoniadis et al.,The International Pulsar Timing Array second data release: Search for an isotropic gravitational wave background,Mon","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.703610Z"},"links":{"cited_paper":"/paper/2201.03980","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:676b8a944d50b32c81f1993e30f6179464569fe15eec6d530d4d994ea19d98d7","observation_id":"994846d8-cb33-4020-833b-bfc85c85a9e9","resolution":{"observed_at":"2026-08-08T00:43:56.703610Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.13125","last_updated":"2021-01-12T09:42:19Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2019-10-29T07:58:57Z","title":"Detecting gravitational waves from cosmological phase transitions with LISA: an update","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.13125","snapshot_observed_at":"2026-08-08T00:43:56.706775Z","title":"Caprini et al.,Detecting gravitational waves from cosmological phase transitions with LISA: an update,JCAP03(2020) 024 [1910.13125]","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.706775Z"},"links":{"cited_paper":"/paper/1910.13125","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:aef8696c25a83e99ad3340e675c30996890e23d25a152bbdea1fad661f4d46e0","observation_id":"0213370b-9088-4d05-81de-1f79811641e3","resolution":{"observed_at":"2026-08-08T00:43:56.706775Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.02357","last_updated":"2024-01-22T08:56:34Z","snapshot_observed_at":"2026-08-08T07:37:24.501613Z","submitted_at":"2023-05-03T18:00:08Z","title":"Cosmological phase transitions: from perturbative particle physics to gravitational waves","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.02357","snapshot_observed_at":"2026-08-08T00:43:56.709895Z","title":"Athron, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.709895Z"},"links":{"cited_paper":"/paper/2305.02357","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:b2d668ca74189710e888bf4f0a7a450ce1cb0654f58d0c16d09876ebdffaafa7","observation_id":"222d74d5-5fd1-49a6-afe7-6c720393ee0d","resolution":{"observed_at":"2026-08-08T00:43:56.709895Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.713140Z","title":"Croon and D.J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.713140Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:24ff68764f482bd1078c5a706124af2053c9db532dcfbb44c7463ea1f1dc334e","observation_id":"91f5712e-b869-4df2-8a52-ef2cef5ed7d7","resolution":{"observed_at":"2026-08-08T00:43:56.713140Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.715834Z","title":"Dolan and R","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.715834Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:79e3389f8d4e185ed427b224aa5e0a8e227add18c116aab81e672381fdc4c42e","observation_id":"cb2e277b-ef15-4389-b2b2-077cc1fbd0a2","resolution":{"observed_at":"2026-08-08T00:43:56.715834Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.718572Z","title":"Weinberg,Gauge and Global Symmetries at High Temperature,Phys","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.718572Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:dafb5d1770f26abcf7e5eaa38fcaa217e9557045c762ccaa1ccccb6cbffd2e02","observation_id":"20fada6d-a98c-4884-897a-1e10ad5f1a90","resolution":{"observed_at":"2026-08-08T00:43:56.718572Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.721234Z","title":"Kirzhnits and A.D","venue":null,"work_id":null,"year":1976},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.721234Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:866656f74ea29a8bc1322a0a895d055b00631c725eebde8bfc643c931f08a668","observation_id":"98ce21d5-15c2-4352-84eb-ed12070a13d9","resolution":{"observed_at":"2026-08-08T00:43:56.721234Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0102028","last_updated":"2001-02-21T10:19:00Z","snapshot_observed_at":"2026-07-07T04:39:08.132477Z","submitted_at":"2001-02-06T19:22:34Z","title":"Chiral gauge theories revisited","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0102028","snapshot_observed_at":"2026-08-08T00:43:56.724079Z","title":"Luscher,Chiral gauge theories revisited,Subnucl","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.724079Z"},"links":{"cited_paper":"/paper/hep-th/0102028","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:ca1a9c2754d070f87fd356752071b424cca5eecf13977b1edc086050a67b5138","observation_id":"931ee1f1-6bd4-42a7-b667-b6433326c845","resolution":{"observed_at":"2026-08-08T00:43:56.724079Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.726949Z","title":"Linde,Infrared Problem in Thermodynamics of the Yang-Mills Gas,Phys","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.726949Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:d60091066c67bd813159c5ae220b499f8e3a2290f0ec63a7e5d28f55bb4bc643","observation_id":"d43021a4-4774-43b7-8186-f19900ea5406","resolution":{"observed_at":"2026-08-08T00:43:56.726949Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.729638Z","title":"Gross, R.D","venue":null,"work_id":null,"year":1981},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.729638Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:9afc0ad54b7952cfb940e325365c248739f83bf75dc95786b439b72e84ef6e93","observation_id":"65bafc94-ff8c-4e17-a346-4960cd501a48","resolution":{"observed_at":"2026-08-08T00:43:56.729638Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.01554","last_updated":"2022-01-14T16:57:11Z","snapshot_observed_at":"2026-08-08T13:42:22.052090Z","submitted_at":"2017-01-06T06:39:49Z","title":"Basics of thermal field theory -- a tutorial on perturbative computations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.01554","snapshot_observed_at":"2026-08-08T00:43:56.732471Z","title":"Laine and A","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.732471Z"},"links":{"cited_paper":"/paper/1701.01554","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:9d09b3c91b4d96f2f1163c08648f914e940bf9ec91c9449ff1d07bb753be661d","observation_id":"4915d9ca-5a51-45c9-923a-dac0d1db92b8","resolution":{"observed_at":"2026-08-08T00:43:56.732471Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0003111","last_updated":"2000-05-23T16:04:34Z","snapshot_observed_at":"2026-07-07T03:47:57.608369Z","submitted_at":"2000-03-13T09:10:31Z","title":"Two-loop dimensional reduction and effective potential without temperature expansions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0003111","snapshot_observed_at":"2026-08-08T00:43:56.735356Z","title":"Laine and M","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.735356Z"},"links":{"cited_paper":"/paper/hep-ph/0003111","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:911cd917aea98ec256f0d8146f775e90ced62a1eb0151185e872580f2c00495f","observation_id":"040c8677-aa8f-4809-a8f4-7a81b9db7d28","resolution":{"observed_at":"2026-08-08T00:43:56.735356Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0404164","last_updated":"2004-08-17T11:38:20Z","snapshot_observed_at":"2026-08-01T14:47:05.825174Z","submitted_at":"2004-04-20T15:18:03Z","title":"Resummation in Hot Field Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0404164","snapshot_observed_at":"2026-08-08T00:43:56.738540Z","title":"Andersen and M","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.738540Z"},"links":{"cited_paper":"/paper/hep-ph/0404164","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:fb1d91faa3ceb798f70aba53773eaee89bfa775757e986809ba66542e9dda644","observation_id":"2e27d59b-99de-4b6d-b5f5-178e66688ec0","resolution":{"observed_at":"2026-08-08T00:43:56.738540Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.741820Z","title":"Carrington,The Effective potential at finite temperature in the Standard Model,Phys","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.741820Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:6f564cd53b4e9bb512161bdc3c58b20fdb977dc70cbf04ae0471c83c016d0a3a","observation_id":"c8c88571-0337-49f6-a7bb-7ab4720a3324","resolution":{"observed_at":"2026-08-08T00:43:56.741820Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9212235","snapshot_observed_at":"2026-08-08T00:43:56.744938Z","title":"Arnold and O","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.744938Z"},"links":{"cited_paper":"/paper/hep-ph/9212235","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:b78059f8993eccbd5fa29be8077fe610a3b3470f96c6190c1c82ddc773ccf9a5","observation_id":"b3136986-4c57-4584-877e-ede55c4a37d4","resolution":{"observed_at":"2026-08-08T00:43:56.744938Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9204216","last_updated":"1992-04-10T04:03:55Z","snapshot_observed_at":"2026-08-05T09:52:22.302331Z","submitted_at":"1992-04-10T04:03:55Z","title":"Resummation in a Hot Scalar Field Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9204216","snapshot_observed_at":"2026-08-08T00:43:56.748182Z","title":"Parwani,Resummation in a hot scalar field theory,Phys","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.748182Z"},"links":{"cited_paper":"/paper/hep-ph/9204216","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:bcd8466bfee46909663dfb1ffa743caef234ae9c54718d716a8039ffe7d155c4","observation_id":"66ab1d9c-51ef-42fb-a5fe-b2abbcc76208","resolution":{"observed_at":"2026-08-08T00:43:56.748182Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9404201","last_updated":"1994-04-01T12:09:00Z","snapshot_observed_at":"2026-07-07T04:17:00.564341Z","submitted_at":"1994-04-01T12:09:00Z","title":"3D Physics and the Electroweak Phase Transition: Perturbation Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9404201","snapshot_observed_at":"2026-08-08T00:43:56.752198Z","title":"Farakos, K","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.752198Z"},"links":{"cited_paper":"/paper/hep-ph/9404201","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:66a714162958c25647b537dc4214c2a9b297a951491f6db87f124ef4ef960a0b","observation_id":"fcee8e4a-0ad6-49d5-abeb-f5a6c9f848b8","resolution":{"observed_at":"2026-08-08T00:43:56.752198Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9508379","last_updated":"1995-08-27T17:00:19Z","snapshot_observed_at":"2026-08-04T10:09:33.703228Z","submitted_at":"1995-08-27T17:00:19Z","title":"Generic Rules for High Temperature Dimensional Reduction and Their Application to the Standard Model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9508379","snapshot_observed_at":"2026-08-08T00:43:56.755590Z","title":"Kajantie, M","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.755590Z"},"links":{"cited_paper":"/paper/hep-ph/9508379","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:01e9bbb381ad89b89eb18f061bd5644240efaa223a89c150581baf43e96e6b73","observation_id":"a9a8da9e-8cbc-4b0c-bcc7-1c7408cc62f4","resolution":{"observed_at":"2026-08-08T00:43:56.755590Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9501375","last_updated":"1995-01-25T20:47:46Z","snapshot_observed_at":"2026-08-06T12:07:28.654979Z","submitted_at":"1995-01-25T20:47:46Z","title":"Effective Field Theory Approach to High-Temperature Thermodynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9501375","snapshot_observed_at":"2026-08-08T00:43:56.759513Z","title":"Braaten and A","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.759513Z"},"links":{"cited_paper":"/paper/hep-ph/9501375","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:8558ec3cbe61bc27420fa3c40e213bf7a9f50aea7fde69170bae053655a8f53c","observation_id":"0fa5dd64-ca8e-4d91-939c-f29ec13d7f2c","resolution":{"observed_at":"2026-08-08T00:43:56.759513Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/9510020","last_updated":"1995-10-12T18:32:43Z","snapshot_observed_at":"2026-08-07T14:30:58.057125Z","submitted_at":"1995-10-12T18:32:43Z","title":"The Electroweak Phase Transition: A Non-Perturbative Analysis","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/9510020","snapshot_observed_at":"2026-08-08T00:43:56.763154Z","title":"Kajantie, M","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.763154Z"},"links":{"cited_paper":"/paper/hep-lat/9510020","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:817563271a6160ed8f81bc878f4a0ac3256ba5a03c9f0cf859b3a450f89ff4e3","observation_id":"9d16d7c0-a512-4069-85d8-1f7ddc53e8b0","resolution":{"observed_at":"2026-08-08T00:43:56.763154Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.18349","last_updated":"2024-05-28T16:46:00Z","snapshot_observed_at":"2026-08-07T17:28:28.965748Z","submitted_at":"2024-05-28T16:46:00Z","title":"Cosmological phase transitions at three loops: the final verdict on perturbation theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.18349","snapshot_observed_at":"2026-08-08T00:43:56.766901Z","title":"Ekstedt, P","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.766901Z"},"links":{"cited_paper":"/paper/2405.18349","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:6775ee56d27cf842287d5c65d77c20b9c9baa1e0e53a2be9154006fb7faa4b53","observation_id":"732dfcd0-4fd0-4f1b-b72d-245b86596332","resolution":{"observed_at":"2026-08-08T00:43:56.766901Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.01672","last_updated":"2023-09-04T15:35:50Z","snapshot_observed_at":"2026-08-06T01:49:20.256519Z","submitted_at":"2023-09-04T15:35:50Z","title":"Perturbative effective field theory expansions for cosmological phase transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.01672","snapshot_observed_at":"2026-08-08T00:43:56.770132Z","title":"Gould and T.V.I","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.770132Z"},"links":{"cited_paper":"/paper/2309.01672","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:a73e8ea5e7ba00b1bfb21cfe4232bdf3447d51090cb0913f9ad47d9051a17633","observation_id":"ba259b21-0a77-4c1c-8737-74216b068c57","resolution":{"observed_at":"2026-08-08T00:43:56.770132Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.07479","last_updated":"2017-05-19T08:57:09Z","snapshot_observed_at":"2026-07-06T05:31:14.242311Z","submitted_at":"2017-02-24T07:16:16Z","title":"Thermal phase transition with full 2-loop effective potential","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.07479","snapshot_observed_at":"2026-08-08T00:43:56.773058Z","title":"Laine, M","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.773058Z"},"links":{"cited_paper":"/paper/1702.07479","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:fae2aca3295544ad4037ee22ad30de96689d6644289303adba5fb5748831196d","observation_id":"a3998a09-ab3e-470b-828d-f31b00b7d543","resolution":{"observed_at":"2026-08-08T00:43:56.773058Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1904.01329","snapshot_observed_at":"2026-08-08T00:43:56.776353Z","title":"Kainulainen, V","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.776353Z"},"links":{"cited_paper":"/paper/1904.01329","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:1e6ab74bdee4dbf065a0a77d88b854018ac63ea2ee75e35f8ffdd95ff8e742b7","observation_id":"17b37eca-1a93-465e-8519-c99bd3497639","resolution":{"observed_at":"2026-08-08T00:43:56.776353Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.01191","last_updated":"2024-08-10T09:29:05Z","snapshot_observed_at":"2026-08-06T20:54:48.825620Z","submitted_at":"2024-05-02T11:32:02Z","title":"Nonperturbative study of the electroweak phase transition in the real scalar singlet extended Standard Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.01191","snapshot_observed_at":"2026-08-08T00:43:56.779133Z","title":"Niemi, M.J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.779133Z"},"links":{"cited_paper":"/paper/2405.01191","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:0f504a50cdccd6016bbdc20243dee0cab3e6388e02de5ad6210e04096d3480c8","observation_id":"79cf9ead-c582-40f2-99fa-63b9b24ad659","resolution":{"observed_at":"2026-08-08T00:43:56.779133Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.02667","last_updated":"2024-10-10T13:26:40Z","snapshot_observed_at":"2026-08-06T22:47:15.010721Z","submitted_at":"2024-06-04T18:00:00Z","title":"Higher-order corrections to phase-transition parameters in dimensional reduction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.02667","snapshot_observed_at":"2026-08-08T00:43:56.782189Z","title":"Chala, J.C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.782189Z"},"links":{"cited_paper":"/paper/2406.02667","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:51c07a0544540696ccc6086ff9abd8bf88cf11521b9d586d2f5febb77e993ce9","observation_id":"9b0ced0e-c709-4ec9-a2ee-aab87fa89844","resolution":{"observed_at":"2026-08-08T00:43:56.782189Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.20016","last_updated":"2026-04-24T12:03:33Z","snapshot_observed_at":"2026-07-06T20:58:41.966283Z","submitted_at":"2025-03-25T19:00:00Z","title":"The High-Temperature Limit of the SM(EFT)","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.20016","snapshot_observed_at":"2026-08-08T00:43:56.785468Z","title":"Chala and G","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.785468Z"},"links":{"cited_paper":"/paper/2503.20016","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:7577804d71062faa9b679ef764281a2827641cbe3099ce1135d4798d8e012490","observation_id":"50f60952-6529-45ce-acc9-2318b9192c3c","resolution":{"observed_at":"2026-08-08T00:43:56.785468Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.14335","last_updated":"2025-05-20T13:20:49Z","snapshot_observed_at":"2026-08-08T03:51:33.373048Z","submitted_at":"2025-05-20T13:20:49Z","title":"Phase Transitions in Dimensional Reduction up to Three Loops","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.14335","snapshot_observed_at":"2026-08-08T00:43:56.788933Z","title":"Chala, L","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.788933Z"},"links":{"cited_paper":"/paper/2505.14335","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:cb5ba6527269cd4f2834e252245c2decd9f739edd74e6fdecfcf8593b6590758","observation_id":"622f214e-ac0c-4bc4-8574-4551f1f7ef78","resolution":{"observed_at":"2026-08-08T00:43:56.788933Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.18904","last_updated":"2026-05-29T21:09:14Z","snapshot_observed_at":"2026-08-07T16:40:33.859982Z","submitted_at":"2025-03-24T17:16:28Z","title":"Higher-dimensional operators at finite-temperature affect gravitational-wave predictions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.18904","snapshot_observed_at":"2026-08-08T00:43:56.792098Z","title":"Bernardo, P","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.792098Z"},"links":{"cited_paper":"/paper/2503.18904","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:f153ed17df9ece0f4dfa891eb3814221d40adf41581b1b1db55fca880d870f8f","observation_id":"d5f98391-d205-44ed-a413-de56f4033478","resolution":{"observed_at":"2026-08-08T00:43:56.792098Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2607.18233","last_updated":"2026-07-20T17:59:02Z","snapshot_observed_at":"2026-08-07T23:30:12.823484Z","submitted_at":"2026-07-20T17:59:02Z","title":"Theoretical uncertainties in reconstructing model parameters with gravitational waves from supercooled phase transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2607.18233","snapshot_observed_at":"2026-08-08T00:43:56.795190Z","title":"Kierkla, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.795190Z"},"links":{"cited_paper":"/paper/2607.18233","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:3c635db2ad5a0096bf12f6f286f20c724ffcdf4086263b79638a12daf13920ac","observation_id":"2f5f7a3b-285f-47c1-88f6-ddcbdc6dcae4","resolution":{"observed_at":"2026-08-08T00:43:56.795190Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9304254","last_updated":"1993-04-15T00:17:19Z","snapshot_observed_at":"2026-08-03T00:44:59.846254Z","submitted_at":"1993-04-15T00:17:19Z","title":"Resummation Methods at Finite Temperature: The Tadpole Way","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9304254","snapshot_observed_at":"2026-08-08T00:43:56.798282Z","title":"Boyd, D.E","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.798282Z"},"links":{"cited_paper":"/paper/hep-ph/9304254","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:d7ed7c69de4be09977040ed4ca9af123f567e9971400d199093770d49874a2d3","observation_id":"f102e7e4-65bf-4264-b581-f39586dcac9a","resolution":{"observed_at":"2026-08-08T00:43:56.798282Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1210.1737","last_updated":"2013-02-27T13:19:48Z","snapshot_observed_at":"2026-07-06T02:57:02.001372Z","submitted_at":"2012-10-05T12:40:41Z","title":"Two-loop effective potential, thermal resummation and first-order phase transitions: Beyond the high-temperature expansion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1210.1737","snapshot_observed_at":"2026-08-08T00:43:56.801180Z","title":"Funakubo and E","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.801180Z"},"links":{"cited_paper":"/paper/1210.1737","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:85ef80060619d6e2e14a2e1ff389699fc432c50fb014146015226ed2c31fbb2a","observation_id":"67cecac5-4ff9-4b46-89e4-7d1767c50ec3","resolution":{"observed_at":"2026-08-08T00:43:56.801180Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.03508","last_updated":"2016-01-07T20:42:14Z","snapshot_observed_at":"2026-07-06T04:23:40.944905Z","submitted_at":"2015-07-13T16:17:36Z","title":"Scale Invariant Resummed Perturbation at Finite Temperatures","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.03508","snapshot_observed_at":"2026-08-08T00:43:56.804456Z","title":"Kneur and M.B","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.804456Z"},"links":{"cited_paper":"/paper/1507.03508","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:797d57b95afc0c02271147ce02fe7ea17426c1b1fec1699cbe654209290a18ba","observation_id":"36c64a4d-b2c5-4047-9bab-7a34d13d95ae","resolution":{"observed_at":"2026-08-08T00:43:56.804456Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.00466","last_updated":"2016-12-01T21:03:08Z","snapshot_observed_at":"2026-08-06T10:55:48.558692Z","submitted_at":"2016-12-01T21:03:08Z","title":"Thermal Resummation and Phase Transitions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.00466","snapshot_observed_at":"2026-08-08T00:43:56.807539Z","title":"Curtin, P","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.807539Z"},"links":{"cited_paper":"/paper/1612.00466","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:937a92a6671af585ccc7cd0ac3c44b0ea1856091e4f167f8a5fde016076ef62a","observation_id":"b38cafe0-33d1-43c2-aa91-6dd59b48791d","resolution":{"observed_at":"2026-08-08T00:43:56.807539Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.08218","last_updated":"2024-06-03T14:31:37Z","snapshot_observed_at":"2026-07-06T14:18:37.979687Z","submitted_at":"2022-11-15T15:40:34Z","title":"Gravitational waves and tadpole resummation: Efficient and easy convergence of finite temperature QFT","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.08218","snapshot_observed_at":"2026-08-08T00:43:56.810644Z","title":"Curtin, J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.810644Z"},"links":{"cited_paper":"/paper/2211.08218","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:63d32d16daff388ce3540f44ff2addb08550376e410fbae60d8818edf8b3c0db","observation_id":"d743d0b8-6618-43f8-a182-0001f94807ca","resolution":{"observed_at":"2026-08-08T00:43:56.810644Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.02153","last_updated":"2024-03-28T01:40:48Z","snapshot_observed_at":"2026-08-07T10:31:46.589105Z","submitted_at":"2023-07-05T09:50:07Z","title":"A renormalization group improvement for thermally resummed effective potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.02153","snapshot_observed_at":"2026-08-08T00:43:56.813871Z","title":"Funakubo and E","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.813871Z"},"links":{"cited_paper":"/paper/2307.02153","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:55329a195110f30004b48ebfb4454257673436a61d808060f15ee9136fa7ad1e","observation_id":"8c555796-2704-4bda-b068-59591f9f4092","resolution":{"observed_at":"2026-08-08T00:43:56.813871Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.15876","last_updated":"2024-03-10T07:15:49Z","snapshot_observed_at":"2026-07-06T16:12:10.861522Z","submitted_at":"2023-08-30T09:00:03Z","title":"Refined renormalization group improvement for thermally resummed effective potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.15876","snapshot_observed_at":"2026-08-08T00:43:56.819032Z","title":"Funakubo and E","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.819032Z"},"links":{"cited_paper":"/paper/2308.15876","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:8b4c8af3a2ecc7c44e77e47ae9520ff01b3a9f20c71b69778cd5ba489d9cbf6e","observation_id":"a8c0b614-ae3f-48da-97f9-d8388e7392af","resolution":{"observed_at":"2026-08-08T00:43:56.819032Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2404.12439","last_updated":"2024-08-25T21:15:29Z","snapshot_observed_at":"2026-07-06T18:02:23.732670Z","submitted_at":"2024-04-18T18:01:01Z","title":"Improved Thermal Resummation for Multi-Field Potentials","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2404.12439","snapshot_observed_at":"2026-08-08T00:43:56.822277Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.822277Z"},"links":{"cited_paper":"/paper/2404.12439","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:9548684e853b844e9e024c42f20d850f4b7d7b66eb16ed43a4dbcfef904e365b","observation_id":"62d9c8b1-5e9b-46ae-ac07-db2942e6cb39","resolution":{"observed_at":"2026-08-08T00:43:56.822277Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.825234Z","title":"Bittar, S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.825234Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:f558470e5b07c300cb9630ed3514acdabdb7ea9f106b31ff7431497e859e7f9e","observation_id":"aaf1714c-c3ee-4d3c-9e61-94b989f696b4","resolution":{"observed_at":"2026-08-08T00:43:56.825234Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.07014","last_updated":"2025-07-09T16:44:17Z","snapshot_observed_at":"2026-08-06T19:18:31.167597Z","submitted_at":"2025-07-09T16:44:17Z","title":"Cosmological phase transitions without high-temperature expansions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.07014","snapshot_observed_at":"2026-08-08T00:43:56.828055Z","title":"Navarrete, R","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.828055Z"},"links":{"cited_paper":"/paper/2507.07014","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:f49d3b1eff2149e1599fa51e32e30ab6deca27766d19c454a2d3ac055df3e4d7","observation_id":"dd82811a-1211-49d3-bf6c-99880b6a135e","resolution":{"observed_at":"2026-08-08T00:43:56.828055Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2607.21252","last_updated":"2026-07-23T12:23:01Z","snapshot_observed_at":"2026-08-06T12:13:37.755522Z","submitted_at":"2026-07-23T12:23:01Z","title":"Thermal Resummation for Very Strong First-order Phase Transitions","version":1},"cited_work":{"arxiv_id":"2607.21252","doi":null,"metadata_source":"pith","pith_arxiv_id":"2607.21252","snapshot_observed_at":"2026-08-08T00:44:06.985155Z","title":"Thermal Resummation for Very Strong First-order Phase Transitions","venue":"hep-ph","work_id":"5362823a-a296-4258-af96-5f1a4c19b755","year":2026},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.831157Z"},"links":{"cited_paper":"/paper/2607.21252","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:f357c2b7611905a301d1ba3e6f35bc8defa9fb24cd00c213b6dae0028c8d74ac","observation_id":"da8212f6-8871-4da7-af73-9ed45b2975e5","resolution":{"observed_at":"2026-08-08T00:44:07.026969Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.834412Z","title":"Jackiw,Functional evaluation of the effective potential,Phys","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.834412Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:094106608197ed0b7e518e90f61f758925f0843eeb21c619547945587078e8d2","observation_id":"89fd855c-882d-43dd-9268-737a1ac24139","resolution":{"observed_at":"2026-08-08T00:43:56.834412Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.837836Z","title":"Cornwall, R","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.837836Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:862ffd1eb422cd47d7a6beb6e6ea128c22eee602d7a5213f1e9c593555744abb","observation_id":"267ec2d8-d59f-42fc-a603-7ceb445886d1","resolution":{"observed_at":"2026-08-08T00:43:56.837836Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9211211","last_updated":"1992-11-11T23:20:56Z","snapshot_observed_at":"2026-08-06T01:57:26.174749Z","submitted_at":"1992-11-04T17:09:46Z","title":"Self-consistent Improvement of the Finite Temperature Effective Potential","version":2},"cited_work":{"arxiv_id":"hep-ph/9211211","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9211211","snapshot_observed_at":"2026-08-08T00:44:06.774745Z","title":"Self-consistent Improvement of the Finite Temperature Effective Potential","venue":"hep-ph","work_id":"7a026fdd-41e2-48d4-affb-2445cd60a870","year":1992},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.841274Z"},"links":{"cited_paper":"/paper/hep-ph/9211211","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:59e79d42e403d99a611b7abeb2aa6cc385d463479238355482538d21334c4adc","observation_id":"6d4dc087-21fa-4ea7-9f17-2ea7b663b5da","resolution":{"observed_at":"2026-08-08T00:44:06.804829Z","resolver_source":"local_arxiv","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9305222","last_updated":"1994-01-19T23:24:22Z","snapshot_observed_at":"2026-08-08T00:03:45.680693Z","submitted_at":"1993-05-07T00:31:18Z","title":"Self-consistently Improved Finite Temperature Effective Potential for Gauge Theories","version":2},"cited_work":{"arxiv_id":"hep-ph/9305222","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9305222","snapshot_observed_at":"2026-08-08T00:44:06.594745Z","title":"Self-consistently Improved Finite Temperature Effective Potential for Gauge Theories","venue":"hep-ph","work_id":"95424a63-e2e2-4de6-8bd6-a525d573cca7","year":1993},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.844695Z"},"links":{"cited_paper":"/paper/hep-ph/9305222","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:b695dbcbef3bb1273ad4f2d9da5751689d6bd096252a335ddae401200ece4c0b","observation_id":"1530cad8-c9f9-4a4b-b7a1-82c028629f7b","resolution":{"observed_at":"2026-08-08T00:44:06.624750Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2105.09598","last_updated":"2022-01-03T09:26:45Z","snapshot_observed_at":"2026-08-01T04:58:18.692559Z","submitted_at":"2021-05-20T08:49:43Z","title":"Non-equilibrium dynamics of a scalar field with quantum backreaction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.09598","snapshot_observed_at":"2026-08-08T00:43:56.847804Z","title":"Kainulainen and O","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.847804Z"},"links":{"cited_paper":"/paper/2105.09598","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:7a029717174695ec340b717f3b09dd2c02ee0ae22b705a115b9eb553de963c28","observation_id":"a18e6553-f013-40ba-891a-6ae9d580ec26","resolution":{"observed_at":"2026-08-08T00:43:56.847804Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0503240","last_updated":"2005-10-11T13:46:04Z","snapshot_observed_at":"2026-07-07T04:07:01.540964Z","submitted_at":"2005-03-23T16:26:51Z","title":"Nonperturbative renormalization for 2PI effective action techniques","version":2},"cited_work":{"arxiv_id":"hep-ph/0503240","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0503240","snapshot_observed_at":"2026-08-08T00:44:06.144741Z","title":"Nonperturbative renormalization for 2PI effective action techniques","venue":"hep-ph","work_id":"6553d269-fc1b-48bd-8c5a-d687b51909e1","year":2005},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.851124Z"},"links":{"cited_paper":"/paper/hep-ph/0503240","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:ec1db835e54ef3300b59e5915a73740846bf9bed6a84d37d8ffd04173665e104","observation_id":"d57443d0-5048-4f1e-8d09-ea5c56a8a7fc","resolution":{"observed_at":"2026-08-08T00:44:06.184738Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0107200","last_updated":"2001-08-29T14:09:14Z","snapshot_observed_at":"2026-07-07T03:53:05.112770Z","submitted_at":"2001-07-18T20:59:15Z","title":"Renormalization in Self-Consistent Approximations schemes at Finite Temperature I: Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0107200","snapshot_observed_at":"2026-08-08T00:43:56.854696Z","title":"van Hees and J","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.854696Z"},"links":{"cited_paper":"/paper/hep-ph/0107200","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:23af37ebcd9d5eec1508d111ed2edbc6c16392a79972c825e86584a312a48013","observation_id":"2e8fc3fc-1d03-4e4f-bd78-7c921022f1ac","resolution":{"observed_at":"2026-08-08T00:43:56.854696Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0111193","last_updated":"2002-02-05T13:40:05Z","snapshot_observed_at":"2026-07-07T03:54:14.918367Z","submitted_at":"2001-11-15T18:16:19Z","title":"Renormalization of Self-consistent Approximation schemes Finite Temperature II: Applications to the Sunset Diagram","version":4},"cited_work":{"arxiv_id":"hep-ph/0111193","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0111193","snapshot_observed_at":"2026-08-08T00:44:05.774742Z","title":"Renormalization of Self-consistent Approximation schemes Finite Temperature II: Applications to the Sunset Diagram","venue":"hep-ph","work_id":"1d589346-b83f-4153-8260-41194d160628","year":2001},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.858255Z"},"links":{"cited_paper":"/paper/hep-ph/0111193","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:3b5be444c2f88776de7888c56e4d4a0127b163482ce7494c128d51d3b4850320","observation_id":"db8968ff-ae81-44d1-b0d1-0eb5e317efa3","resolution":{"observed_at":"2026-08-08T00:44:05.814743Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0301201","last_updated":"2003-01-23T14:18:21Z","snapshot_observed_at":"2026-07-07T03:58:55.468815Z","submitted_at":"2003-01-23T14:18:21Z","title":"Renormalizability of Phi-derivable approximations in scalar phi^4 theory","version":1},"cited_work":{"arxiv_id":"hep-ph/0301201","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0301201","snapshot_observed_at":"2026-08-08T00:44:05.514757Z","title":"Renormalizability of Phi-derivable approximations in scalar phi^4 theory","venue":"hep-ph","work_id":"d016667b-292f-4e98-83e8-c1bbd4fce07f","year":2003},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.865177Z"},"links":{"cited_paper":"/paper/hep-ph/0301201","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:ebf8e800d08fecfb218ab4f1737f270a2ab34fcb96cb897cf2633c32dd8c9b93","observation_id":"8a2a86c5-f8f1-4950-90c7-01ce403bbd90","resolution":{"observed_at":"2026-08-08T00:44:05.584751Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0312085","last_updated":"2003-12-05T18:38:47Z","snapshot_observed_at":"2026-07-07T04:02:11.350156Z","submitted_at":"2003-12-05T18:38:47Z","title":"Renormalization of \\Phi-derivable approximations in scalar field theories","version":1},"cited_work":{"arxiv_id":"hep-ph/0312085","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0312085","snapshot_observed_at":"2026-08-08T00:44:05.264749Z","title":"Renormalization of \\Phi-derivable approximations in scalar field theories","venue":"hep-ph","work_id":"db9dd8c8-3d2b-4988-b026-7198aff0c79b","year":2003},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.868994Z"},"links":{"cited_paper":"/paper/hep-ph/0312085","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:7571fb8eb33e89adec2ca14744119b9cace3530e5d91b7f1cc5a3916d74d0d63","observation_id":"0c6a7715-6749-47e7-9b5d-db262987cee9","resolution":{"observed_at":"2026-08-08T00:44:05.314733Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1404.0710","last_updated":"2014-04-02T21:20:59Z","snapshot_observed_at":"2026-07-06T03:40:12.415849Z","submitted_at":"2014-04-02T21:20:59Z","title":"Renormalization group methods and the 2PI effective action","version":1},"cited_work":{"arxiv_id":"1404.0710","doi":null,"metadata_source":"pith","pith_arxiv_id":"1404.0710","snapshot_observed_at":"2026-08-08T00:44:05.065048Z","title":"Renormalization group methods and the 2PI effective action","venue":"hep-ph","work_id":"cef8aa01-c102-4d23-baa7-8cd8113a589f","year":2014},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.872428Z"},"links":{"cited_paper":"/paper/1404.0710","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:2ad721492f4d1f8bd8bc704bf0d006635920234a14223170b2ed69f976fb6f48","observation_id":"e83fdf97-4849-43e1-8597-5bd098846a29","resolution":{"observed_at":"2026-08-08T00:44:05.084753Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1711.09135","last_updated":"2017-11-24T20:51:49Z","snapshot_observed_at":"2026-07-06T06:11:05.659423Z","submitted_at":"2017-11-24T20:51:49Z","title":"The 2PI effective theory at next-to-leading order using the functional renormalization group","version":1},"cited_work":{"arxiv_id":"1711.09135","doi":null,"metadata_source":"pith","pith_arxiv_id":"1711.09135","snapshot_observed_at":"2026-08-08T00:44:04.844752Z","title":"The 2PI effective theory at next-to-leading order using the functional renormalization group","venue":"hep-th","work_id":"79b488b1-bc71-46e2-ad54-e18d1b914756","year":2017},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.876128Z"},"links":{"cited_paper":"/paper/1711.09135","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:3cc6a28a35ed69661f718c81d1cc175eb50e14b0e2dc649ccd59a142586537d0","observation_id":"b117872e-dd7a-4f37-b7a4-eef527afbc25","resolution":{"observed_at":"2026-08-08T00:44:04.884748Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0806.2554","last_updated":"2008-09-22T14:50:33Z","snapshot_observed_at":"2026-07-06T01:40:50.879555Z","submitted_at":"2008-06-16T12:02:41Z","title":"Counterterm resummation for 2PI-approximation in constant background","version":3},"cited_work":{"arxiv_id":"0806.2554","doi":null,"metadata_source":"pith","pith_arxiv_id":"0806.2554","snapshot_observed_at":"2026-08-08T00:44:04.644751Z","title":"Counterterm resummation for 2PI-approximation in constant background","venue":"hep-ph","work_id":"fcdf225d-3c18-4a49-a0c8-59ffca4a0812","year":2008},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.879852Z"},"links":{"cited_paper":"/paper/0806.2554","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:a730ceb66da4cfb043415dd47181d0bc49171c6151b653a5007cacd028e31f1f","observation_id":"31dbcb62-55e5-4b78-be5c-7c809db1c17f","resolution":{"observed_at":"2026-08-08T00:44:04.686739Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0809.3551","last_updated":"2008-09-22T14:50:30Z","snapshot_observed_at":"2026-07-06T01:45:36.231048Z","submitted_at":"2008-09-22T14:50:30Z","title":"Non-perturbative construction of counterterms for 2PI-approximation","version":1},"cited_work":{"arxiv_id":"0809.3551","doi":null,"metadata_source":"pith","pith_arxiv_id":"0809.3551","snapshot_observed_at":"2026-08-08T00:44:04.454754Z","title":"Non-perturbative construction of counterterms for 2PI-approximation","venue":"hep-ph","work_id":"b71f29eb-ae76-4854-b798-5d6a2cd4eb95","year":2008},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.883471Z"},"links":{"cited_paper":"/paper/0809.3551","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:9280345ca57d93f1f2ae4ce47b30ceb9ed1e4a04dd6b2345af6d0d2b8bf759db","observation_id":"07574a5b-9208-48da-b41c-db2ea9ef0ef4","resolution":{"observed_at":"2026-08-08T00:44:04.514754Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1305.3221","last_updated":"2013-06-19T10:57:03Z","snapshot_observed_at":"2026-07-06T03:13:21.304490Z","submitted_at":"2013-05-14T17:46:31Z","title":"Symmetry Improved CJT Effective Action","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1305.3221","snapshot_observed_at":"2026-08-08T00:43:56.888861Z","title":"Pilaftsis and D","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.888861Z"},"links":{"cited_paper":"/paper/1305.3221","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:d0d6bcf8d37e626c01b1cc9b0393b2b090ee838150ea3f1bb9afd16e0de395cb","observation_id":"12c7b3cb-7370-4f64-b187-c4aa3b15a8d4","resolution":{"observed_at":"2026-08-08T00:43:56.888861Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.07986","last_updated":"2015-02-27T17:55:47Z","snapshot_observed_at":"2026-07-06T04:10:30.439601Z","submitted_at":"2015-02-27T17:55:47Z","title":"Symmetry Improved 2PI Effective Action and the Infrared Divergences of the Standard Model","version":1},"cited_work":{"arxiv_id":"1502.07986","doi":null,"metadata_source":"pith","pith_arxiv_id":"1502.07986","snapshot_observed_at":"2026-08-08T00:44:03.983307Z","title":"Symmetry Improved 2PI Effective Action and the Infrared Divergences of the Standard Model","venue":"hep-ph","work_id":"77eb77e0-433c-48d2-8c29-daf4c78ae7fd","year":2015},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.892093Z"},"links":{"cited_paper":"/paper/1502.07986","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:d4abf72f2b578e78642d044209400c697c3e9406122cdda852581cb5a01b8155","observation_id":"6bb48ea0-d173-40a1-8b1e-c6b3e9330ab9","resolution":{"observed_at":"2026-08-08T00:44:04.054754Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1611.05226","last_updated":"2016-12-20T11:48:04Z","snapshot_observed_at":"2026-07-06T05:18:53.043219Z","submitted_at":"2016-11-16T11:21:56Z","title":"Soft symmetry improvement of two particle irreducible effective actions","version":2},"cited_work":{"arxiv_id":"1611.05226","doi":null,"metadata_source":"pith","pith_arxiv_id":"1611.05226","snapshot_observed_at":"2026-08-08T00:44:03.749759Z","title":"Soft symmetry improvement of two particle irreducible effective actions","venue":"hep-th","work_id":"5addca74-338a-43fc-95f4-86ace4decd3b","year":2016},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.895476Z"},"links":{"cited_paper":"/paper/1611.05226","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:3e2a693315976088c05c4cf4edf00f662e0d204c8c73b23d2268601922e5182c","observation_id":"dd705ae4-576e-4780-92bf-6d9d29f3eb4c","resolution":{"observed_at":"2026-08-08T00:44:03.794754Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1703.02079","last_updated":"2017-04-27T13:53:13Z","snapshot_observed_at":"2026-08-01T22:58:32.740484Z","submitted_at":"2017-03-06T19:36:37Z","title":"Exact RG Invariance and Symmetry Improved 2PI Effective Potential","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.02079","snapshot_observed_at":"2026-08-08T00:43:56.898704Z","title":"Pilaftsis and D","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.898704Z"},"links":{"cited_paper":"/paper/1703.02079","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:421ca5a0ce18a487da1fa2f7f6a9f6f185f8b13eda8d3b66175e568f136146d1","observation_id":"581b4e49-3765-4100-b46d-d922cec3e8d0","resolution":{"observed_at":"2026-08-08T00:43:56.898704Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0005003","last_updated":"2000-08-25T15:00:53Z","snapshot_observed_at":"2026-07-07T03:48:22.006719Z","submitted_at":"2000-04-29T21:50:37Z","title":"Approximately self-consistent resummations for the thermodynamics of the quark-gluon plasma. I. Entropy and density","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0005003","snapshot_observed_at":"2026-08-08T00:43:56.903347Z","title":"Blaizot, E","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.903347Z"},"links":{"cited_paper":"/paper/hep-ph/0005003","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:2720fae04bfa2270a01660d74a701a8cbacb7f5ba1c2b3bcfb1f5ba55bc5ad4d","observation_id":"bdb78271-76f1-4252-8938-126d48c899e1","resolution":{"observed_at":"2026-08-08T00:43:56.903347Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0406163","last_updated":"2004-08-16T13:53:12Z","snapshot_observed_at":"2026-07-07T04:03:58.130205Z","submitted_at":"2004-06-15T14:13:35Z","title":"Three-loop Phi-derivable Approximation in QED","version":2},"cited_work":{"arxiv_id":"hep-ph/0406163","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0406163","snapshot_observed_at":"2026-08-08T00:44:03.143894Z","title":"Three-loop Phi-derivable Approximation in QED","venue":"hep-ph","work_id":"5ea721d5-d307-4120-bef9-5aa3f8c68d30","year":2004},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.934741Z"},"links":{"cited_paper":"/paper/hep-ph/0406163","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:aa0126e9d9fae8523e855b551677be0dbc8e3830d09f2d35876c8c29000936d4","observation_id":"097ecc3c-a0d9-468b-93e0-6ab8fa91b6aa","resolution":{"observed_at":"2026-08-08T00:44:03.180156Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0409123","last_updated":"2005-05-10T06:50:04Z","snapshot_observed_at":"2026-07-07T04:04:53.002745Z","submitted_at":"2004-09-10T16:35:33Z","title":"Renormalized thermodynamics from the 2PI effective action","version":2},"cited_work":{"arxiv_id":"hep-ph/0409123","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/0409123","snapshot_observed_at":"2026-08-08T00:44:02.944888Z","title":"Renormalized thermodynamics from the 2PI effective action","venue":"hep-ph","work_id":"dd4452c5-8bed-4452-834c-fba01b6fc42c","year":2004},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.954745Z"},"links":{"cited_paper":"/paper/hep-ph/0409123","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:65287a49688fcc3a2fe2d225912be424da030c5ffe0bf25783724db2f84ef89b","observation_id":"e3dd3e42-b065-411f-9ad9-608b3c22ae76","resolution":{"observed_at":"2026-08-08T00:44:02.975483Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.963474Z","title":"Braaten and R.D","venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.963474Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:581e738f83b5b00f9ca34d18fd097d3077f1eee588a3c147ebc5aa433a06e550","observation_id":"8c5fed38-6e27-40dc-b192-74d27bce84ca","resolution":{"observed_at":"2026-08-08T00:43:56.963474Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9910309","last_updated":"1999-11-03T19:48:52Z","snapshot_observed_at":"2026-07-07T04:34:43.157892Z","submitted_at":"1999-10-12T13:49:05Z","title":"Self-consistent hard-thermal-loop thermodynamics for the quark-gluon plasma","version":2},"cited_work":{"arxiv_id":"hep-ph/9910309","doi":null,"metadata_source":"pith","pith_arxiv_id":"hep-ph/9910309","snapshot_observed_at":"2026-08-08T00:44:02.731110Z","title":"Self-consistent hard-thermal-loop thermodynamics for the quark-gluon plasma","venue":"hep-ph","work_id":"c79f92e6-d287-4b07-ac03-d40ac058a29d","year":1999},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.966464Z"},"links":{"cited_paper":"/paper/hep-ph/9910309","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:68eddee783f4b258e8471a0dea2f73116e89381d1daff1b24de34ddc96344717","observation_id":"0d398a5a-b06f-463c-8c23-3b5672577e54","resolution":{"observed_at":"2026-08-08T00:44:02.774748Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1603.02085","last_updated":"2016-03-07T14:31:16Z","snapshot_observed_at":"2026-07-06T04:48:33.584517Z","submitted_at":"2016-03-07T14:31:16Z","title":"The 2PI effective action at four loop order in $\\varphi^4$ theory","version":1},"cited_work":{"arxiv_id":"1603.02085","doi":null,"metadata_source":"pith","pith_arxiv_id":"1603.02085","snapshot_observed_at":"2026-08-08T00:44:02.474755Z","title":"The 2PI effective action at four loop order in $\\varphi^4$ theory","venue":"hep-th","work_id":"9c28b675-4ed5-42c5-9f98-21003bad5d09","year":2016},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.970593Z"},"links":{"cited_paper":"/paper/1603.02085","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:3aeddf75026a2c5d1532f93d35683eb86e1d667f504360b5577aff3f2ff45ed0","observation_id":"26edee20-ed56-4a7e-bb58-73f91af78702","resolution":{"observed_at":"2026-08-08T00:44:02.524748Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2307.14983","last_updated":"2023-07-27T16:24:14Z","snapshot_observed_at":"2026-07-06T15:59:23.019044Z","submitted_at":"2023-07-27T16:24:14Z","title":"Renormalized equations of motions for scalars and fermions in the 2PI formalism","version":1},"cited_work":{"arxiv_id":"2307.14983","doi":null,"metadata_source":"pith","pith_arxiv_id":"2307.14983","snapshot_observed_at":"2026-08-08T00:44:02.244755Z","title":"Renormalized equations of motions for scalars and fermions in the 2PI formalism","venue":"hep-ph","work_id":"7e6d38e4-3fe0-41e8-9afc-04c379d51bc9","year":2023},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.974090Z"},"links":{"cited_paper":"/paper/2307.14983","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:9fdd61bf26eca02a4a1f4a94d16e40c7f3c1d8e91f29af7c0763582151803c24","observation_id":"5fcc0fd7-cd55-4802-ab58-335784c3b396","resolution":{"observed_at":"2026-08-08T00:44:02.304750Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.978993Z","title":"Keldysh,Diagram technique for nonequilibrium processes,Zh","venue":null,"work_id":null,"year":1964},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.978993Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:db3b2ac85b5323498d753817ec5fe13d8a8e6dd0d8daedc9a74e2ae5850fa13d","observation_id":"ddb4251c-d141-48e2-96f2-d0181e626b8a","resolution":{"observed_at":"2026-08-08T00:43:56.978993Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.981520Z","title":"Bogoliubow and O.S","venue":null,"work_id":null,"year":1957},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.981520Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:67e168e7c697eacf2723200be84cdf536332f7f49d19ac3c01edcd6cfdc7fad3","observation_id":"bc3532e4-1dcd-4012-a41e-15b5c30b4081","resolution":{"observed_at":"2026-08-08T00:43:56.981520Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.984269Z","title":"Bogoliubov and O.S","venue":null,"work_id":null,"year":1957},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.984269Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:64b35bce781f25937a184065f8d6a1e5e76dece4c68a5adba12fb6d490cfd94d","observation_id":"157e7d3a-2816-41db-affe-1d1c21fe5ce8","resolution":{"observed_at":"2026-08-08T00:43:56.984269Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.987432Z","title":"Hepp,Proof of the Bogolyubov-Parasiuk theorem on renormalization,Commun","venue":null,"work_id":null,"year":1966},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.987432Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:777675c0b0740ff1d3dc31cd4825ba2ac6e63b4717cb5f1affff580ffbcdf666","observation_id":"928d4198-79f1-4972-86d7-566f4e66a981","resolution":{"observed_at":"2026-08-08T00:43:56.987432Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:56.990318Z","title":"Zimmermann,Convergence of Bogolyubov’s method of renormalization in momentum space,Commun","venue":null,"work_id":null,"year":1969},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.990318Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:7dd29dd8e5b560cdad1307866988cdfe2725e79233c35da255d6a51ee3ca1dec","observation_id":"841592a9-1dc7-487b-8b62-c0c620bde587","resolution":{"observed_at":"2026-08-08T00:43:56.990318Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0711.2933","last_updated":"2008-02-03T22:02:29Z","snapshot_observed_at":"2026-07-06T01:32:51.072335Z","submitted_at":"2007-11-19T13:57:38Z","title":"Renormalisability of the 2PI-Hartree approximation of multicomponent scalar models in the broken symmetry phase","version":2},"cited_work":{"arxiv_id":"0711.2933","doi":null,"metadata_source":"pith","pith_arxiv_id":"0711.2933","snapshot_observed_at":"2026-08-08T00:44:02.020976Z","title":"Renormalisability of the 2PI-Hartree approximation of multicomponent scalar models in the broken symmetry phase","venue":"hep-ph","work_id":"ee9340b5-d0e2-4789-8b15-b30d9935255c","year":2007},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.993259Z"},"links":{"cited_paper":"/paper/0711.2933","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:6c69109ffc1fdfc968ccfbfed4d8fb2aa9db677a91a1e96c5a611eaa7ff41dc3","observation_id":"9610db8f-225c-4d7d-88ce-4fb1987e635f","resolution":{"observed_at":"2026-08-08T00:44:02.062369Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1409.0005","last_updated":"2015-05-04T21:37:03Z","snapshot_observed_at":"2026-08-01T18:35:16.364837Z","submitted_at":"2014-08-29T20:00:05Z","title":"Testing Electroweak Baryogenesis with Future Colliders","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.0005","snapshot_observed_at":"2026-08-08T00:43:56.997433Z","title":"Curtin, P","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:56.997433Z"},"links":{"cited_paper":"/paper/1409.0005","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:cf9fb3c16613ad5fd9ec54852c2a38fcc96d250c4cb7dceaf0ae3cb704bce808","observation_id":"a8aaecc5-0bfc-4217-9452-99d0299aff05","resolution":{"observed_at":"2026-08-08T00:43:56.997433Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1911.10206","last_updated":"2020-10-15T04:14:48Z","snapshot_observed_at":"2026-07-06T08:39:23.776757Z","submitted_at":"2019-11-22T19:00:01Z","title":"Electroweak $\\!$phase $\\!$transition $\\!$with $\\!$spontaneous $\\!$$Z_2$-breaking","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1911.10206","snapshot_observed_at":"2026-08-08T00:43:57.000557Z","title":"Carena, Z","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.000557Z"},"links":{"cited_paper":"/paper/1911.10206","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:ed0f501d5c308cd89921544378fdc1676de62138dcf4c3853fe7ef48ee08003f","observation_id":"354aa485-515f-476b-857f-ae653b588e28","resolution":{"observed_at":"2026-08-08T00:43:57.000557Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.02393","last_updated":"2021-11-03T17:58:29Z","snapshot_observed_at":"2026-07-06T12:05:07.980255Z","submitted_at":"2021-11-03T17:58:29Z","title":"Electroweak bubble wall expansion: gravitational waves and baryogenesis in Standard Model-like thermal plasma","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.02393","snapshot_observed_at":"2026-08-08T00:43:57.010350Z","title":"Lewicki, M","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.010350Z"},"links":{"cited_paper":"/paper/2111.02393","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:d16b709a78d785c44844eebee294270ada75794dcf48ff01eeebf9ad58942da9","observation_id":"e5638b49-0439-4df5-8bf6-bf7765109e9f","resolution":{"observed_at":"2026-08-08T00:43:57.010350Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.16305","last_updated":"2022-10-28T17:59:09Z","snapshot_observed_at":"2026-07-06T14:11:51.163337Z","submitted_at":"2022-10-28T17:59:09Z","title":"The Scalar Singlet Extension of the Standard Model: Gravitational Waves versus Baryogenesis","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.16305","snapshot_observed_at":"2026-08-08T00:43:57.016257Z","title":"Ellis, M","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.016257Z"},"links":{"cited_paper":"/paper/2210.16305","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:d1dd91ee86e0cd76bb6efac299e1fe2008322960a4b79030f320cd5b078e2b53","observation_id":"aec81ca6-8a25-4872-a340-004d63272e76","resolution":{"observed_at":"2026-08-08T00:43:57.016257Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-lat/0103036","last_updated":"2001-03-29T09:26:15Z","snapshot_observed_at":"2026-07-07T03:40:36.170779Z","submitted_at":"2001-03-29T09:26:15Z","title":"Non-perturbative computation of the bubble nucleation rate in the cubic anisotropy model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-lat/0103036","snapshot_observed_at":"2026-08-08T00:43:57.019720Z","title":"Moore, K","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.019720Z"},"links":{"cited_paper":"/paper/hep-lat/0103036","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:c24c40a9a7ec6c68af5f5ec306e941e5c0c97ee2d312db1f2b2182129acecfa8","observation_id":"f4b790db-fe46-44ed-b4a7-3e9425783ebd","resolution":{"observed_at":"2026-08-08T00:43:57.019720Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.07238","last_updated":"2024-10-16T14:31:38Z","snapshot_observed_at":"2026-08-08T10:12:45.463722Z","submitted_at":"2022-05-15T09:47:17Z","title":"First-order electroweak phase transitions: a nonperturbative update","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.07238","snapshot_observed_at":"2026-08-08T00:43:57.023037Z","title":"Gould, S","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.023037Z"},"links":{"cited_paper":"/paper/2205.07238","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:1d40c21d76d11098f8b14058dd12c57e348ca733cd2a57bf8747b4b84bd77eb6","observation_id":"5a8e7547-1276-44a4-bf40-2a7449c9dfac","resolution":{"observed_at":"2026-08-08T00:43:57.023037Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:57.026946Z","title":"Gould, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.026946Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:1d21fe028be5b0d748f44f425a03f12909168f54ac0016e475c90fc0b2426e47","observation_id":"bdcd357c-1cfb-4d81-b79a-56871868b3da","resolution":{"observed_at":"2026-08-08T00:43:57.026946Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.04185","last_updated":"2025-02-06T16:16:37Z","snapshot_observed_at":"2026-08-04T17:20:01.140313Z","submitted_at":"2025-02-06T16:16:37Z","title":"Testing nucleation calculations for strong phase transitions","version":1},"cited_work":{"arxiv_id":"2502.04185","doi":null,"metadata_source":"pith","pith_arxiv_id":"2502.04185","snapshot_observed_at":"2026-08-08T00:44:00.969956Z","title":"Testing nucleation calculations for strong phase transitions","venue":"hep-lat","work_id":"3fbc3c7c-4813-4008-be12-2db644ed5c49","year":2025},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.032847Z"},"links":{"cited_paper":"/paper/2502.04185","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:ee29e0e9afa06cb2f005f763ad0f8e6619768a3c839251374d256f491122dad6","observation_id":"075ec16d-6e1e-4c53-b6c8-7ed05c8e6742","resolution":{"observed_at":"2026-08-08T00:44:00.985904Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2505.22732","last_updated":"2025-05-28T18:00:06Z","snapshot_observed_at":"2026-08-07T12:59:38.137353Z","submitted_at":"2025-05-28T18:00:06Z","title":"Langer's nucleation rate reproduced on the lattice","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.22732","snapshot_observed_at":"2026-08-08T00:43:57.036364Z","title":"Hirvonen and O","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.036364Z"},"links":{"cited_paper":"/paper/2505.22732","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:179a7130aadf8ff1326f1c46da212ff9ff724c2d3d18cfd66c856f7ddb5d8820","observation_id":"23493ed7-de50-41d5-8350-1d137deb6d13","resolution":{"observed_at":"2026-08-08T00:43:57.036364Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:57.040045Z","title":"Langer,Statistical theory of the decay of metastable states,Annals Phys.54(1969) 258","venue":null,"work_id":null,"year":1969},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.040045Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:b8e0e762a40c94afdddf5af526f4449ed50effb77e4c81436b64a3945e8a11d1","observation_id":"38e89b4a-9919-4889-8f43-539b53c3c4f8","resolution":{"observed_at":"2026-08-08T00:43:57.040045Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0009132","last_updated":"2000-11-16T22:39:35Z","snapshot_observed_at":"2026-07-07T03:49:47.697309Z","submitted_at":"2000-09-11T19:26:25Z","title":"Electroweak Bubble Nucleation, Nonperturbatively","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0009132","snapshot_observed_at":"2026-08-08T00:43:57.043420Z","title":"Moore and K","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.043420Z"},"links":{"cited_paper":"/paper/hep-ph/0009132","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:9b5eaa6aec153d585f8fafbde40fa918b29d8fb95997c41b58a8436192bf178f","observation_id":"6246872b-4b78-496b-8ed5-255ec1f5974f","resolution":{"observed_at":"2026-08-08T00:43:57.043420Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"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":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.10080","snapshot_observed_at":"2026-08-08T00:43:57.046770Z","title":"Croon, O","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.046770Z"},"links":{"cited_paper":"/paper/2009.10080","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:736d30cdd250cf7fb5a9c2053175b19270ea6896b1b9319458bacd2c4e24cf53","observation_id":"aeb69924-3bc0-4e74-b42e-45af64f10b92","resolution":{"observed_at":"2026-08-08T00:43:57.046770Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.15652","last_updated":"2024-01-09T14:28:48Z","snapshot_observed_at":"2026-07-06T16:12:02.944409Z","submitted_at":"2023-08-29T22:06:23Z","title":"BubbleDet: A Python package to compute functional determinants for bubble nucleation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.15652","snapshot_observed_at":"2026-08-08T00:43:57.050229Z","title":"Ekstedt, O","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.050229Z"},"links":{"cited_paper":"/paper/2308.15652","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:f45ad3d98bb5defe2c39cfc399219c5837c25c2dc01368276bb35d01a92140db","observation_id":"a83afb43-49c6-46b4-8cb6-f41ed959ed69","resolution":{"observed_at":"2026-08-08T00:43:57.050229Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.04377","last_updated":"2021-12-08T14:55:28Z","snapshot_observed_at":"2026-08-01T18:30:56.069380Z","submitted_at":"2021-08-09T22:29:26Z","title":"Effective field theory approach to thermal bubble nucleation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.04377","snapshot_observed_at":"2026-08-08T00:43:57.053253Z","title":"Gould and J","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.053253Z"},"links":{"cited_paper":"/paper/2108.04377","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:6e89878cbd0369f60767cc1bd239701ef6af6f98c46eee5a50d3bdc6fdf573bd","observation_id":"a3c512b0-a870-4cfb-94c1-6572cd8c3fc0","resolution":{"observed_at":"2026-08-08T00:43:57.053253Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.04206","last_updated":"2024-01-07T12:32:09Z","snapshot_observed_at":"2026-07-06T16:28:42.964476Z","submitted_at":"2023-10-06T12:44:48Z","title":"Real-time dynamics of false vacuum decay","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.04206","snapshot_observed_at":"2026-08-08T00:43:57.057244Z","title":"Batini, A","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.057244Z"},"links":{"cited_paper":"/paper/2310.04206","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:082a262d697aa59b346c1a12f5c4b1097a3849a223a58a1f910902ffcdd1cc72","observation_id":"64226d11-a5b5-4639-a376-e5e3da1b6c96","resolution":{"observed_at":"2026-08-08T00:43:57.057244Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.18421","last_updated":"2025-05-12T08:23:14Z","snapshot_observed_at":"2026-07-06T19:58:00.412286Z","submitted_at":"2024-11-27T15:03:30Z","title":"False vacuum decay beyond the quadratic approximation: summation of non-local self-energies","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.18421","snapshot_observed_at":"2026-08-08T00:43:57.077298Z","title":"Carosi and B","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.077298Z"},"links":{"cited_paper":"/paper/2411.18421","citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:9a0406bb7dff0eb7ff8b8e4e85ef0b3d3edcc6f4cfc1fb95d32874d8f927aea9","observation_id":"907bdf6d-3c56-4be5-8292-1934e4f960fc","resolution":{"observed_at":"2026-08-08T00:43:57.077298Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:57.082998Z","title":"Coleman,The Fate of the False Vacuum","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.082998Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:ff76b213ba193761db427267648b0edd5c29096de0fd14e7cce2aca8f24b0eb4","observation_id":"012bad48-3c55-45b5-a6dd-bffe2deb9c83","resolution":{"observed_at":"2026-08-08T00:43:57.082998Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:57.086246Z","title":"Callan, Jr","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.086246Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:e893ca61d767fa7196bef440fa172ac5a10867a90f55fce56e6e9b7f6854a121","observation_id":"74219c51-1431-42c5-9610-600c53159726","resolution":{"observed_at":"2026-08-08T00:43:57.086246Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:57.088979Z","title":"Linde,Fate of the False Vacuum at Finite Temperature: Theory and Applications, Phys","venue":null,"work_id":null,"year":1981},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":101,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.088979Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:9d2cca36b6bf1354b2beaa922c06ff07276f08c89aab9eafba34ad7d3fc591bd","observation_id":"b6c9844a-3edc-440f-8bf5-ad27e8c078e6","resolution":{"observed_at":"2026-08-08T00:43:57.088979Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T00:43:57.092370Z","title":"Linde,Decay of the False Vacuum at Finite Temperature,Nucl","venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods","version":1},"reference_index":102,"source":"pdf_text","source_observed_at":"2026-08-08T00:43:57.092370Z"},"links":{"citing_paper":"/paper/2608.04102"},"observation_digest":"sha256:2c119c2670babb067c07abdb8aa68bfd891ca5ef05a645efe7d8a1d692e51cd5","observation_id":"1118bb63-6796-43b5-b3b4-49bc460a1ab0","resolution":{"observed_at":"2026-08-08T00:43:57.092370Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2608.04102","last_updated":"2026-08-04T18:00:55Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-08T16:10:59.422605Z","submitted_at":"2026-08-04T18:00:55Z","title":"Consistent Thermal Resummation and Phase Transitions with 2PI Methods"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":1,"parse_uncertain":0,"unresolved":80,"verified_exact":19,"verified_fuzzy":0},"total_outbound_references":134},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"thesis":"As of 8 August 2026, this Paper Citation Record lists 100 of 134 outbound references and 0 inbound Pith citation observations for arXiv:2608.04102."}