{"as_of":"2026-08-15T02:20:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:dc1d28cd3fbd7a022c5256a2137036f05594895b1b5011c82a113ff10f2ffaf6","coverage":[{"denominator":37,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":37,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-14T11:07:32.209428Z","state":"measured"},{"denominator":37,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":37,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-14T06:32:32.682623+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/1908.09796/citation-record","integrity":"/paper/1908.09796/integrity","json":"/paper/1908.09796/citation-record.json","paper":"/paper/1908.09796"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:07:32.951027Z","title":"Pines and D","venue":null,"work_id":"5eb54586-74bf-4c7f-b5aa-57699c401117","year":1952},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.029992Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:474d836a815633caf560c32041e1afee7c5ee3627c5914d55a83fdc59f5561e1","observation_id":"00fa58e2-aae5-4114-ac31-dece7eb2dc77","resolution":{"observed_at":"2026-08-14T11:07:32.956465Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:07:32.933966Z","title":"Bohm and D","venue":null,"work_id":"05ffd87d-770e-4a37-96fd-eaef1e151d03","year":1953},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.036363Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:124f526356a245ecbe02ec30fda15a81be814427fda02f25b36ae3b992df7976","observation_id":"ae0898d8-b36e-49da-a92b-15778d6f9434","resolution":{"observed_at":"2026-08-14T11:07:32.939200Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9302213","last_updated":"1993-02-03T21:56:52Z","snapshot_observed_at":"2026-07-07T04:15:01.181188Z","submitted_at":"1993-02-03T21:56:52Z","title":"Neutrino Energy Loss from the Plasma Process at all Temperatures and Densities","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9302213","snapshot_observed_at":"2026-08-14T11:07:32.042611Z","title":"Braaten and D","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.042611Z"},"links":{"cited_paper":"/paper/hep-ph/9302213","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:345835a0e686223fd00e46f59509949c8fc565abfa8dfba4c1bae3cf65462753","observation_id":"0f32a3a2-d206-485f-ba85-eedb2aa8ffec","resolution":{"observed_at":"2026-08-14T11:07:32.042611Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.08623","last_updated":"2019-02-22T19:00:00Z","snapshot_observed_at":"2026-08-14T17:12:33.931391Z","submitted_at":"2019-02-22T19:00:00Z","title":"Making dark matter out of light: freeze-in from plasma effects","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.08623","snapshot_observed_at":"2026-08-14T11:07:32.047975Z","title":"Dvorkin, T","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.047975Z"},"links":{"cited_paper":"/paper/1902.08623","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:56a068a8d299151c217e526dcb4ac2f53b125509649a49f8567ad6600f8fedcc","observation_id":"a80823f2-4b8c-47bc-9c2c-84b9ea991ebe","resolution":{"observed_at":"2026-08-14T11:07:32.047975Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.08230","last_updated":"2018-05-23T02:48:52Z","snapshot_observed_at":"2026-08-14T19:33:41.706345Z","submitted_at":"2018-03-22T05:23:14Z","title":"The radio telescope search for the resonant conversion of cold dark matter axions from the magnetized astrophysical sources","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.08230","snapshot_observed_at":"2026-08-14T11:07:32.053265Z","title":null,"venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.053265Z"},"links":{"cited_paper":"/paper/1803.08230","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:97c929ab3028e3d9b8dcbf1abcfb59f1ce535760544f48cfcad964e0c4a0bb9e","observation_id":"0fb25b39-86cf-42b3-888e-e208d451505a","resolution":{"observed_at":"2026-08-14T11:07:32.053265Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:07:32.916871Z","title":null,"venue":null,"work_id":"ffcd1839-400e-43fe-8fdb-0a5b57769d91","year":2011},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.059034Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:d36795d097abb67bf1327ea33aa363b7d9c769c9fd88bf58fa67ba41ce71b605","observation_id":"998213a6-3655-46ea-817b-b5837c819859","resolution":{"observed_at":"2026-08-14T11:07:32.922496Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1605.07720","last_updated":"2016-07-20T06:36:40Z","snapshot_observed_at":"2026-08-14T21:55:51.839661Z","submitted_at":"2016-05-25T03:51:48Z","title":"Neutrino dynamics below the electroweak crossover","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1605.07720","snapshot_observed_at":"2026-08-14T11:07:32.064465Z","title":"Ghiglieri and M","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.064465Z"},"links":{"cited_paper":"/paper/1605.07720","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:6ca52bc1e10529a47c2f8cf70a70f39285504b921930e1c1fbabdddd84a4241f","observation_id":"4c7d4246-233c-4084-b282-284838cd2c78","resolution":{"observed_at":"2026-08-14T11:07:32.064465Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.06087","last_updated":"2017-05-29T06:31:20Z","snapshot_observed_at":"2026-08-14T21:11:18.538476Z","submitted_at":"2017-03-17T16:30:28Z","title":"GeV-scale hot sterile neutrino oscillations: a derivation of evolution equations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.06087","snapshot_observed_at":"2026-08-14T11:07:32.069564Z","title":"Ghiglieri and M","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.069564Z"},"links":{"cited_paper":"/paper/1703.06087","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:64d1305e091b5b1671615c09c061cc48b10ccfa7fcb1f9c735f96b45f4b750de","observation_id":"0424b790-7e0a-4db2-825c-b6e5ebe9a6f6","resolution":{"observed_at":"2026-08-14T11:07:32.069564Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1811.01971","last_updated":"2019-02-08T08:26:24Z","snapshot_observed_at":"2026-08-14T18:03:54.924130Z","submitted_at":"2018-11-05T19:00:06Z","title":"Precision study of GeV-scale resonant leptogenesis","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1811.01971","snapshot_observed_at":"2026-08-14T11:07:32.074541Z","title":"Ghiglieri and M","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.074541Z"},"links":{"cited_paper":"/paper/1811.01971","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:0cd5171ce1cc77a9a58e7af4d5a579711803ad6c7cb770ef43bb8a29e4f7f95f","observation_id":"4bf18508-5522-4ef0-9f49-bbd2b7e18800","resolution":{"observed_at":"2026-08-14T11:07:32.074541Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.12880","last_updated":"2019-10-28T18:00:04Z","snapshot_observed_at":"2026-07-06T08:32:52.015278Z","submitted_at":"2019-10-28T18:00:04Z","title":"A thermal neutrino interaction rate at NLO","version":1},"cited_work":{"arxiv_id":"1910.12880","doi":null,"metadata_source":"pith","pith_arxiv_id":"1910.12880","snapshot_observed_at":"2026-08-14T11:07:32.708412Z","title":"A thermal neutrino interaction rate at NLO","venue":"hep-ph","work_id":"b51004bc-d649-453a-9f85-0d3356b6e6e2","year":2019},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.079564Z"},"links":{"cited_paper":"/paper/1910.12880","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:6c2b62a984af765f8c0189455c357eb3f3f90c49c5b576e6c1991598bbb99e29","observation_id":"c1c62d91-8bff-43cc-a334-f57acd85e493","resolution":{"observed_at":"2026-08-14T11:07:32.713759Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:07:32.899739Z","title":"Kunszt and D","venue":null,"work_id":"5b26484a-b0bb-4ea0-b64b-65793ca32cac","year":1988},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.084778Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:cf0e52eb13885c0cb64c5018354dc2b737d95155234e95b6eba314f7b1b18ed1","observation_id":"4fcc31af-9b26-4517-83bc-31653c287352","resolution":{"observed_at":"2026-08-14T11:07:32.905739Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1902.06738","last_updated":"2019-03-27T07:53:53Z","snapshot_observed_at":"2026-08-14T17:15:48.534750Z","submitted_at":"2019-02-15T16:25:46Z","title":"On the Feynman Rules of Massive Gauge Theory in Physical Gauges","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.06738","snapshot_observed_at":"2026-08-14T11:07:32.089393Z","title":"Chen (2019), 1902.06738","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.089393Z"},"links":{"cited_paper":"/paper/1902.06738","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:515dd5413f4cc3f3fe96dc797c16aa0623bf52f8c68e15f86a4eb3f961cecd96","observation_id":"4a556173-6fdb-459b-b9e1-c1f38a8138a2","resolution":{"observed_at":"2026-08-14T11:07:32.089393Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1611.00788","last_updated":"2018-01-18T14:40:19Z","snapshot_observed_at":"2026-08-14T21:32:14.493583Z","submitted_at":"2016-11-02T20:21:41Z","title":"Electroweak Splitting Functions and High Energy Showering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1611.00788","snapshot_observed_at":"2026-08-14T11:07:32.094141Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.094141Z"},"links":{"cited_paper":"/paper/1611.00788","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:868d13d5d09480d91a51e53aff0272f33e26e16c201bcd627e954ebe74b511ce","observation_id":"d06a7916-1f2e-48fb-a2cd-6c14730348a1","resolution":{"observed_at":"2026-08-14T11:07:32.094141Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:07:32.883897Z","title":null,"venue":null,"work_id":"07f7bfc4-ab04-4082-85ad-dd64a93db316","year":1987},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.099087Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:4ee6a238f43cf798b9c92e7831029f2905d6c06bc72956acdbb5755d6517bad5","observation_id":"02a6e71f-ee8b-4db3-9d23-409009fe92a0","resolution":{"observed_at":"2026-08-14T11:07:32.888687Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"ph/9303251","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:07:32.648153Z","title":"Buchmuller, Z","venue":null,"work_id":"e1ac281c-4f6b-4f20-8628-b21c625e40c2","year":1994},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.103649Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:7f77964598abfe558f278531b6f693f430833ae704f30b460d149f5dd6d7db4a","observation_id":"a74d5ca4-7fff-4736-abad-3fb05c0f748d","resolution":{"observed_at":"2026-08-14T11:07:32.656270Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+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":"2026-08-14T11:07:32.108339Z","title":null,"venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.108339Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:80cb6316b2bee656b319c2b49bf41ee47d75964a007752f6a93bb334fc1e09fd","observation_id":"47618bb4-12a2-40c6-87bb-a671655f45a9","resolution":{"observed_at":"2026-08-14T11:07:32.108339Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:07:32.855878Z","title":null,"venue":null,"work_id":"8d9cc246-99d4-4552-8ec4-3c6e85c0ad06","year":1982},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.112917Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:123cfcb170a42d764b1c99e6fce73ed33bc24c963b091779b85fc4aabcfcb9fc","observation_id":"9c82f586-65d6-4218-9e58-b718103098f5","resolution":{"observed_at":"2026-08-14T11:07:32.861833Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-14T11:07:32.836872Z","title":"Frenkel and J","venue":null,"work_id":"2b080d76-724d-471e-bfd2-f97f6f4011cb","year":1992},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.117544Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:b606c130eca4bef463deb98140f5df5e1391f1d6bc0f1f9abc377bca4ee9f97a","observation_id":"031730b6-d37c-4068-9aef-a02866eafa60","resolution":{"observed_at":"2026-08-14T11:07:32.843883Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+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":"2026-08-14T11:07:32.122293Z","title":"Braaten and R","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.122293Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:a902513183e454c6d1ec7d8add8574d203dca57056fa1c041b271aee0950c56c","observation_id":"700291b2-d7d7-44ed-a656-b782ce0e60b0","resolution":{"observed_at":"2026-08-14T11:07:32.122293Z","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":"2026-08-14T21:22:20.706465Z","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":"2026-08-14T11:07:32.126779Z","title":"Laine and A","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.126779Z"},"links":{"cited_paper":"/paper/1701.01554","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:e5bab6a86223550ec5e00bc143f5fefc341db21bc4eeca1a31f50deb1c335c88","observation_id":"6a9b3ad4-506c-48ca-9249-688d6a7d078a","resolution":{"observed_at":"2026-08-14T11:07:32.126779Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1503.04935","last_updated":"2015-07-23T12:35:10Z","snapshot_observed_at":"2026-08-14T22:56:03.211145Z","submitted_at":"2015-03-17T06:37:44Z","title":"Standard Model thermodynamics across the electroweak crossover","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1503.04935","snapshot_observed_at":"2026-08-14T11:07:32.131781Z","title":"Laine and M","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.131781Z"},"links":{"cited_paper":"/paper/1503.04935","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:f3247c2a86d0c816f3de66481c6ec37e6c18f35e510253c5eb1986cb68d7296a","observation_id":"636d0659-8c76-4002-b9f2-2361e9ff65b5","resolution":{"observed_at":"2026-08-14T11:07:32.131781Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.09304","last_updated":"2017-05-30T06:24:52Z","snapshot_observed_at":"2026-08-14T21:09:45.459674Z","submitted_at":"2017-03-27T20:45:50Z","title":"On the Gauge Invariance of the Decay Rate of False Vacuum","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.09304","snapshot_observed_at":"2026-08-14T11:07:32.136565Z","title":null,"venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.136565Z"},"links":{"cited_paper":"/paper/1703.09304","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:c0c3e52d5546723be8a062c3532bc7d0e6a5025be54dc34f35d7a0e08be5c6e3","observation_id":"22af68d8-414c-4daa-957e-4645bdfec01c","resolution":{"observed_at":"2026-08-14T11:07:32.136565Z","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":"2026-08-14T11:07:32.141363Z","title":"Tanabashi, K","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.141363Z"},"links":{"citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:e48b710db16a291c1e4e5ebb0d6831cda67589867a8779440808b663df104310","observation_id":"89e8f0ed-5890-4a50-8237-ef11581e49dc","resolution":{"observed_at":"2026-08-14T11:07:32.141363Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0404175","last_updated":"2004-08-13T15:46:27Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2004-04-21T13:12:59Z","title":"Particle Dark Matter: Evidence, Candidates and Constraints","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0404175","snapshot_observed_at":"2026-08-14T11:07:32.145977Z","title":"Bertone, D","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.145977Z"},"links":{"cited_paper":"/paper/hep-ph/0404175","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:b3df2b3a72a69257a9b0c93e1634d7dcb7065a09b17de3f4ee3d42c6d10e2e46","observation_id":"b11fbc56-1d7d-4c56-8609-d3d49e19abe5","resolution":{"observed_at":"2026-08-14T11:07:32.145977Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.1120","last_updated":"2009-12-08T18:32:29Z","snapshot_observed_at":"2026-07-06T01:59:52.714720Z","submitted_at":"2009-11-05T20:41:44Z","title":"Freeze-In Production of FIMP Dark Matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0911.1120","snapshot_observed_at":"2026-08-14T11:07:32.150795Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.150795Z"},"links":{"cited_paper":"/paper/0911.1120","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:35a89138a1d16d8c303ecd5420312baa4ae7f5071a4f2b6e515d1ca568e64084","observation_id":"440f602d-703d-4c4e-9788-81cd29fe4878","resolution":{"observed_at":"2026-08-14T11:07:32.150795Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.07647","last_updated":"2017-02-28T14:37:45Z","snapshot_observed_at":"2026-08-14T21:38:20.135175Z","submitted_at":"2016-09-24T17:25:33Z","title":"Production of heavy sterile neutrinos from vector boson decay at electroweak temperatures","version":3},"cited_work":{"arxiv_id":"1609.07647","doi":null,"metadata_source":"pith","pith_arxiv_id":"1609.07647","snapshot_observed_at":"2026-08-14T11:07:32.453496Z","title":"Production of heavy sterile neutrinos from vector boson decay at electroweak temperatures","venue":"hep-ph","work_id":"1ca1acfe-d004-4c75-a182-9dbaa8f04242","year":2016},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.155583Z"},"links":{"cited_paper":"/paper/1609.07647","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:6f61b3db98ff92a9733215fe965655add950f4e564c0343ed3322b1f3752973f","observation_id":"6832dbe0-dd5d-4d7e-9105-7a4141f1261f","resolution":{"observed_at":"2026-08-14T11:07:32.459072Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1606.00017","last_updated":"2016-08-12T13:28:05Z","snapshot_observed_at":"2026-08-14T21:54:49.706917Z","submitted_at":"2016-05-31T20:00:29Z","title":"Higgs doublet decay as the origin of the baryon asymmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1606.00017","snapshot_observed_at":"2026-08-14T11:07:32.160685Z","title":"Hambye and D","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.160685Z"},"links":{"cited_paper":"/paper/1606.00017","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:b75895234020d0d99b444f980286c240951fbbff3bcd57c76d76e42403937cc1","observation_id":"f72bb882-0a74-4645-aec9-2bb4dd40f130","resolution":{"observed_at":"2026-08-14T11:07:32.160685Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.1205","last_updated":"2012-02-28T08:24:37Z","snapshot_observed_at":"2026-07-06T02:38:52.425105Z","submitted_at":"2011-12-06T09:40:31Z","title":"Thermal right-handed neutrino production rate in the non-relativistic regime","version":2},"cited_work":{"arxiv_id":"1112.1205","doi":null,"metadata_source":"pith","pith_arxiv_id":"1112.1205","snapshot_observed_at":"2026-08-14T11:07:32.414146Z","title":"Thermal right-handed neutrino production rate in the non-relativistic regime","venue":"hep-ph","work_id":"a1df8344-89ad-48be-a00f-d42e679afa12","year":2011},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.165516Z"},"links":{"cited_paper":"/paper/1112.1205","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:d9120dcb7a8ba052016089043abd7258a7574d974402f8cd289685a5e4f62b8a","observation_id":"86f8d399-0318-4cab-a360-88bbaaa39068","resolution":{"observed_at":"2026-08-14T11:07:32.419596Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1307.4909","last_updated":"2013-09-04T14:28:46Z","snapshot_observed_at":"2026-08-15T00:09:54.879617Z","submitted_at":"2013-07-18T11:28:30Z","title":"Thermal right-handed neutrino production rate in the relativistic regime","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.4909","snapshot_observed_at":"2026-08-14T11:07:32.170232Z","title":"Laine, JHEP 08, 138 (2013), 1307.4909","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.170232Z"},"links":{"cited_paper":"/paper/1307.4909","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:a1311f64eb8e8e910bc2f94dabc0ab1b0f627e240b9ee9a77234834e258415af","observation_id":"c63e66ba-79fc-4afe-97df-351840b1ff0f","resolution":{"observed_at":"2026-08-14T11:07:32.170232Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1302.0743","last_updated":"2013-02-14T19:15:23Z","snapshot_observed_at":"2026-08-15T00:30:00.318269Z","submitted_at":"2013-02-04T16:14:36Z","title":"Right-Handed Neutrino Production at Finite Temperature: Radiative Corrections, Soft and Collinear Divergences","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1302.0743","snapshot_observed_at":"2026-08-14T11:07:32.175260Z","title":"Garbrecht, F","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.175260Z"},"links":{"cited_paper":"/paper/1302.0743","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:92a5186895ff9b29c5aee117e7d676c870dc6538beec4b3ba031d391157c36aa","observation_id":"6cbf7778-c64b-4b90-ad16-74eb52b76b03","resolution":{"observed_at":"2026-08-14T11:07:32.175260Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.02899","last_updated":"2016-03-08T16:56:21Z","snapshot_observed_at":"2026-08-14T22:19:19.088768Z","submitted_at":"2015-12-09T15:30:27Z","title":"Dark matter annihilation into right-handed neutrinos and the galactic center gamma-ray excess","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.02899","snapshot_observed_at":"2026-08-14T11:07:32.180355Z","title":"Tang and S.-h","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.180355Z"},"links":{"cited_paper":"/paper/1512.02899","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:39550109c62be97d93efbb9111245944da73a8458ee6def2c10ea264d131a9d4","observation_id":"6baae0be-f06a-4c0c-bef9-fefb68ddd2a0","resolution":{"observed_at":"2026-08-14T11:07:32.180355Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.07841","last_updated":"2017-01-18T04:31:27Z","snapshot_observed_at":"2026-08-14T21:38:14.491232Z","submitted_at":"2016-09-26T03:38:36Z","title":"Dark Matter Relic Abundance and Light Sterile Neutrinos","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.07841","snapshot_observed_at":"2026-08-14T11:07:32.185155Z","title":"Tang and S.-h","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.185155Z"},"links":{"cited_paper":"/paper/1609.07841","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:aae891516ea70dcef21aca2c894dcb5cd2c46a1ca272fec9d5574d78fa567174","observation_id":"baf85d20-eb53-441e-87dd-92896e2b1f38","resolution":{"observed_at":"2026-08-14T11:07:32.185155Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.08708","last_updated":"2018-12-13T22:14:28Z","snapshot_observed_at":"2026-08-14T21:04:13.181121Z","submitted_at":"2017-04-27T18:27:28Z","title":"Indirect Detection of Neutrino Portal Dark Matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.08708","snapshot_observed_at":"2026-08-14T11:07:32.189952Z","title":"Batell, T","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.189952Z"},"links":{"cited_paper":"/paper/1704.08708","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:9ad2e000707a09f90ef649d6e0b026a72f1b2c0507b8853fcbc98e68b696a25b","observation_id":"e2fcf7df-f957-4ad1-af78-ebd068c4b38b","resolution":{"observed_at":"2026-08-14T11:07:32.189952Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1709.07001","last_updated":"2017-09-20T18:00:01Z","snapshot_observed_at":"2026-08-14T20:31:18.824265Z","submitted_at":"2017-09-20T18:00:01Z","title":"Thermal Dark Matter Through the Dirac Neutrino Portal","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1709.07001","snapshot_observed_at":"2026-08-14T11:07:32.194611Z","title":"Batell, T","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.194611Z"},"links":{"cited_paper":"/paper/1709.07001","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:2200ddc50a4f6cc57e6ffe109da00153dc483ad17955035e04f23b9191d7187f","observation_id":"25315db8-b9e0-460f-be0c-7878bd1f07ac","resolution":{"observed_at":"2026-08-14T11:07:32.194611Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1607.02373","last_updated":"2017-07-12T00:45:44Z","snapshot_observed_at":"2026-08-14T21:49:13.354667Z","submitted_at":"2016-07-08T14:13:04Z","title":"Sterile Neutrino portal to Dark Matter II: Exact Dark symmetry","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1607.02373","snapshot_observed_at":"2026-08-14T11:07:32.199842Z","title":"Escudero, N","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.199842Z"},"links":{"cited_paper":"/paper/1607.02373","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:5f2fae970fe8326cf345cec6406e663a875f68ad02684beeb8db7e59be49219a","observation_id":"8d9e9900-8036-4e41-9201-0f117953d79b","resolution":{"observed_at":"2026-08-14T11:07:32.199842Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.03110","last_updated":"2016-12-09T18:00:41Z","snapshot_observed_at":"2026-08-14T21:26:16.000440Z","submitted_at":"2016-12-09T18:00:41Z","title":"Indirect Signals from Solar Dark Matter Annihilation to Long-lived Right-handed Neutrinos","version":1},"cited_work":{"arxiv_id":"1612.03110","doi":null,"metadata_source":"pith","pith_arxiv_id":"1612.03110","snapshot_observed_at":"2026-08-14T11:07:32.274842Z","title":"Indirect Signals from Solar Dark Matter Annihilation to Long-lived Right-handed Neutrinos","venue":"hep-ph","work_id":"34750fcd-4f89-4641-9e6d-9dd0cfea0787","year":2016},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.204614Z"},"links":{"cited_paper":"/paper/1612.03110","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:d4f2308ef8df9371ba5a4255e3fdf5ee9c6692ad936606e8e115073d468d0bef","observation_id":"f06b6e6b-a822-47fd-989d-6ba9a24494be","resolution":{"observed_at":"2026-08-14T11:07:32.282964Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1807.05122","last_updated":"2018-12-06T13:55:05Z","snapshot_observed_at":"2026-08-14T18:52:15.107107Z","submitted_at":"2018-07-13T15:02:16Z","title":"Scrutinizing Right-Handed Neutrino Portal Dark Matter With Yukawa Effect","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1807.05122","snapshot_observed_at":"2026-08-14T11:07:32.209428Z","title":"Bandyopadhyay, E","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge","version":6},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-14T11:07:32.209428Z"},"links":{"cited_paper":"/paper/1807.05122","citing_paper":"/paper/1908.09796"},"observation_digest":"sha256:e73f153d195dbd874dcd9562d933bb330435b5155038b25ad0090c6e6f468dba","observation_id":"682fb1c1-835d-4687-8833-80ffff5c354a","resolution":{"observed_at":"2026-08-14T11:07:32.209428Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"1908.09796","last_updated":"2020-10-30T04:08:29Z","latest_version":6,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-14T21:51:22.950485Z","submitted_at":"2019-08-26T16:56:12Z","title":"Structures of the Massive Vector Boson Propagators at Finite Temperature Illuminated by the Goldstone Equivalence Gauge"},"reference_resolution":{"displayed":37,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":28,"verified_exact":5,"verified_fuzzy":4},"total_outbound_references":37},"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":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"As of 15 August 2026, this Paper Citation Record lists 37 of 37 outbound references and 0 inbound Pith citation observations for arXiv:1908.09796."}