{"as_of":"2026-08-08T06:39:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6bdf9e7071b90027308efad064829f8687f34b4bab939d974d95d93abf49b4e2","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":8,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":8,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-08T06:32:00.761636+00:00","state":"measured"},{"denominator":8,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":8,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-07T15:43:30.414816Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-03T09:27:48.920386Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2207.12207","last_updated":"2022-10-14T09:49:26Z","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.12207","snapshot_observed_at":"2026-08-07T15:43:30.414816Z","title":"Biondini, P","venue":null,"work_id":null,"year":2022},"citing_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},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-07T15:43:30.414816Z"},"links":{"cited_paper":"/paper/2207.12207","citing_paper":"/paper/2505.14335"},"observation_digest":"sha256:0eb5e2d68862cd6e0f61a4ffdf9595301a45d20ce1e295f4d93284ee43c0f43b","observation_id":"fb087dc2-2e83-41d7-8f95-35f352bcc413","resolution":{"observed_at":"2026-08-07T15:43:30.414816Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.12207","last_updated":"2022-10-14T09:49:26Z","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.12207","snapshot_observed_at":"2026-08-06T21:11:40.619665Z","title":"Biondini, P","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.00925","last_updated":"2026-08-02T11:16:38Z","snapshot_observed_at":"2026-08-08T03:50:17.496512Z","submitted_at":"2025-07-01T16:31:48Z","title":"Connecting $t$-channel Dark Matter Models to the Standard Model Effective Field Theory","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T21:11:40.619665Z"},"links":{"cited_paper":"/paper/2207.12207","citing_paper":"/paper/2507.00925"},"observation_digest":"sha256:be770c90fc900e4538c63e4d9aae2d1426b6aa01fa7cf99f2d4d9118d7e1906d","observation_id":"9003ee85-324a-4033-8501-a7a23a2360cd","resolution":{"observed_at":"2026-08-06T21:11:40.619665Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.12207","last_updated":"2022-10-14T09:49:26Z","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.12207","snapshot_observed_at":"2026-08-06T18:56:41.049005Z","title":"Biondini, P","venue":null,"work_id":null,"year":null},"citing_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},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-06T18:56:41.049005Z"},"links":{"cited_paper":"/paper/2207.12207","citing_paper":"/paper/2507.07014"},"observation_digest":"sha256:54b07b5a966bfe570440b0a30738880eb9590433bd28f71db1a30efc8d86d8b9","observation_id":"42e96d07-90b4-43f9-87aa-d356ca3f78bf","resolution":{"observed_at":"2026-08-06T18:56:41.049005Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.12207","last_updated":"2022-10-14T09:49:26Z","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.12207","snapshot_observed_at":"2026-08-06T15:08:43.547218Z","title":"Biondini, P","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.16905","last_updated":"2026-07-08T13:19:52Z","snapshot_observed_at":"2026-08-07T11:07:13.044045Z","submitted_at":"2025-07-22T18:00:04Z","title":"Hot news on the phase structure of the SMEFT","version":2},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-06T15:08:43.547218Z"},"links":{"cited_paper":"/paper/2207.12207","citing_paper":"/paper/2507.16905"},"observation_digest":"sha256:7e92e6d24d745ea7eb5ae989a0151617401b6a24431f7a6fcde9d771854346a8","observation_id":"93137913-7548-4313-a3f7-19184f878ef7","resolution":{"observed_at":"2026-08-06T15:08:43.547218Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.12207","last_updated":"2022-10-14T09:49:26Z","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.12207","snapshot_observed_at":"2026-08-03T03:46:47.360379Z","title":"Biondini, P","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.06962","last_updated":"2026-07-07T12:35:17Z","snapshot_observed_at":"2026-08-08T04:20:11.678400Z","submitted_at":"2026-02-06T18:59:46Z","title":"Hard thermal contributions to phase transition observables at NNLO","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-03T03:46:47.360379Z"},"links":{"cited_paper":"/paper/2207.12207","citing_paper":"/paper/2602.06962"},"observation_digest":"sha256:94c78df59e2816aa82fc70c9e9d3ac26244cf663b9a929b2598abb47172d1fe7","observation_id":"423ea390-e200-43c4-a0c4-bf6b8b444fae","resolution":{"observed_at":"2026-08-03T03:46:47.360379Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.12207","last_updated":"2022-10-14T09:49:26Z","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models","version":2},"cited_work":{"arxiv_id":"2207.12207","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2207.12207","snapshot_observed_at":"2026-07-03T09:27:48.920386Z","title":"Biondini, P","venue":null,"work_id":"bae3d3d7-46c1-4d65-b28e-ddd7a9e4f54c","year":2022},"citing_paper":{"arxiv_id":"2604.21972","last_updated":"2026-04-23T18:00:01Z","snapshot_observed_at":"2026-07-06T23:08:28.444591Z","submitted_at":"2026-04-23T18:00:01Z","title":"Matchotter: An Automated Tool for Dimensional Reduction at Finite Temperature","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-05-09T21:01:53.532819Z"},"links":{"cited_paper":"/paper/2207.12207","citing_paper":"/paper/2604.21972"},"observation_digest":"sha256:e900837df6d662e9629c565eea863e8fa5e2a976b4e97b012a5116903cc43a8b","observation_id":"8a99c1ec-5947-4056-b0ee-21dce953cfaa","resolution":{"observed_at":"2026-05-11T14:47:25.613547Z","resolver_source":"arxiv_id","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":"2207.12207","last_updated":"2022-10-14T09:49:26Z","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models","version":2},"cited_work":{"arxiv_id":"2207.12207","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2207.12207","snapshot_observed_at":"2026-07-03T09:27:48.920386Z","title":"Biondini, P","venue":null,"work_id":"bae3d3d7-46c1-4d65-b28e-ddd7a9e4f54c","year":2022},"citing_paper":{"arxiv_id":"2605.06775","last_updated":"2026-05-07T18:00:02Z","snapshot_observed_at":"2026-08-03T00:40:30.255493Z","submitted_at":"2026-05-07T18:00:02Z","title":"SIRENA -- Sum-Integral REductioN Algorithm","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-05-11T00:52:24.927995Z"},"links":{"cited_paper":"/paper/2207.12207","citing_paper":"/paper/2605.06775"},"observation_digest":"sha256:22ab9b51138698af6bba9376332c6ec797ed4a95298456c05688dce08e75159f","observation_id":"d8071b08-807a-4fc9-b41d-6996a226a4f5","resolution":{"observed_at":"2026-05-11T05:05:57.902788Z","resolver_source":"arxiv_id","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":"2207.12207","last_updated":"2022-10-14T09:49:26Z","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models","version":2},"cited_work":{"arxiv_id":"2207.12207","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2207.12207","snapshot_observed_at":"2026-07-03T09:27:48.920386Z","title":"Biondini, P","venue":null,"work_id":"bae3d3d7-46c1-4d65-b28e-ddd7a9e4f54c","year":2022},"citing_paper":{"arxiv_id":"2607.02505","last_updated":"2026-07-02T17:58:57Z","snapshot_observed_at":"2026-07-07T00:07:56.573640Z","submitted_at":"2026-07-02T17:58:57Z","title":"A critical look at low-scale cosmological phase transitions in the PTA era","version":1},"reference_index":223,"source":"pdf_text","source_observed_at":"2026-07-03T09:23:17.300830Z"},"links":{"cited_paper":"/paper/2207.12207","citing_paper":"/paper/2607.02505"},"observation_digest":"sha256:9b581d5cddd440978392b4227f3138eb00c73b0290b69950083dcbc423030b2b","observation_id":"c931532b-21a8-4902-a4b9-a1737272f54f","resolution":{"observed_at":"2026-07-03T09:27:48.922014Z","resolver_source":"arxiv_id","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"}}],"links":{"evidence":"/evidence","html":"/paper/2207.12207/citation-record","integrity":"/paper/2207.12207/integrity","json":"/paper/2207.12207/citation-record.json","paper":"/paper/2207.12207"},"outbound":[],"paper":{"arxiv_id":"2207.12207","last_updated":"2022-10-14T09:49:26Z","latest_version":2,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-07T13:58:28.950652Z","submitted_at":"2022-07-25T13:54:28Z","title":"Strong electroweak phase transition in $t$-channel simplified dark matter models"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"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 0 of 0 outbound references and 8 inbound Pith citation observations for arXiv:2207.12207."}