{"as_of":"2026-08-21T18:41:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:bce20bbfed19cb8a587e96f5084040221663d59dd2b536778b1a761b65541e2f","coverage":[{"denominator":32,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":32,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-02T22:04:55.221221Z","state":"measured"},{"denominator":32,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":32,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+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/2602.18578/citation-record","integrity":"/paper/2602.18578/integrity","json":"/paper/2602.18578/citation-record.json","paper":"/paper/2602.18578"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2312.09042","last_updated":"2025-01-27T21:39:19Z","snapshot_observed_at":"2026-08-16T14:34:44.126067Z","submitted_at":"2023-12-14T15:39:27Z","title":"Cosmological gravitational particle production and its implications for cosmological relics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.09042","snapshot_observed_at":"2026-08-02T22:04:51.666792Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:51.666792Z"},"links":{"cited_paper":"/paper/2312.09042","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:a07217cf50bbeb074494ccd7d0e2aafb59a7f77eee3b7a47fc0a439b050250f3","observation_id":"5596b850-081d-4d2b-91de-708f5ae1f7da","resolution":{"observed_at":"2026-08-02T22:04:51.666792Z","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":"2026-08-02T22:04:51.727645Z","title":null,"venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:51.727645Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:46ece3f5a9e39ba8e0471892777c2f0bac37ee0399dfcbeaaea2cf80e1fa5d31","observation_id":"0c4fe075-f7d0-4817-bab6-745fe0e48555","resolution":{"observed_at":"2026-08-02T22:04:51.727645Z","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":"2026-08-02T22:04:51.769684Z","title":null,"venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:51.769684Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:e76daa38296348ba4eace157b4341dbaf015b2e7314b25996a2cbb1758e1c565","observation_id":"3366302c-8cba-458d-81d2-ada07ca22017","resolution":{"observed_at":"2026-08-02T22:04:51.769684Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.16303","last_updated":"2023-12-26T19:16:07Z","snapshot_observed_at":"2026-08-16T14:31:31.259977Z","submitted_at":"2023-12-26T19:16:07Z","title":"Resummed heat kernel and effective action for Yukawa and QED","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.16303","snapshot_observed_at":"2026-08-02T22:04:51.830481Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:51.830481Z"},"links":{"cited_paper":"/paper/2312.16303","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:3188e7526bfc24348d51384e66646c0ea126515a73862591b1af969a2601cd86","observation_id":"fd1ff034-fa19-44ef-8944-4cc652dc715a","resolution":{"observed_at":"2026-08-02T22:04:51.830481Z","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":"2026-08-02T22:04:51.935308Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:51.935308Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:b648fa489e90ff8baffb9c809f0de441329f318e40d6d8b0d83937a96c82c6e8","observation_id":"a38307a0-f088-4f4d-a667-71ab457d479b","resolution":{"observed_at":"2026-08-02T22:04:51.935308Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0602176","last_updated":"2006-03-30T21:00:13Z","snapshot_observed_at":"2026-08-17T03:36:00.609508Z","submitted_at":"2006-02-17T22:34:07Z","title":"Worldline Instantons II: The Fluctuation Prefactor","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0602176","snapshot_observed_at":"2026-08-02T22:04:52.059639Z","title":null,"venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:52.059639Z"},"links":{"cited_paper":"/paper/hep-th/0602176","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:4483180d6532f258ca422c36ac2ecd5ef8ba4e76ab846047f6d63abed6a5a3cb","observation_id":"36c3ae10-0690-4ecd-9017-184de4c731c3","resolution":{"observed_at":"2026-08-02T22:04:52.059639Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.09203","last_updated":"2017-06-14T12:44:26Z","snapshot_observed_at":"2026-08-14T21:09:48.073882Z","submitted_at":"2017-03-27T17:45:13Z","title":"Dynamically assisted Sauter-Schwinger effect - non-perturbative versus perturbative aspects","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.09203","snapshot_observed_at":"2026-08-02T22:04:52.169364Z","title":"Torgrimsson, C","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:52.169364Z"},"links":{"cited_paper":"/paper/1703.09203","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:5d8795c7ebc148004412a8e48d4aef1862cfaf9f82be268fe8d58dbb8220841d","observation_id":"e03649d4-1e38-4e7c-aca3-284825e05163","resolution":{"observed_at":"2026-08-02T22:04:52.169364Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.01901","last_updated":"2025-08-03T19:25:33Z","snapshot_observed_at":"2026-08-18T20:00:42.212408Z","submitted_at":"2025-08-03T19:25:33Z","title":"Worldline instantons for nonperturbative particle production by space and time dependent gravitational fields","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.01901","snapshot_observed_at":"2026-08-02T22:04:52.294415Z","title":"Semr´ en and G","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:52.294415Z"},"links":{"cited_paper":"/paper/2508.01901","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:aad29b4d9fca87548b196939b25cf6084409374df52bcd05de56f45bfadbf658","observation_id":"52fc26bf-68b9-448a-ada3-babd79a21ff0","resolution":{"observed_at":"2026-08-02T22:04:52.294415Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1108.0336","last_updated":"2011-11-13T16:22:48Z","snapshot_observed_at":"2026-08-19T01:37:32.087064Z","submitted_at":"2011-08-01T15:22:21Z","title":"On the Creation of Scalar Particles in a Flat Robertson-Walker Space-time","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1108.0336","snapshot_observed_at":"2026-08-02T22:04:52.410344Z","title":"Haouat and R","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:52.410344Z"},"links":{"cited_paper":"/paper/1108.0336","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:6f460eb27e4e15c2887be649ab8f3d7e292f04cc4bbdb1b15269feccd60e07b2","observation_id":"7e8a65e4-a7ed-47c8-a34e-4765430f0db9","resolution":{"observed_at":"2026-08-02T22:04:52.410344Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1904.03207","last_updated":"2019-04-05T18:04:26Z","snapshot_observed_at":"2026-08-19T06:56:25.816105Z","submitted_at":"2019-04-05T18:04:26Z","title":"Generalized Schwinger effect and particle production in an expanding universe","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1904.03207","snapshot_observed_at":"2026-08-02T22:04:52.533714Z","title":"Rajeev, S","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:52.533714Z"},"links":{"cited_paper":"/paper/1904.03207","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:f0d8f0f878dffb6427cf2232145f4dbb36c876cf04ac66c56de3ce7ce27d51dd","observation_id":"4d2c8e29-87da-49fb-bbb0-ed8b8329297c","resolution":{"observed_at":"2026-08-02T22:04:52.533714Z","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":"2026-08-02T22:04:52.649093Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:52.649093Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:050f0375bb37be1a8df7019030577ab902f45a3537603ff733547c918441eb67","observation_id":"fd1836c7-b8e1-4199-bef6-14287533ee71","resolution":{"observed_at":"2026-08-02T22:04:52.649093Z","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":"2026-08-02T22:04:52.808148Z","title":"Parker, Thermal radiation produced by the expansion of the Universe, Nature261, 20 (1976)","venue":null,"work_id":null,"year":1976},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:52.808148Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:c54bb62ba3910d1f21f2ad60695e3ebe49d7cf144f4ecd9dae67721cd566a795","observation_id":"2875c7ed-2988-40dc-adbb-5f344d77664a","resolution":{"observed_at":"2026-08-02T22:04:52.808148Z","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":"2026-08-02T22:04:52.937103Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:52.937103Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:cc251832383d2858e8050f1e3bef54f177864134a1c2b9a97d386bf32f2241a3","observation_id":"1df51506-bd58-40b0-87d8-2dd9a6203809","resolution":{"observed_at":"2026-08-02T22:04:52.937103Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.03340","last_updated":"2025-06-12T12:40:32Z","snapshot_observed_at":"2026-08-12T12:23:52.587774Z","submitted_at":"2024-12-04T14:14:18Z","title":"Nonlocal effective action and particle creation in $D$ dimensions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.03340","snapshot_observed_at":"2026-08-02T22:04:53.051676Z","title":"Boasso, S","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:53.051676Z"},"links":{"cited_paper":"/paper/2412.03340","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:73def5c4fb55b73937afe591b3726cf8c6216cd3e4ce3534a562b7540ab14341","observation_id":"32186e4b-f62a-47e2-93e8-12d9d5e47b66","resolution":{"observed_at":"2026-08-02T22:04:53.051676Z","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":"2026-08-02T22:04:53.187403Z","title":null,"venue":null,"work_id":null,"year":1987},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:53.187403Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:e4a4d0e29a4db11eddbefa732bb9b128a06164f6ab80e1db28b06df5fd04daf4","observation_id":"3cd4896f-bbc1-42bf-a681-027efbc07f10","resolution":{"observed_at":"2026-08-02T22:04:53.187403Z","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":"2026-08-02T22:04:53.271239Z","title":"Hollands and R","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:53.271239Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:0b663d594541e78fbf80b8adcc6554c596706944f3be15f1db7267a299dee028","observation_id":"14e14a73-bcf4-4ea8-8361-6d4e3f2cbe48","resolution":{"observed_at":"2026-08-02T22:04:53.271239Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.07666","last_updated":"2024-02-15T07:26:20Z","snapshot_observed_at":"2026-08-16T19:33:59.593081Z","submitted_at":"2023-12-12T19:01:02Z","title":"Universal definition of the non-conformal trace anomaly","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.07666","snapshot_observed_at":"2026-08-02T22:04:53.353173Z","title":"Ferrero, S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:53.353173Z"},"links":{"cited_paper":"/paper/2312.07666","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:96433723d60776c39d5e9e266be0356a8b1e4448249cee42db99768d23f3d198","observation_id":"30b490db-fd97-4dc7-ac63-0d6495968b60","resolution":{"observed_at":"2026-08-02T22:04:53.353173Z","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":"2026-08-02T22:04:53.524981Z","title":"Audretsch and G","venue":null,"work_id":null,"year":1978},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:53.524981Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:4407420feb9a50b91ab51593bd8ee4c324cbd03e8bc33a1c0d39d492d68a4d55","observation_id":"469f9038-b2fc-43d6-9a10-d85d6b55db29","resolution":{"observed_at":"2026-08-02T22:04:53.524981Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1803.08930","last_updated":"2022-01-22T06:18:51Z","snapshot_observed_at":"2026-08-19T00:06:41.996425Z","submitted_at":"2018-03-23T18:00:05Z","title":"The Big Bang, CPT, and neutrino dark matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1803.08930","snapshot_observed_at":"2026-08-02T22:04:53.672852Z","title":"Boyle, K","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:53.672852Z"},"links":{"cited_paper":"/paper/1803.08930","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:92eb211ead6d059bf2c92015fce9b70109e536f19faef859f7a9a5688aca9b65","observation_id":"ea816cf6-932f-4501-932e-5cec34be3f55","resolution":{"observed_at":"2026-08-02T22:04:53.672852Z","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":"2026-08-02T22:04:53.748022Z","title":null,"venue":null,"work_id":null,"year":1982},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:53.748022Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:96a1195ac3770a47eb7b7ba54c29cea88eb5d141bb94adcba22a9b61b30b53f3","observation_id":"1b284940-3478-46d5-9cc6-5706e7b656e7","resolution":{"observed_at":"2026-08-02T22:04:53.748022Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2302.08812","last_updated":"2024-08-26T08:50:13Z","snapshot_observed_at":"2026-08-16T15:54:39.147821Z","submitted_at":"2023-02-17T11:12:01Z","title":"Low Energy States and CPT invariance at the Big Bang","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.08812","snapshot_observed_at":"2026-08-02T22:04:53.865568Z","title":"Nadal-Gisbert, J","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:53.865568Z"},"links":{"cited_paper":"/paper/2302.08812","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:ee06af0a3d5d30e6b459cd1e2fbd9069a18e5e03321659da979e971ac1e0a6e5","observation_id":"2a08cc47-710c-44d7-9c2f-67932a4c527c","resolution":{"observed_at":"2026-08-02T22:04:53.865568Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.13937","last_updated":"2020-06-15T17:14:23Z","snapshot_observed_at":"2026-08-10T03:30:59.145357Z","submitted_at":"2019-10-30T15:44:56Z","title":"Gravitational production of scalar dark matter","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.13937","snapshot_observed_at":"2026-08-02T22:04:54.030673Z","title":null,"venue":null,"work_id":null,"year":1910},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.030673Z"},"links":{"cited_paper":"/paper/1910.13937","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:010ebd1441ea2575cf039f427b398306ada5d0747be6c48352d77e39491b5f7a","observation_id":"0dab13c1-935d-43c1-940c-3c27136024fb","resolution":{"observed_at":"2026-08-02T22:04:54.030673Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.08236","last_updated":"2019-04-23T10:23:09Z","snapshot_observed_at":"2026-08-14T18:37:24.717965Z","submitted_at":"2018-08-24T18:00:08Z","title":"Despicable Dark Relics: generated by gravity with unconstrained masses","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.08236","snapshot_observed_at":"2026-08-02T22:04:54.129149Z","title":"Fairbairn, K","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.129149Z"},"links":{"cited_paper":"/paper/1808.08236","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:2e384917071b292ac41a37e91669ee0830708f4d5c7fef92b680d26345d85e7c","observation_id":"1165c1f2-1193-4f0a-ad13-85cb088fcbab","resolution":{"observed_at":"2026-08-02T22:04:54.129149Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.07288","last_updated":"2017-02-02T21:07:14Z","snapshot_observed_at":"2026-08-14T22:17:18.887378Z","submitted_at":"2015-12-22T22:36:24Z","title":"Dark matter from gravitational particle production at reheating","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.07288","snapshot_observed_at":"2026-08-02T22:04:54.243016Z","title":"Markkanen and S","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.243016Z"},"links":{"cited_paper":"/paper/1512.07288","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:d564193efe70f1e0c420bfc7a7579c483d36e55ae6ec91f5627b870d7c7693d1","observation_id":"1e0ffeb7-2162-4bb7-9043-02b6ac870ab9","resolution":{"observed_at":"2026-08-02T22:04:54.243016Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.10161","last_updated":"2021-05-21T06:56:10Z","snapshot_observed_at":"2026-08-21T16:34:07.935693Z","submitted_at":"2021-05-21T06:56:10Z","title":"Wick rotation and the positivity of energy in quantum field theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.10161","snapshot_observed_at":"2026-08-02T22:04:54.346373Z","title":"Kontsevich and G","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.346373Z"},"links":{"cited_paper":"/paper/2105.10161","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:6f68ff2aa78818ab905e1a6290a034bada0fa3eedb1e7b4be7acaba212359a1f","observation_id":"3b49eddf-cae8-43e9-8dad-d2fe1ef8fd33","resolution":{"observed_at":"2026-08-02T22:04:54.346373Z","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":"2026-08-02T22:04:54.452326Z","title":"Padmanabhan, Quantum theory in external electro- magnetic and gravitational fields: A Comparison of some conceptual issues, Pramana37, 179 (1991)","venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.452326Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:e71862adaf70ebad0b4b073d1198b86744da7bb7b33667f6233b7738d7cd854e","observation_id":"4c07b383-4102-451d-9aa0-d486884037e1","resolution":{"observed_at":"2026-08-02T22:04:54.452326Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1204.3654","last_updated":"2012-11-21T17:35:18Z","snapshot_observed_at":"2026-08-15T04:12:52.536023Z","submitted_at":"2012-04-16T21:07:08Z","title":"Particle creation due to tachyonic instability in relativistic stars","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1204.3654","snapshot_observed_at":"2026-08-02T22:04:54.577716Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.577716Z"},"links":{"cited_paper":"/paper/1204.3654","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:8147c98f453f11f39b7bbe3e8f118f0a41dead69be040de7bede29261f0acf88","observation_id":"1f992eaa-b191-437b-9cd2-d953ee5bcab0","resolution":{"observed_at":"2026-08-02T22:04:54.577716Z","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":"2026-08-02T22:04:54.707512Z","title":"Schroer, R","venue":null,"work_id":null,"year":1970},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.707512Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:2e5e8a9eb071653bd583dc4c37588e41d3ccf1e2304d461616122fede5b5411e","observation_id":"4b4f4f01-a6d6-45c6-aa08-9e2523046381","resolution":{"observed_at":"2026-08-02T22:04:54.707512Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1910.01205","last_updated":"2020-02-28T19:55:15Z","snapshot_observed_at":"2026-08-16T17:09:09.402223Z","submitted_at":"2019-10-02T20:31:32Z","title":"Chiral Anomaly, Schwinger Effect, Euler-Heisenberg Lagrangian, and application to axion inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1910.01205","snapshot_observed_at":"2026-08-02T22:04:54.790335Z","title":"Domcke, Y","venue":null,"work_id":null,"year":1910},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.790335Z"},"links":{"cited_paper":"/paper/1910.01205","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:91e8316307eb29ea0060a772474b70237a19e9df14993a00ed9179775a342eab","observation_id":"d43e8b7b-67e2-416f-9450-765e341bad9b","resolution":{"observed_at":"2026-08-02T22:04:54.790335Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.16538","last_updated":"2025-04-11T13:11:47Z","snapshot_observed_at":"2026-08-16T13:22:55.166677Z","submitted_at":"2024-08-29T13:53:16Z","title":"On the Schwinger effect during axion inflation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.16538","snapshot_observed_at":"2026-08-02T22:04:54.935295Z","title":"von Eckardstein, K","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:54.935295Z"},"links":{"cited_paper":"/paper/2408.16538","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:7d26c437af2ce050c0c5bdc138208920fa5fa2a89d4c528a33406ee98c33387c","observation_id":"15038c03-194a-491f-a4b8-c309b2eaa27d","resolution":{"observed_at":"2026-08-02T22:04:54.935295Z","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":"2026-08-02T22:04:55.094978Z","title":"Vicente Garc ´ ıa-Consuegra and A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:55.094978Z"},"links":{"citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:5736d833e73221470cac9ba508c763a820245681c191eed59f032bbbb9c0f763","observation_id":"5e2881fd-bf71-4f60-a8ff-a8ac48dc2cfc","resolution":{"observed_at":"2026-08-02T22:04:55.094978Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.00997","last_updated":"2025-08-01T18:05:45Z","snapshot_observed_at":"2026-08-21T18:24:58.661846Z","submitted_at":"2025-08-01T18:05:45Z","title":"Tunnelling amplitudes and Hawking radiation from worldline QFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.00997","snapshot_observed_at":"2026-08-02T22:04:55.221221Z","title":"Ilderton and K","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-02T22:04:55.221221Z"},"links":{"cited_paper":"/paper/2508.00997","citing_paper":"/paper/2602.18578"},"observation_digest":"sha256:390784172529bc91da1904a730745c26f9c757cf7f0552c67ad5a26fb4486938","observation_id":"38477af6-40ad-46dc-ab4f-71ba8f9713af","resolution":{"observed_at":"2026-08-02T22:04:55.221221Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2602.18578","last_updated":"2026-07-27T10:47:59Z","latest_version":2,"primary_category":"hep-th","snapshot_observed_at":"2026-08-17T16:40:20.217220Z","submitted_at":"2026-02-20T19:35:47Z","title":"Conformally-flat gravitational analogues to the Schwinger effect"},"reference_resolution":{"displayed":32,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":32,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":32},"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":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"thesis":"As of 21 August 2026, this Paper Citation Record lists 32 of 32 outbound references and 0 inbound Pith citation observations for arXiv:2602.18578."}