{"as_of":"2026-08-03T23:22:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:300ea60762a11eea694bfaba1baa4617070484109cecf4f6e130a68655c1e87c","coverage":[{"denominator":90,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":90,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-11T11:50:26.030339Z","state":"measured"},{"denominator":91,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":91,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-03T06:30:56.289259+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-13T06:30:17.396440Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.21736","snapshot_observed_at":"2026-07-13T06:30:17.396440Z","title":"Mallik and G","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.08815","last_updated":"2026-07-09T18:00:00Z","snapshot_observed_at":"2026-07-15T23:17:53.279969Z","submitted_at":"2026-07-09T18:00:00Z","title":"A Small-Throat Boundary Condition for the Tunneling Wave Function of the Universe","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-07-13T06:30:17.396440Z"},"links":{"cited_paper":"/paper/2604.21736","citing_paper":"/paper/2607.08815"},"observation_digest":"sha256:b476338a08710a9aa968a8202b300103efefc844555855611264bd4e29259971","observation_id":"a3236d07-8712-45da-a4ea-cfc1c48a9d0f","resolution":{"observed_at":"2026-07-13T06:30:17.396440Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2604.21736/citation-record","integrity":"/paper/2604.21736/integrity","json":"/paper/2604.21736/citation-record.json","paper":"/paper/2604.21736"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"This boundary condition corresponds to fixing the Hubble radius 30 (H1 =K/3), which is more physically sensible compared to the fixed size [29, 34]","venue":null,"work_id":"5d0c1255-53a1-4cb6-af4e-459d67838f93","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:c9da7a950fa19f0b6cda4f49d78ef0d2e4ae498e5850efb27d77e46d90fc1a16","observation_id":"8fdb1912-cae5-4abf-823b-59daa8163391","resolution":{"observed_at":"2026-05-23T15:48:08.753243Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"24fa858e-7da7-4bfc-a1a6-bab2550dc10e","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:4f0e1c3e2ccc8fb92b7c03e4b3ce39024bc409d32792e8141d2015e037c25a18","observation_id":"d1019747-5d86-45bf-ab77-c437dca759a7","resolution":{"observed_at":"2026-05-23T15:48:08.789419Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"(131), can be computed via Picard-Lefschetz methods","venue":null,"work_id":"03aa0374-947a-4910-b26d-3f5f0151d9e0","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:aa1956c4c467f4a4da65ecc925edcb0422fe2a9ff08809bc07d21a43d0aa791d","observation_id":"0e994e80-9d3f-43a7-9467-8f5354120ebd","resolution":{"observed_at":"2026-05-23T15:48:08.785435Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Clearly, forH 1 ≪H, {∆l h(Nc)}−gl/2 ∼ H1 −2gl , which is divergent forH 1 →0","venue":null,"work_id":"7c309c5c-3bd5-4d78-83ec-570d0ee43f82","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:914a68b4bcf0040c63a852b1a7cc444d771eb0f746b6b1de37177efab7f35c11","observation_id":"06e5290b-69a5-40a0-95a5-bead771e061d","resolution":{"observed_at":"2026-05-23T15:48:08.760729Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"pinching","venue":null,"work_id":"f5086aa4-f608-43d1-ae7a-5564a0a18ec9","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:29810fdf41a8f6d2f56278f4fd23682fe036d5389070e92d6b85d40a6acee53c","observation_id":"08bb79b7-3795-4c71-808c-d80913b01c69","resolution":{"observed_at":"2026-05-23T15:48:08.774191Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Note that Λ deformation introduces aniϵcorrection to the determinant","venue":null,"work_id":"38662c65-2e57-4efb-9624-17c5a5da7312","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:e98b6cbca4a763bbba5de999e9fdfe763b563be2ff345a781bc83ad3fc1cec91","observation_id":"3d3c451b-50c0-4deb-b595-747499af5b84","resolution":{"observed_at":"2026-05-23T15:48:08.757001Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"(143) whenϵ= 0","venue":null,"work_id":"9d0eceed-484a-45fd-9284-f2ec876c8560","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:63a1306599141dcdae4b6e64766b9f232955c1b9cf48cf5b08f55f219641cd6a","observation_id":"5f236d21-9e32-44c7-b38e-c408476b9eff","resolution":{"observed_at":"2026-05-23T15:48:08.734720Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"spurious","venue":null,"work_id":"09c4c584-f8b5-43ed-8cec-3fca231a6a4c","year":2026},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:01e3051a88c2a547f7d5199d4d81ace3d3b3dc03aec61ec636ebb2cfe11d5f47","observation_id":"d968a8bd-c3bb-4875-9bb4-29cdbf471620","resolution":{"observed_at":"2026-05-23T15:48:08.731424Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"It implies the fundamental solutions PandQsatisfy the same property","venue":null,"work_id":"2aacdb70-8394-4235-a0d5-4fc806a92b08","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:772444c7ada0ca7f1be8cff7531a6855608b7f5a89a2a4112ab90448791a2185","observation_id":"0e52e56b-9bd6-4f0b-996d-e319b6c93185","resolution":{"observed_at":"2026-05-23T15:48:08.768708Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.15.2752","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-03T08:37:45.889735Z","title":"Action Integrals and Partition Functions in Quantum Gravity","venue":null,"work_id":"d794a386-690a-4a5a-8de8-d727d28afc2a","year":1977},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:55ffeccfccf883d85084203a42f4217c271a9bb16bae5eea65460c6f41310631","observation_id":"9d115794-d140-4bfb-b7b0-23ffbbe50434","resolution":{"observed_at":"2026-05-09T21:38:30.325266Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0550-3213(78)90161-x","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Path Integrals and the Indefiniteness of the Gravitational Action","venue":null,"work_id":"446f2684-b717-436c-801b-a21d89784e2d","year":1978},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:8be8ae4d948349d0dc890c826590ac7b456fc453e885fcb875a93f3bff5dbb84","observation_id":"5d88d783-e4e3-45af-be27-90d6c1699d05","resolution":{"observed_at":"2026-05-09T21:38:30.426481Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.28.2960","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-02T11:36:54.550879Z","title":"Hartle and S","venue":null,"work_id":"79b5b555-705e-432f-8510-c66443464ce5","year":1983},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:24d4cb9ab7c004a2c30e78cb6474c056e6ac9e20a5990eaad67d48eda89307be","observation_id":"3670c27b-26e0-4d36-a304-74ae2e662149","resolution":{"observed_at":"2026-05-09T21:38:30.424092Z","resolver_source":"doi","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2403.10510","last_updated":"2024-10-02T21:53:22Z","snapshot_observed_at":"2026-07-06T17:45:23.748539Z","submitted_at":"2024-03-15T17:49:13Z","title":"Comments on the no boundary wavefunction and slow roll inflation","version":2},"cited_work":{"arxiv_id":"2403.10510","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2403.10510","snapshot_observed_at":"2026-07-04T18:20:04.098230Z","title":"Maldacena,Comments on the no boundary wavefunction and slow roll inflation","venue":null,"work_id":"9b985a65-4f4e-471d-98ed-64894d541f20","year":2024},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"cited_paper":"/paper/2403.10510","citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:23ed3bc2690b4bbf48e1c80d63f46b2a131f0b278b3ee31ee44d8984849fc227","observation_id":"7136e521-4f2b-4c74-9e3f-8053674944a5","resolution":{"observed_at":"2026-05-11T14:36:04.097654Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/s10714-008-0661-1","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-08T04:54:31.947993Z","title":"The Dynamics of general relativity","venue":null,"work_id":"740f5ae5-d2b6-46e8-bbf2-64f5ad9a7637","year":2008},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:a8be7cb63173f8c6edb900f4e4e55183cfa2079f501cd458616ca8085f2ca01a","observation_id":"e3245b6b-5b35-46ac-b59f-730cac0b4436","resolution":{"observed_at":"2026-05-09T21:38:30.416945Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-07-10T19:19:34.618255+00:00","source":"crossref_status_cache"},{"observed_at":"2026-07-10T19:19:34.618255+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1001.2933","last_updated":"2010-08-28T04:23:48Z","snapshot_observed_at":"2026-08-01T00:32:08.169500Z","submitted_at":"2010-01-18T17:02:17Z","title":"Analytic Continuation Of Chern-Simons Theory","version":4},"cited_work":{"arxiv_id":"1001.2933","doi":"10.48550/arxiv.1001.2933","metadata_source":"pith","pith_arxiv_id":"1001.2933","snapshot_observed_at":"2026-07-10T06:15:00.866473Z","title":"Analytic Continuation Of Chern-Simons Theory","venue":"hep-th","work_id":"815246a9-676d-4915-8c07-40d2f7a6fee9","year":2010},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"cited_paper":"/paper/1001.2933","citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:e8f4650cb6d37e8a27e4aa634622e9d1d7c23188ea85873ec8b1fd8f0636b93d","observation_id":"c0d1bcec-8ac5-47be-bbfe-9ff7260df7d9","resolution":{"observed_at":"2026-05-11T14:36:04.077178Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"One loop divergencies in the theory of gravitation","venue":null,"work_id":"50d85528-ce78-4e7d-ade3-1c5e6bdf248d","year":1974},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:06ef2d1cd4337454e9f351360c6b3a1b8d8565f3162d0ba27cf252ab718e35f9","observation_id":"c4fa0412-4523-4675-a4f4-4f6d6b35504e","resolution":{"observed_at":"2026-05-23T15:48:08.738216Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0370-","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-09T17:26:25.208929Z","title":"Laporta and E","venue":null,"work_id":"cc369e6a-407b-4744-9ca6-79549b2e5bf8","year":1980},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:efb47e9e21c4d17df2584a2c62b1c6a51af01039f147a301e97d55abf93ff083","observation_id":"ea4ab547-fa10-4e0e-bf54-e3e25e83a6c4","resolution":{"observed_at":"2026-05-09T21:38:30.436714Z","resolver_source":"doi","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0550-3213(86)90193-8","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-02T23:37:26.802842Z","title":"The Ultraviolet Behavior of Einstein Gravity","venue":null,"work_id":"48a31176-5efe-4d26-9bd0-2a59dffbf3e3","year":1986},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:6607547fffa3ad1b2f7a0c9d897947476d115db15e992c7abce1f7ec6e045a06","observation_id":"72e151a5-b3f5-4388-9dd7-7e6d5b72f8d1","resolution":{"observed_at":"2026-05-09T21:38:30.434009Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.18.4480","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Remarks on High-energy Stability and Renormalizability of Gravity Theory","venue":null,"work_id":"7715091f-fb3d-4dc4-85ca-acb887a8a3cc","year":1978},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:4bac9dd8c543d21889944193f548e64635473f9fd8c69415201d0cadbfeb9a1f","observation_id":"200c2562-021e-4b32-a6f8-04fb3f8668ec","resolution":{"observed_at":"2026-05-09T21:38:30.419290Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/j.physletb.2012.03.070","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Short Distance Freedom of Quantum Gravity","venue":null,"work_id":"5ea39cd1-c4f0-44b0-8dd7-b5bfd175a741","year":2012},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:cb080e2303ce734418ebc2dda1b28c0eb75bf6147e6c191dd732416acb58bd46","observation_id":"84f5dd6f-54ee-4c41-b1c3-7b156f4b0db7","resolution":{"observed_at":"2026-05-09T21:38:30.404802Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Amplification of gravitational waves in an isotropic universe","venue":null,"work_id":"0e846c64-1963-4b0b-8752-d45a1ce7872f","year":1975},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:13094f564257be04a95869b973376da38185ce52838b467400d2fc6ccb049c10","observation_id":"ab775992-595b-4527-8fa8-526d2709ad5f","resolution":{"observed_at":"2026-05-23T15:48:08.749336Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevlett.133.021501","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Inflationary Cosmology from Anti-de Sitter Worm- holes","venue":null,"work_id":"cd3ec86d-4f7e-42b1-b74e-cc1582d54bc6","year":2024},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:4e7c8a44f40037c6a23b7950ef276e2de70bb8884e255b754c180111b3013ddb","observation_id":"499fb7b5-098f-4d5f-bd10-10ceda75d296","resolution":{"observed_at":"2026-05-09T21:38:30.392751Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.38.2468","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Derivation of the Wheeler-De Witt Equation from a Path Integral for Min- isuperspace Models","venue":null,"work_id":"f1b6beae-082d-4483-b79e-07fd2773af24","year":1988},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:54396ecccf1bb7e07ba6e8676215dbcbcd9b3a56ae485a467d8f5053f586b046","observation_id":"91fbd3d4-3ae0-4ca6-b3f0-007e93a3675c","resolution":{"observed_at":"2026-05-09T21:38:30.409756Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0370-2693(77)90553-","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Relativistic S Matrix of Dynamical Systems with Boson and Fermion Constraints","venue":null,"work_id":"2b34064b-0fc8-4caf-a1b3-af4aecf537e1","year":1977},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:745912bbc2e8a98cf1f54bb587eceb2a5e8034ceabeda218f11d531952287d6e","observation_id":"9221942a-09c8-4d80-ad93-575ccf3e3296","resolution":{"observed_at":"2026-05-09T21:38:30.373811Z","resolver_source":"doi","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0370-2693(89)90387-0","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"The phase of the sum over spheres","venue":null,"work_id":"45be8a26-7cdf-4b62-b151-0ce49f7fd820","year":1989},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:f9a1ea263f2ac3ffde3197cc41738aa451cdfe62ae05c2d72bbf63ba3d3e5b72","observation_id":"5c2137cf-cbd5-4b85-b763-c0439e74f752","resolution":{"observed_at":"2026-05-09T21:38:30.390284Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2504.00920","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-11T00:07:45.655796Z","title":"Physical instabilities and the phase of the Euclidean path integral","venue":null,"work_id":"2eb2a9f4-f2bd-4f17-b69f-a22c8dfdfd37","year":2025},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:0c228918e2382de5a0adffc4b5110a6b6e1a5a4f65399efd6f4d21aa651d4afe","observation_id":"48f757dd-5f39-402a-b370-178ff56a4385","resolution":{"observed_at":"2026-05-11T14:36:04.173465Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.95.103508","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Feldbrugge, J.-L","venue":null,"work_id":"b1763bad-5041-428c-9413-877d8650a0f9","year":2017},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:3fd4e68ea12373d624913384792cf38d977019521eff9e6b3d08218752aee61c","observation_id":"8585714c-ed6f-408d-8747-dc4bd2d654c2","resolution":{"observed_at":"2026-05-09T21:38:30.438911Z","resolver_source":"doi","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.25.3159","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Teitelboim, Quantum mechanics of the gravi- tational field , Phys","venue":null,"work_id":"fb9dce6e-44fc-4345-b4b8-e34917e876ae","year":1982},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:da79b3407313ceab8536d52a447cea7275b1ea8b6bf1c8c52916fc317506dff3","observation_id":"98da901f-563e-4a91-a6b0-8b439958cfed","resolution":{"observed_at":"2026-05-09T21:38:30.397819Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.28.297","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"The Proper Time Gauge in Quantum Theory of Gravitation","venue":null,"work_id":"55b95cce-7e0a-408d-b401-1bf447da9e4e","year":1983},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:daa5316eedd7edf0c77ba38b25dd68858338fe2f13e6676d8e7469e87aa3d79e","observation_id":"1471e7d9-3923-46e9-898a-5709ae4fcfdc","resolution":{"observed_at":"2026-05-09T21:38:30.376130Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.97.023509","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"No rescue for the no boundary proposal: Pointers to the future of quantum cosmology","venue":null,"work_id":"f89270e3-6ddd-4f97-ba73-f352a1bb6227","year":2018},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:fdeac6416df926fafcd0042ed0bbd80695fe678418398f30d5ab458c97827aa9","observation_id":"ef957af3-0dfa-481d-a0ff-45b46a3cefc3","resolution":{"observed_at":"2026-05-09T21:38:30.400240Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0370-2693(67)90067-6","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-29T06:43:09.354327Z","title":"Feynman Diagrams for the Yang-Mills Field","venue":null,"work_id":"246fc939-a3d1-471b-a336-e238347c93ac","year":1967},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:9b448536f4f3408ea4f6e69350ef1328ee17838b8157c870a4429d0726623e99","observation_id":"8bfad83a-ad1d-4da3-b855-516885057aea","resolution":{"observed_at":"2026-05-09T21:38:30.371215Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/0264-","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-09T15:56:19.422123Z","title":"Thermodynamics of Kerr-Newman-AdS Black Holes and Conformal Field Theories","venue":null,"work_id":"7039cda4-2c01-4de1-a09f-e8e79a272588","year":2004},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:0514583ca768bef707cd4042548a969a99a8c8eadbce3f7b538060d1e0c3a162","observation_id":"b0ed41b2-dc5b-432e-b6e2-d93a9dc3e114","resolution":{"observed_at":"2026-05-09T21:38:30.431564Z","resolver_source":"doi","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1142/s0217732320500571","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"AdS backgrounds and induced gravity","venue":null,"work_id":"f34a188b-b5cf-4542-a74d-84cedaa46d68","year":2019},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:d8aadcc25ae436712de4366aed63d8049a363c8596457071941751dee94c920d","observation_id":"74c6307c-8e5c-49ce-82fe-18f8862c65e8","resolution":{"observed_at":"2026-05-09T21:38:30.448414Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1142/s0129055x21400043","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-26T08:09:10.588020Z","title":"A note on boundary conditions in Euclidean gravity","venue":null,"work_id":"f83eb18d-9373-47fe-afed-0a08a55d31bc","year":2021},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:7856b718da2903115eb99aa255665d02e420a056246cf3ff659bb4d8744dac16","observation_id":"1c483906-fb92-4d21-97c5-75a6aa64dfd1","resolution":{"observed_at":"2026-05-09T21:38:30.414749Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.107.104054","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Generalized boundary conditions in closed cosmologies","venue":null,"work_id":"d3d2b496-7a6a-4edd-a3c6-68acc4e23130","year":2023},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:6b63cd289d7577b844415e75c28405c9dc16a949d24f026fc5580b9559859b8f","observation_id":"00b82dd8-1405-484c-8603-208c7404e91c","resolution":{"observed_at":"2026-05-09T21:38:30.388074Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2407.17724","last_updated":"2025-04-07T07:30:04Z","snapshot_observed_at":"2026-07-06T18:51:36.869948Z","submitted_at":"2024-07-25T02:53:21Z","title":"Monte Carlo studies of quantum cosmology by the generalized Lefschetz thimble method","version":3},"cited_work":{"arxiv_id":"2407.17724","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2407.17724","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Monte Carlo studies of quantum cosmology by the generalized Lefschetz thimble method","venue":null,"work_id":"d42574bc-5930-4feb-b661-b3369ab218aa","year":2025},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"cited_paper":"/paper/2407.17724","citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:e85b427ccec92f2a8ff32329ebdd45d24dd223c67ed51da93ed3b3b45aac74a7","observation_id":"6c4c64fe-5cb8-4273-990e-ba058cfca337","resolution":{"observed_at":"2026-05-11T14:36:04.149870Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.59.103501","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Lorentzian condition in quantum gravity","venue":null,"work_id":"ce41846f-0f17-47fd-ba97-3923a6cec993","year":1999},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:566bcade60623b5247c2743aab321b3f465b8efb17cf4b308328458a29e6a233","observation_id":"5d1dd5e8-b24a-4bf1-9f35-58541154dcc7","resolution":{"observed_at":"2026-05-09T21:38:30.395177Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2602.02682","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-03T18:28:48.595499Z","title":"Consistent Evaluation of the No-Boundary Proposal","venue":null,"work_id":"90a30276-f118-4b68-bd12-4f3c3d5bf69b","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:3792877186b9adadce0a8d72b316bf9b93b8a97cc6b72c3b5176e7c302f82798","observation_id":"e5c40ca0-d9c6-4f0a-ac02-3ee9aa8717d2","resolution":{"observed_at":"2026-05-11T14:36:04.117385Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1742-6596/883/1/012011","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Robin Gravity","venue":null,"work_id":"c9d46230-fe04-471c-aa50-2c022ca0715e","year":2017},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:df01818876b334c1dae8127df2df3ce149d9a1152c53f435ac3416dbea05c89f","observation_id":"9fd5bed9-abfa-47e0-90e4-7de1b9e69393","resolution":{"observed_at":"2026-05-09T21:38:30.383346Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/j.physrep.2023.06.002","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Review of the no-boundary wave function","venue":null,"work_id":"19ebac8a-7385-46e6-ad02-fbfe6eb16ef0","year":2023},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:5b4c5a7e99c78fb7f1f4f5304c0b258250ee57618fb6244282f9546374df04ff","observation_id":"6f3bb3c8-0e2b-4b39-8404-87d758494258","resolution":{"observed_at":"2026-05-09T21:38:30.385739Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.98.103506","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Unstable no-boundary fluctuations from sums over reg- ular metrics","venue":null,"work_id":"237ab598-7230-4b45-8043-8e8348781176","year":2018},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:5201b8cd4e38f276b70700dcfcd5353f0a8d028f561173bce62c869b3e463e1d","observation_id":"5334bd20-e6d0-4689-94e3-1e1f59a7e576","resolution":{"observed_at":"2026-05-09T21:38:30.402493Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevlett.119.171301","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"No smooth beginning for spacetime","venue":null,"work_id":"8ca84667-7f4b-4af7-82f6-70c4f8e62077","year":2017},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:9de1ef231528a4cc296787c767d9ad729646c6abd97fb49fdcb7ecfb1c7cbbfb","observation_id":"de6224ac-aaee-401a-a212-b3aa419ada06","resolution":{"observed_at":"2026-05-09T21:38:30.446195Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.100.123543","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"No-boundary prescriptions in Lorentzian quan- tum cosmology","venue":null,"work_id":"122bf108-342b-44c5-8b20-dd4e5d30b9a6","year":2019},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:ad207a5d9217bf271297babfb830ab9d4ec9600c1732e3f8bf32c4af207e5192","observation_id":"2f48b6ee-8baa-4000-9bb4-188d28d45a13","resolution":{"observed_at":"2026-05-09T21:38:30.378529Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevlett.122.201302","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"No-Boundary Proposal as a Path Integral with Robin Boundary Conditions","venue":null,"work_id":"26af2eac-ba9c-4f12-8edd-1036c7867f4e","year":2019},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:7be467dbf08467d63a6d7961e6ef08757662720f3bc4b19a7cc036a5e7daf53e","observation_id":"3c81814f-62e1-4302-be20-e33fd4fd2575","resolution":{"observed_at":"2026-05-09T21:38:30.380994Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0003-4916(92)90347-o","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"One loop quantum cosmology: Zeta function technique for the Hartle-Hawking wave function of the universe","venue":null,"work_id":"72762714-effc-42a4-9ede-5046d8f6f173","year":1992},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:a4ef35f4f3a53991c357b32d16139339ef14a174a5f5b9389b22346455e33138","observation_id":"26b18e07-879e-4022-9919-93da5d626c85","resolution":{"observed_at":"2026-05-09T21:38:30.443966Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/jhep09(2011)045","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"On graviton non-Gaussianities during inflation","venue":null,"work_id":"ba01da1c-352b-456c-873f-712bb98c4f03","year":2011},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:b3720233ee1915d3eeeae0f2158e4f530413c6bc4ac8a7ec2be3372ca9d798e4","observation_id":"5dea9482-d8f2-4e5d-bc0f-5fb733eab1f4","resolution":{"observed_at":"2026-05-09T21:38:30.428899Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1126-6708/2003/05/013","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-27T14:20:58.843983Z","title":"2003 , bdsk-url-1 =","venue":null,"work_id":"174894a5-9af2-4a70-836b-964bc52483de","year":2003},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:ef58092163a19ef8a0264897a570905fd5daad56734dd48b2847e1a9c195943e","observation_id":"c169e424-2ca8-48af-90c8-8506b6f01752","resolution":{"observed_at":"2026-05-09T21:38:30.441520Z","resolver_source":"doi","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-05-20T15:24:15.564946+00:00","source":"crossref_status_cache"},{"observed_at":"2026-05-20T15:24:15.564946+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1475-7516/2011/01/023","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Semiclassical relations and IR effects in de Sitter and slow- roll space-times","venue":null,"work_id":"d18e1d14-cb4c-47a3-925c-066b4b06d916","year":2011},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:d8f43365932652cb7a2b3a120c8e889d48bea1ba6b9cf13269b12c91ef67cb8d","observation_id":"ccebc45d-bb18-4e54-af3c-3bfd49bc4f59","resolution":{"observed_at":"2026-05-09T21:38:30.407244Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-05-20T15:24:05.932073+00:00","source":"crossref_status_cache"},{"observed_at":"2026-05-20T15:24:05.932073+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.84.063528","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Cosmological observables, IR growth of fluc- tuations, and scale-dependent anisotropies","venue":null,"work_id":"9f2febcd-f2c7-48c8-81ba-ebe0078c6496","year":2011},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:998866d52beefbfda7b718ea6f0c8cf4cdd2ea42d4df84cba5a58182088ec670","observation_id":"86191b13-c26c-4741-b948-6b20ae9598f3","resolution":{"observed_at":"2026-05-09T21:38:30.412403Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-05-20T15:24:06.417108+00:00","source":"crossref_status_cache"},{"observed_at":"2026-05-20T15:24:06.417108+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/jhep01(2024)124","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Lorentzian Robin Universe","venue":null,"work_id":"7b318f0b-a285-413f-8cde-42cc755c0de4","year":2024},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:3d033f4933d4f8705ad13d7ff88c6ebea8ea6103cefad100e553721aedfdc358","observation_id":"edef20f0-fc07-4e10-b772-7777616b7981","resolution":{"observed_at":"2026-05-09T21:38:30.327710Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/s10714-025-03369-2","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Lorentzian Robin Universe of Gauss-Bonnet Gravity","venue":null,"work_id":"c4d9f2fa-a9b7-4005-a344-b2cea214f9e0","year":2025},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:1653024adff60ac5df62b9a494eb4f617f26c5b46df05d2775d62d891585f82e","observation_id":"84748e6a-fa12-4f75-a35f-2bb03e06094c","resolution":{"observed_at":"2026-05-09T21:38:30.306570Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/ytxr-4x1d","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Boundary choices and one-loop complex gravi- tational path integral","venue":null,"work_id":"0daae691-38ee-4d53-9bb9-4c52c7678c02","year":2025},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:ab61d2d1102b1f2f00089d57f071e2f719170e54f5540f8522309d4b66e95d07","observation_id":"8c5f20b6-4991-4890-81ca-dd51ba7f53be","resolution":{"observed_at":"2026-05-09T21:38:30.297397Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.110.023503","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"No smooth spacetime: Exploring primordial perturbations in Lorentzian quan- tum cosmology","venue":null,"work_id":"b5852509-b00f-43a5-84c9-13a3f3214ca0","year":2024},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:82ceaf675340ccb16ee7f7b0aaead6fa375d2b4d51a1e036384f76a39e675e30","observation_id":"b6d154ab-317d-4fef-8f98-c475b4346ed9","resolution":{"observed_at":"2026-05-09T21:38:30.348932Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/jhep04(2022)153","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Surprises in Lorentzian path-integral of Gauss-Bonnet gravity","venue":null,"work_id":"6373d884-ee39-4d57-bd19-e6d613fcbefb","year":2022},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:0a2daa0c2ee0dd4eede3b70bd3e091d0129ae6929108e59a11fa9e08a28c38e6","observation_id":"89fde12e-ce41-4c26-a8cb-6450b89d3c67","resolution":{"observed_at":"2026-05-09T21:38:30.366134Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/jhep05(2021)273","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"On Gauss-bonnet gravity and boundary conditions in Lorentzian path integral quantization","venue":null,"work_id":"cf617fa8-e288-4794-a18f-35f55ca89907","year":2021},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:3bf7dd922b22cae6052938f7675f3225d777458a088dba85f895b58eeac67e1d","observation_id":"9bebbaa3-ad55-4f47-8a44-b34244a3439d","resolution":{"observed_at":"2026-05-09T21:38:30.292629Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2507.10537","last_updated":"2026-04-13T06:30:35Z","snapshot_observed_at":"2026-07-06T21:57:03.414218Z","submitted_at":"2025-07-14T17:57:09Z","title":"Resolving Degeneracies in Complex $\\mathbb{R}\\times S^3$ and $\\theta$-KSW","version":2},"cited_work":{"arxiv_id":"2507.10537","doi":"10.1007/jhep02(2026)249","metadata_source":"pith","pith_arxiv_id":"2507.10537","snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Resolving Degeneracies in Complex $\\mathbb{R}\\times S^3$ and $\\theta$-KSW","venue":"hep-th","work_id":"2ba3d66c-e23d-4624-a285-f803739d8ddd","year":2025},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-07-11T11:50:26.030339Z"},"links":{"cited_paper":"/paper/2507.10537","citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:7d4a793f859fb94f344fb68a7c1c31441fde05bde00d4540ff703fe3cc3aaad2","observation_id":"c7e5edab-99e8-4c71-a211-39c9bd5b996a","resolution":{"observed_at":"2026-05-09T21:38:30.336689Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/z59k-v3l8","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"New regularization scheme for the wave function of the Universe in the Lorentzian path integral","venue":null,"work_id":"4a9ecfd5-9001-4a04-b5af-8c5c8ab559f0","year":2026},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:94061b788c34dcb10b5cada5a1102aedab73f4e0236f479678b619b2b0d95bc2","observation_id":"17779126-613b-4936-8876-e3c9e46812c3","resolution":{"observed_at":"2026-05-09T21:38:30.294977Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/j.aop.2014.09.003","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Real-time Feynman path integral with Picard–Lefschetz theory and its applications to quantum tunneling","venue":null,"work_id":"65a16924-0e12-412d-be1a-6356696d6d31","year":2014},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:9846e29cad10c2ad8f843121f90c25b03c00ae1bb4bad5cea1497cb294c1fd0c","observation_id":"0aa0016f-42ff-464d-9cf7-0a66d8d8506d","resolution":{"observed_at":"2026-05-09T21:38:30.314787Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1093/qmath/haab027","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-26T03:08:55.735491Z","title":"doi: 10.1093/qmath/haab027 arXiv: 2105.10161 [hep-th] 13, 18 References156","venue":null,"work_id":"d521d1d5-a1f8-4e1a-a528-5ae3c54bd037","year":2021},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:a6c4fc7c49944bf0dc5988b3e4af9f39de50f50f0cdf4900476af030f119c520","observation_id":"71f98831-79db-41c9-b56d-5bd19d3b1532","resolution":{"observed_at":"2026-05-09T21:38:30.341580Z","resolver_source":"doi","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2111.06514","last_updated":"2022-02-11T14:11:38Z","snapshot_observed_at":"2026-07-06T12:07:45.652474Z","submitted_at":"2021-11-12T00:54:56Z","title":"A Note On Complex Spacetime Metrics","version":2},"cited_work":{"arxiv_id":"2111.06514","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2111.06514","snapshot_observed_at":"2026-07-04T14:39:57.901487Z","title":"Witten,A Note On Complex Spacetime Metrics","venue":null,"work_id":"cf411d64-f024-4290-b41e-7721e3161467","year":2021},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"cited_paper":"/paper/2111.06514","citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:635418efe1e2c96e9a8aaa7b0e241e77fc950deb59ff21b2f07024ac8dbaaf68","observation_id":"bfafadf8-3507-42b4-8c28-453c74ad83cb","resolution":{"observed_at":"2026-05-11T14:36:04.183667Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/jhep08(2022)284","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Uses of complex metrics in cosmology","venue":null,"work_id":"b7f2e55a-99da-434b-b664-fa354b0583b6","year":2022},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:afabcfd759737876c6db5e12e688e3c6935c0511977cb11ebe42beb8a734a846","observation_id":"9dfc94d5-3b75-473e-956f-c97f1b9fa34a","resolution":{"observed_at":"2026-05-09T21:38:30.358923Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevlett.131.191501","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Kontsevich-Segal Criterion in the No- Boundary State Constrains Inflation","venue":null,"work_id":"267ffb92-dd27-4e4d-8554-df653d1e3842","year":2023},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:910fb4a5f6f9d1f4ed5a708c73e81d124372978b43e938dbe87b0eac1afabf71","observation_id":"3970051b-5a25-443b-8ba5-e8c5a7d611e9","resolution":{"observed_at":"2026-05-09T21:38:30.339204Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.105.026022","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Allowable complex metrics in minisuperspace quantum cosmology","venue":null,"work_id":"0ef24702-1368-4109-a667-6995bbdd00b4","year":2022},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:b0de6edd95f923a079fc8517ab8e3f41a3c6e963a8ddaf46dbc914e1a953986e","observation_id":"1597812b-8a8d-451a-a246-65429b1df3a0","resolution":{"observed_at":"2026-05-09T21:38:30.332617Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2603.23457","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Note on KSW-allowability of Wine-Glass Geometry","venue":null,"work_id":"1bec2605-3d84-4897-938c-a6d20c8d48d0","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:d213f1776170b76ca4a8321ba1ebe338fcef6fb577f6731367a077460ce4e5f4","observation_id":"a2ffa4b7-b5ea-41e9-a9e7-7c502dfa4450","resolution":{"observed_at":"2026-05-11T14:36:04.197092Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0550-3213(81)90371-0","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T09:11:48.769187Z","title":"The Background Field Method Beyond One Loop","venue":null,"work_id":"2efb86a4-c5cf-4568-8cf9-2da1b4e7e20b","year":1981},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:92a101dbdbcde0baf35432aa733d446c6f47faf8be882d2fe751d6bd8fea148c","observation_id":"459592d2-f503-4aa4-9cdc-049ba807eb41","resolution":{"observed_at":"2026-05-09T21:38:30.299708Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"A GAUGE INVARIANT EFFECTIVE ACTION","venue":null,"work_id":"9f62e9ea-8395-4530-8f39-67ead9fbde07","year":2024},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:9a4a11dfab7fc2e8bc74b4c95bf38d0f7d5f776ecb2739c70e9ef1659f67de9c","observation_id":"aac6656e-c4e1-4577-a39d-066e83047da9","resolution":{"observed_at":"2026-05-23T15:48:08.777928Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.18.1773","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Homogeneous Collapsing Star: Tensor and Vec- 56 tor Harmonics for Matter and Field Asymmetries","venue":null,"work_id":"bb9d7cc5-8eb2-473e-b5bc-6cbe13afbeac","year":1978},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:80afd56557a264fec2308254df01efc19353f1a7a4427b0eb0aea540c44e227e","observation_id":"29fe1d88-9f08-48bd-8e5d-73bc1fc7a327","resolution":{"observed_at":"2026-05-09T21:38:30.290401Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1063/1.527513","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Symmetric Tensor Spherical Harmonics on theNSphere and Their Application to the De Sitter Group SO(N,1)","venue":null,"work_id":"34f8fec6-fcbc-48d6-83d1-b57048cad117","year":1987},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:b52117cf1e9817ada8a377c68abb21b6a7107a9bb7e4766dddc66e8fc3f2c7d8","observation_id":"33e5d8f8-3284-4b03-8e09-003f329f44bf","resolution":{"observed_at":"2026-05-09T21:38:30.287822Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[{"edge_observation":{"observed_at":"2026-07-11T04:03:03.851137+00:00","source":"paper_reference_links","state":"open"},"event_date":"2002-12-02","event_type":"correction","notice_doi":"10.1063/1.1515382","provenance":{"observed_at":"2026-07-11T03:04:18.595476+00:00","source":"crossref","source_record_id":"10.1063/1.1515382->10.1063/1.527513:correction"}}],"reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1007/bf01626516","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T09:11:48.715993Z","title":"Zeta Function Regularization of Path Integrals in Curved Space-Time","venue":null,"work_id":"6d15c091-12dc-44e7-a56b-c6692bf2722d","year":1977},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:299d9db39f1939d8de9f3b311065ead598f8d5b88ad274075dc3a8803e45eb8e","observation_id":"7cee7384-ea53-4f56-ac99-9c38dbe3a036","resolution":{"observed_at":"2026-05-09T21:38:30.346443Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1142/2065","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Elizalde, S","venue":null,"work_id":"0131939e-4c96-424b-ad52-70b86af0234b","year":1994},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:444fcc2f263e376bb79aca99cdbdb054909eb6e9b116597a2ab0b58d3ac8dcb2","observation_id":"566a93cd-4347-425f-8c71-c0698176153d","resolution":{"observed_at":"2026-05-09T21:38:30.361429Z","resolver_source":"doi","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.94.085013","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Partition function on spheres: How to use zeta function regularization","venue":null,"work_id":"b38345a3-9fc7-4cc7-ad23-95a7b766ddae","year":2016},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:ef810469210ea9debe920a4abfae46c1e4049cc2c2ebc4bfe047c8ed3b7eaf34","observation_id":"40ca1b2d-2d29-45bb-a47d-1a75f6fbbdae","resolution":{"observed_at":"2026-05-09T21:38:30.368532Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/j.physrep.2003.09.002","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-28T11:42:04.737251Z","title":"Heat Kernel Expansion: User’s Manual","venue":null,"work_id":"dc93a6f6-9f39-45b4-82a6-32981c4b7b19","year":2003},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:e7901776fc571a5b0308ca840a91de0388b07bf61cb0db81eb1d8539c405212f","observation_id":"c87abdee-938f-4500-b7e4-9358d190a1f2","resolution":{"observed_at":"2026-05-09T21:38:30.363770Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-05-23T17:24:01.50283+00:00","source":"crossref_status_cache"},{"observed_at":"2026-05-23T17:24:01.50283+00:00","source":"openalex_status_cache"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.88.085009","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Perturbative nonequilibrium thermal field theory","venue":null,"work_id":"8b42ff21-2964-4e39-9615-ea1f1074df8b","year":2013},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:d4bc1151638c353bb3564a8f6b5aa8c41e4222ac1dea9896d73dfbfdf6cf0878","observation_id":"c378b0e3-81e6-4a6c-b0b9-e88c4271971d","resolution":{"observed_at":"2026-05-09T21:38:30.317338Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.59.125012","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Two mechanisms for elimination of pinch singularities in / out of equilibrium thermal field theories","venue":null,"work_id":"f81e77bc-9dbe-4b97-a48a-282a0ae7a3ac","year":1999},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:9ae58dd473e6102e68c30351b3908a0878245bcd02a828053270dcb34ecbec0d","observation_id":"91b67199-6c6c-4251-b6b1-f3524dafe7dd","resolution":{"observed_at":"2026-05-09T21:38:30.356370Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1063/1.1703636","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Integration in functional spaces and it applications in quantum physics","venue":null,"work_id":"40a5c487-c2b7-4bd2-9901-fd0dbde8b681","year":1960},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:f0d2cb549a3f15db562bf595e4b05e5f5daed6d656e295c51166bb22936f2caf","observation_id":"295b5159-37b4-4927-a81b-4f570a6c65ad","resolution":{"observed_at":"2026-05-09T21:38:30.308893Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/1751-8113/41/30/304006","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"536b8701-ae6d-4aee-a147-f73326163c59","year":2008},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:261a284e22f856e780e5c5b526ca8207efa20c3559e12acbc3d6cba2001111a2","observation_id":"3a613519-ebfd-43d5-830a-c46772a88c68","resolution":{"observed_at":"2026-05-09T21:38:30.351291Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1088/0305-4470/37/16/014","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Functional determinants for general Sturm-Liouville prob- lems","venue":null,"work_id":"9a70b158-a7b9-4792-81cd-0e76054d7067","year":2004},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:d2f94ed0681349afc72f9218fb77b96c3e2966d1c088f88562628471af7584a9","observation_id":"cde4bc02-b9c3-4e1a-ab3c-23b450044128","resolution":{"observed_at":"2026-05-09T21:38:30.344046Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/s0003-4916(03)00149-0","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Functional determinants by contour integration methods","venue":null,"work_id":"765a0791-2ed1-42b2-9c8c-c98e88a4de4e","year":2003},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:f2a4bf4707e56f87e7a630d595fb5a0496a32401b8f4ef9234a01ad1b0320372","observation_id":"c8a36e0e-5fd6-44c0-9b52-9940d02d77b3","resolution":{"observed_at":"2026-05-09T21:38:30.319824Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Abramowitz and I","venue":null,"work_id":"3a95a270-50be-454f-afc0-3a4efb170a4d","year":1965},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:92d4c2416c756f0e5c9817fb6503975ee55396118d222cbb5ab86ebdd054460f","observation_id":"0921aa00-30bb-44f6-86eb-a26b93934698","resolution":{"observed_at":"2026-05-23T15:48:08.745228Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"57b77564-a1ee-45a9-b728-11118e7ddc48","year":2025},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:524bf42820411bec1fb4e44d55e5c2a6b6a502b6bf049b4583bd16ed9232f3e8","observation_id":"07f45a62-3746-48b9-a24e-4609aea89923","resolution":{"observed_at":"2026-05-23T15:48:08.764918Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2512.21549","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Functional Determinants for Constrained Path Integrals in Minisuperspace Jackiw-Teitelboim Gravity","venue":null,"work_id":"528d42b6-a024-46f2-8fe7-c8309fae6085","year":null},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:4ea881368cad26cd31594a824da1dc78d26dbd7dfaec03fefb0baf628f170615","observation_id":"fa1f31d9-1d81-474a-b385-b29d5676490a","resolution":{"observed_at":"2026-05-11T14:36:04.010807Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2026.140198","doi":"10.1016/j.physletb.2026.140198","metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-11T11:50:26.030339Z","title":"Stable evaluation of Lefschetz thimble intersection numbers:Towards real-time path integrals","venue":null,"work_id":"84660191-032f-4b4d-9694-d33237b3c1a6","year":2026},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:da5e3ed3f748c90b16ede8ded83573c3692b63202a4a2b49a8fe1258c90771be","observation_id":"b6aa93ce-9f85-4afd-8527-380533f42aef","resolution":{"observed_at":"2026-05-09T21:38:30.312216Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevlett.28.1082","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-03T08:37:45.875044Z","title":"Role of conformal three geometry in the dynamics of gravitation","venue":null,"work_id":"7090d85e-641e-4e51-8019-c44889c953ac","year":1972},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:d2d95265c6c42cee169449bec67fbdd799a434177abf58af969ad7ba78ab6fb3","observation_id":"8cf1cda2-4aed-499c-ae20-ace0fd7ae7cb","resolution":{"observed_at":"2026-05-09T21:38:30.285151Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2512.10930","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-07-04T11:19:48.953083Z","title":"Galante, R.C","venue":null,"work_id":"16959e39-b562-4944-97b3-c8e1783a1144","year":2025},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:b4799bbb66841819e2c65bf80ba58f6bef99684f7b0e495d7e46f4fb426d3e2c","observation_id":"25f55a97-262c-4937-9a1e-64d73aa99349","resolution":{"observed_at":"2026-05-11T14:36:04.049831Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/nwpg-5mld","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Quantum properties of non-Dirichlet boundary conditions in gravity","venue":null,"work_id":"8a343140-308c-4845-8074-37278c1ccece","year":2026},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:140e31c974464fba9856a7ce4ed7f25d35b4156beba894e04ec43608bb8bb96f","observation_id":"cb02621e-e0a9-4622-ad67-f04edc0b4106","resolution":{"observed_at":"2026-05-09T21:38:30.353755Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.2307/2008099","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":null,"venue":null,"work_id":"42bbb489-2275-499c-a037-0f22dfc58381","year":1986},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:b232e02430ffd41175b96fd3a999fe60fc37b83ba681175092456f4a2288207a","observation_id":"a277f997-e35b-4919-b415-d56e4374635c","resolution":{"observed_at":"2026-05-09T21:38:30.304239Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1142/s0218271814300018","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Lecture notes on interacting quantum fields in de Sitter space","venue":null,"work_id":"de9f3340-ee11-4348-80f8-5d18fb2949a3","year":2014},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:66c0cb003018a2847708ed69a5773ccce8e052e8f52f1bb464adf4304d77cafb","observation_id":"02bd5697-0340-4d8b-b7f9-735a3869aa3f","resolution":{"observed_at":"2026-05-09T21:38:30.322532Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1103/physrevd.99.086009","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Characters of different secular ef- fects in various patches of de Sitter space","venue":null,"work_id":"41445045-7fb1-4c52-a00d-7bd14c6c3f4f","year":2019},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:62b20553e4f27d0bc999956c58e96f726bc81fd28a7420faf1c261ef1901472a","observation_id":"47bd9b29-8272-4ffb-929b-90232bf7b540","resolution":{"observed_at":"2026-05-09T21:38:30.330202Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.11106","last_updated":"2024-11-17T15:50:28Z","snapshot_observed_at":"2026-07-06T19:51:37.262377Z","submitted_at":"2024-11-17T15:50:28Z","title":"Light fields in various patches of de Sitter space-time","version":1},"cited_work":{"arxiv_id":"2411.11106","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2411.11106","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Light fields in various patches of de Sitter space-time","venue":null,"work_id":"04b5fcfc-ff56-4e10-bbcc-602e25c3c07e","year":2025},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"cited_paper":"/paper/2411.11106","citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:eb17f8d84dd0af94a4633c31c4d3e70752eb36400c09dd1ab02d7de8e7efbed6","observation_id":"01e3af46-858b-412b-931f-04d8cf2ea6cb","resolution":{"observed_at":"2026-05-11T14:36:04.141358Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0370-2693(88)91373-1","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Gravitational Instantons and Creation of Expanding Universes","venue":null,"work_id":"d3f3caee-2e99-464f-8688-418321cb47e6","year":1988},"citing_paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-05-09T21:35:15.689585Z"},"links":{"citing_paper":"/paper/2604.21736"},"observation_digest":"sha256:9285464ae1249e1e0883f4eae01e18e899b4cd98bea8da2c24d8d1a5fb60fff5","observation_id":"17fd992c-8fb5-4ba6-b671-3ac2d0af2d80","resolution":{"observed_at":"2026-05-09T21:38:30.301941Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-03T06:30:56.289259+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2604.21736","last_updated":"2026-04-23T14:40:02Z","latest_version":1,"primary_category":"hep-th","snapshot_observed_at":"2026-07-06T23:08:14.631453Z","submitted_at":"2026-04-23T14:40:02Z","title":"IR behaviour of one-loop complex $\\mathbb{R}\\times S^3$ saddles"},"reference_resolution":{"displayed":90,"state_counts":{"malformed_identifier":4,"metadata_mismatch":5,"parse_uncertain":0,"unresolved":2,"verified_exact":67,"verified_fuzzy":12},"total_outbound_references":90},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-03T06:30:56.289259+00:00","source":"crossref"},{"observed_at":"2026-08-03T06:30:50.922721+00:00","source":"retraction_watch"}],"thesis":"As of 3 August 2026, this Paper Citation Record lists 90 of 90 outbound references and 1 inbound Pith citation observation for arXiv:2604.21736."}