{"as_of":"2026-08-08T17:13:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:83db5e61567b73384b29dfd320a207544be9f556a9929d1fac0e334c0af27261","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":5,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":5,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-08T06:32:00.761636+00:00","state":"measured"},{"denominator":5,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":5,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-07T13:11:47.762979Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-02T04:16:36.150164Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"1609.01253","last_updated":"2020-11-18T07:46:25Z","snapshot_observed_at":"2026-07-06T05:09:28.383987Z","submitted_at":"2016-09-05T18:54:09Z","title":"Fully stable cosmological solutions with a non-singular classical bounce","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.01253","snapshot_observed_at":"2026-08-07T13:11:47.762979Z","title":"Ijjas and P","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.22763","last_updated":"2025-07-23T14:17:25Z","snapshot_observed_at":"2026-08-08T13:28:31.687487Z","submitted_at":"2025-05-28T18:27:39Z","title":"Probability of the Initial Conditions for Inflation and Slow Contraction","version":3},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-07T13:11:47.762979Z"},"links":{"cited_paper":"/paper/1609.01253","citing_paper":"/paper/2505.22763"},"observation_digest":"sha256:47ae2a7a0783a482ca82f4f6df8622af1cc857a1876c057fd8fd4f09d0bdde6f","observation_id":"3c923b30-5946-409c-89c6-7ecaf65da450","resolution":{"observed_at":"2026-08-07T13:11:47.762979Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.01253","last_updated":"2020-11-18T07:46:25Z","snapshot_observed_at":"2026-07-06T05:09:28.383987Z","submitted_at":"2016-09-05T18:54:09Z","title":"Fully stable cosmological solutions with a non-singular classical bounce","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.01253","snapshot_observed_at":"2026-08-02T22:42:41.930943Z","title":"Fully stable cosmological solutions with a non-singular classical bounce,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2602.16292","last_updated":"2026-07-02T07:44:17Z","snapshot_observed_at":"2026-08-03T21:25:59.220004Z","submitted_at":"2026-02-18T09:20:24Z","title":"Gravitational Waves from Primordial Black Holes formed by Null Energy Condition Violation during Inflation","version":2},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-02T22:42:41.930943Z"},"links":{"cited_paper":"/paper/1609.01253","citing_paper":"/paper/2602.16292"},"observation_digest":"sha256:7885c2bf9cdd1172a5bcddf91a22ea7a17495a98f5a55c4c1bd3f7fa34c186d1","observation_id":"b91c272e-8e18-4abd-9f8c-64881f72b980","resolution":{"observed_at":"2026-08-02T22:42:41.930943Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1609.01253","last_updated":"2020-11-18T07:46:25Z","snapshot_observed_at":"2026-07-06T05:09:28.383987Z","submitted_at":"2016-09-05T18:54:09Z","title":"Fully stable cosmological solutions with a non-singular classical bounce","version":5},"cited_work":{"arxiv_id":"1609.01253","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1609.01253","snapshot_observed_at":"2026-07-02T04:16:36.150164Z","title":"Ijjas and P","venue":null,"work_id":"6a06a979-b7d1-43b1-9ca3-4fa909f9b0f1","year":2017},"citing_paper":{"arxiv_id":"2603.23564","last_updated":"2026-03-24T07:53:46Z","snapshot_observed_at":"2026-07-06T22:50:23.931381Z","submitted_at":"2026-03-24T07:53:46Z","title":"Energy conditions of bouncing solutions in quadratic curvature gravity coupled with a scalar field","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-05-15T01:15:13.552208Z"},"links":{"cited_paper":"/paper/1609.01253","citing_paper":"/paper/2603.23564"},"observation_digest":"sha256:b00f26b105b6c3d40276b8be0d8b2d913d3beec03787dc1927d8642faac0a4af","observation_id":"d5fc653d-1892-45fb-a62b-215a3f8d156c","resolution":{"observed_at":"2026-05-15T01:18:26.744413Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1609.01253","last_updated":"2020-11-18T07:46:25Z","snapshot_observed_at":"2026-07-06T05:09:28.383987Z","submitted_at":"2016-09-05T18:54:09Z","title":"Fully stable cosmological solutions with a non-singular classical bounce","version":5},"cited_work":{"arxiv_id":"1609.01253","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1609.01253","snapshot_observed_at":"2026-07-02T04:16:36.150164Z","title":"Ijjas and P","venue":null,"work_id":"6a06a979-b7d1-43b1-9ca3-4fa909f9b0f1","year":2017},"citing_paper":{"arxiv_id":"2604.27103","last_updated":"2026-06-04T18:02:39Z","snapshot_observed_at":"2026-07-06T23:12:38.453388Z","submitted_at":"2026-04-29T18:47:37Z","title":"Geodesically Complete Curvature-Bounce Inflation","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-05-07T08:50:31.703521Z"},"links":{"cited_paper":"/paper/1609.01253","citing_paper":"/paper/2604.27103"},"observation_digest":"sha256:0eec0f9a9f6fec38be8c7c1d1d9a3b257e4bed83ee33befbf6c1f67c775e6f4a","observation_id":"f0ad608d-c895-4ef9-a8e6-3816919f8598","resolution":{"observed_at":"2026-05-12T09:56:26.770938Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1609.01253","last_updated":"2020-11-18T07:46:25Z","snapshot_observed_at":"2026-07-06T05:09:28.383987Z","submitted_at":"2016-09-05T18:54:09Z","title":"Fully stable cosmological solutions with a non-singular classical bounce","version":5},"cited_work":{"arxiv_id":"1609.01253","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"1609.01253","snapshot_observed_at":"2026-07-02T04:16:36.150164Z","title":"Ijjas and P","venue":null,"work_id":"6a06a979-b7d1-43b1-9ca3-4fa909f9b0f1","year":2017},"citing_paper":{"arxiv_id":"2606.03302","last_updated":"2026-06-02T08:15:32Z","snapshot_observed_at":"2026-08-01T13:41:06.245621Z","submitted_at":"2026-06-02T08:15:32Z","title":"Non-Gaussianity and Strong-Coupling Problem in a Two-Field DHOST Bouncing Model","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-06-28T09:14:24.999785Z"},"links":{"cited_paper":"/paper/1609.01253","citing_paper":"/paper/2606.03302"},"observation_digest":"sha256:795f5cba2aea8e8d58bccc7c7b6d1b6c092a89bd0bed9718657807f67dcab7e6","observation_id":"a7890e7e-f750-4e78-b31a-9e6a90ca39ce","resolution":{"observed_at":"2026-07-02T04:16:36.152273Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-08T06:32:00.761636+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"state":"measured"}}],"links":{"evidence":"/evidence","html":"/paper/1609.01253/citation-record","integrity":"/paper/1609.01253/integrity","json":"/paper/1609.01253/citation-record.json","paper":"/paper/1609.01253"},"outbound":[],"paper":{"arxiv_id":"1609.01253","last_updated":"2020-11-18T07:46:25Z","latest_version":5,"primary_category":"gr-qc","snapshot_observed_at":"2026-07-06T05:09:28.383987Z","submitted_at":"2016-09-05T18:54:09Z","title":"Fully stable cosmological solutions with a non-singular classical bounce"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"thesis":"As of 8 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 5 inbound Pith citation observations for arXiv:1609.01253."}