{"as_of":"2026-08-14T12:37:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:1dc047b302b5eb0042d69e77114933ec45d6482c4b76230a0620e75b98b2070d","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":"2026-08-14T06:32:32.682623+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":"2026-08-12T19:22:55.720488Z","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":"2026-07-01T11:05:42.552682Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2201.02630","last_updated":"2022-01-07T19:00:00Z","snapshot_observed_at":"2026-08-13T17:02:47.859606Z","submitted_at":"2022-01-07T19:00:00Z","title":"The low-end of the black hole mass function at cosmic dawn","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.02630","snapshot_observed_at":"2026-08-12T19:22:55.720488Z","title":"The low-end of the black hole mass function at cosmic dawn,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2411.10847","last_updated":"2025-01-04T17:23:02Z","snapshot_observed_at":"2026-08-13T11:02:43.035842Z","submitted_at":"2024-11-16T17:42:52Z","title":"Black Holes and Baryon Number Violation: Unveiling the Origins of Early Galaxies and the Low-Mass Gap","version":2},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-12T19:22:55.720488Z"},"links":{"cited_paper":"/paper/2201.02630","citing_paper":"/paper/2411.10847"},"observation_digest":"sha256:a26e3a95eae3bacbe41c5772df68ddfa62e8ee48f7a886c88e19b7e69cb2f40d","observation_id":"c6eea7ee-dfb7-4192-aa3d-5ef3d430586d","resolution":{"observed_at":"2026-08-12T19:22:55.720488Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.02630","last_updated":"2022-01-07T19:00:00Z","snapshot_observed_at":"2026-08-13T17:02:47.859606Z","submitted_at":"2022-01-07T19:00:00Z","title":"The low-end of the black hole mass function at cosmic dawn","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.02630","snapshot_observed_at":"2026-08-11T21:08:52.499762Z","title":"The low-end of the black hole mass function at cosmic dawn","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.04983","last_updated":"2024-12-06T12:07:44Z","snapshot_observed_at":"2026-08-14T07:19:12.269532Z","submitted_at":"2024-12-06T12:07:44Z","title":"Red, hot, and very metal poor: extreme properties of a massive accreting black hole in the first 500 Myr","version":1},"reference_index":168,"source":"pdf_text","source_observed_at":"2026-08-11T21:08:52.499762Z"},"links":{"cited_paper":"/paper/2201.02630","citing_paper":"/paper/2412.04983"},"observation_digest":"sha256:8531d2a1597cbd53d18341c9d30efa9a10b0ac4e29e2a173b9527862d97081e1","observation_id":"78d488b0-ee1b-4fb4-ba69-fcbdd203893c","resolution":{"observed_at":"2026-08-11T21:08:52.499762Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.02630","last_updated":"2022-01-07T19:00:00Z","snapshot_observed_at":"2026-08-13T17:02:47.859606Z","submitted_at":"2022-01-07T19:00:00Z","title":"The low-end of the black hole mass function at cosmic dawn","version":1},"cited_work":{"arxiv_id":"2201.02630","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2201.02630","snapshot_observed_at":"2026-07-01T11:05:42.552682Z","title":"The low-end of the black hole mass function at cosmic dawn","venue":null,"work_id":"19ac4966-47b3-44e4-9f25-11f7f45803b6","year":2022},"citing_paper":{"arxiv_id":"2509.25325","last_updated":"2026-04-14T18:06:24Z","snapshot_observed_at":"2026-07-06T22:31:10.099674Z","submitted_at":"2025-09-29T18:00:03Z","title":"Direct Collapse Black Hole Candidates from Decaying Dark Matter","version":3},"reference_index":130,"source":"pdf_text","source_observed_at":"2026-05-18T12:06:32.865011Z"},"links":{"cited_paper":"/paper/2201.02630","citing_paper":"/paper/2509.25325"},"observation_digest":"sha256:86e507861bb37cf4b405b4e12a0311d5994c979e4d14e0e638a8361df890ba82","observation_id":"cab1d4cd-4016-44d3-89b1-9dd586a5d761","resolution":{"observed_at":"2026-05-18T12:11:22.448170Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2201.02630","last_updated":"2022-01-07T19:00:00Z","snapshot_observed_at":"2026-08-13T17:02:47.859606Z","submitted_at":"2022-01-07T19:00:00Z","title":"The low-end of the black hole mass function at cosmic dawn","version":1},"cited_work":{"arxiv_id":"2201.02630","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2201.02630","snapshot_observed_at":"2026-07-01T11:05:42.552682Z","title":"The low-end of the black hole mass function at cosmic dawn","venue":null,"work_id":"19ac4966-47b3-44e4-9f25-11f7f45803b6","year":2022},"citing_paper":{"arxiv_id":"2606.31436","last_updated":"2026-06-30T10:08:58Z","snapshot_observed_at":"2026-08-04T03:59:39.214659Z","submitted_at":"2026-06-30T10:08:58Z","title":"Estimation of black hole spins in low-mass AGNs and comparison with other types of AGNs","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-07-01T04:44:05.059342Z"},"links":{"cited_paper":"/paper/2201.02630","citing_paper":"/paper/2606.31436"},"observation_digest":"sha256:313a3412da4040bd9a7c4506314fc3c62302f0682a25dc921e4fec76cb7321fc","observation_id":"d51adbdc-a21d-4421-b9e1-35311aa28094","resolution":{"observed_at":"2026-07-01T11:05:42.554089Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-14T06:32:32.682623+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2201.02630","last_updated":"2022-01-07T19:00:00Z","snapshot_observed_at":"2026-08-13T17:02:47.859606Z","submitted_at":"2022-01-07T19:00:00Z","title":"The low-end of the black hole mass function at cosmic dawn","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.02630","snapshot_observed_at":"2026-08-01T13:38:32.167871Z","title":", keywords =","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.19057","last_updated":"2026-07-21T12:45:36Z","snapshot_observed_at":"2026-08-14T12:22:56.355344Z","submitted_at":"2026-07-21T12:45:36Z","title":"An (in)complete NIRSpec census of Balmer absorption in Type 1 AGN -- radiation-driven outflows in little red dots, quasars and variable stars","version":1},"reference_index":115,"source":"arxiv_source","source_observed_at":"2026-08-01T13:38:32.167871Z"},"links":{"cited_paper":"/paper/2201.02630","citing_paper":"/paper/2607.19057"},"observation_digest":"sha256:f3115dbe96278c2f8f2ed45946dc5ae13c0c31d49255dceea6401815c9676f91","observation_id":"30c860f7-3fd9-4ab8-b6ac-a82a1aa693d4","resolution":{"observed_at":"2026-08-01T13:38:32.167871Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2201.02630/citation-record","integrity":"/paper/2201.02630/integrity","json":"/paper/2201.02630/citation-record.json","paper":"/paper/2201.02630"},"outbound":[],"paper":{"arxiv_id":"2201.02630","last_updated":"2022-01-07T19:00:00Z","latest_version":1,"primary_category":"astro-ph.GA","snapshot_observed_at":"2026-08-13T17:02:47.859606Z","submitted_at":"2022-01-07T19:00:00Z","title":"The low-end of the black hole mass function at cosmic dawn"},"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":"2026-08-14T06:32:32.682623+00:00","source":"crossref"},{"observed_at":"2026-08-14T06:32:18.44784+00:00","source":"retraction_watch"}],"thesis":"As of 14 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 5 inbound Pith citation observations for arXiv:2201.02630."}