{"as_of":"2026-08-10T13:22:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:88bec4c0a42c0933cad467c3fc3fd6841a2f0faf34ecbe731342c72971681279","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":9,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":9,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":9,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":9,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-07T11:35:06.310999Z","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":"2026-07-04T18:50:05.424948Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":"2401.00455","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-07-04T18:50:05.424948Z","title":"Miller, B","venue":null,"work_id":"9aa0d0d3-36f4-4d3f-a742-d6b0b8a36bbe","year":2024},"citing_paper":{"arxiv_id":"2407.00366","last_updated":"2025-12-17T10:16:02Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2024-06-29T08:31:38Z","title":"Comparison of 4.5PN and 2SF gravitational energy fluxes from quasicircular compact binaries","version":2},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-05-23T23:17:55.191990Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2407.00366"},"observation_digest":"sha256:53c4712b5f43fbe7652d0e64db48c75527a017eab44cc304af4407216d8d06aa","observation_id":"0b8edc22-332f-4344-935f-7445b157e900","resolution":{"observed_at":"2026-05-23T23:18:35.961443Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-08-07T11:35:06.310999Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2506.02189","last_updated":"2025-06-02T19:24:06Z","snapshot_observed_at":"2026-08-07T15:45:20.754859Z","submitted_at":"2025-06-02T19:24:06Z","title":"Self-force framework for merger-ringdown waveforms","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-07T11:35:06.310999Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2506.02189"},"observation_digest":"sha256:4616df65aa88365caf870fa1e2afee4d8c09a98468698832cb4017ebb53c76d6","observation_id":"61d6f429-00d6-4eb2-9097-5ca80e224cf1","resolution":{"observed_at":"2026-08-07T11:35:06.310999Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-08-06T18:34:53.225882Z","title":"Miller, B","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.08081","last_updated":"2025-07-10T18:00:03Z","snapshot_observed_at":"2026-08-07T18:16:31.003795Z","submitted_at":"2025-07-10T18:00:03Z","title":"Post-adiabatic dynamics and waveform generation in self-force theory: an invariant pseudo-Hamiltonian framework","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T18:34:53.225882Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2507.08081"},"observation_digest":"sha256:d4b92f21e9cb232cba70f298151c21b26399486d4f383fa93d3a303b2227f500","observation_id":"1fb8a708-ef93-40c8-b54c-9a55b55adf68","resolution":{"observed_at":"2026-08-06T18:34:53.225882Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":"2401.00455","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-07-04T18:50:05.424948Z","title":"Miller, B","venue":null,"work_id":"9aa0d0d3-36f4-4d3f-a742-d6b0b8a36bbe","year":2024},"citing_paper":{"arxiv_id":"2510.16113","last_updated":"2026-04-26T06:30:13Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-10-17T18:00:38Z","title":"Post-adiabatic self-force waveforms: slowly spinning primary and precessing secondary","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-18T05:52:48.547252Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2510.16113"},"observation_digest":"sha256:15878f2788e535fcb3ccb034734308cda7f31801277ad3974917ff4de0fe0914","observation_id":"207fd751-eb10-48af-a2ab-e74b08101512","resolution":{"observed_at":"2026-05-18T05:55:57.433757Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":"2401.00455","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-07-04T18:50:05.424948Z","title":"Miller, B","venue":null,"work_id":"9aa0d0d3-36f4-4d3f-a742-d6b0b8a36bbe","year":2024},"citing_paper":{"arxiv_id":"2606.04998","last_updated":"2026-06-03T15:16:34Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2026-06-03T15:16:34Z","title":"Self-force calculations with numerical relativity methods","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-06-28T05:18:23.572842Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2606.04998"},"observation_digest":"sha256:1283dfbe4575d438c65a47a0a95cdabd373c71cd3b8747f096ae0b26da93a1aa","observation_id":"92331e89-05f9-485a-a30a-8143f96c7e78","resolution":{"observed_at":"2026-07-02T10:06:51.809941Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":"2401.00455","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-07-04T18:50:05.424948Z","title":"Miller, B","venue":null,"work_id":"9aa0d0d3-36f4-4d3f-a742-d6b0b8a36bbe","year":2024},"citing_paper":{"arxiv_id":"2606.24816","last_updated":"2026-06-23T17:02:02Z","snapshot_observed_at":"2026-08-05T22:27:09.666712Z","submitted_at":"2026-06-23T17:02:02Z","title":"The Bondi--Sachs gauge, BMS frames, and memory in black hole perturbation theory","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-06-25T22:19:51.278679Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2606.24816"},"observation_digest":"sha256:2cffdabd6abea2b4ead64d50817856e3529727c7b2abaf093e4bc8fbfb6103c5","observation_id":"59f2edb1-8edc-4db0-8733-e6697ad8c07c","resolution":{"observed_at":"2026-07-04T18:50:05.426407Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":"2401.00455","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-07-04T18:50:05.424948Z","title":"Miller, B","venue":null,"work_id":"9aa0d0d3-36f4-4d3f-a742-d6b0b8a36bbe","year":2024},"citing_paper":{"arxiv_id":"2606.28937","last_updated":"2026-06-27T14:17:05Z","snapshot_observed_at":"2026-07-31T02:51:36.064755Z","submitted_at":"2026-06-27T14:17:05Z","title":"Quadrupole and quadratic-in-spin effects in quasicircular, spinning, asymmetric binaries","version":1},"reference_index":171,"source":"pdf_text","source_observed_at":"2026-06-30T08:47:20.958239Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2606.28937"},"observation_digest":"sha256:044bfbf05ff0045dedd3cb4fa46b58922495b6aa5a06063df816b2c8b8eb80d6","observation_id":"c5de88da-da16-4a8b-ab43-de3a72af1a1f","resolution":{"observed_at":"2026-06-30T08:54:30.041159Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-10T06:31:04.303077+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-08-04T21:28:07.709322Z","title":"Miller, B","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.01774","last_updated":"2026-08-05T10:22:12Z","snapshot_observed_at":"2026-08-08T23:10:43.781147Z","submitted_at":"2026-08-03T06:47:21Z","title":"High-Post-Newtonian-Order Dynamics Induced by Tail-of-Tail Interactions: The Non-Geodesic Terms","version":1},"reference_index":105,"source":"pdf_text","source_observed_at":"2026-08-04T21:28:07.709322Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2608.01774"},"observation_digest":"sha256:463d95b3e10419e61e35d15646aa2fb9ad98d7eec6ec5c37fe2062a0ea1f285a","observation_id":"fc250948-f81a-4195-bf0c-3e8471dbdcb6","resolution":{"observed_at":"2026-08-04T21:28:07.709322Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2401.00455","snapshot_observed_at":"2026-08-07T00:15:14.388995Z","title":"Miller, B","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.01774","last_updated":"2026-08-05T10:22:12Z","snapshot_observed_at":"2026-08-08T23:10:43.781147Z","submitted_at":"2026-08-03T06:47:21Z","title":"High-Post-Newtonian-Order Dynamics Induced by Tail-of-Tail Interactions: The Non-Geodesic Terms","version":2},"reference_index":105,"source":"pdf_text","source_observed_at":"2026-08-07T00:15:14.388995Z"},"links":{"cited_paper":"/paper/2401.00455","citing_paper":"/paper/2608.01774"},"observation_digest":"sha256:0268065fd7479071bcabd9b02bb9c7cdb8213080fa5c405be7e331a635f09fc0","observation_id":"e78bab1e-9bfb-493b-b1bb-1ef63a04bec4","resolution":{"observed_at":"2026-08-07T00:15:14.388995Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2401.00455/citation-record","integrity":"/paper/2401.00455/integrity","json":"/paper/2401.00455/citation-record.json","paper":"/paper/2401.00455"},"outbound":[],"paper":{"arxiv_id":"2401.00455","last_updated":"2024-10-26T18:56:05Z","latest_version":2,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-09T05:11:42.560536Z","submitted_at":"2023-12-31T11:15:41Z","title":"Worldtube puncture scheme for first- and second-order self-force calculations in the Fourier domain"},"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":"2026-08-10T06:31:04.303077+00:00","source":"crossref"},{"observed_at":"2026-08-10T06:30:57.382061+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 9 inbound Pith citation observations for arXiv:2401.00455."}