{"as_of":"2026-08-21T09:11:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:f2ecec132732634b01fae03a8105b46fa3e2a7856d856327cca9b3ddf9decd81","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":39,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":39,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":39,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":39,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-16T05:42:51.562420Z","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":"2026-06-30T20:15:04.748542Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-12T21:59:49.041513Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2411.08176","last_updated":"2024-11-12T20:43:55Z","snapshot_observed_at":"2026-08-16T02:45:33.773466Z","submitted_at":"2024-11-12T20:43:55Z","title":"Spinning bodies in general relativity from bosonic worldline oscillators","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-12T21:59:49.041513Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2411.08176"},"observation_digest":"sha256:aaab4a40230f3dea4877019138f57c71a0d5b46d42dbc3add366197a7384d471","observation_id":"a5265ef0-1b1b-4c7a-ba31-dad95aa817f3","resolution":{"observed_at":"2026-08-12T21:59:49.041513Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-12T21:24:00.459187Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2411.09016","last_updated":"2025-05-25T05:48:56Z","snapshot_observed_at":"2026-08-16T10:00:40.408576Z","submitted_at":"2024-11-13T20:41:25Z","title":"Classical Observables from Causal Response Functions","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-12T21:24:00.459187Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2411.09016"},"observation_digest":"sha256:11572c33b43f0a8fa68dfdd90207c76d1c13d28e1642c45cb545e008e3bd1ac5","observation_id":"1f963b0e-6559-4649-9072-1f40bf4b0b20","resolution":{"observed_at":"2026-08-12T21:24:00.459187Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-12T20:33:01.243247Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics atO(G4),","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2411.09652","last_updated":"2025-03-14T14:52:17Z","snapshot_observed_at":"2026-08-16T10:15:21.188043Z","submitted_at":"2024-11-14T18:20:24Z","title":"Strong Field Scattering of Black Holes: Assessing Resummation Strategies","version":2},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-12T20:33:01.243247Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2411.09652"},"observation_digest":"sha256:96c3d5c06e603c21b7b580fcce04a78ea0702c1d48659f71e65709f1a334e112","observation_id":"b3f4c71c-3b08-4ca5-814d-e4065e9e0013","resolution":{"observed_at":"2026-08-12T20:33:01.243247Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2411.11846","last_updated":"2025-03-19T13:39:55Z","snapshot_observed_at":"2026-08-19T23:41:19.283144Z","submitted_at":"2024-11-18T18:59:58Z","title":"Emergence of Calabi-Yau manifolds in high-precision black hole scattering","version":2},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-05-21T18:31:21.767862Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2411.11846"},"observation_digest":"sha256:90ee570c3f5d8464bd38f223c74a69edd313dce212fa528892b1bf83f6df2685","observation_id":"bce6581e-f017-4471-a4d9-4329967bfb86","resolution":{"observed_at":"2026-05-21T18:31:22.260825Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-11T23:59:08.211685Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.02034","last_updated":"2024-12-20T23:50:50Z","snapshot_observed_at":"2026-08-15T01:30:16.575604Z","submitted_at":"2024-12-02T23:31:41Z","title":"One-Loop Observables to Higher Order in Spin","version":2},"reference_index":111,"source":"pdf_text","source_observed_at":"2026-08-11T23:59:08.211685Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2412.02034"},"observation_digest":"sha256:a152685b01b6669997b75b73c00102d73ea681882397cd03e9cbedada7c361ee","observation_id":"74f7a2a5-05ea-4859-b987-f615d369614a","resolution":{"observed_at":"2026-08-11T23:59:08.211685Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-11T15:36:19.781086Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.10864","last_updated":"2025-06-30T08:56:10Z","snapshot_observed_at":"2026-08-17T22:30:51.119056Z","submitted_at":"2024-12-14T15:30:13Z","title":"Classical worldlines from scattering amplitudes","version":2},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-11T15:36:19.781086Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2412.10864"},"observation_digest":"sha256:dbdb73492c455c746423d5de01c6e8f421baf2bc26524bbdde0422353a61b8c1","observation_id":"4920dfe2-eaad-4014-ae25-50ab7c552bb6","resolution":{"observed_at":"2026-08-11T15:36:19.781086Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-10T22:11:05.852175Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4),","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.02904","last_updated":"2025-06-30T10:18:18Z","snapshot_observed_at":"2026-08-15T11:03:17.777056Z","submitted_at":"2025-01-06T10:28:48Z","title":"Radiation-Reaction and Angular Momentum Loss at $\\mathcal{O}(G^4)$","version":3},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-10T22:11:05.852175Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2501.02904"},"observation_digest":"sha256:5b24a6b376a5ae0b50c8935696695b28a557a8da3d75621b50a65118bd16cebd","observation_id":"da426789-ffdb-4f47-9870-fd4bacdafb07","resolution":{"observed_at":"2026-08-10T22:11:05.852175Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-10T04:36:57.085485Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.17818","last_updated":"2025-01-29T18:10:08Z","snapshot_observed_at":"2026-08-14T19:54:06.503867Z","submitted_at":"2025-01-29T18:10:08Z","title":"Gleaning gravitational amplitudes -- a double copy for canceling dilatons","version":1},"reference_index":192,"source":"pdf_text","source_observed_at":"2026-08-10T04:36:57.085485Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2501.17818"},"observation_digest":"sha256:83ad39f95294f5d74f3b5b02e97cd332f4480ee1b638c1e9ea9a20b99b145633","observation_id":"e8f6d6d3-796e-4abc-97f6-f4ce8f11b702","resolution":{"observed_at":"2026-08-10T04:36:57.085485Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-07T23:10:24.079506Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4),","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2502.08961","last_updated":"2025-07-30T17:13:45Z","snapshot_observed_at":"2026-08-12T17:27:09.962464Z","submitted_at":"2025-02-13T04:55:12Z","title":"First Look at Quartic-in-Spin Binary Dynamics at Third Post-Minkowskian Order","version":3},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-07T23:10:24.079506Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2502.08961"},"observation_digest":"sha256:5e5736bdee4748dadeaa19f6e428ccd549468d01da97c4874f0f7ae8fcfcda37","observation_id":"8118e2cd-6fbb-4432-b08b-40c684d1dd66","resolution":{"observed_at":"2026-08-07T23:10:24.079506Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2503.12263","last_updated":"2025-08-29T11:52:35Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-03-15T21:04:14Z","title":"The Science of the Einstein Telescope","version":2},"reference_index":227,"source":"pdf_text","source_observed_at":"2026-05-22T23:56:23.754079Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2503.12263"},"observation_digest":"sha256:744b5976c04bc00e7f01b3b0bffd90fd10535538054a4ba008727ca8d048a588","observation_id":"eb537ce0-eff2-4479-aec2-a844ea22ab93","resolution":{"observed_at":"2026-05-09T06:19:15.526174Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-16T05:42:51.562420Z","title":"Scattering Ampli- tudes, the Tail Effect, and Conservative Binary Dynamics at O(G4),","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2504.20204","last_updated":"2025-04-28T19:12:33Z","snapshot_observed_at":"2026-08-19T01:55:52.797305Z","submitted_at":"2025-04-28T19:12:33Z","title":"High Precision Black Hole Scattering: Tutti Frutti vs Worldline Effective Field Theory","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-16T05:42:51.562420Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2504.20204"},"observation_digest":"sha256:c6fa6bc0538224c2de887cf90e264cffccf747ed0da28160d2c40f164aabc121","observation_id":"20bcc559-915b-45ce-8bed-4e16071c276f","resolution":{"observed_at":"2026-08-16T05:42:51.562420Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-15T21:48:38.769795Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.09052","last_updated":"2025-06-17T01:56:18Z","snapshot_observed_at":"2026-08-18T12:17:18.949839Z","submitted_at":"2025-05-14T01:18:00Z","title":"Dictionary revision for mapping boundary data to bound states","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-15T21:48:38.769795Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2505.09052"},"observation_digest":"sha256:cc1195ed1559a677efadb344f62b9856450eb7b01eba0fc32d558f703707ad6c","observation_id":"baeb296a-497e-45eb-b586-c57659f19714","resolution":{"observed_at":"2026-08-15T21:48:38.769795Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-15T20:58:04.454623Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.11488","last_updated":"2025-05-16T17:50:51Z","snapshot_observed_at":"2026-08-19T19:08:05.556689Z","submitted_at":"2025-05-16T17:50:51Z","title":"Higher-spin effects in black hole and neutron star binary dynamics: worldline supersymmetry beyond minimal coupling","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-15T20:58:04.454623Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2505.11488"},"observation_digest":"sha256:aab0739101b46cbdf8da48380eab59b3042f62975fb9b439c7cefed81ceea57f","observation_id":"2e990611-c738-413b-be06-6ec4a792636d","resolution":{"observed_at":"2026-08-15T20:58:04.454623Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-07T10:39:18.164404Z","title":"Scattering Ampli- tudes, the Tail Effect, and Conservative Binary Dynamics at O(G4),","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2506.04876","last_updated":"2025-06-05T10:49:58Z","snapshot_observed_at":"2026-08-15T13:26:13.032620Z","submitted_at":"2025-06-05T10:49:58Z","title":"Scattering angle in a Topological Star spacetime: a self-force approach","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-07T10:39:18.164404Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2506.04876"},"observation_digest":"sha256:c1802eae784e5c1b8e76839a1850547489ecbcf6597ddbaead0042ea4a93e737","observation_id":"d8a6b1fa-55af-45f7-8d0d-dfd14e48f0f8","resolution":{"observed_at":"2026-08-07T10:39:18.164404Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-15T19:53:20.322639Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2506.14626","last_updated":"2025-07-11T12:51:42Z","snapshot_observed_at":"2026-08-16T00:02:30.130772Z","submitted_at":"2025-06-17T15:22:30Z","title":"Spinning the Probe in Kerr with WQFT","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-15T19:53:20.322639Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2506.14626"},"observation_digest":"sha256:5ae0320762bf4ce2134c74c7ce47b1378f48f0f27553e8a668c22221fbfbe6ab","observation_id":"388ded3d-34ce-42aa-9a5c-155dab1dc5a3","resolution":{"observed_at":"2026-08-15T19:53:20.322639Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-06T22:50:46.077112Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2506.20665","last_updated":"2025-06-25T17:58:02Z","snapshot_observed_at":"2026-08-15T15:18:17.192254Z","submitted_at":"2025-06-25T17:58:02Z","title":"Local-in-Time Conservative Binary Dynamics at Fifth Post-Minkowskian and First Self-Force Orders","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-06T22:50:46.077112Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2506.20665"},"observation_digest":"sha256:4b17c07bd6be58ec80de658118e3275464624360c305f83146c4ec003e78c20d","observation_id":"21c90654-60f7-47cf-9da5-3b1367e97d05","resolution":{"observed_at":"2026-08-06T22:50:46.077112Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-06T22:50:06.513335Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2506.20733","last_updated":"2025-06-25T18:01:09Z","snapshot_observed_at":"2026-08-20T19:31:09.655498Z","submitted_at":"2025-06-25T18:01:09Z","title":"Nonlinear Gravitational Memory in the Post-Minkowskian Expansion","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-06T22:50:06.513335Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2506.20733"},"observation_digest":"sha256:5bbbb984adb4dd55dd56f263214533f9c4d42c4974125742728716ef924fcb35","observation_id":"03a2e7a0-8f9e-4f5c-b68c-d3bfc477c5da","resolution":{"observed_at":"2026-08-06T22:50:06.513335Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-06T20:16:08.738797Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4),","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2507.03442","last_updated":"2025-07-04T09:58:39Z","snapshot_observed_at":"2026-08-18T13:31:19.441447Z","submitted_at":"2025-07-04T09:58:39Z","title":"Scattering of a point mass by a Schwarzschild black hole: radiated energy and angular momentum","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-06T20:16:08.738797Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2507.03442"},"observation_digest":"sha256:d4a40a8152d0a040053ef36d034a9e0e35e2bc5f086867c7d25c3ec19920f2d2","observation_id":"efcaf6e0-eee2-4566-b664-e4964e029936","resolution":{"observed_at":"2026-08-06T20:16:08.738797Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2508.10761","last_updated":"2026-05-06T18:01:50Z","snapshot_observed_at":"2026-08-10T15:24:49.464137Z","submitted_at":"2025-08-14T15:46:29Z","title":"Unexpected Symmetries of Kerr Black Hole Scattering","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-05-18T23:12:31.732350Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2508.10761"},"observation_digest":"sha256:ca145001a3d07c03cb081f17e11c4dc6894d623f4baa1676588ce7a987609906","observation_id":"237dc577-b1a1-4b82-b67b-3853ff534e3d","resolution":{"observed_at":"2026-05-18T23:12:53.271192Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2509.04425","last_updated":"2026-04-14T21:38:16Z","snapshot_observed_at":"2026-08-11T01:39:51.322036Z","submitted_at":"2025-09-04T17:46:45Z","title":"Hidden simplicity in the scattering for neutron stars and black holes","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-05-18T18:53:09.818269Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2509.04425"},"observation_digest":"sha256:eeb00106f5525a59b69824c244574ecaba80f9fc0945bcb878d70817a4ce8040","observation_id":"38e34e1d-93d8-4c21-96d6-14f59df08a38","resolution":{"observed_at":"2026-05-18T18:56:46.713328Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-04T13:25:39.985677Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4),","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.00989","last_updated":"2026-07-07T10:35:11Z","snapshot_observed_at":"2026-08-14T00:58:07.614909Z","submitted_at":"2025-10-01T15:00:01Z","title":"Generalized Unitarity Method for Worldline Field Theory","version":6},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-04T13:25:39.985677Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2510.00989"},"observation_digest":"sha256:53b77fd510fe507a3ac3a33ab5659f56a3c3d5d52fde9b9257fcd4b69095b688","observation_id":"aa3beb33-3892-4a61-983b-dfb652056607","resolution":{"observed_at":"2026-08-04T13:25:39.985677Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2510.07390","last_updated":"2026-04-19T14:09:41Z","snapshot_observed_at":"2026-08-09T11:48:22.893315Z","submitted_at":"2025-10-08T18:00:06Z","title":"Heterotic Footprints in Classical Gravity: PM dynamics from On-Shell soft amplitudes at one loop","version":3},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-05-18T09:18:11.581260Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2510.07390"},"observation_digest":"sha256:d0b52bdf9ff0f4680588116973be5e75a0521a06267423ab71031913e76624ae","observation_id":"5a71e324-15b6-427d-862d-7f5d4d1f4dbf","resolution":{"observed_at":"2026-05-18T09:21:10.536694Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-04T07:01:25.370623Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.27676","last_updated":"2026-05-26T20:24:18Z","snapshot_observed_at":"2026-08-18T17:27:02.713687Z","submitted_at":"2025-10-31T17:42:42Z","title":"Renormalisation Group approach to General Relativity","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-04T07:01:25.370623Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2510.27676"},"observation_digest":"sha256:c44f6a014958ece390eae7c05109be1e4d3a865e094254d74f6bab15280f313d","observation_id":"65fd8d2e-9264-4817-b5e2-bc4d56ee4227","resolution":{"observed_at":"2026-08-04T07:01:25.370623Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2512.10518","last_updated":"2026-05-20T17:03:56Z","snapshot_observed_at":"2026-08-16T22:04:26.017977Z","submitted_at":"2025-12-11T10:41:45Z","title":"Fano and Reflexive Polytopes from Feynman Integrals","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-05-21T17:23:37.427013Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2512.10518"},"observation_digest":"sha256:8289d41abbebecf05b595bccc4bcf73f1dc0141c4b3ca310b222c301d3d00030","observation_id":"2aafac36-1928-4953-9ac7-fc44d7f5da44","resolution":{"observed_at":"2026-05-21T17:24:16.528460Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2601.08252","last_updated":"2026-04-20T06:52:41Z","snapshot_observed_at":"2026-08-15T12:27:31.235290Z","submitted_at":"2026-01-13T06:19:05Z","title":"Resumming Scattering Amplitudes for Waveforms","version":3},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-05-16T15:40:24.570941Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2601.08252"},"observation_digest":"sha256:f25ae60c2a128b260686bd192bef46a4b4db780bd6e84098250acdc1c8326e3c","observation_id":"1c2708f6-0e3c-4fb1-bca7-56ccf891cff0","resolution":{"observed_at":"2026-05-16T15:41:04.781649Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-03T08:40:25.610682Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2601.16256","last_updated":"2026-07-13T19:47:59Z","snapshot_observed_at":"2026-08-19T22:46:31.970431Z","submitted_at":"2026-01-22T19:00:01Z","title":"Conservative Black Hole Scattering at Fifth Post-Minkowskian and Second Self-Force Order","version":4},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-03T08:40:25.610682Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2601.16256"},"observation_digest":"sha256:18a3f5e01e832772ac836b57a5cf63f601dc100e74ec2fd2d86dcf8e73a954bc","observation_id":"8807b550-15d8-44e5-925b-dda3388ed068","resolution":{"observed_at":"2026-08-03T08:40:25.610682Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-03T04:12:05.214213Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4),","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.05766","last_updated":"2026-07-02T14:09:04Z","snapshot_observed_at":"2026-08-20T05:30:06.483322Z","submitted_at":"2026-02-05T15:30:42Z","title":"\"Waveforms\" at the Horizon","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-03T04:12:05.214213Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2602.05766"},"observation_digest":"sha256:5195ebc7c0b870ed6629fb0add72f25857a9c240f8acf3db7862d3832af45d01","observation_id":"e5385d4e-0588-4626-a530-d5590e58b3e9","resolution":{"observed_at":"2026-08-03T04:12:05.214213Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2602.06947","last_updated":"2026-04-09T15:42:30Z","snapshot_observed_at":"2026-07-31T17:35:32.003805Z","submitted_at":"2026-02-06T18:44:09Z","title":"The gravitational Compton amplitude at third post-Minkowskian order","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-05-16T06:25:50.003086Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2602.06947"},"observation_digest":"sha256:a05a3c81edc8dc8bae2e7be486c2a3748c10de45df8a6ae71700b7b50238e900","observation_id":"1e7d837d-4256-4343-89bb-f7a6265beb4c","resolution":{"observed_at":"2026-05-16T06:27:27.578874Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-03T01:23:10.339543Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2602.10089","last_updated":"2026-05-26T10:19:54Z","snapshot_observed_at":"2026-08-16T02:35:41.580103Z","submitted_at":"2026-02-10T18:55:21Z","title":"Resummed energy loss in extreme-mass-ratio scattering using critical orbits","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-03T01:23:10.339543Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2602.10089"},"observation_digest":"sha256:3a6616e770d830d39347e36c7e4fbf0769eacdc742ce43af20f5b7211c81c1ae","observation_id":"f13f1dd9-ee06-4ed3-a950-e291cbedea33","resolution":{"observed_at":"2026-08-03T01:23:10.339543Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2603.22467","last_updated":"2026-03-23T18:36:33Z","snapshot_observed_at":"2026-08-11T13:09:30.833117Z","submitted_at":"2026-03-23T18:36:33Z","title":"High-order effective-one-body tidal interactions and gravitational scattering","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-05-15T00:29:44.714103Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2603.22467"},"observation_digest":"sha256:f024302edc4b304417a025de29083f42d6836807241de80a30f5d2b0181121d2","observation_id":"dbf7b2e7-3a23-4a96-8a49-3c5aef3c098e","resolution":{"observed_at":"2026-05-15T00:33:23.583301Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2604.09545","last_updated":"2026-04-28T15:33:16Z","snapshot_observed_at":"2026-07-06T22:58:25.877654Z","submitted_at":"2026-04-10T17:58:53Z","title":"Black Hole Dynamics at Fifth Post-Newtonian Order","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-05-10T16:55:41.646845Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2604.09545"},"observation_digest":"sha256:633ac086ef2841d68de2c227eb80b742f13f57e7356732404ee94d669997cadb","observation_id":"f3f2bfce-e8f5-4b8f-8405-6e8bf8736974","resolution":{"observed_at":"2026-05-11T07:55:58.578166Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2604.22009","last_updated":"2026-08-05T16:00:09Z","snapshot_observed_at":"2026-08-16T12:12:11.112684Z","submitted_at":"2026-04-23T18:55:30Z","title":"Black Hole Response Theory and its Exact Shockwave Limit","version":2},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-05-09T20:41:26.438912Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2604.22009"},"observation_digest":"sha256:2b121db2abe16a000f426f5ef24d36c8874fa6b38a1540204dd6fe298f0e9564","observation_id":"2a32f336-6993-4f39-9998-aba402541f60","resolution":{"observed_at":"2026-05-11T15:01:07.278342Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2604.25916","last_updated":"2026-04-28T17:59:10Z","snapshot_observed_at":"2026-08-18T09:38:33.297497Z","submitted_at":"2026-04-28T17:59:10Z","title":"Nonlocal-in-time tail effects in gravitational scattering to fifth Post-Minkowskian and tenth self-force orders","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-05-07T15:40:27.649636Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2604.25916"},"observation_digest":"sha256:61f29ad347a46d9edbd7f6197cb809c188a5d660f7738c22556af4865461166c","observation_id":"b352aab4-f676-4ed7-857d-8921e0e73647","resolution":{"observed_at":"2026-05-12T00:11:18.451571Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2605.04224","last_updated":"2026-05-05T19:08:04Z","snapshot_observed_at":"2026-08-02T06:06:02.086759Z","submitted_at":"2026-05-05T19:08:04Z","title":"Black-Hole Scattering in Einstein-scalar-Gauss-Bonnet: Numerical Relativity Meets Analytics","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-05-08T18:21:53.144889Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2605.04224"},"observation_digest":"sha256:802db548b1cc4aafed4a84bc4d46cca8ae04272f052e8cc8f6481c9d950a51b0","observation_id":"b04cbaba-9ded-4b96-a734-cf94b955ac79","resolution":{"observed_at":"2026-05-09T06:35:37.789715Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2605.14958","last_updated":"2026-05-14T15:26:44Z","snapshot_observed_at":"2026-08-07T09:03:41.144810Z","submitted_at":"2026-05-14T15:26:44Z","title":"Conservative and dissipative sectors in a nonlinear scalar model for the gravitational self-force problem","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-06-30T20:13:18.780946Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2605.14958"},"observation_digest":"sha256:bee2432816091808f7e4731dd38819b5373a8141eff0857413bd13fbe0863b95","observation_id":"044a90db-c6f0-4cce-9e02-bc0cef42e710","resolution":{"observed_at":"2026-06-30T20:15:04.751556Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2605.18544","last_updated":"2026-05-18T15:24:32Z","snapshot_observed_at":"2026-08-15T11:48:27.446831Z","submitted_at":"2026-05-18T15:24:32Z","title":"The Classical Gravitational Impulse at High Energies","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-05-20T09:28:44.735486Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2605.18544"},"observation_digest":"sha256:1427cfc69da5bc17f1b9a02ebfdc4e07a578968f06db560cc1e3a79ee938b2e9","observation_id":"408bc765-b749-4ee2-9f36-32e0cd3c72bc","resolution":{"observed_at":"2026-05-20T09:33:10.742477Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":"2112.10750","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-06-30T20:15:04.748542Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at O(G4)","venue":null,"work_id":"b716a1b4-d3c3-4f79-bac1-59f65ef07ac6","year":2022},"citing_paper":{"arxiv_id":"2606.27544","last_updated":"2026-06-25T20:47:33Z","snapshot_observed_at":"2026-08-05T04:01:17.135525Z","submitted_at":"2026-06-25T20:47:33Z","title":"Gravitational wave scattering at $\\mathcal{O}(G^4)$: Murua construction and elliptics","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-06-29T00:55:32.996852Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2606.27544"},"observation_digest":"sha256:c1152dd034f6193656925fbf1c05fe9a666a4f54cf3edf16c76ed00ab8a61879","observation_id":"3d9f619b-e4ee-4635-bfa4-866014b0b052","resolution":{"observed_at":"2026-06-29T01:02:56.452031Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-07-31T17:56:03.699117Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.24335","last_updated":"2026-08-05T14:51:40Z","snapshot_observed_at":"2026-08-13T04:12:18.679383Z","submitted_at":"2026-07-27T12:11:50Z","title":"The Magnusian generator for dissipative systems and application to leading 2.5PN radiation-reaction dynamics","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-07-31T17:56:03.699117Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2607.24335"},"observation_digest":"sha256:61cfc1287a4f27cfa333810d10dee60c167d768a8f605c642e366693cac57a91","observation_id":"dd497413-5df1-4d92-a152-523a65985ba0","resolution":{"observed_at":"2026-07-31T17:56:03.699117Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.10750","snapshot_observed_at":"2026-08-11T00:28:41.383872Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.07699","last_updated":"2026-08-07T18:40:48Z","snapshot_observed_at":"2026-08-17T14:15:16.537050Z","submitted_at":"2026-08-07T18:40:48Z","title":"Supertranslations are Soft Dressings","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-11T00:28:41.383872Z"},"links":{"cited_paper":"/paper/2112.10750","citing_paper":"/paper/2608.07699"},"observation_digest":"sha256:c022e901da02e8523737ab62cc88658187811fea963d5e3c1010725e11b2d393","observation_id":"1927a3e3-0eaf-4d7e-96f8-dc48d3201cb3","resolution":{"observed_at":"2026-08-11T00:28:41.383872Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2112.10750/citation-record","integrity":"/paper/2112.10750/integrity","json":"/paper/2112.10750/citation-record.json","paper":"/paper/2112.10750"},"outbound":[],"paper":{"arxiv_id":"2112.10750","last_updated":"2021-12-20T18:55:13Z","latest_version":1,"primary_category":"hep-th","snapshot_observed_at":"2026-08-18T14:44:10.924372Z","submitted_at":"2021-12-20T18:55:13Z","title":"Scattering Amplitudes, the Tail Effect, and Conservative Binary Dynamics at $O(G^4)$"},"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":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"thesis":"As of 21 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 39 inbound Pith citation observations for arXiv:2112.10750."}