{"as_of":"2026-08-10T09:06:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:400b66ffadaafa25544e2b9d6800a4f6a9298d0817d55f477a663e5692a68f6f","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":17,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":17,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-10T06:31:04.303077+00:00","state":"measured"},{"denominator":17,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":17,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-09T20:53:38.493670Z","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":"2026-07-02T19:27:18.935500Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-09T20:53:38.493670Z","title":"Fucito, J.F","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-09T22:30:00.033083Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.493670Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:07cad6bc9231c2674d8569adf697b056ec41d18ecda2d446d29ad290afd22aac","observation_id":"d4aed82b-0483-4c3f-9649-6580342d85e6","resolution":{"observed_at":"2026-08-09T20:53:38.493670Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-08T17:27:11.247348Z","title":"Fucito, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2502.05941","last_updated":"2025-08-02T05:57:20Z","snapshot_observed_at":"2026-08-09T13:55:57.388417Z","submitted_at":"2025-02-09T15:56:05Z","title":"Waveform, memory and classical soft scalar theorems","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-08T17:27:11.247348Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2502.05941"},"observation_digest":"sha256:431103079edc97b66e4dcaa46f0cb1e7f8d893e0701bb3525c0b75f669271026","observation_id":"b6ced022-1adf-494d-8d59-b0eecd9be7aa","resolution":{"observed_at":"2026-08-08T17:27:11.247348Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":"2408.07329","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-07-02T19:27:18.935500Z","title":"Fucito, J","venue":null,"work_id":"31b08559-5e38-487e-b8ed-4a217e37267e","year":2025},"citing_paper":{"arxiv_id":"2504.07862","last_updated":"2026-04-07T01:10:37Z","snapshot_observed_at":"2026-08-07T22:39:17.138826Z","submitted_at":"2025-04-10T15:39:05Z","title":"Resummation of Universal Tails in Gravitational Waveforms","version":2},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-05-22T20:14:28.137677Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2504.07862"},"observation_digest":"sha256:3296af336d53f546806fd240cb8ea868b43ce1a7e38de634c6380b1fa61bff69","observation_id":"d7c08527-d9d6-4135-b022-3ab3f64877aa","resolution":{"observed_at":"2026-05-22T20:15:05.209756Z","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":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":"2408.07329","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-07-02T19:27:18.935500Z","title":"Fucito, J","venue":null,"work_id":"31b08559-5e38-487e-b8ed-4a217e37267e","year":2025},"citing_paper":{"arxiv_id":"2505.21489","last_updated":"2026-04-07T01:15:16Z","snapshot_observed_at":"2026-08-07T20:50:14.586787Z","submitted_at":"2025-05-27T17:54:52Z","title":"5-Dimensional Gravitational Raman Scattering: Scalar Wave Perturbations in Schwarzschild-Tangherlini Spacetime","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-05-19T12:39:37.173441Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2505.21489"},"observation_digest":"sha256:38f25a58240cef9d1b7c250390b86f79969debec0ee8127c25222a590b1a205c","observation_id":"0854792c-a220-428a-943c-4313df710276","resolution":{"observed_at":"2026-05-19T12:42:18.750181Z","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":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-07T00:23:42.686366Z","title":"Fucito, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2506.14326","last_updated":"2025-06-17T09:10:55Z","snapshot_observed_at":"2026-08-07T00:15:31.122109Z","submitted_at":"2025-06-17T09:10:55Z","title":"Exact expressions for the 5-Point Liouville conformal block with a level-two degenerate field insertion","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-07T00:23:42.686366Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2506.14326"},"observation_digest":"sha256:5472ed04d16d269ac6cbf9d64dd3a7db8fd3555648868d89ac3eece3f78d0345","observation_id":"2ccdd4bf-72e4-4d2d-9ecf-2805785dd162","resolution":{"observed_at":"2026-08-07T00:23:42.686366Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-06T22:50:06.813877Z","title":"Fucito, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2506.20733","last_updated":"2025-06-25T18:01:09Z","snapshot_observed_at":"2026-08-08T15:20:46.369709Z","submitted_at":"2025-06-25T18:01:09Z","title":"Nonlinear Gravitational Memory in the Post-Minkowskian Expansion","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-06T22:50:06.813877Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2506.20733"},"observation_digest":"sha256:6c55f9e843b5da9fdab2e9f15d3396ca79ef1f3aeb3e4e2bee137f999414a346","observation_id":"53115c10-7804-45a8-a6da-121bc0c3b467","resolution":{"observed_at":"2026-08-06T22:50:06.813877Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-06T18:22:07.977020Z","title":"Gravitational wave forms for extreme mass ratio collisions from su- persymmetric gauge theories,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.08708","last_updated":"2025-07-11T16:06:22Z","snapshot_observed_at":"2026-08-07T00:30:16.755994Z","submitted_at":"2025-07-11T16:06:22Z","title":"High-post-Newtonian-order dynamical effects induced by tail-of-tail interactions in a two body system","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-06T18:22:07.977020Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2507.08708"},"observation_digest":"sha256:0ec886116286f39b5f8d5c8a02a08bcfe213a347238479a8a48d502a3db83b01","observation_id":"0b992dcf-7e98-4f52-b9a9-42505613d568","resolution":{"observed_at":"2026-08-06T18:22:07.977020Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-05T15:24:55.223992Z","title":"Fucito, J.F","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2508.19960","last_updated":"2025-08-27T15:16:51Z","snapshot_observed_at":"2026-08-08T08:02:51.650703Z","submitted_at":"2025-08-27T15:16:51Z","title":"Regular and Floquet bases for gauge and gravity theories: a non perturbative approach","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-05T15:24:55.223992Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2508.19960"},"observation_digest":"sha256:2bb21da81e331966c0f6dac195508c64ff29146d50d9e81121b259c571206b63","observation_id":"6b989254-a46c-44fd-a273-732473c34515","resolution":{"observed_at":"2026-08-05T15:24:55.223992Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":"2408.07329","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-07-02T19:27:18.935500Z","title":"Fucito, J","venue":null,"work_id":"31b08559-5e38-487e-b8ed-4a217e37267e","year":2025},"citing_paper":{"arxiv_id":"2601.08252","last_updated":"2026-04-20T06:52:41Z","snapshot_observed_at":"2026-07-06T22:41:33.987055Z","submitted_at":"2026-01-13T06:19:05Z","title":"Resumming Scattering Amplitudes for Waveforms","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-16T15:40:24.570941Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2601.08252"},"observation_digest":"sha256:4034d53bfc80c6d53633575eb936d69f2eea968296ffb4057c8f03cd47ed40f4","observation_id":"3fc40774-6e5a-48ad-bcfa-e20260a92ea0","resolution":{"observed_at":"2026-05-16T15:41:04.731644Z","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":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-03T04:12:08.599654Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.05766","last_updated":"2026-07-02T14:09:04Z","snapshot_observed_at":"2026-08-09T23:05:58.523592Z","submitted_at":"2026-02-05T15:30:42Z","title":"\"Waveforms\" at the Horizon","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-03T04:12:08.599654Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2602.05766"},"observation_digest":"sha256:84f32d7dfa66ccfc056cb91584d08f53956398765efde377db228d3f03954cae","observation_id":"90bd0668-668e-435b-8293-c8d48e31e6e1","resolution":{"observed_at":"2026-08-03T04:12:08.599654Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-03T03:14:27.444036Z","title":"Fucito, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.08833","last_updated":"2026-06-03T07:14:45Z","snapshot_observed_at":"2026-08-08T16:50:53.058912Z","submitted_at":"2026-02-09T16:02:24Z","title":"From the confluent Heun equation to a new factorized and resummed gravitational waveform for circularized, nonspinning, compact binaries","version":2},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-03T03:14:27.444036Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2602.08833"},"observation_digest":"sha256:6bed13df74e4bca3ccde2d5c3004391fbbfed194b1458cf2ed8fb1c2d0cf7f88","observation_id":"aa7f38c7-1923-40a9-8300-d7fa5b6eab4a","resolution":{"observed_at":"2026-08-03T03:14:27.444036Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":"2408.07329","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-07-02T19:27:18.935500Z","title":"Fucito, J","venue":null,"work_id":"31b08559-5e38-487e-b8ed-4a217e37267e","year":2025},"citing_paper":{"arxiv_id":"2604.14112","last_updated":"2026-05-01T02:54:52Z","snapshot_observed_at":"2026-07-06T23:02:00.082783Z","submitted_at":"2026-04-15T17:32:10Z","title":"Gravitational Sommerfeld Effects: Formalism, Renormalization, and Perturbation to $O(G^{10})$","version":2},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-05-10T13:01:12.211003Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2604.14112"},"observation_digest":"sha256:27b37b0779f249c7b7a76147b4b3f38a838a004ac3e5bb4046f26a7d234b75f9","observation_id":"b9255c3f-4410-473a-aebb-7cb23d6d1a94","resolution":{"observed_at":"2026-05-10T13:05:25.318603Z","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":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":"2408.07329","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-07-02T19:27:18.935500Z","title":"Fucito, J","venue":null,"work_id":"31b08559-5e38-487e-b8ed-4a217e37267e","year":2025},"citing_paper":{"arxiv_id":"2606.07070","last_updated":"2026-07-15T13:27:10Z","snapshot_observed_at":"2026-08-06T09:06:31.976049Z","submitted_at":"2026-06-05T09:09:12Z","title":"Gravitational waveforms from binaries in higher-derivative gravity: a Love story","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-06-27T21:30:42.265543Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2606.07070"},"observation_digest":"sha256:e64e9ba68c13df8fe25a9a7301e8978271b58b63da10b405dba8bf95cb47b955","observation_id":"888135cb-7454-4f68-8d3f-139357b9e203","resolution":{"observed_at":"2026-07-02T19:27:18.936822Z","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":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-02T12:15:43.782138Z","title":"Fucito, J","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2606.07070","last_updated":"2026-07-15T13:27:10Z","snapshot_observed_at":"2026-08-06T09:06:31.976049Z","submitted_at":"2026-06-05T09:09:12Z","title":"Gravitational waveforms from binaries in higher-derivative gravity: a Love story","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-02T12:15:43.782138Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2606.07070"},"observation_digest":"sha256:b552db5059c98711cd5ca51a94048993d5a88383424c69d943549ad81b36076c","observation_id":"a3abef29-7bd0-4b22-8c96-47caec107434","resolution":{"observed_at":"2026-08-02T12:15:43.782138Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-01T07:19:13.395493Z","title":"Fucito, J.F","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.27478","last_updated":"2026-07-29T21:37:53Z","snapshot_observed_at":"2026-08-08T05:39:17.649723Z","submitted_at":"2026-07-29T21:37:53Z","title":"Kerr Soft Dressing and the $w_{1+\\infty}$ Frame Algebra at Null Infinity","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-01T07:19:13.395493Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2607.27478"},"observation_digest":"sha256:b93ef7cbdd90b28a8a06a92e517086dc7e96dd26e98e795b990fc94029917b0b","observation_id":"a13b6277-9b11-43f2-bb39-e0277284d273","resolution":{"observed_at":"2026-08-01T07:19:13.395493Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-04T21:28:07.749752Z","title":"Fucito, J","venue":null,"work_id":null,"year":2025},"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":114,"source":"pdf_text","source_observed_at":"2026-08-04T21:28:07.749752Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2608.01774"},"observation_digest":"sha256:a59fb6d77371d10d37b381cdb5993c84e3de03370a3fe6c75cd0e20dea6fe13a","observation_id":"7348a2ea-8462-4783-8947-2bbc8adc36e7","resolution":{"observed_at":"2026-08-04T21:28:07.749752Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07329","snapshot_observed_at":"2026-08-07T00:15:14.434863Z","title":"Fucito, J","venue":null,"work_id":null,"year":2025},"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":114,"source":"pdf_text","source_observed_at":"2026-08-07T00:15:14.434863Z"},"links":{"cited_paper":"/paper/2408.07329","citing_paper":"/paper/2608.01774"},"observation_digest":"sha256:6aa8d04c76cc3de867c90263c37a9f6a92593cd0b95f5a5c4d9dde1112a322b6","observation_id":"c1820bd0-2902-4098-845a-fd9be81baca3","resolution":{"observed_at":"2026-08-07T00:15:14.434863Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2408.07329/citation-record","integrity":"/paper/2408.07329/integrity","json":"/paper/2408.07329/citation-record.json","paper":"/paper/2408.07329"},"outbound":[],"paper":{"arxiv_id":"2408.07329","last_updated":"2025-02-18T15:16:07Z","latest_version":4,"primary_category":"hep-th","snapshot_observed_at":"2026-08-10T08:44:27.620158Z","submitted_at":"2024-08-14T07:09:21Z","title":"Gravitational wave forms for extreme mass ratio collisions from supersymmetric gauge theories"},"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 17 inbound Pith citation observations for arXiv:2408.07329."}