{"as_of":"2026-08-19T03:34:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:9d40ee23a33bd40453e857036d9c9cb847488b9c27526f1be241f6009162e6af","coverage":[{"denominator":91,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":91,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-09T20:53:38.871933Z","state":"measured"},{"denominator":109,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":109,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-18T06:34:40.430872+00:00","state":"measured"},{"denominator":18,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":18,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-16T12:40:54.475748Z","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":"2026-07-02T19:27:18.995809Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-16T12:40:54.475748Z","title":"Cipriani, G","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2504.12235","last_updated":"2025-07-23T08:55:47Z","snapshot_observed_at":"2026-08-17T19:40:18.450792Z","submitted_at":"2025-04-16T16:35:22Z","title":"Rotating Topological Stars","version":2},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-16T12:40:54.475748Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2504.12235"},"observation_digest":"sha256:b68f6d5ec4404e4278ed9740b411374831edc2fffe5019dca40b496ddaa97c77","observation_id":"c6e08b5c-d134-43aa-a623-b2fb7e1d7f34","resolution":{"observed_at":"2026-08-16T12:40:54.475748Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-07T10:39:20.250471Z","title":"Resumming Post- Minkowskian and Post-Newtonian gravitational wave- form expansions,","venue":null,"work_id":null,"year":null},"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":44,"source":"pdf_text","source_observed_at":"2026-08-07T10:39:20.250471Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2506.04876"},"observation_digest":"sha256:e1cfe37e8e80a3d7d3b56a56e9fbcc6019cc615d4e4b621ce410c01a6529f2e5","observation_id":"b5a92547-1a74-4a18-8a42-7d40ae9de781","resolution":{"observed_at":"2026-08-07T10:39:20.250471Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-07T00:23:43.463070Z","title":"Cipriani, G","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2506.14326","last_updated":"2025-06-17T09:10:55Z","snapshot_observed_at":"2026-08-15T22:45:09.655280Z","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":41,"source":"pdf_text","source_observed_at":"2026-08-07T00:23:43.463070Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2506.14326"},"observation_digest":"sha256:da3fbd22300cfca325b3206a676d54ce14afc804d41645af939e9c7c21d2b6a5","observation_id":"f296fb68-9da4-48a0-8415-2adda09241eb","resolution":{"observed_at":"2026-08-07T00:23:43.463070Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-07T00:32:36.452404Z","title":"Resumming Post- Minkowskian and Post-Newtonian gravitational wave- form expansions,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2506.14442","last_updated":"2025-06-17T12:05:42Z","snapshot_observed_at":"2026-08-18T03:02:34.704926Z","submitted_at":"2025-06-17T12:05:42Z","title":"Topological Stars and scalar wave equation: Exact resummation of the renormalized angular momentum in the eikonal limit","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-07T00:32:36.452404Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2506.14442"},"observation_digest":"sha256:3aa9a80e6f2748bfe0604d5e3c4a240eabf7a4e05aec6261b86d33d07f391ad5","observation_id":"b88b7897-d39c-44bc-be46-ecb5031ad9e6","resolution":{"observed_at":"2026-08-07T00:32:36.452404Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-05T15:24:55.311712Z","title":"Cipriani, G","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2508.19960","last_updated":"2025-08-27T15:16:51Z","snapshot_observed_at":"2026-08-13T12:11:03.245202Z","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":32,"source":"pdf_text","source_observed_at":"2026-08-05T15:24:55.311712Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2508.19960"},"observation_digest":"sha256:5f2f8ea6f75d8f956e7797ecbf16829c00eaa23e0ecce40f8e9138254d055065","observation_id":"504acd1a-99ea-452a-b10c-863913941a70","resolution":{"observed_at":"2026-08-05T15:24:55.311712Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-03T04:12:09.291818Z","title":"Resumming post-Minkowskian and post-Newtonian gravitational waveform expansions,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.05766","last_updated":"2026-07-02T14:09:04Z","snapshot_observed_at":"2026-08-12T22:56:42.187686Z","submitted_at":"2026-02-05T15:30:42Z","title":"\"Waveforms\" at the Horizon","version":2},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-03T04:12:09.291818Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2602.05766"},"observation_digest":"sha256:5063ec33fc51bbbd5fc7f47078f99f626eb63c24dcba148a3725f23c6c0777b9","observation_id":"2a36f15a-da2f-4393-b0a8-f19cd78d513b","resolution":{"observed_at":"2026-08-03T04:12:09.291818Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-03T03:14:27.427112Z","title":"Cipriani, G","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2602.08833","last_updated":"2026-06-03T07:14:45Z","snapshot_observed_at":"2026-08-17T20:10:03.716748Z","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":34,"source":"pdf_text","source_observed_at":"2026-08-03T03:14:27.427112Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2602.08833"},"observation_digest":"sha256:2334c24547b84cd66ffddf7ac3cd8dc50eccc6f0989e2345a45b227f7f9ff7c3","observation_id":"a0ed276d-f8b4-4e1d-8a62-8d6b469c2952","resolution":{"observed_at":"2026-08-03T03:14:27.427112Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-03T01:23:16.111159Z","title":"Cipriani, G","venue":null,"work_id":null,"year":2025},"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":71,"source":"pdf_text","source_observed_at":"2026-08-03T01:23:16.111159Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2602.10089"},"observation_digest":"sha256:9cd79a3ef4535c2d9723b78593e2cb279ed936e8a1f07254372f1e28dd21334d","observation_id":"7032c335-88da-4e53-bd33-5bb78dd6053c","resolution":{"observed_at":"2026-08-03T01:23:16.111159Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":"2501.19257","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-07-02T19:27:18.995809Z","title":"Cipriani, G","venue":null,"work_id":"61a537a9-a24f-4d6f-bf86-06bce16d0ab5","year":2025},"citing_paper":{"arxiv_id":"2604.14112","last_updated":"2026-05-01T02:54:52Z","snapshot_observed_at":"2026-08-13T00:53:19.616873Z","submitted_at":"2026-04-15T17:32:10Z","title":"Gravitational Sommerfeld Effects: Formalism, Renormalization, and Perturbation to $O(G^{10})$","version":2},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-05-10T13:01:12.211003Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2604.14112"},"observation_digest":"sha256:db1d489b9090e08744f4660c5eef5cc82cc86232103a3e57add2353171097948","observation_id":"627ff497-272f-444f-9a37-e9b0563a22e2","resolution":{"observed_at":"2026-05-10T13:05:25.320876Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":"2501.19257","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-07-02T19:27:18.995809Z","title":"Cipriani, G","venue":null,"work_id":"61a537a9-a24f-4d6f-bf86-06bce16d0ab5","year":2025},"citing_paper":{"arxiv_id":"2605.09250","last_updated":"2026-06-25T02:39:11Z","snapshot_observed_at":"2026-08-14T23:51:10.108139Z","submitted_at":"2026-05-10T01:28:01Z","title":"Efficient and Stable Computation of Gravitational-Wave Fluxes from Generic Kerr Orbits via a Unified HeunC Framework","version":1},"reference_index":113,"source":"pdf_text","source_observed_at":"2026-05-12T03:04:27.279604Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2605.09250"},"observation_digest":"sha256:0cada657259c0e1460d72fee8e9f115f111b59bf2b29813d8aaac7f32c2531d4","observation_id":"e4f10930-d3d5-43eb-881a-dfc61d263481","resolution":{"observed_at":"2026-05-12T03:06:19.310805Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":"2501.19257","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-07-02T19:27:18.995809Z","title":"Cipriani, G","venue":null,"work_id":"61a537a9-a24f-4d6f-bf86-06bce16d0ab5","year":2025},"citing_paper":{"arxiv_id":"2605.09250","last_updated":"2026-06-25T02:39:11Z","snapshot_observed_at":"2026-08-14T23:51:10.108139Z","submitted_at":"2026-05-10T01:28:01Z","title":"Efficient and Stable Computation of Gravitational-Wave Fluxes from Generic Kerr Orbits via a Unified HeunC Framework","version":2},"reference_index":113,"source":"pdf_text","source_observed_at":"2026-05-13T07:47:14.054826Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2605.09250"},"observation_digest":"sha256:bc01e821864fad0402e6e289cdb7fc32b24fdfe58f63b859095d292e4df47952","observation_id":"6b4cbc39-8ea7-41d1-a6d7-abb7e0c1c670","resolution":{"observed_at":"2026-05-13T07:47:32.196426Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":"2501.19257","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-07-02T19:27:18.995809Z","title":"Cipriani, G","venue":null,"work_id":"61a537a9-a24f-4d6f-bf86-06bce16d0ab5","year":2025},"citing_paper":{"arxiv_id":"2605.09250","last_updated":"2026-06-25T02:39:11Z","snapshot_observed_at":"2026-08-14T23:51:10.108139Z","submitted_at":"2026-05-10T01:28:01Z","title":"Efficient and Stable Computation of Gravitational-Wave Fluxes from Generic Kerr Orbits via a Unified HeunC Framework","version":3},"reference_index":113,"source":"pdf_text","source_observed_at":"2026-06-30T23:08:26.953490Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2605.09250"},"observation_digest":"sha256:a95bf61a70bf997575d0a10fed3d8d2cf797d6117c7121795f3d49a4fad4f1d6","observation_id":"a374a95f-13ee-41b8-b6f8-1545153a5ff5","resolution":{"observed_at":"2026-07-01T13:35:45.554190Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":"2501.19257","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-07-02T19:27:18.995809Z","title":"Cipriani, G","venue":null,"work_id":"61a537a9-a24f-4d6f-bf86-06bce16d0ab5","year":2025},"citing_paper":{"arxiv_id":"2606.07070","last_updated":"2026-07-15T13:27:10Z","snapshot_observed_at":"2026-08-17T02:23:46.469708Z","submitted_at":"2026-06-05T09:09:12Z","title":"Gravitational waveforms from binaries in higher-derivative gravity: a Love story","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-06-27T21:30:42.265543Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2606.07070"},"observation_digest":"sha256:e21f2a474f64b48b30e316f8029d9311a5baea2e0614d3c87a45001e81b44529","observation_id":"7d65127e-7c94-4800-9e89-1200fd376795","resolution":{"observed_at":"2026-07-02T19:27:18.997163Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-02T12:15:43.752053Z","title":"Cipriani, G","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2606.07070","last_updated":"2026-07-15T13:27:10Z","snapshot_observed_at":"2026-08-17T02:23:46.469708Z","submitted_at":"2026-06-05T09:09:12Z","title":"Gravitational waveforms from binaries in higher-derivative gravity: a Love story","version":2},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-02T12:15:43.752053Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2606.07070"},"observation_digest":"sha256:02e42e0e5b886cf93e3823bdd9c96378060a02797791dea27e8d23608acba4fa","observation_id":"03863122-2452-404b-955b-410b1397c560","resolution":{"observed_at":"2026-08-02T12:15:43.752053Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":"2501.19257","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-07-02T19:27:18.995809Z","title":"Cipriani, G","venue":null,"work_id":"61a537a9-a24f-4d6f-bf86-06bce16d0ab5","year":2025},"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":193,"source":"pdf_text","source_observed_at":"2026-06-30T08:47:20.958239Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2606.28937"},"observation_digest":"sha256:b70d223e89a62e45f28c198aa1568710f5424d0e6896e14c3eb206d6bd09f114","observation_id":"c85a7945-af53-42e5-9a75-34f0ad06bf85","resolution":{"observed_at":"2026-06-30T09:04:32.970482Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-02T08:03:15.999798Z","title":"Resumming post- Minkowskian and post-Newtonian gravitational wave- form expansions,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.08280","last_updated":"2026-07-16T10:10:08Z","snapshot_observed_at":"2026-08-14T14:58:04.414891Z","submitted_at":"2026-07-09T09:22:33Z","title":"5d Schwarzschild-Tangherlini spacetime: MST-like formalism for a Reduced Confluent Heun Equation","version":2},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-02T08:03:15.999798Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2607.08280"},"observation_digest":"sha256:24dfa6cfc77cea1c3d65de031cac11ae2dbd74859d00a385a516c88d0b6a6bbf","observation_id":"7d0a0340-b76e-4c76-bd72-25e70596a93d","resolution":{"observed_at":"2026-08-02T08:03:15.999798Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-02T01:05:57.362450Z","title":"Resumming post- Minkowskian and post-Newtonian gravitational wave- form expansions,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.14802","last_updated":"2026-07-16T10:19:10Z","snapshot_observed_at":"2026-08-16T10:48:15.903476Z","submitted_at":"2026-07-16T10:19:10Z","title":"The radial action for massive particles in spherically symmetric geometries: Exact resummation at any PM order","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-02T01:05:57.362450Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2607.14802"},"observation_digest":"sha256:00e65d1e1c42f41302476185a07a8cc3559ff56f6d0327a246878550df808945","observation_id":"c6434b4a-2421-4b78-8134-c478a50ba3d5","resolution":{"observed_at":"2026-08-02T01:05:57.362450Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2501.19257","snapshot_observed_at":"2026-08-05T04:17:53.819213Z","title":"Resumming post-Minkowskian and post-Newtonian gravitational waveform expansions,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.00363","last_updated":"2026-08-01T00:24:38Z","snapshot_observed_at":"2026-08-18T18:08:38.724689Z","submitted_at":"2026-08-01T00:24:38Z","title":"Projecting Gravitational Fluctuations onto Near-Horizon Throats","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-05T04:17:53.819213Z"},"links":{"cited_paper":"/paper/2501.19257","citing_paper":"/paper/2608.00363"},"observation_digest":"sha256:d04ba9637682c85647ea86d19cd2dfa3308d9422c44c2db6580f022b86c3fd41","observation_id":"6fe7d6c7-2705-4293-94f5-eeb1eb6d5cc3","resolution":{"observed_at":"2026-08-05T04:17:53.819213Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2501.19257/citation-record","integrity":"/paper/2501.19257/integrity","json":"/paper/2501.19257/citation-record.json","paper":"/paper/2501.19257"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2205.01597","last_updated":"2022-05-03T16:20:16Z","snapshot_observed_at":"2026-08-16T17:02:52.550577Z","submitted_at":"2022-05-03T16:20:16Z","title":"New Horizons for Fundamental Physics with LISA","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.01597","snapshot_observed_at":"2026-08-09T20:53:37.681298Z","title":"Rel.25 (2022) 4 [2205.01597]","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.681298Z"},"links":{"cited_paper":"/paper/2205.01597","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:172950259c721bc7e69e8a3cb482d9d50c973991462640f95f8f3acdd152f6ec","observation_id":"96bb5eb2-8e46-43f0-86dc-4ed07991794e","resolution":{"observed_at":"2026-08-09T20:53:37.681298Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1904.05363","last_updated":"2019-06-13T08:23:28Z","snapshot_observed_at":"2026-07-06T07:45:18.053726Z","submitted_at":"2019-04-10T18:00:05Z","title":"Testing the nature of dark compact objects: a status report","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1904.05363","snapshot_observed_at":"2026-08-09T20:53:37.697090Z","title":"Cardoso and P","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.697090Z"},"links":{"cited_paper":"/paper/1904.05363","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:3849c987f82cec6edd56fd5b912d193ab7dc03743d403f5078149baec61e0fc1","observation_id":"09450f37-8f25-4596-8880-08e70e0fd9bb","resolution":{"observed_at":"2026-08-09T20:53:37.697090Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.5575","last_updated":"2013-09-13T21:16:58Z","snapshot_observed_at":"2026-08-16T00:44:59.697572Z","submitted_at":"2012-12-21T20:04:28Z","title":"Testing General Relativity with Low-Frequency, Space-Based Gravitational-Wave Detectors","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.5575","snapshot_observed_at":"2026-08-09T20:53:37.703865Z","title":null,"venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.703865Z"},"links":{"cited_paper":"/paper/1212.5575","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:9433a3729023e5815c22f8fb2d4f192142bd767afafff5c197ee1ce66512b7f0","observation_id":"a370888f-7ad4-4101-9c8e-5d9f24c62c99","resolution":{"observed_at":"2026-08-09T20:53:37.703865Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1304.3473","last_updated":"2013-11-05T15:48:58Z","snapshot_observed_at":"2026-08-15T00:21:45.830365Z","submitted_at":"2013-04-11T20:14:32Z","title":"Gravitational Wave Tests of General Relativity with Ground-Based Detectors and Pulsar Timing Arrays","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1304.3473","snapshot_observed_at":"2026-08-09T20:53:37.710189Z","title":"Yunes and X","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.710189Z"},"links":{"cited_paper":"/paper/1304.3473","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:97fa5df5a5d7a658b76c72d74fbb8d0d3edd7d78c2ed3b97a949859b3e1712be","observation_id":"aae87164-3680-4751-b525-b7fe828fecc0","resolution":{"observed_at":"2026-08-09T20:53:37.710189Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:37.721213Z","title":"Thorne,Multipole Expansions of Gravitational Radiation, Rev","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.721213Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:e97cb6032bcd1306aa4df6ee98df2e04e90b0a36952a451f47d3416bb96f07a8","observation_id":"10cd1a2e-ad30-4e16-a4fc-41aaf6bc325f","resolution":{"observed_at":"2026-08-09T20:53:37.721213Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:37.727692Z","title":"Damour,GRAVITATIONAL RADIATION AND THE MOTION OF COMPACT BODIES, inLes Houches Summer School on Gravitational Radiation, 8, 1982","venue":null,"work_id":null,"year":1982},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.727692Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:3724cbab6ab16baad8437c524a6151d76408eb8d8be87f814dffd75ab31a24c0","observation_id":"3a4f6850-4177-4eb0-9885-755de98c3f8f","resolution":{"observed_at":"2026-08-09T20:53:37.727692Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1310.1528","last_updated":"2024-07-12T19:24:23Z","snapshot_observed_at":"2026-07-06T03:24:52.562608Z","submitted_at":"2013-10-06T02:23:37Z","title":"Post-Newtonian Theory for Gravitational Waves","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1310.1528","snapshot_observed_at":"2026-08-09T20:53:37.769999Z","title":"Blanchet,Post-Newtonian Theory for Gravitational Waves, Living Rev","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.769999Z"},"links":{"cited_paper":"/paper/1310.1528","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:b389756c960e805aad9d3441921b626d2a41f3be9bb5b83fed692a4289cd33bd","observation_id":"b4d458b7-f563-48d0-89bd-0a312fc1118c","resolution":{"observed_at":"2026-08-09T20:53:37.769999Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:37.800381Z","title":"Teukolsky,Perturbations of a rotating black hole","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.800381Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:e05ca3ce4d7cb4d4e5ef1e89343aa0c039043e4dd191f43ad2420479f291fae6","observation_id":"a52d495f-13ab-4d42-b29c-d52209958174","resolution":{"observed_at":"2026-08-09T20:53:37.800381Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:37.824404Z","title":"Poisson,Gravitational radiation from a particle in circular orbit around a black hole","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.824404Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:c8cb8512a6d26ce5def86f7a5072acbfcfd7537724f8403a533d0e00ec3069a8","observation_id":"e12dc6cf-5de1-42cc-aa53-2a07fe0431b8","resolution":{"observed_at":"2026-08-09T20:53:37.824404Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:37.866870Z","title":"Tagoshi and T","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.866870Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:372833571698827f3b61d5e8c2bb3d49fac2f5f6bcaf7a69ec775a5f18d2278e","observation_id":"b5c2edc8-0e95-45b5-89a2-04ef0d4108d6","resolution":{"observed_at":"2026-08-09T20:53:37.866870Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9412027","last_updated":"1994-12-08T18:50:20Z","snapshot_observed_at":"2026-07-07T03:25:05.188192Z","submitted_at":"1994-12-08T18:50:20Z","title":"Gravitational radiation from a particle in circular orbit around a black hole. V. Black-hole absorption and tail corrections","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9412027","snapshot_observed_at":"2026-08-09T20:53:37.892836Z","title":"Poisson and M","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.892836Z"},"links":{"cited_paper":"/paper/gr-qc/9412027","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:6b58fef16ccfcda314631ea3cfeebad857903790687825afbd816060327a2819","observation_id":"a575e88e-434e-4dec-ae85-c46679439ab1","resolution":{"observed_at":"2026-08-09T20:53:37.892836Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9409054","last_updated":"1994-09-27T10:26:08Z","snapshot_observed_at":"2026-07-07T03:24:55.788627Z","submitted_at":"1994-09-27T10:26:08Z","title":"Gravitational Waves from a Particle Orbiting Around a Rotating Black Holes: Post-Newtonian Expansion","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9409054","snapshot_observed_at":"2026-08-09T20:53:37.919797Z","title":"Shibata, M","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.919797Z"},"links":{"cited_paper":"/paper/gr-qc/9409054","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:a6c1e0dcd8750ddf6f0d068694757074387548eded5f0ce537f406f7729410db","observation_id":"0b3d97bb-1403-4d81-b568-ea4d9b882fc0","resolution":{"observed_at":"2026-08-09T20:53:37.919797Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9405062","last_updated":"1994-05-26T01:47:37Z","snapshot_observed_at":"2026-07-07T03:24:45.763672Z","submitted_at":"1994-05-26T01:47:37Z","title":"Post-Newtonian expansion of gravitational waves from a particle in circular orbit around a Schwarzschild black hole","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9405062","snapshot_observed_at":"2026-08-09T20:53:37.943444Z","title":"Tagoshi and M","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.943444Z"},"links":{"cited_paper":"/paper/gr-qc/9405062","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:abd8b7bf4fb9a7fb1594b36f6a6bc7af98f43959f86515edc864f188e2ebea31","observation_id":"321975a5-6881-4f1a-9c27-cbc35228dcd2","resolution":{"observed_at":"2026-08-09T20:53:37.943444Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9701050","last_updated":"1997-01-23T11:43:37Z","snapshot_observed_at":"2026-07-07T03:27:12.065931Z","submitted_at":"1997-01-23T11:43:37Z","title":"Gravitational Waves by a Particle in Circular Orbits around a Schwarzschild black hole -5.5 Post-Newtonian Formula-","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9701050","snapshot_observed_at":"2026-08-09T20:53:37.948855Z","title":"Tanaka, H","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.948855Z"},"links":{"cited_paper":"/paper/gr-qc/9701050","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:4fbba57cea5977d3206e462bee01cd949850425dd1bcbdda0e872210630767c0","observation_id":"55bcd8c0-5249-4e95-9072-6af45e9f17e5","resolution":{"observed_at":"2026-08-09T20:53:37.948855Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9603020","last_updated":"1996-03-19T11:02:41Z","snapshot_observed_at":"2026-08-03T02:19:57.709639Z","submitted_at":"1996-03-13T11:36:48Z","title":"Analytic Solutions of the Teukolsky Equation and their Low Frequency Expansions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9603020","snapshot_observed_at":"2026-08-09T20:53:37.954091Z","title":null,"venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.954091Z"},"links":{"cited_paper":"/paper/gr-qc/9603020","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:439abb2721154e15666320ca83e1268024cb342019786fa0638ea650752a32a8","observation_id":"326cb6f8-ebab-4a26-b081-9e7ed633ead0","resolution":{"observed_at":"2026-08-09T20:53:37.954091Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9712057","last_updated":"1997-12-12T09:46:08Z","snapshot_observed_at":"2026-08-14T20:10:53.581348Z","submitted_at":"1997-12-12T09:46:08Z","title":"Black Hole Perturbation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9712057","snapshot_observed_at":"2026-08-09T20:53:37.960074Z","title":null,"venue":null,"work_id":null,"year":1997},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.960074Z"},"links":{"cited_paper":"/paper/gr-qc/9712057","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:2f739da3959bb8d33cd54ba5f3ed3f57f8148abce0cdcf825d47c9a1a650b8e2","observation_id":"7fc25759-227f-42a0-94ca-567b722adedc","resolution":{"observed_at":"2026-08-09T20:53:37.960074Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/9805064","last_updated":"1998-05-18T08:45:42Z","snapshot_observed_at":"2026-07-07T03:28:59.266332Z","submitted_at":"1998-05-18T08:45:42Z","title":"Perturbations of Kerr-de Sitter Black Hole and Heun's Equations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/9805064","snapshot_observed_at":"2026-08-09T20:53:37.966004Z","title":"Suzuki, E","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.966004Z"},"links":{"cited_paper":"/paper/gr-qc/9805064","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:083ace2d135a24df3199dbe8972add077811b74b401c2fd898bd9ba24e310e9a","observation_id":"e4e8c5fe-2c78-43c4-8d31-f8c11a645661","resolution":{"observed_at":"2026-08-09T20:53:37.966004Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1005.2266","last_updated":"2010-09-01T11:30:12Z","snapshot_observed_at":"2026-08-17T17:45:58.856103Z","submitted_at":"2010-05-13T08:00:18Z","title":"Spherical harmonic modes of 5.5 post-Newtonian gravitational wave polarizations and associated factorized resummed waveforms for a particle in circular orbit around a Schwarzschild black hol","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1005.2266","snapshot_observed_at":"2026-08-09T20:53:37.972899Z","title":"Fujita and B.R","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.972899Z"},"links":{"cited_paper":"/paper/1005.2266","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:a7007157038b9ada32d5c9a9d7bc0cf89d70f2cfd7cc602ec9ddafc12a5e7c41","observation_id":"7fa7d288-5743-4b6c-a65a-8c6a4d71311d","resolution":{"observed_at":"2026-08-09T20:53:37.972899Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1104.5615","last_updated":"2012-08-27T15:40:01Z","snapshot_observed_at":"2026-08-17T20:44:42.053724Z","submitted_at":"2011-04-29T12:51:19Z","title":"Gravitational radiation for extreme mass ratio inspirals to the 14th post-Newtonian order","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1104.5615","snapshot_observed_at":"2026-08-09T20:53:37.978852Z","title":"Fujita,Gravitational radiation for extreme mass ratio inspirals to the 14th post-Newtonian order, Prog","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.978852Z"},"links":{"cited_paper":"/paper/1104.5615","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:552682fb293fb77cdfe1c096aa30ed4258bf2afb275b25585628c3985427961d","observation_id":"dbdbe480-492e-4eda-8ba8-f6bdc1633a5d","resolution":{"observed_at":"2026-08-09T20:53:37.978852Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1211.5535","last_updated":"2012-11-23T16:04:44Z","snapshot_observed_at":"2026-08-15T00:38:22.600035Z","submitted_at":"2012-11-23T16:04:44Z","title":"Gravitational Waves from a Particle in Circular Orbits around a Schwarzschild Black Hole to the 22nd Post-Newtonian Order","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1211.5535","snapshot_observed_at":"2026-08-09T20:53:37.984680Z","title":"Fujita,Gravitational Waves from a Particle in Circular Orbits around a Schwarzschild Black Hole to the 22nd Post-Newtonian Order, Prog","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.984680Z"},"links":{"cited_paper":"/paper/1211.5535","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:71ee30afaaff59025f4e984f389ac55614da0e0ee593fd98704ca4bb3e62b896","observation_id":"060d4310-a65f-46a9-833c-a8282d587a90","resolution":{"observed_at":"2026-08-09T20:53:37.984680Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:37.992007Z","title":"Cutler, E","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:37.992007Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:b1d722edfc79a68be7ffd48cc016e319f1848cf800751e9a708523ceaca6dfe9","observation_id":"375c3f90-33d2-48ce-8ea9-85ac821a1191","resolution":{"observed_at":"2026-08-09T20:53:37.992007Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0811.2069","last_updated":"2009-03-11T13:55:12Z","snapshot_observed_at":"2026-08-15T10:02:08.006230Z","submitted_at":"2008-11-13T11:33:11Z","title":"Improved resummation of post-Newtonian multipolar waveforms from circularized compact binaries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0811.2069","snapshot_observed_at":"2026-08-09T20:53:38.003708Z","title":"Damour, B.R","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.003708Z"},"links":{"cited_paper":"/paper/0811.2069","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:91815e160e4725d69384445c22405e18ee1743baef8ca8ae7e82cb94edc04916","observation_id":"074bd1fc-f180-4294-864f-6ae933a8e094","resolution":{"observed_at":"2026-08-09T20:53:38.003708Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0902.0136","last_updated":"2009-03-19T16:07:44Z","snapshot_observed_at":"2026-08-16T11:29:16.214056Z","submitted_at":"2009-02-02T18:58:48Z","title":"An improved analytical description of inspiralling and coalescing black-hole binaries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0902.0136","snapshot_observed_at":"2026-08-09T20:53:38.013931Z","title":"Damour and A","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.013931Z"},"links":{"cited_paper":"/paper/0902.0136","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:ee299232c4d6b0b32838974d6606a6922605489540222074524faefa640f925a","observation_id":"8f08e297-e0e5-4d90-8658-d25ae20d853d","resolution":{"observed_at":"2026-08-09T20:53:38.013931Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0907.0700","last_updated":"2009-07-03T19:31:53Z","snapshot_observed_at":"2026-08-15T05:44:27.431525Z","submitted_at":"2009-07-03T19:31:53Z","title":"Comparison of post-Newtonian templates for compact binary inspiral signals in gravitational-wave detectors","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0907.0700","snapshot_observed_at":"2026-08-09T20:53:38.020379Z","title":"Buonanno, B","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.020379Z"},"links":{"cited_paper":"/paper/0907.0700","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:8c1183ee33e1c20544a129b79eef20de0e89dfe1843c6dc3bb3e76926f0e4efe","observation_id":"5440c0b7-40a7-4ff3-b9a9-6906b9d5d963","resolution":{"observed_at":"2026-08-09T20:53:38.020379Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1212.4357","last_updated":"2013-04-15T10:35:39Z","snapshot_observed_at":"2026-08-18T05:01:50.542367Z","submitted_at":"2012-12-18T14:19:28Z","title":"Improved effective-one-body description of coalescing nonspinning black-hole binaries and its numerical-relativity completion","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1212.4357","snapshot_observed_at":"2026-08-09T20:53:38.027429Z","title":"Damour, A","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.027429Z"},"links":{"cited_paper":"/paper/1212.4357","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:32e2de229330a9117a36badb150aa016a9798a7b63cccc062ad31ddbc4605cd8","observation_id":"6856b00a-40e5-4c90-9b89-125ea42e4229","resolution":{"observed_at":"2026-08-09T20:53:38.027429Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2006.06111","last_updated":"2020-06-10T23:30:06Z","snapshot_observed_at":"2026-08-03T15:37:21.999327Z","submitted_at":"2020-06-10T23:30:06Z","title":"Black Hole Quasinormal Modes and Seiberg-Witten Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2006.06111","snapshot_observed_at":"2026-08-09T20:53:38.033019Z","title":"Aminov, A","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.033019Z"},"links":{"cited_paper":"/paper/2006.06111","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:1d96cbbcb16aa01b0de8364093c53f5fdd3bf81d3db4bc95e4f2f2af9ed69c3b","observation_id":"fad37884-43c0-441b-b59b-19b581e8660b","resolution":{"observed_at":"2026-08-09T20:53:38.033019Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.04245","last_updated":"2021-06-21T15:19:54Z","snapshot_observed_at":"2026-08-19T00:55:02.099126Z","submitted_at":"2021-05-10T10:19:52Z","title":"QNMs of branes, BHs and fuzzballs from Quantum SW geometries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.04245","snapshot_observed_at":"2026-08-09T20:53:38.038648Z","title":"Bianchi, D","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.038648Z"},"links":{"cited_paper":"/paper/2105.04245","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:f1993e78969f90c91bcc53986daea387cc38c6ffa7e9631ba011b143e58009b3","observation_id":"64728f82-4a72-44e3-8c25-6fae2d0c42ff","resolution":{"observed_at":"2026-08-09T20:53:38.038648Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.09804","last_updated":"2022-01-11T15:23:32Z","snapshot_observed_at":"2026-08-16T17:55:18.610974Z","submitted_at":"2021-09-20T19:24:30Z","title":"More on the SW-QNM correspondence","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.09804","snapshot_observed_at":"2026-08-09T20:53:38.043915Z","title":"Bianchi, D","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.043915Z"},"links":{"cited_paper":"/paper/2109.09804","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:4668fd66d6e9d614be9b0f69a243b4fdf38f8e3c24f965d9aa62fa736646ee77","observation_id":"77b67942-2f2f-4486-b7ae-565384fcac9e","resolution":{"observed_at":"2026-08-09T20:53:38.043915Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2105.04483","last_updated":"2021-10-13T11:14:02Z","snapshot_observed_at":"2026-08-16T18:25:48.272192Z","submitted_at":"2021-05-10T16:21:44Z","title":"Exact solution of Kerr black hole perturbations via CFT$_2$ and instanton counting. Greybody factor, Quasinormal modes and Love numbers","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2105.04483","snapshot_observed_at":"2026-08-09T20:53:38.049792Z","title":"Bonelli, C","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.049792Z"},"links":{"cited_paper":"/paper/2105.04483","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:b1968e41ffcc6f43a84d4a1314cddc65133ee019e5b1d5e87943d728459ad990","observation_id":"f1ebe78b-84d1-4a82-a8c0-9f014b17c667","resolution":{"observed_at":"2026-08-09T20:53:38.049792Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.04491","last_updated":"2022-08-27T14:04:37Z","snapshot_observed_at":"2026-08-19T02:50:50.614196Z","submitted_at":"2022-01-12T14:33:27Z","title":"Irregular Liouville correlators and connection formulae for Heun functions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.04491","snapshot_observed_at":"2026-08-09T20:53:38.080134Z","title":"Bonelli, C","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.080134Z"},"links":{"cited_paper":"/paper/2201.04491","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:c8536aa1f302c9a31c5880b252509516d32c4ea425f153e895980168aa34526c","observation_id":"e9eba44b-01f5-4e77-a327-3c8b7ab0f087","resolution":{"observed_at":"2026-08-09T20:53:38.080134Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.09437","last_updated":"2022-09-13T12:30:57Z","snapshot_observed_at":"2026-08-16T16:51:56.320174Z","submitted_at":"2022-06-19T15:59:21Z","title":"CFT description of BH's and ECO's: QNMs, superradiance, echoes and tidal responses","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.09437","snapshot_observed_at":"2026-08-09T20:53:38.124794Z","title":"Consoli, F","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.124794Z"},"links":{"cited_paper":"/paper/2206.09437","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:eb78d426ded6aa9a1f14e22a0f84cea9e8f352e611b9741bec55aeaf0eea8966","observation_id":"372ed7f7-1d7b-4875-be1e-59bbaa4bcf36","resolution":{"observed_at":"2026-08-09T20:53:38.124794Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.05965","last_updated":"2024-07-30T23:00:11Z","snapshot_observed_at":"2026-08-18T16:24:39.991999Z","submitted_at":"2023-12-10T18:44:29Z","title":"Black Hole Perturbation Theory Meets CFT$_2$: Kerr Compton Amplitudes from Nekrasov-Shatashvili Functions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.05965","snapshot_observed_at":"2026-08-09T20:53:38.153317Z","title":"Bautista, G","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.153317Z"},"links":{"cited_paper":"/paper/2312.05965","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:cddd91f3e4ffc540e58aba1bd124e01e917e02661672027daaced1041b93e66e","observation_id":"2f619839-02f6-4fcd-b6f8-c194fc1a50c8","resolution":{"observed_at":"2026-08-09T20:53:38.153317Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.10141","last_updated":"2023-11-16T16:54:46Z","snapshot_observed_at":"2026-08-16T15:14:56.451499Z","submitted_at":"2023-07-19T17:10:16Z","title":"Black hole perturbation theory and multiple polylogarithms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.10141","snapshot_observed_at":"2026-08-09T20:53:38.184894Z","title":"Aminov, P","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.184894Z"},"links":{"cited_paper":"/paper/2307.10141","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:fcb4674922e2d31e3dbdac59c097e1ef04f472dd553153e4bddf725da87bdc16","observation_id":"01a0ab15-67cd-43f6-9547-63fbcd0f73a1","resolution":{"observed_at":"2026-08-09T20:53:38.184894Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.10960","last_updated":"2021-09-22T08:10:34Z","snapshot_observed_at":"2026-08-17T23:35:20.733107Z","submitted_at":"2021-03-19T18:00:04Z","title":"Black-hole microstate spectroscopy: ringdown, quasinormal modes, and echoes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.10960","snapshot_observed_at":"2026-08-09T20:53:38.216463Z","title":"Ikeda, M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.216463Z"},"links":{"cited_paper":"/paper/2103.10960","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:ee9d4abccf8af8c61900df328d872911bec24f619df1c0a7063db4194faac714","observation_id":"ba5824c2-7e04-4b0c-ac88-6e7c4159998e","resolution":{"observed_at":"2026-08-09T20:53:38.216463Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.14637","last_updated":"2024-02-21T11:02:52Z","snapshot_observed_at":"2026-08-16T22:27:53.947081Z","submitted_at":"2023-11-24T18:09:25Z","title":"Post Newtonian emission of gravitational waves from binary systems: a gauge theory perspective","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.14637","snapshot_observed_at":"2026-08-09T20:53:38.227468Z","title":"Fucito and J.F","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.227468Z"},"links":{"cited_paper":"/paper/2311.14637","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:7b313e373cae82cd7e1b78a54cdcfa88dd89c7108247191924f28db531b5a362","observation_id":"4c102097-2f5e-4cb0-ba0f-7492c30c4e52","resolution":{"observed_at":"2026-08-09T20:53:38.227468Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.14925","last_updated":"2024-02-03T16:18:44Z","snapshot_observed_at":"2026-08-17T15:15:33.054592Z","submitted_at":"2023-09-26T13:34:04Z","title":"Comparing One-loop Gravitational Bremsstrahlung Amplitudes to the Multipolar-Post-Minkowskian Waveform","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.14925","snapshot_observed_at":"2026-08-09T20:53:38.233201Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.233201Z"},"links":{"cited_paper":"/paper/2309.14925","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:08d17ec810cb3c9df117df46043f194d593938acfbe103dc06d843b7cc633bb9","observation_id":"97a1ff1a-3967-48e3-9369-bfd2161325bb","resolution":{"observed_at":"2026-08-09T20:53:38.233201Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.02076","last_updated":"2024-07-02T09:08:32Z","snapshot_observed_at":"2026-08-16T13:37:49.813790Z","submitted_at":"2024-07-02T09:08:32Z","title":"Gravitational Bremsstrahlung Waveform at the fourth Post-Minkowskian order and the second Post-Newtonian level","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.02076","snapshot_observed_at":"2026-08-09T20:53:38.243104Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.243104Z"},"links":{"cited_paper":"/paper/2407.02076","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:1127959766f3dc659beb19b563962dd677a5f98fea5261664f73e529f658febf","observation_id":"fa5080d5-1197-4a47-b5d2-b29b4a2f86ea","resolution":{"observed_at":"2026-08-09T20:53:38.243104Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.06604","last_updated":"2024-06-21T16:06:26Z","snapshot_observed_at":"2026-08-18T01:36:28.681420Z","submitted_at":"2024-02-09T18:29:57Z","title":"Gravitational Waveform: A Tale of Two Formalisms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.06604","snapshot_observed_at":"2026-08-09T20:53:38.250016Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.250016Z"},"links":{"cited_paper":"/paper/2402.06604","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:63a923e67814017cfa189b79ed7588401d869659eefb0dabe3af8a932015b0c3","observation_id":"81c43200-9a79-4306-8724-4309953d2557","resolution":{"observed_at":"2026-08-09T20:53:38.250016Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2101.12688","last_updated":"2021-04-22T15:48:02Z","snapshot_observed_at":"2026-08-18T23:49:33.084935Z","submitted_at":"2021-01-29T17:17:17Z","title":"Classical Gravitational Bremsstrahlung from a Worldline Quantum Field Theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2101.12688","snapshot_observed_at":"2026-08-09T20:53:38.257584Z","title":"Jakobsen, G","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.257584Z"},"links":{"cited_paper":"/paper/2101.12688","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:0bd909c69b1162e010e562a9d91c779b85aebf984da41a49e258723fbd245893","observation_id":"d6600f22-0e34-40fd-b1e5-7082d87f7ea2","resolution":{"observed_at":"2026-08-09T20:53:38.257584Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2102.08339","last_updated":"2021-06-25T15:58:36Z","snapshot_observed_at":"2026-08-17T11:01:08.484513Z","submitted_at":"2021-02-16T18:24:44Z","title":"Gravitational Bremsstrahlung in the Post-Minkowskian Effective Field Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.08339","snapshot_observed_at":"2026-08-09T20:53:38.264009Z","title":"Mougiakakos, M.M","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.264009Z"},"links":{"cited_paper":"/paper/2102.08339","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:f58c052ebdd6c1fcd090e002fb648358c32b04fe8b3a88174c100374ebd470cd","observation_id":"a50d95e0-6016-406e-8e8e-564b652b4706","resolution":{"observed_at":"2026-08-09T20:53:38.264009Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.10193","last_updated":"2021-07-21T16:36:14Z","snapshot_observed_at":"2026-08-16T18:08:26.737930Z","submitted_at":"2021-07-21T16:36:14Z","title":"Waveforms from Amplitudes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.10193","snapshot_observed_at":"2026-08-09T20:53:38.271081Z","title":"Cristofoli, R","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.271081Z"},"links":{"cited_paper":"/paper/2107.10193","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:535424beda8c50d7406bd3aa4f57f30426c63f4a2073afb1628684e2c360dac6","observation_id":"2a8f33d7-4026-4345-b357-eecfa57d7a0a","resolution":{"observed_at":"2026-08-09T20:53:38.271081Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.16488","last_updated":"2024-07-04T16:47:55Z","snapshot_observed_at":"2026-08-16T15:20:17.105673Z","submitted_at":"2023-06-28T18:22:02Z","title":"The gravitational eikonal: from particle, string and brane collisions to black-hole encounters","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.16488","snapshot_observed_at":"2026-08-09T20:53:38.278809Z","title":"Di Vecchia, C","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.278809Z"},"links":{"cited_paper":"/paper/2306.16488","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:9d04062ed8557ade415d55113b1e70499af0cf4b995e27350715ecc7aa58bd15","observation_id":"9651904f-3952-439e-9a4c-72a4a845de3d","resolution":{"observed_at":"2026-08-09T20:53:38.278809Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.06111","last_updated":"2024-11-06T23:11:44Z","snapshot_observed_at":"2026-08-18T20:45:20.666843Z","submitted_at":"2023-03-10T17:59:59Z","title":"One-loop Gravitational Bremsstrahlung and Waveforms from a Heavy-Mass Effective Field Theory","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.06111","snapshot_observed_at":"2026-08-09T20:53:38.286652Z","title":"Brandhuber, G.R","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.286652Z"},"links":{"cited_paper":"/paper/2303.06111","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:d330dd2b54716d12f92ee3b03fb8ba670ddcee25cda48f9a6919de2ac7d67d2f","observation_id":"cd5645ae-1f9a-4cf8-ac84-447a881d91aa","resolution":{"observed_at":"2026-08-09T20:53:38.286652Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.06112","last_updated":"2023-12-22T17:04:34Z","snapshot_observed_at":"2026-08-18T01:35:02.888421Z","submitted_at":"2023-03-10T18:00:02Z","title":"The Sub-Leading Scattering Waveform from Amplitudes","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.06112","snapshot_observed_at":"2026-08-09T20:53:38.293151Z","title":"Herderschee, R","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.293151Z"},"links":{"cited_paper":"/paper/2303.06112","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:18cce1b9a61f510c735ce04a87c8f2e997bac113ee8bcd8fae6611d25a596d1d","observation_id":"0ffb81d9-df1d-47a0-9ba7-2eedcff09fda","resolution":{"observed_at":"2026-08-09T20:53:38.293151Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.06211","last_updated":"2024-05-15T12:05:10Z","snapshot_observed_at":"2026-08-17T08:00:50.653711Z","submitted_at":"2023-03-10T21:18:45Z","title":"Radiation and Reaction at One Loop","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.06211","snapshot_observed_at":"2026-08-09T20:53:38.300050Z","title":"Elkhidir, D","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.300050Z"},"links":{"cited_paper":"/paper/2303.06211","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:12c0cfb35f9ffab958f7b436fd48ad8da30770e8a8fd78dfdcf7e8a9776fa1b8","observation_id":"1899d352-634d-4560-907d-3b222e117946","resolution":{"observed_at":"2026-08-09T20:53:38.300050Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.07006","last_updated":"2023-12-25T08:48:32Z","snapshot_observed_at":"2026-08-18T01:36:26.968600Z","submitted_at":"2023-03-13T11:01:49Z","title":"Inelastic Exponentiation and Classical Gravitational Scattering at One Loop","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.07006","snapshot_observed_at":"2026-08-09T20:53:38.305611Z","title":"Georgoudis, C","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.305611Z"},"links":{"cited_paper":"/paper/2303.07006","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:a9df99de33c91a53f57178ab4f0df7a2627a9a5fff7321b244dc9bfbd92f186e","observation_id":"76812a38-9da5-4111-8b65-8409a8845a6e","resolution":{"observed_at":"2026-08-09T20:53:38.305611Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.17429","last_updated":"2023-11-02T17:39:26Z","snapshot_observed_at":"2026-08-17T17:41:32.006578Z","submitted_at":"2023-09-29T17:41:24Z","title":"Spinning waveforms from KMOC at leading order","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.17429","snapshot_observed_at":"2026-08-09T20:53:38.315231Z","title":"De Angelis, R","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.315231Z"},"links":{"cited_paper":"/paper/2309.17429","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:ba658ba3f67849deccf7f48d6a454b80bc6fde130969b3d402bfa577e0de6a09","observation_id":"c6114227-e6a0-4cdf-8d69-8f24b5d417a8","resolution":{"observed_at":"2026-08-09T20:53:38.315231Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.04405","last_updated":"2024-02-16T19:15:07Z","snapshot_observed_at":"2026-08-16T14:54:23.761352Z","submitted_at":"2023-10-06T17:54:57Z","title":"Resummed spinning waveforms from five-point amplitudes","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.04405","snapshot_observed_at":"2026-08-09T20:53:38.331826Z","title":"Brandhuber, G.R","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.331826Z"},"links":{"cited_paper":"/paper/2310.04405","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:02c20831c490e3ceb8cc3b67d8baf68207e8db3e63099b2436a93e5dc4ad08f0","observation_id":"87f5c76f-264c-4ac4-a70f-f35b9523206a","resolution":{"observed_at":"2026-08-09T20:53:38.331826Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.07452","last_updated":"2024-01-19T14:45:42Z","snapshot_observed_at":"2026-08-18T01:36:28.107650Z","submitted_at":"2023-12-12T17:25:10Z","title":"An eikonal-inspired approach to the gravitational scattering waveform","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.07452","snapshot_observed_at":"2026-08-09T20:53:38.338613Z","title":"Georgoudis, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.338613Z"},"links":{"cited_paper":"/paper/2312.07452","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:49509964113f0790784e210811ed73fa4ce89eaef632deaf698f0e4010a33edf","observation_id":"610f05c8-5bdf-4f18-95c6-5215fb3edc67","resolution":{"observed_at":"2026-08-09T20:53:38.338613Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.14710","last_updated":"2023-12-22T14:08:18Z","snapshot_observed_at":"2026-08-16T14:32:13.016200Z","submitted_at":"2023-12-22T14:08:18Z","title":"More on the Subleading Gravitational Waveform","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.14710","snapshot_observed_at":"2026-08-09T20:53:38.354923Z","title":"Georgoudis, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.354923Z"},"links":{"cited_paper":"/paper/2312.14710","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:35c7d8f9178d3d46c3b1400baa720f6be431c996d79675e736a65f767bc616f5","observation_id":"b3244d97-1429-47d4-bcf9-e96345bb5b74","resolution":{"observed_at":"2026-08-09T20:53:38.354923Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.06361","last_updated":"2024-05-21T18:25:02Z","snapshot_observed_at":"2026-08-18T01:35:01.738690Z","submitted_at":"2024-02-09T12:12:53Z","title":"Post-Newtonian Multipoles from the Next-to-Leading Post-Minkowskian Gravitational Waveform","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.06361","snapshot_observed_at":"2026-08-09T20:53:38.403366Z","title":"Georgoudis, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.403366Z"},"links":{"cited_paper":"/paper/2402.06361","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:95fcb8a98346eabdc00639dc6ad31af85a8a251927b0df10d8eb10ceaff3386b","observation_id":"4ecadfdf-a222-4d9f-8d77-4f2cb8280910","resolution":{"observed_at":"2026-08-09T20:53:38.403366Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.08009","last_updated":"2024-12-14T16:51:01Z","snapshot_observed_at":"2026-08-16T14:10:27.025980Z","submitted_at":"2024-03-12T18:18:57Z","title":"An Improved Framework for Computing Waveforms","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.08009","snapshot_observed_at":"2026-08-09T20:53:38.435739Z","title":"Brunello and S","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.435739Z"},"links":{"cited_paper":"/paper/2403.08009","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:87828fdc3e56e2f0d6e78d9f7f793019e8a10db65d639f08284907daa9875fe1","observation_id":"421d0884-3d29-4c60-a9e0-71f6c7cecd51","resolution":{"observed_at":"2026-08-09T20:53:38.435739Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.04128","last_updated":"2024-12-30T16:41:43Z","snapshot_observed_at":"2026-08-16T13:36:57.579965Z","submitted_at":"2024-07-04T19:05:04Z","title":"Logarithmic soft theorems and soft spectra","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.04128","snapshot_observed_at":"2026-08-09T20:53:38.467249Z","title":"Alessio, P","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.467249Z"},"links":{"cited_paper":"/paper/2407.04128","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:43d4a6954242296e6de01b52dba4010743d6522d2c99ba09293b61e6a8cbf892","observation_id":"f230545e-2e67-43f1-9bb4-d2038246eed6","resolution":{"observed_at":"2026-08-09T20:53:38.467249Z","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":"2026-08-16T13:26:34.845855Z","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":"2026-08-18T08:51:43.957004Z","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:ffa4882d96de352519ae1721a106eb51531422b04911dd137731660da41f69f1","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":"0912.4254","last_updated":"2010-07-21T19:34:22Z","snapshot_observed_at":"2026-08-15T05:30:39.907937Z","submitted_at":"2009-12-21T20:50:54Z","title":"Gravitational radiative corrections from effective field theory","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0912.4254","snapshot_observed_at":"2026-08-09T20:53:38.506593Z","title":"Goldberger and A","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.506593Z"},"links":{"cited_paper":"/paper/0912.4254","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:aa04c4538352871443de5c63e939e176ff4dbf4ad1b7ac9c24caf8b00973e5f5","observation_id":"58e31f80-97e1-4c43-8cbc-000744eab7af","resolution":{"observed_at":"2026-08-09T20:53:38.506593Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2301.09395","last_updated":"2024-02-15T16:50:18Z","snapshot_observed_at":"2026-08-16T16:00:45.932708Z","submitted_at":"2023-01-23T12:32:10Z","title":"Gravitational-wave tails of memory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2301.09395","snapshot_observed_at":"2026-08-09T20:53:38.515268Z","title":"Trestini and L","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.515268Z"},"links":{"cited_paper":"/paper/2301.09395","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:565df8b58f438cc32cb9b7855cf066d8297aa625086da96f3e648c49b2242d73","observation_id":"9ff562b7-ba73-4bf8-ab1f-4abdb0360ad3","resolution":{"observed_at":"2026-08-09T20:53:38.515268Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2107.02634","last_updated":"2025-05-23T01:40:57Z","snapshot_observed_at":"2026-08-16T18:11:58.631969Z","submitted_at":"2021-07-06T14:18:52Z","title":"Gravitational Multipole Renormalization","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2107.02634","snapshot_observed_at":"2026-08-09T20:53:38.522852Z","title":"Almeida, S","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.522852Z"},"links":{"cited_paper":"/paper/2107.02634","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:1ce94e4b39c7e3b39735a9bbcaa76404ebeb4093a323c355e11ea6d8e75d6e36","observation_id":"2aca2a58-3304-4ff9-9983-59fe3ce2e0ee","resolution":{"observed_at":"2026-08-09T20:53:38.522852Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.20066","last_updated":"2024-08-24T20:21:19Z","snapshot_observed_at":"2026-08-18T22:51:24.688611Z","submitted_at":"2023-10-30T22:31:34Z","title":"Higher-order tails and RG flows due to scattering of gravitational radiation from binary inspirals","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2310.20066","snapshot_observed_at":"2026-08-09T20:53:38.535374Z","title":"Edison and M","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.535374Z"},"links":{"cited_paper":"/paper/2310.20066","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:03900ea3247f6cb0d81a414794a162c5b97e933800ad50a583d4c4c7cd8c4e22","observation_id":"e8eeed84-717e-4264-bc8f-decf65a47805","resolution":{"observed_at":"2026-08-09T20:53:38.535374Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.11434","last_updated":"2022-03-25T18:16:20Z","snapshot_observed_at":"2026-08-16T17:32:53.218629Z","submitted_at":"2021-12-21T18:52:09Z","title":"A new method for exact results on Quasinormal Modes of Black Holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.11434","snapshot_observed_at":"2026-08-09T20:53:38.542137Z","title":"Fioravanti and D","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.542137Z"},"links":{"cited_paper":"/paper/2112.11434","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:955904e8dafc80830a00796b616d6ba85453b8fcb9f876636b4a8161530cf63f","observation_id":"f0e77f71-2648-43eb-9f41-4355ab33a8c3","resolution":{"observed_at":"2026-08-09T20:53:38.542137Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.14900","last_updated":"2022-03-28T17:04:45Z","snapshot_observed_at":"2026-08-16T17:11:13.757697Z","submitted_at":"2022-03-28T17:04:45Z","title":"Turning rotating D-branes and BHs inside out their photon-halo","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.14900","snapshot_observed_at":"2026-08-09T20:53:38.549335Z","title":"Bianchi and G","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.549335Z"},"links":{"cited_paper":"/paper/2203.14900","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:b20afa790b98635fb0cb6c64ec47f4d230853f22cb72a31595521ecb567edead","observation_id":"42c84d30-a991-4677-a57e-58f63f474bd0","resolution":{"observed_at":"2026-08-09T20:53:38.549335Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2204.09749","last_updated":"2022-08-30T12:12:30Z","snapshot_observed_at":"2026-08-16T17:05:42.197092Z","submitted_at":"2022-04-20T19:18:05Z","title":"Gravitational orbits, double-twist mirage, and many-body scars","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2204.09749","snapshot_observed_at":"2026-08-09T20:53:38.555125Z","title":"Dodelson and A","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.555125Z"},"links":{"cited_paper":"/paper/2204.09749","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:d0d7372731ad08f650f296801f70ac1d113f4adef39eb0f28ead0de750a5ca37","observation_id":"8870853f-53ee-4a0c-868f-12a5448c469c","resolution":{"observed_at":"2026-08-09T20:53:38.555125Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2206.07720","last_updated":"2022-09-16T18:20:34Z","snapshot_observed_at":"2026-08-16T16:52:43.938816Z","submitted_at":"2022-06-15T18:00:01Z","title":"Holographic thermal correlators from supersymmetric instantons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.07720","snapshot_observed_at":"2026-08-09T20:53:38.560661Z","title":"Dodelson, A","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.560661Z"},"links":{"cited_paper":"/paper/2206.07720","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:9361027c5da0f202c0ac6e0303ecfd7e918170e184e68cf875559b68eb266446","observation_id":"625aa0ee-1a18-4ca5-959c-b853f3b321f9","resolution":{"observed_at":"2026-08-09T20:53:38.560661Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.09961","last_updated":"2022-09-28T08:05:00Z","snapshot_observed_at":"2026-08-16T16:44:32.642667Z","submitted_at":"2022-07-20T15:12:19Z","title":"Quasi-normal modes for the D3-branes and Exact WKB analysis","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.09961","snapshot_observed_at":"2026-08-09T20:53:38.568079Z","title":"Imaizumi,Quasi-normal modes for the D3-branes and Exact WKB analysis, Phys","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.568079Z"},"links":{"cited_paper":"/paper/2207.09961","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:e4747f8cba99e7676366295cbb2f78c9210973ae115195399b68a360b7a9582b","observation_id":"3b36c33f-d314-4267-a3a8-41a798e5a8a6","resolution":{"observed_at":"2026-08-09T20:53:38.568079Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:38.574142Z","title":"Fioravanti, D","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.574142Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:16f8bff1b257a899de6eacdb36d8aa50a8595f9a5699840aeea4b4fac8037ac9","observation_id":"bcd58b0f-531d-4fbe-943d-e1053420c708","resolution":{"observed_at":"2026-08-09T20:53:38.574142Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.04738","last_updated":"2022-12-09T09:16:33Z","snapshot_observed_at":"2026-08-16T16:09:51.247197Z","submitted_at":"2022-12-09T09:16:33Z","title":"Exact conditions for Quasi-normal modes of extremal M5-branes and Exact WKB analysis","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.04738","snapshot_observed_at":"2026-08-09T20:53:38.580113Z","title":"Imaizumi,Exact conditions for quasi-normal modes of extremal M5-branes and exact WKB analysis, Nucl","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.580113Z"},"links":{"cited_paper":"/paper/2212.04738","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:cafb808a26ef1c91bf7cc229964d9028e868b72b758008fde3b0f322471861c8","observation_id":"6e2c699a-9e85-421e-8779-ef048142e045","resolution":{"observed_at":"2026-08-09T20:53:38.580113Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.07504","last_updated":"2022-12-14T21:04:57Z","snapshot_observed_at":"2026-08-18T22:51:25.197397Z","submitted_at":"2022-12-14T21:04:57Z","title":"2-charge circular fuzz-balls and their perturbations","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.07504","snapshot_observed_at":"2026-08-09T20:53:38.588866Z","title":"Bianchi and G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.588866Z"},"links":{"cited_paper":"/paper/2212.07504","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:89939c43fcaa04afb9fa2470b9aa181314a0960efcee76ae766cf2a199c5ab5d","observation_id":"d4ebd234-b1d3-4c7e-8f6f-10943725c7d1","resolution":{"observed_at":"2026-08-09T20:53:38.588866Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2304.12339","last_updated":"2023-09-15T15:25:50Z","snapshot_observed_at":"2026-08-16T15:38:05.412312Z","submitted_at":"2023-04-24T18:00:00Z","title":"A thermal product formula","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2304.12339","snapshot_observed_at":"2026-08-09T20:53:38.595813Z","title":"Dodelson, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.595813Z"},"links":{"cited_paper":"/paper/2304.12339","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:a57d0bbe613f15b2705aeaca875a0ed4206ad944aa1fe181b6a86a0d8e33b9ec","observation_id":"ca001565-567d-4b42-8ccb-4bdb3ff7822f","resolution":{"observed_at":"2026-08-09T20:53:38.595813Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.00865","last_updated":"2023-05-01T15:07:01Z","snapshot_observed_at":"2026-08-16T15:36:30.557962Z","submitted_at":"2023-05-01T15:07:01Z","title":"Charge instability of JMaRT geometries","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.00865","snapshot_observed_at":"2026-08-09T20:53:38.601194Z","title":"Bianchi, C","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.601194Z"},"links":{"cited_paper":"/paper/2305.00865","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:cb140d892d4ad5692e144018d060f052874f9d07da5af9d0ac437a86e98ef9e3","observation_id":"f7092d54-8708-4f39-98d0-e413f7fd8396","resolution":{"observed_at":"2026-08-09T20:53:38.601194Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.15105","last_updated":"2023-09-01T10:12:22Z","snapshot_observed_at":"2026-08-18T17:30:58.520491Z","submitted_at":"2023-05-24T12:48:14Z","title":"On the stability and deformability of top stars","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.15105","snapshot_observed_at":"2026-08-09T20:53:38.607695Z","title":"Bianchi, G","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.607695Z"},"links":{"cited_paper":"/paper/2305.15105","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:7035a65d8e4c69d506adf7163210169813629e06a6026de094a61c5511270bca","observation_id":"ed0eb800-3439-4d23-b368-89f176b50916","resolution":{"observed_at":"2026-08-09T20:53:38.607695Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.15305","last_updated":"2023-11-08T09:46:19Z","snapshot_observed_at":"2026-08-17T23:35:36.930164Z","submitted_at":"2023-06-27T08:48:33Z","title":"The black hole behind the cut","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.15305","snapshot_observed_at":"2026-08-09T20:53:38.614943Z","title":"Giusto, C","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.614943Z"},"links":{"cited_paper":"/paper/2306.15305","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:40bd1019dc28ed70df915455ad1dc0d57e450643ef5258dd56480b93a9808ee6","observation_id":"153dc5aa-bed7-4c99-8405-43ddc238c0fb","resolution":{"observed_at":"2026-08-09T20:53:38.614943Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2307.12824","last_updated":"2023-07-24T14:22:25Z","snapshot_observed_at":"2026-08-16T15:13:45.929352Z","submitted_at":"2023-07-24T14:22:25Z","title":"Absorption cross section in gravity's rainbow from confluent Heun equation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.12824","snapshot_observed_at":"2026-08-09T20:53:38.636620Z","title":"Barragán Amado, K","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.636620Z"},"links":{"cited_paper":"/paper/2307.12824","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:e837e082507bacf40f3c829f8eedb949882e8eb89c5c768e21cbb9f2b3ee2277","observation_id":"eaba7a7d-0399-43fd-861f-6097abeb56f7","resolution":{"observed_at":"2026-08-09T20:53:38.636620Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2308.16677","last_updated":"2024-01-30T15:41:29Z","snapshot_observed_at":"2026-08-16T15:04:19.359430Z","submitted_at":"2023-08-31T12:28:39Z","title":"Quasinormal Modes of C-metric from SCFTs","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2308.16677","snapshot_observed_at":"2026-08-09T20:53:38.658020Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.658020Z"},"links":{"cited_paper":"/paper/2308.16677","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:b0c5a2b417010ae0c47cf7cca91f1bd2c41576f33866f6c2a49e6c9ca5ae7d05","observation_id":"be5461a9-de6c-43a5-938b-888af8533e64","resolution":{"observed_at":"2026-08-09T20:53:38.658020Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.11355","last_updated":"2024-02-24T13:43:52Z","snapshot_observed_at":"2026-08-16T14:59:05.664054Z","submitted_at":"2023-09-20T14:36:36Z","title":"Scalar quasi-normal modes of accelerating Kerr-Newman-AdS black holes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.11355","snapshot_observed_at":"2026-08-09T20:53:38.679862Z","title":"Barragán Amado and B","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.679862Z"},"links":{"cited_paper":"/paper/2309.11355","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:2ca512f10cb93d44dc7f5df1068128eeaeaacfba04eccbb070e2af05ec19b142","observation_id":"1aa8d139-410f-47ce-8035-2e17642c10e4","resolution":{"observed_at":"2026-08-09T20:53:38.679862Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.17441","last_updated":"2024-02-27T11:54:00Z","snapshot_observed_at":"2026-08-16T14:14:56.238523Z","submitted_at":"2024-02-27T11:54:00Z","title":"Duality between Seiberg-Witten Theory and Black Hole Superradiance","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.17441","snapshot_observed_at":"2026-08-09T20:53:38.701670Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.701670Z"},"links":{"cited_paper":"/paper/2402.17441","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:230195b727c893da8614bd06f736790c1632052bc94b4d022a4c8634bea968cf","observation_id":"438656c4-93c6-4d99-a5aa-954379dee958","resolution":{"observed_at":"2026-08-09T20:53:38.701670Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.06566","last_updated":"2024-05-20T09:40:30Z","snapshot_observed_at":"2026-08-18T08:50:56.976160Z","submitted_at":"2024-05-10T16:10:39Z","title":"Charge (in)stability and superradiance of Topological Stars","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.06566","snapshot_observed_at":"2026-08-09T20:53:38.722343Z","title":"Cipriani, C","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.722343Z"},"links":{"cited_paper":"/paper/2405.06566","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:95daf002a2b69c09df14c8ac11468e77b774fa0bebdf52169b2562f5f352b6c3","observation_id":"c9fc27c8-5212-4c07-b752-e997c6234aa1","resolution":{"observed_at":"2026-08-09T20:53:38.722343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.13830","last_updated":"2025-01-13T13:40:10Z","snapshot_observed_at":"2026-08-17T01:10:35.580856Z","submitted_at":"2024-05-22T16:58:05Z","title":"One loop effective actions in Kerr-(A)dS Black Holes","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.13830","snapshot_observed_at":"2026-08-09T20:53:38.744015Z","title":"Arnaudo, G","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.744015Z"},"links":{"cited_paper":"/paper/2405.13830","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:4dbc9258bcbcedc07ba4153ac8b30043e583973e86e6f2f0811948a949de6849","observation_id":"ac615d1e-5923-4ba7-97a4-c3a9eda2aeb1","resolution":{"observed_at":"2026-08-09T20:53:38.744015Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.10868","last_updated":"2024-07-15T16:14:28Z","snapshot_observed_at":"2026-08-18T16:56:06.360323Z","submitted_at":"2024-07-15T16:14:28Z","title":"Scalar perturbations in a Top-Star spacetime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.10868","snapshot_observed_at":"2026-08-09T20:53:38.750974Z","title":"Bianchi, D","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.750974Z"},"links":{"cited_paper":"/paper/2407.10868","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:3d9ccf56bfb76b26620ea987b4a776d97878697df0b1c2395f7fd8159d7a01d7","observation_id":"2a934dd7-82ea-44c6-ba30-567fb3d3539a","resolution":{"observed_at":"2026-08-09T20:53:38.750974Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.03243","last_updated":"2024-08-06T15:05:24Z","snapshot_observed_at":"2026-08-16T13:28:10.755679Z","submitted_at":"2024-08-06T15:05:24Z","title":"Gauge theory meets cosmology","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.03243","snapshot_observed_at":"2026-08-09T20:53:38.756894Z","title":"Bianchi, G","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.756894Z"},"links":{"cited_paper":"/paper/2408.03243","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:cab641dfba4fdb9c78b5e3d311c2fdda40ab1cf51007d2ecab30c98d11aeeafd","observation_id":"a4c9da50-7cdd-4a08-9ae0-320b403b5418","resolution":{"observed_at":"2026-08-09T20:53:38.756894Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.06621","last_updated":"2024-02-09T18:55:40Z","snapshot_observed_at":"2026-08-18T19:50:41.934556Z","submitted_at":"2024-02-09T18:55:40Z","title":"Tidal resonances for fuzzballs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.06621","snapshot_observed_at":"2026-08-09T20:53:38.763616Z","title":"Di Russo, F","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.763616Z"},"links":{"cited_paper":"/paper/2402.06621","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:3bec0399a7e477aa27567ccb6871912113404a6fb0c3ce116f6092d5027bc54a","observation_id":"f5091291-1f74-4a3d-af9e-df916afeb23e","resolution":{"observed_at":"2026-08-09T20:53:38.763616Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2411.19612","last_updated":"2024-11-29T11:04:51Z","snapshot_observed_at":"2026-08-16T02:31:50.400919Z","submitted_at":"2024-11-29T11:04:51Z","title":"Scalar waves in a Topological Star spacetime: self-force and radiative losses","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.19612","snapshot_observed_at":"2026-08-09T20:53:38.769607Z","title":"Bianchi, D","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.769607Z"},"links":{"cited_paper":"/paper/2411.19612","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:1d49d3c8ee36b2c357ce4115cd59bea0d307b4a2342b9f8783937ab5c9e33a76","observation_id":"d05212e0-dace-4b46-aa82-b1135c0a1d3a","resolution":{"observed_at":"2026-08-09T20:53:38.769607Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.06760","last_updated":"2024-09-25T14:35:19Z","snapshot_observed_at":"2026-08-16T13:19:40.878845Z","submitted_at":"2024-09-10T17:31:26Z","title":"Basics of Multiple Polyexponential Integrals","version":2},"cited_work":{"arxiv_id":"2409.06760","doi":null,"metadata_source":"pith","pith_arxiv_id":"2409.06760","snapshot_observed_at":"2026-08-09T20:53:39.303658Z","title":"Basics of Multiple Polyexponential Integrals","venue":"math.CA","work_id":"ca6232a6-663f-4310-b087-cd5f2af30ff6","year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.804023Z"},"links":{"cited_paper":"/paper/2409.06760","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:c6d2bccf74acf4ebb15dc399e17fd68e7c427a9600de9deead56100e963ec6d8","observation_id":"b9aab628-bdbe-49cd-89ea-65bc6651349e","resolution":{"observed_at":"2026-08-09T20:53:39.309767Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.07370","last_updated":"2024-09-11T16:01:24Z","snapshot_observed_at":"2026-08-16T13:19:24.098335Z","submitted_at":"2024-09-11T16:01:24Z","title":"The effect of resummation on retarded Green's function and greybody factor in $AdS$ black holes","version":1},"cited_work":{"arxiv_id":"2409.07370","doi":null,"metadata_source":"pith","pith_arxiv_id":"2409.07370","snapshot_observed_at":"2026-08-09T20:53:39.193867Z","title":"The effect of resummation on retarded Green's function and greybody factor in $AdS$ black holes","venue":"hep-th","work_id":"b039fd0c-2be1-41eb-bb74-c63f690eaa64","year":2024},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.813873Z"},"links":{"cited_paper":"/paper/2409.07370","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:5779494622b718547e507aa9d3ccbb8bf5a9ab859aa8145e08426b3db6682d07","observation_id":"304dda7f-7d22-49fa-8719-9adbf125bd21","resolution":{"observed_at":"2026-08-09T20:53:39.246459Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2411.03382","last_updated":"2025-01-22T15:19:00Z","snapshot_observed_at":"2026-08-16T13:02:40.335590Z","submitted_at":"2024-11-05T18:11:00Z","title":"Absorptive Effects in Black Hole Scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2411.03382","snapshot_observed_at":"2026-08-09T20:53:38.824916Z","title":"Bautista, Y.-T","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.824916Z"},"links":{"cited_paper":"/paper/2411.03382","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:b14ad5a0c01baf61eb3838c6eaee0a54113b70a43f96ff0c6ff523cb85f4890d","observation_id":"3055b62b-92aa-4f47-ba81-1dc3e61244eb","resolution":{"observed_at":"2026-08-09T20:53:38.824916Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.18359","last_updated":"2025-06-06T03:54:35Z","snapshot_observed_at":"2026-08-16T12:59:59.166944Z","submitted_at":"2024-12-24T11:43:08Z","title":"Notes on Quasinormal Modes of charged de Sitter Blackholes from Quiver Gauge Theories","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.18359","snapshot_observed_at":"2026-08-09T20:53:38.831687Z","title":"Liu and R.-D","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.831687Z"},"links":{"cited_paper":"/paper/2412.18359","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:ad0b1fb8906b935f087b57b1145008a79c48a8bf435a4b455d3d0aa8f74943ad","observation_id":"15ad00da-765c-4401-b0b3-71255fdf6307","resolution":{"observed_at":"2026-08-09T20:53:38.831687Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.17488","last_updated":"2025-05-12T16:20:24Z","snapshot_observed_at":"2026-08-16T12:57:09.707758Z","submitted_at":"2025-02-18T22:59:31Z","title":"Kerr-Newman quasinormal modes and Seiberg-Witten theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.17488","snapshot_observed_at":"2026-08-09T20:53:38.838553Z","title":"Silva, J.-W","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.838553Z"},"links":{"cited_paper":"/paper/2502.17488","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:021097d03c057c6122da868da25b9b8170e8fbb39fd3af13513d37149af8489a","observation_id":"bf56c57b-2f7b-4186-9c25-9e05a9fb732f","resolution":{"observed_at":"2026-08-09T20:53:38.838553Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.02855","last_updated":"2025-07-17T11:39:14Z","snapshot_observed_at":"2026-08-16T21:33:03.260394Z","submitted_at":"2025-03-04T18:32:25Z","title":"Four-point correlators with BPS bound states in AdS$_3$ and AdS$_5$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.02855","snapshot_observed_at":"2026-08-09T20:53:38.843695Z","title":"Aprile, S","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.843695Z"},"links":{"cited_paper":"/paper/2503.02855","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:7064b22b75abfccc7ed20f41e77ff3db862585f384ec97c18a2798c739cf1eb1","observation_id":"841ef59f-f19f-454b-9b6f-14e6068a7488","resolution":{"observed_at":"2026-08-09T20:53:38.843695Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.22805","last_updated":"2025-03-28T18:09:23Z","snapshot_observed_at":"2026-08-16T12:45:51.524850Z","submitted_at":"2025-03-28T18:09:23Z","title":"Greybody Factor in AdS Black Brane Spectroscopy: A Study with Scalar and Electromagnetic Perturbations","version":1},"cited_work":{"arxiv_id":"2503.22805","doi":null,"metadata_source":"pith","pith_arxiv_id":"2503.22805","snapshot_observed_at":"2026-08-09T20:53:38.977177Z","title":"Greybody Factor in AdS Black Brane Spectroscopy: A Study with Scalar and Electromagnetic Perturbations","venue":"hep-th","work_id":"7bb3352a-bcd1-4fa6-a147-625df9dd71c3","year":2025},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.849787Z"},"links":{"cited_paper":"/paper/2503.22805","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:407f4c64c868d6576f0eb306a928c72aa1102240d7f33eea67dbef8f99eb0a67","observation_id":"bec1e4be-47e6-4d8b-915b-c95b24712278","resolution":{"observed_at":"2026-08-09T20:53:39.033275Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:38.855389Z","title":"Black Hole Perturbation Toolkit","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.855389Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:9b7ef7dafa54db9ad0c42bfbd0371558307b4d6f290a48af2dba740ca9ffbed7","observation_id":"4c0ec207-e875-4913-9a81-159d6bab9128","resolution":{"observed_at":"2026-08-09T20:53:38.855389Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0908.4052","last_updated":"2009-08-27T18:21:13Z","snapshot_observed_at":"2026-08-18T19:07:35.167853Z","submitted_at":"2009-08-27T18:21:13Z","title":"Quantization of Integrable Systems and Four Dimensional Gauge Theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0908.4052","snapshot_observed_at":"2026-08-09T20:53:38.860862Z","title":"Nekrasov and S.L","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.860862Z"},"links":{"cited_paper":"/paper/0908.4052","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:dbe92c1e1b2e3d98668ef1fa58ed3161180a72810053e6d256bf744438ee83cf","observation_id":"82630e36-3dc9-4544-acfb-d43f0114b2e1","resolution":{"observed_at":"2026-08-09T20:53:38.860862Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-09T20:53:38.866326Z","title":"Newman and R","venue":null,"work_id":null,"year":1962},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.866326Z"},"links":{"citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:9ecd2ebe0b4e7076e5c94aa31e4bfe35e17d44b77b2c18e02219664dd2c0baa6","observation_id":"5f38c226-7ab8-4bd2-883d-0e30b78a4045","resolution":{"observed_at":"2026-08-09T20:53:38.866326Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.08498","last_updated":"2021-05-19T05:29:54Z","snapshot_observed_at":"2026-08-16T19:12:55.412894Z","submitted_at":"2020-10-16T16:55:21Z","title":"Recursion relation for instanton counting for $SU(2)$ ${\\cal N}=2$ SYM in NS limit of $\\Omega$ background","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.08498","snapshot_observed_at":"2026-08-09T20:53:38.871933Z","title":"Poghosyan,Recursion relation for instanton counting for SU(2)N = 2 SYM in NS limit of Ω background, JHEP 05 (2021) 088 [2010.08498]","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions","version":5},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-09T20:53:38.871933Z"},"links":{"cited_paper":"/paper/2010.08498","citing_paper":"/paper/2501.19257"},"observation_digest":"sha256:72bc3b7dbdc48faffa28739156b080649306a7e40872c1d880fd5cd842d76fcf","observation_id":"fa3ca50e-341d-487a-ac33-8e4bccf23d7f","resolution":{"observed_at":"2026-08-09T20:53:38.871933Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2501.19257","last_updated":"2025-07-23T20:42:58Z","latest_version":5,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-18T08:51:43.957004Z","submitted_at":"2025-01-31T16:16:00Z","title":"Resumming Post-Minkowskian and Post-Newtonian gravitational waveform expansions"},"reference_resolution":{"displayed":91,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":88,"verified_exact":3,"verified_fuzzy":0},"total_outbound_references":91},"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":"2026-08-18T06:34:40.430872+00:00","source":"crossref"},{"observed_at":"2026-08-18T06:34:34.496301+00:00","source":"retraction_watch"}],"thesis":"As of 19 August 2026, this Paper Citation Record lists 91 of 91 outbound references and 18 inbound Pith citation observations for arXiv:2501.19257."}