{"as_of":"2026-08-21T18:48:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:15d3b5ad33f7af01b676325be2a615eebe32408e2d43ba4f2f8f2b58f247803d","coverage":[{"denominator":103,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-15T23:13:02.964913Z","state":"measured"},{"denominator":106,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":106,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":6,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":6,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-15T21:35:08.284582Z","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":"2026-07-01T17:45:52.085249Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.05368","snapshot_observed_at":"2026-08-15T21:35:08.284582Z","title":"BMS representations for generic supermomentum,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.09499","last_updated":"2025-05-14T15:49:34Z","snapshot_observed_at":"2026-08-16T01:42:06.987673Z","submitted_at":"2025-05-14T15:49:34Z","title":"Shadow Celestial Operator Product Expansions","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-15T21:35:08.284582Z"},"links":{"cited_paper":"/paper/2505.05368","citing_paper":"/paper/2505.09499"},"observation_digest":"sha256:593efc404f46cc0f7c3991c43609a39c85625750ca95e379bda4965f72977af1","observation_id":"4b273266-ec16-48cf-a5f3-1a4716cc94c2","resolution":{"observed_at":"2026-08-15T21:35:08.284582Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.05368","snapshot_observed_at":"2026-08-07T11:30:40.364908Z","title":"BMS representations for generic supermo- mentum,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2506.02240","last_updated":"2025-06-02T20:32:47Z","snapshot_observed_at":"2026-08-18T00:54:08.715826Z","submitted_at":"2025-06-02T20:32:47Z","title":"Wheeler-DeWitt equation and Bondi-Metzner-Sachs (BMS) symmetry","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-07T11:30:40.364908Z"},"links":{"cited_paper":"/paper/2505.05368","citing_paper":"/paper/2506.02240"},"observation_digest":"sha256:2bac8c409d28e4105911e53470eb3f44062ab23a472f2100cbac37beaac7a868","observation_id":"fa224c23-af91-4faf-84cf-49b15bbc1f89","resolution":{"observed_at":"2026-08-07T11:30:40.364908Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.05368","snapshot_observed_at":"2026-08-03T22:35:44.540182Z","title":"Bekaert and Y","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2511.10162","last_updated":"2026-06-19T09:06:59Z","snapshot_observed_at":"2026-08-16T00:10:42.843275Z","submitted_at":"2025-11-13T10:17:50Z","title":"Lectures on Carrollian Holography","version":3},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-03T22:35:44.540182Z"},"links":{"cited_paper":"/paper/2505.05368","citing_paper":"/paper/2511.10162"},"observation_digest":"sha256:b9df72a216eddac7cac0df1475f80ff5c399b5c5a3f6f39f3421dcea63e6201f","observation_id":"7952f82e-3750-4e92-8357-6a5534366727","resolution":{"observed_at":"2026-08-03T22:35:44.540182Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"cited_work":{"arxiv_id":"2505.05368","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2505.05368","snapshot_observed_at":"2026-07-01T17:45:52.085249Z","title":"Bekaert and Y","venue":null,"work_id":"fbaf6c70-9fab-43c9-a67f-cfe1545a458f","year":2026},"citing_paper":{"arxiv_id":"2603.11993","last_updated":"2026-04-03T04:10:58Z","snapshot_observed_at":"2026-08-18T03:40:01.034822Z","submitted_at":"2026-03-12T14:44:15Z","title":"More on Bulk Local State Reconstruction in Flat/Carr CFT","version":2},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-05-15T12:03:24.538680Z"},"links":{"cited_paper":"/paper/2505.05368","citing_paper":"/paper/2603.11993"},"observation_digest":"sha256:c74ae43d865a340300aa396e8f3b7c522af7988d9b639fb3b80dd75690ba6bfb","observation_id":"a92609b6-e480-4070-9bd6-9001ba371754","resolution":{"observed_at":"2026-05-15T12:05:33.549761Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"cited_work":{"arxiv_id":"2505.05368","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2505.05368","snapshot_observed_at":"2026-07-01T17:45:52.085249Z","title":"Bekaert and Y","venue":null,"work_id":"fbaf6c70-9fab-43c9-a67f-cfe1545a458f","year":2026},"citing_paper":{"arxiv_id":"2606.28245","last_updated":"2026-06-26T16:32:14Z","snapshot_observed_at":"2026-08-14T06:57:40.908261Z","submitted_at":"2026-06-26T16:32:14Z","title":"Spinor-helicity formalism for continuous-spin particles","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-06-29T03:07:35.817118Z"},"links":{"cited_paper":"/paper/2505.05368","citing_paper":"/paper/2606.28245"},"observation_digest":"sha256:a61d1bb6f68cbc6883418c8df494c966d7176576596801586217b0a9b8c70e58","observation_id":"639cdd50-f3ab-47cc-a0d4-c88b29179d75","resolution":{"observed_at":"2026-07-01T17:45:52.087266Z","resolver_source":"arxiv_id","status":"metadata_mismatch"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2505.05368","snapshot_observed_at":"2026-08-01T21:12:23.545928Z","title":"BMS Representations for Generic Supermomentum,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2607.16179","last_updated":"2026-07-17T17:56:51Z","snapshot_observed_at":"2026-08-17T23:57:38.360000Z","submitted_at":"2026-07-17T17:56:51Z","title":"Dressed States Call for Logarithmic Asymptotic Symmetries","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-01T21:12:23.545928Z"},"links":{"cited_paper":"/paper/2505.05368","citing_paper":"/paper/2607.16179"},"observation_digest":"sha256:2ceba091b48b13e776806b5f69e0d548454b59e4da3bcf10b022826e3a1b9775","observation_id":"c84b93e2-579c-4b6a-bf6b-d5373cceb517","resolution":{"observed_at":"2026-08-01T21:12:23.545928Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2505.05368/citation-record","integrity":"/paper/2505.05368/integrity","json":"/paper/2505.05368/citation-record.json","paper":"/paper/2505.05368"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:02.612309Z","title":"Gravitational waves in general relativity, VII. Waves from axi-symmetric isolated system,","venue":null,"work_id":null,"year":1962},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.612309Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:9847a0ccf1884262fb4a5f19b2ba6861862db9109d63e66544e30e20fb50ead3","observation_id":"df5cd4f0-9967-463f-a8ee-a1d61cb5c18f","resolution":{"observed_at":"2026-08-15T23:13:02.612309Z","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":"2026-08-15T23:13:02.616466Z","title":"Gravitational waves in general relativity. 8. Waves in asymptotically flat space-times,","venue":null,"work_id":null,"year":1962},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.616466Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:b4ac7728da416e7d22744c6de30e05fe5142d063a261a65a03b1858a0e04ed26","observation_id":"28c57eaf-1724-4533-8e7c-b515d6ddf816","resolution":{"observed_at":"2026-08-15T23:13:02.616466Z","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":"2026-08-15T23:13:02.619981Z","title":"Asymptotic structure of space-time,","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.619981Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:2f96c12974b487c86751bce5e751f4c11754948a3d3101d66048298d0c0e7f34","observation_id":"eb9a3cbe-52b5-4e88-a4d7-622948fee0c2","resolution":{"observed_at":"2026-08-15T23:13:02.619981Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.5894","last_updated":"2014-04-03T08:10:10Z","snapshot_observed_at":"2026-08-14T23:43:33.346201Z","submitted_at":"2014-02-24T17:10:17Z","title":"Conformal Carroll groups and BMS symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.5894","snapshot_observed_at":"2026-08-15T23:13:02.623366Z","title":"Conformal Carroll groups and BMS symmetry,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.623366Z"},"links":{"cited_paper":"/paper/1402.5894","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:f6393620d1f5e670108ca081cd55c8cb6788f6126ae381d2d7f4c7f196481737","observation_id":"757d2127-fd7a-4884-867a-4fc49984839b","resolution":{"observed_at":"2026-08-15T23:13:02.623366Z","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":"2026-08-15T23:13:02.626787Z","title":"Ashtekar, Asymptotic Quantization: Based on 1984 Naples Lectures,","venue":null,"work_id":null,"year":1984},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.626787Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:2ec830cc82b939469097c690cddb764c775d16e407f5d33bc772fdc8b88475fd","observation_id":"33e1b6fa-9bc7-4a28-9a94-b8afc503db73","resolution":{"observed_at":"2026-08-15T23:13:02.626787Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1312.2229","last_updated":"2014-01-23T20:36:55Z","snapshot_observed_at":"2026-08-14T23:52:27.264397Z","submitted_at":"2013-12-08T15:33:34Z","title":"On BMS Invariance of Gravitational Scattering","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1312.2229","snapshot_observed_at":"2026-08-15T23:13:02.630353Z","title":"On BMS Invariance of Gravitational Scattering,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.630353Z"},"links":{"cited_paper":"/paper/1312.2229","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:89cff356090a4f05c6c7276f67f31a233c9d18c206454f70de9f78b5d3f562b1","observation_id":"ae5b446d-d712-45ff-ad03-85fa9ce312a2","resolution":{"observed_at":"2026-08-15T23:13:02.630353Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1401.7026","last_updated":"2015-05-07T18:11:47Z","snapshot_observed_at":"2026-08-15T09:34:07.336106Z","submitted_at":"2014-01-27T21:19:55Z","title":"BMS supertranslations and Weinberg's soft graviton theorem","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1401.7026","snapshot_observed_at":"2026-08-15T23:13:02.634006Z","title":"BMS supertranslations and Weinberg’s soft graviton theorem,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.634006Z"},"links":{"cited_paper":"/paper/1401.7026","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:01fc1c320c56ed1d8965b97f4447fe4acc0fbe03dfa75870ad2c86759b8d7569","observation_id":"4bf20c6b-1ade-407b-86ce-81da35b74d8c","resolution":{"observed_at":"2026-08-15T23:13:02.634006Z","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":"2026-08-15T23:13:02.637709Z","title":"Representations of the bondi-metzner-sachs group","venue":null,"work_id":null,"year":1971},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.637709Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:7ac6efd21a75bdf54b8816399dbe0e469c6808ef820580abd113dc69929f2050","observation_id":"0da893cc-2215-46f7-bd2d-71690bd79495","resolution":{"observed_at":"2026-08-15T23:13:02.637709Z","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":"2026-08-15T23:13:02.641253Z","title":"Asymptotically flat space-times and elementary particles,","venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.641253Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:bf48209b39e3a514b6a978e5d5f3bb7eea3fbfe93dcc412c31b09ab9ce40da9f","observation_id":"8285e078-44ed-4eb6-b23e-5a2b918e3788","resolution":{"observed_at":"2026-08-15T23:13:02.641253Z","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":"2026-08-15T23:13:02.644717Z","title":"Representations of the bondi-metzner-sachs group. i. determination of the representations,","venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.644717Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:20c8e0c3df7691689e2495eb2ff4245be2afdd333425ea98469bd045e53ac4a4","observation_id":"50daac30-d579-4718-bd17-e6e7468737c8","resolution":{"observed_at":"2026-08-15T23:13:02.644717Z","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":"2026-08-15T23:13:02.648269Z","title":"Representations of the bondi-metzner-sachs group. ii. properties and classification of the representations,","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.648269Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:95782eef5bf61ba46794ec568dbe69adb39d57816318e4f958d2b7397cc4d89c","observation_id":"b769b959-85bd-41f3-ae4a-b283ee1c1d6d","resolution":{"observed_at":"2026-08-15T23:13:02.648269Z","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":"2026-08-15T23:13:02.651903Z","title":"Representations of the bondi-metzner-sachs group. iii. poincare spin multiplicities and irreducibility,","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.651903Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:df6e1b3a25884f12e81c7b6783292aa7606c2124557956cc9c9c3304c5be8091","observation_id":"48843644-f91f-4291-b5a9-96bee7189b41","resolution":{"observed_at":"2026-08-15T23:13:02.651903Z","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":"2026-08-15T23:13:02.655136Z","title":"Physical significance of the topology of the bondi-metzner-sachs group,","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.655136Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:59899b5129d4741f9be91168f1cf3e62aff5b23c1fdc2b6336ed100dea916cac","observation_id":"82b5d9d1-989a-4de1-a7a6-cf7ddc4e2638","resolution":{"observed_at":"2026-08-15T23:13:02.655136Z","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":"2026-08-15T23:13:02.658715Z","title":"The bondi-metzner-sachs group in the nuclear topology,","venue":null,"work_id":null,"year":1975},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.658715Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:420dacfc644bd8acad1c81c80e1977bc8fd921c2a97c822e50f33e40a34c3d37","observation_id":"482d5af7-42e3-4265-9f69-33fab0870973","resolution":{"observed_at":"2026-08-15T23:13:02.658715Z","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":"2026-08-15T23:13:02.663281Z","title":"Representations of the bondi-metzner-sachs group. iv. cantoni representations are induced,","venue":null,"work_id":null,"year":1976},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.663281Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:d536672ed7ea8a7c99797921a9d3c926efbd26292833fb0c9a1daac8c0f9482a","observation_id":"64e4f257-4240-4541-bb92-6c53ef833a3d","resolution":{"observed_at":"2026-08-15T23:13:02.663281Z","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":"2026-08-15T23:13:02.667540Z","title":"Lifting of projective representations of the bondi—metzner—sachs group,","venue":null,"work_id":null,"year":1978},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.667540Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:6952902a2a682327b94096c115e0bcdd742816c8141e4d2c017ee54506168dd5","observation_id":"0b196f94-aa6f-4e63-8740-580ac5950cf2","resolution":{"observed_at":"2026-08-15T23:13:02.667540Z","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":"2026-08-15T23:13:02.671138Z","title":"Hyperfunctions and asymptotic symmetries,","venue":null,"work_id":null,"year":1978},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.671138Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:bea5fca4b3af1fdef7813d2413fb4482ddf74857f3246eae4b9cf2481e311ace","observation_id":"761e3e26-6b03-475f-af0b-a15931213ce5","resolution":{"observed_at":"2026-08-15T23:13:02.671138Z","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":"2026-08-15T23:13:02.674317Z","title":"A class of representations of the generalized bondi—metzner group,","venue":null,"work_id":null,"year":1966},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.674317Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:4bfb62d31fd6e64198f2d56635620201c339f9fd3ad4f481a4b748f80167c8ff","observation_id":"269256cd-5424-4f0c-a0f4-89073ace4b7b","resolution":{"observed_at":"2026-08-15T23:13:02.674317Z","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":"2026-08-15T23:13:02.678513Z","title":"Induction of representations of the generalized Bondi-Metzner group,","venue":null,"work_id":null,"year":1967},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.678513Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:0fd3200bbd9750aec81f2d3f4cfd4c83d2af6e922b97a6a116949d977d8270e7","observation_id":"9d88c792-6218-4f37-9300-8e9cd6878332","resolution":{"observed_at":"2026-08-15T23:13:02.678513Z","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":"2026-08-15T23:13:02.681937Z","title":"Reduction of some representations of the generalized bondi-metzner group,","venue":null,"work_id":null,"year":1967},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.681937Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:706ca92c87b5db4f1469543dd12a7322ef756d9bab26878a0dd665844363bc10","observation_id":"1d5a1018-3355-482f-b4fe-9a47098ea98e","resolution":{"observed_at":"2026-08-15T23:13:02.681937Z","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":"2026-08-15T23:13:02.685266Z","title":"Continuous spins in the bondi-metzner-sachs group of asymptotic symmetry in general relativity,","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.685266Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:063234f3e63e502c218184ab7fd319de9c8c39eef04d281d131e5711702c6bdc","observation_id":"77f2a014-0354-4283-aa10-a9969581bba0","resolution":{"observed_at":"2026-08-15T23:13:02.685266Z","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":"2026-08-15T23:13:02.688498Z","title":"Approaching quantum gravity via the representation theory of the BMS group and its variants. Some conceptual issues and a conjecture,","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.688498Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:f6e067384c5b8570b1990afe1646993b05f614d806981b228f1d0769dc8551f8","observation_id":"d486140f-d8fc-4db3-bfa5-7edbf7e8a83c","resolution":{"observed_at":"2026-08-15T23:13:02.688498Z","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":"2026-08-15T23:13:02.691817Z","title":"Open problems and results in the group theoretic approach to quantum gravity via the bms group and its generalizations,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.691817Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:d3775674f96df7072ce17adad84c89924c7f6fad34a400393cee12e6d7b5c96d","observation_id":"139108ea-57bb-443b-8ce6-42649205e8a2","resolution":{"observed_at":"2026-08-15T23:13:02.691817Z","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":"2026-08-15T23:13:02.694972Z","title":"First results on the representation theory of the Ultrahyperbolic BMS group UHB(2, 2),","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.694972Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:c2e8e3af0b079dcbe8113a417d750d3b97ab5102a0194a10d83710f7105e25e2","observation_id":"f5857f33-ac29-46b2-8d27-f5433d92cfb1","resolution":{"observed_at":"2026-08-15T23:13:02.694972Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1403.5803","last_updated":"2014-07-01T10:32:41Z","snapshot_observed_at":"2026-08-19T15:59:59.999396Z","submitted_at":"2014-03-23T21:14:47Z","title":"Notes on the BMS group in three dimensions: I. Induced representations","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1403.5803","snapshot_observed_at":"2026-08-15T23:13:02.698270Z","title":"Notes on the BMS group in three dimensions: I. Induced representations,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.698270Z"},"links":{"cited_paper":"/paper/1403.5803","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:97a9aece3f3eb5d6fc36dbd64b54a946d988bca37aff631022c63722642f3c20","observation_id":"1128231e-360c-40cf-8fcd-affd113ab3a3","resolution":{"observed_at":"2026-08-15T23:13:02.698270Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1502.00010","last_updated":"2015-03-21T10:22:23Z","snapshot_observed_at":"2026-08-19T19:36:31.003894Z","submitted_at":"2015-01-30T21:02:05Z","title":"Notes on the BMS group in three dimensions: II. Coadjoint representation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1502.00010","snapshot_observed_at":"2026-08-15T23:13:02.701507Z","title":"Notes on the BMS group in three dimensions: II. Coadjoint representation,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.701507Z"},"links":{"cited_paper":"/paper/1502.00010","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:32052eb8d53b098ea764f26b151dc5575b45643fbb5b21587ddc8c6a1bc98bbe","observation_id":"18d27678-3055-4fc6-855b-0a839e272af8","resolution":{"observed_at":"2026-08-15T23:13:02.701507Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.08526","last_updated":"2018-01-26T11:19:11Z","snapshot_observed_at":"2026-08-15T12:04:59.786954Z","submitted_at":"2016-10-26T20:00:16Z","title":"BMS Particles in Three Dimensions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.08526","snapshot_observed_at":"2026-08-15T23:13:02.704725Z","title":"Oblak, BMS Particles in Three Dimensions","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.704725Z"},"links":{"cited_paper":"/paper/1610.08526","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:ebb6f596dbec3bfa54020156594f86431da0af2eaf5f2f0e98b76f3e727d964b","observation_id":"5878e10a-551f-4dd9-8b5d-e86dc3e9c379","resolution":{"observed_at":"2026-08-15T23:13:02.704725Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.05980","last_updated":"2017-03-17T12:01:58Z","snapshot_observed_at":"2026-08-17T23:08:26.224098Z","submitted_at":"2017-03-17T12:01:58Z","title":"On the representation theory of the Bondi-Metzner-Sachs group and its variants in three space-time dimensions","version":1},"cited_work":{"arxiv_id":"1703.05980","doi":null,"metadata_source":"pith","pith_arxiv_id":"1703.05980","snapshot_observed_at":"2026-08-15T23:13:03.571862Z","title":"On the representation theory of the Bondi-Metzner-Sachs group and its variants in three space-time dimensions","venue":"math-ph","work_id":"91aef4fa-0c50-4a7c-add4-aea64e38b9f0","year":2017},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.708985Z"},"links":{"cited_paper":"/paper/1703.05980","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:35ebb50d9169c351e4c911109fdcc3969ca1af1022aad6eb16c400897a99ccc3","observation_id":"9a5a83b1-c080-4ddd-ab2d-a07eb1dfedf4","resolution":{"observed_at":"2026-08-15T23:13:03.575779Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2403.19547","last_updated":"2024-12-13T01:45:23Z","snapshot_observed_at":"2026-08-16T14:05:27.703510Z","submitted_at":"2024-03-28T16:28:00Z","title":"On the Definition of the Spin Charge in Asymptotically-Flat Spacetimes","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.19547","snapshot_observed_at":"2026-08-15T23:13:02.712524Z","title":"On the definition of the spin charge in asymptotically-flat spacetimes,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.712524Z"},"links":{"cited_paper":"/paper/2403.19547","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:4a42c1d6dc50bb28ee868e530fc3ab2103b560d850567ad1202c32707860c129","observation_id":"67b93c0d-cbf3-4ebf-b146-69a32aabfb6c","resolution":{"observed_at":"2026-08-15T23:13:02.712524Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9803128","last_updated":"1998-03-16T10:09:51Z","snapshot_observed_at":"2026-08-19T13:28:32.071075Z","submitted_at":"1998-03-16T10:09:51Z","title":"A canonical realization of the BMS algebra","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9803128","snapshot_observed_at":"2026-08-15T23:13:02.716534Z","title":"A Canonical realization of the BMS algebra,","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.716534Z"},"links":{"cited_paper":"/paper/hep-th/9803128","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:3f9e4deb373ecef0c4dfbbca4ec2c0baa2a64e95e8ebadfacff4b9711471ad79","observation_id":"478b128f-2afd-42a2-9b10-588a89ce59ca","resolution":{"observed_at":"2026-08-15T23:13:02.716534Z","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":"2026-08-15T23:13:02.719918Z","title":"BMS particles,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.719918Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:6a1b2e1583c1fe37197da7fbcc892698ab834aebfd23f6b010a3b09e27d4b44a","observation_id":"4c2a4c3f-4972-4ec1-ac5f-1f1f08ae1c6c","resolution":{"observed_at":"2026-08-15T23:13:02.719918Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.11253","last_updated":"2021-06-11T10:07:11Z","snapshot_observed_at":"2026-08-17T16:13:44.223549Z","submitted_at":"2021-03-20T22:08:55Z","title":"Coadjoint representation of the BMS group on celestial Riemann surfaces","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.11253","snapshot_observed_at":"2026-08-15T23:13:02.724092Z","title":"Coadjoint representation of the BMS group on celestial Riemann surfaces,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.724092Z"},"links":{"cited_paper":"/paper/2103.11253","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:16aece8720f0e43a5900b7e450543b65b2de2c63bfa31cf06fe61296360a5b0a","observation_id":"a44af870-b619-499a-b972-edc1ee2a3944","resolution":{"observed_at":"2026-08-15T23:13:02.724092Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2108.11969","last_updated":"2021-11-28T18:06:31Z","snapshot_observed_at":"2026-08-16T18:00:41.666082Z","submitted_at":"2021-08-26T18:00:30Z","title":"BMS Flux Algebra in Celestial Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2108.11969","snapshot_observed_at":"2026-08-15T23:13:02.727975Z","title":"BMS flux algebra in celestial holography,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.727975Z"},"links":{"cited_paper":"/paper/2108.11969","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:8753e74a375e42a7a3994b87a4a70c2eee455f6a608a55a615521d63dd0ad185","observation_id":"976cd137-4fbe-4240-b423-5976d22db99f","resolution":{"observed_at":"2026-08-15T23:13:02.727975Z","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":"2026-08-15T23:13:02.731400Z","title":"Asymptotic Symmetries in Gravitational Theory,","venue":null,"work_id":null,"year":1962},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.731400Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:899a74cf1dee23b4276eb98221a44c7b8e2f45d9cb0ed03b295074971837c53d","observation_id":"2b06ab77-ceee-48bf-9c31-5fc3c376f657","resolution":{"observed_at":"2026-08-15T23:13:02.731400Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.01406","last_updated":"2015-09-04T11:21:10Z","snapshot_observed_at":"2026-08-16T14:10:40.326859Z","submitted_at":"2015-09-04T11:21:10Z","title":"Asymptotic symmetries of gravity and soft theorems for massive particles","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.01406","snapshot_observed_at":"2026-08-15T23:13:02.734611Z","title":"Asymptotic symmetries of gravity and soft theorems for massive particles,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.734611Z"},"links":{"cited_paper":"/paper/1509.01406","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:37ed20365470fb3b41a067da45e7d9cdc5585b114dea36e8a4452e8a00e65299","observation_id":"5d3d1d3f-8bae-43b6-a547-22599aeb5b85","resolution":{"observed_at":"2026-08-15T23:13:02.734611Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.03211","last_updated":"2017-12-08T18:40:11Z","snapshot_observed_at":"2026-08-17T14:35:19.574888Z","submitted_at":"2017-12-08T18:40:11Z","title":"BMS symmetry, soft particles and memory","version":1},"cited_work":{"arxiv_id":"1712.03211","doi":null,"metadata_source":"pith","pith_arxiv_id":"1712.03211","snapshot_observed_at":"2026-08-15T23:13:03.419898Z","title":"BMS symmetry, soft particles and memory","venue":"hep-th","work_id":"76f0779e-843a-42cc-9a3c-1254cc9cc6d4","year":2017},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.738669Z"},"links":{"cited_paper":"/paper/1712.03211","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:55d3955d062261534552b56b83ebef3a9502ba7ec99d667d8fb95809bc2aa459","observation_id":"9fe117de-e8a7-49df-8c3f-38535512df1d","resolution":{"observed_at":"2026-08-15T23:13:03.426308Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1705.04311","last_updated":"2017-05-11T17:56:43Z","snapshot_observed_at":"2026-08-14T21:01:16.540360Z","submitted_at":"2017-05-11T17:56:43Z","title":"Infrared Divergences in QED, Revisited","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.04311","snapshot_observed_at":"2026-08-15T23:13:02.742211Z","title":"Infrared Divergences in QED, Revisited,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.742211Z"},"links":{"cited_paper":"/paper/1705.04311","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:9c349010beecada59e0cb0af6dce9f57c37e0a00ce58afe48f8690c1385a8c75","observation_id":"182da256-1aef-4ab3-84b3-1bfae4a76f09","resolution":{"observed_at":"2026-08-15T23:13:02.742211Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1712.04551","last_updated":"2017-12-12T22:23:13Z","snapshot_observed_at":"2026-08-14T20:04:17.077440Z","submitted_at":"2017-12-12T22:23:13Z","title":"BMS Supertranslation Symmetry Implies Faddeev-Kulish Amplitudes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1712.04551","snapshot_observed_at":"2026-08-15T23:13:02.745648Z","title":"BMS Supertranslation Symmetry Implies Faddeev-Kulish Amplitudes,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.745648Z"},"links":{"cited_paper":"/paper/1712.04551","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:2fee0c49314af884dbca6b6214c453ce0fbf341a8b20ef794047d644bbe836b4","observation_id":"4fc69646-b7c4-4d20-8e26-09a2bedacc59","resolution":{"observed_at":"2026-08-15T23:13:02.745648Z","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":"2026-08-15T23:13:02.748982Z","title":"Asymptotic conditions and infrared divergences in quantum electrodynamics,","venue":null,"work_id":null,"year":1970},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.748982Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:dd76ff2ecfbc79203914560990903d3cadd1ebd887487efcf109d67d000c3d50","observation_id":"77d60f04-f54c-47a3-9369-9a3917163a65","resolution":{"observed_at":"2026-08-15T23:13:02.748982Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1411.5745","last_updated":"2014-11-21T02:30:16Z","snapshot_observed_at":"2026-08-17T19:28:35.790561Z","submitted_at":"2014-11-21T02:30:16Z","title":"Gravitational Memory, BMS Supertranslations and Soft Theorems","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1411.5745","snapshot_observed_at":"2026-08-15T23:13:02.752009Z","title":"Gravitational Memory, BMS Supertranslations and Soft Theorems,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.752009Z"},"links":{"cited_paper":"/paper/1411.5745","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:defe66ca5abd032923a0037517727cd29eb1920697eb5a1c36e9354c0a10b988","observation_id":"27a88dd6-e09a-4dec-bb8f-0eb1da25f495","resolution":{"observed_at":"2026-08-15T23:13:02.752009Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.947478Z","title":"Note on the Bondi-Metzner-Sachs group,","venue":null,"work_id":"047ac01d-8cfb-4422-9b3e-40984b4a058a","year":1966},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.755805Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:62b3302f34de8c09676944c69989680a38c7ad3a6bff1d542659e10f53b53b07","observation_id":"b8a9e7a8-754d-4398-a5c9-92bc435015ac","resolution":{"observed_at":"2026-08-15T23:13:03.950515Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.938408Z","title":"Edth - a differential operator on the sphere,","venue":null,"work_id":"b886f331-4b60-45e3-bdb4-21d5526ccc8c","year":1982},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.759225Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:a2e538c00450c102e65139922bc29b4bd5e323ab582484222a52c8da08a283be","observation_id":"877bb60e-e6b0-48cf-b141-8bfc5b2fd808","resolution":{"observed_at":"2026-08-15T23:13:03.941763Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2110.06066","last_updated":"2022-03-08T06:42:38Z","snapshot_observed_at":"2026-08-20T21:12:47.945777Z","submitted_at":"2021-10-12T15:15:04Z","title":"Celestial $w_{1+\\infty}$ Symmetries from Twistor Space","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.06066","snapshot_observed_at":"2026-08-15T23:13:02.762609Z","title":"Celestial w1`8 Symmetries from Twistor Space,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.762609Z"},"links":{"cited_paper":"/paper/2110.06066","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:76a6e20db9aa4fece1b1da707d0d0925a4010d757e1a59eb6fe398416eaf3429","observation_id":"519cec46-6fee-45a5-90bf-79f401c2a426","resolution":{"observed_at":"2026-08-15T23:13:02.762609Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.02238","last_updated":"2022-11-17T20:31:53Z","snapshot_observed_at":"2026-08-19T06:46:35.710940Z","submitted_at":"2022-03-04T10:54:42Z","title":"Graviton scattering in self-dual radiative space-times","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.02238","snapshot_observed_at":"2026-08-15T23:13:02.766116Z","title":"Graviton scattering in self-dual radiative space-times,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.766116Z"},"links":{"cited_paper":"/paper/2203.02238","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:65df7d6644ee60e86985479e66d768e77e1c18775d72a432a8f5c839d921b633","observation_id":"43aa01b6-9eb5-46e1-96d8-cd1c4a17a47f","resolution":{"observed_at":"2026-08-15T23:13:02.766116Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.929730Z","title":null,"venue":null,"work_id":"4512be54-83fd-49df-a3c1-9ac9337f7935","year":1966},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.769485Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:545d5d0c7350241bfae89ceb7aa0f35e4e22f322211b7a29376babf0740f8697","observation_id":"6d6a1f75-796d-4b0e-aff1-c861245d86ea","resolution":{"observed_at":"2026-08-15T23:13:03.932505Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"0803.4331","last_updated":"2008-03-30T17:54:20Z","snapshot_observed_at":"2026-08-15T10:18:38.496607Z","submitted_at":"2008-03-30T17:54:20Z","title":"A Quartic Conformally Covariant Differential Operator for Arbitrary Pseudo-Riemannian Manifolds (Summary)","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0803.4331","snapshot_observed_at":"2026-08-15T23:13:02.772854Z","title":"A quartic conformally covariant differential operator for arbitrary pseudo-riemannian manifolds (summary),","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.772854Z"},"links":{"cited_paper":"/paper/0803.4331","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:504b8babfa87cfedbc565743b2209afe2f60ab9e755d6811d74b4494f9ffb0f2","observation_id":"c22f79e7-ffc2-4db6-a998-2f7c195f6554","resolution":{"observed_at":"2026-08-15T23:13:02.772854Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.919929Z","title":"Asymptotic freedom in extended conformal supergravities,","venue":null,"work_id":"f5c920fd-88f3-41bc-88e1-b24077602f8f","year":1982},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.776465Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:258d7d95e286872c768aa5a86f0731e6752cce36afc9359580dd9dad35f720e8","observation_id":"843c3de0-83a1-45c1-96c0-370960cf331c","resolution":{"observed_at":"2026-08-15T23:13:03.923444Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.909746Z","title":null,"venue":null,"work_id":"71b9ca47-8556-4f6f-87e2-d88b9de5f96e","year":1964},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.779859Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:c71c3c90583aed5f9ab34154143d40f9f7a7ec60655eca8b796fca900c590a54","observation_id":"a299e586-25a4-4562-bdca-143b8decf521","resolution":{"observed_at":"2026-08-15T23:13:03.913138Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.899526Z","title":"Green’s functions of the edh operators,","venue":null,"work_id":"5884ae0b-75ea-458d-9700-8fffd2dbe8d8","year":1989},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.783273Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:7c9affef53e718c812cdbe77ec2d17c01f3ee36ad33daf7bf3d0ad0db1730b9b","observation_id":"cdcb5ed8-e8b0-4a56-9886-f807a3c0ff0b","resolution":{"observed_at":"2026-08-15T23:13:03.902994Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.889605Z","title":"An introduction to conformal geometry and tractor calculus, with a view to applications in general relativity,","venue":null,"work_id":"86e891a8-6f5d-41e3-9a63-0ed16225bf50","year":2018},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.786589Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:39fd1c28fdd12a9a43cfc31f28db7a75cc660a078965776d3006d8d73a07700b","observation_id":"e952e2f7-f011-4159-b8c7-7c85751b58d6","resolution":{"observed_at":"2026-08-15T23:13:03.892835Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.879136Z","title":"On Unitary Representations of the Inhomogeneous Lorentz Group,","venue":null,"work_id":"2bbb71af-f30d-4da7-bfb0-4ccd25999756","year":1939},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.790394Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:4f41c3a99eee565428a05964bdda9d72f7670e2c57a2fcd80968c210b223f852","observation_id":"2ffdf69f-7780-4efd-be14-308491e06701","resolution":{"observed_at":"2026-08-15T23:13:03.882728Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.869487Z","title":null,"venue":null,"work_id":"66075429-5cda-4b1f-84a7-2a6b9480ebbd","year":1968},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.793706Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:c55e121c0dd73e5511130c81ecd06c7ed6d461570298cabbdc02cc6b003bc3db","observation_id":"e60589b1-ef32-445a-b209-7597fbf9984b","resolution":{"observed_at":"2026-08-15T23:13:03.872627Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.858938Z","title":"Unitary representations of semi-direct product groups with infinite dimensional abelian normal subgroup,","venue":null,"work_id":"94c0c15e-b8b9-471c-8fa3-31cee5a5a44d","year":1977},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.797160Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:75b638a2d6d0661e79e7d8de2016887842e2f74d8aebf874382ced17f8a4e721","observation_id":"51135819-b9c4-4b99-94b0-f3ede0cc0a00","resolution":{"observed_at":"2026-08-15T23:13:03.863174Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.847786Z","title":"Representations of the bondi-metzner-sachs group with the hilbert topology,","venue":null,"work_id":"289cf2d3-3dd2-4c3a-b61e-70d782b94a83","year":1977},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.800571Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:ededab80ce7fd260d7dbc09330a8d964b50c7951f55a967bc5adf164e2daceba","observation_id":"4206475b-7108-4119-a329-b924f649ea83","resolution":{"observed_at":"2026-08-15T23:13:03.851912Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.835021Z","title":"Borel multipliers for the bondi–metzner–sachs group,","venue":null,"work_id":"ce46eadc-a347-42cf-859a-1d388182eb93","year":1979},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.804009Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:73fd376cb25a8b8d36a79a6b2d2e502381262c3ac00db650d9f50eb7c64a990c","observation_id":"3ac346ba-79c0-4cec-90c3-c580ee5942c1","resolution":{"observed_at":"2026-08-15T23:13:03.839265Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.823667Z","title":"On the projective representations of the bondi-metzner-sachs group,","venue":null,"work_id":"9869030f-8076-43ea-bd17-ff11ed68f192","year":2001},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.807933Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:27344e71530a8bf8d9e6d5bd5fa9811be209a5d8ab199f50ce94e19994eab0cd","observation_id":"b6fc1261-e42b-4d29-82df-832fccfba13e","resolution":{"observed_at":"2026-08-15T23:13:03.827879Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.814167Z","title":"Brezis, Functional Analysis, Sobolev Spaces and Partial Differential Equations","venue":null,"work_id":"00e8c2af-4d1b-44ba-8af9-dfcbc0abcc7e","year":2010},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.811560Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:145d6302396406b3b348951e640c206777382e085929d52b204e854f84b9edbe","observation_id":"4989c384-e289-44d6-b1c8-db59af0f2926","resolution":{"observed_at":"2026-08-15T23:13:03.817559Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.791061Z","title":"Quantized gravitational theory and internal symmetries,","venue":null,"work_id":"fa2b0aa1-8233-491b-a90d-2912f32cea90","year":1965},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.814911Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:ab755aeda3929eebce6141500da5fdf0f37a9dea1197a720eb3d523c942f7791","observation_id":"5be96472-68a6-4d2c-b5d2-2c7190d7409b","resolution":{"observed_at":"2026-08-15T23:13:03.806494Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.775040Z","title":"All Possible Symmetries of the S Matrix,","venue":null,"work_id":"245a41ab-f8b4-4bd1-9373-049e711535c7","year":1967},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.818140Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:947c503523bacd822a00cec6e8930479b95fc584fec58ca2892a839dc15d6047","observation_id":"3a725a50-2a49-4a41-9a5c-c1aaf7119f7f","resolution":{"observed_at":"2026-08-15T23:13:03.778568Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.763089Z","title":"Weinberg, The quantum theory of fields","venue":null,"work_id":"e8a6b9cf-b2b6-4884-8df7-a6829c83d7dc","year":2013},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.822286Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:1cafc4451255750763e7180933b23b2fab267ad40fd1ab79dd007c22a3906c37","observation_id":"184e8dd0-a024-45be-83b3-844e2cca7d44","resolution":{"observed_at":"2026-08-15T23:13:03.768261Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1703.05448","last_updated":"2018-02-15T15:52:51Z","snapshot_observed_at":"2026-08-14T21:11:38.177389Z","submitted_at":"2017-03-16T01:26:29Z","title":"Lectures on the Infrared Structure of Gravity and Gauge Theory","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.05448","snapshot_observed_at":"2026-08-15T23:13:02.825681Z","title":"Strominger, Lectures on the Infrared Structure of Gravity and Gauge Theory","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.825681Z"},"links":{"cited_paper":"/paper/1703.05448","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:db1d85cee32a53516395b9eab7fccde5126444ac8f706ba51d1fdda9911d49a4","observation_id":"8cabac7e-bf73-4af0-ba0b-89e942151996","resolution":{"observed_at":"2026-08-15T23:13:02.825681Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.12553","last_updated":"2023-06-30T15:13:48Z","snapshot_observed_at":"2026-08-20T15:55:09.065734Z","submitted_at":"2022-12-23T19:14:18Z","title":"Bridging Carrollian and Celestial Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.12553","snapshot_observed_at":"2026-08-15T23:13:02.828981Z","title":"Bridging Carrollian and celestial holography,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.828981Z"},"links":{"cited_paper":"/paper/2212.12553","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:e01c74bbd093112aae4736ac4884a9a3e2ac819e88f2ef524a74974b6a6be1d6","observation_id":"2733ee7d-83ed-499b-850e-2fac65c26a2e","resolution":{"observed_at":"2026-08-15T23:13:02.828981Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2209.02253","last_updated":"2022-11-26T11:27:35Z","snapshot_observed_at":"2026-08-16T16:34:33.589926Z","submitted_at":"2022-09-06T07:02:47Z","title":"Massless Scalars and Higher-Spin BMS in Any Dimension","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2209.02253","snapshot_observed_at":"2026-08-15T23:13:02.832312Z","title":"Massless scalars and higher-spin BMS in any dimension,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.832312Z"},"links":{"cited_paper":"/paper/2209.02253","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:6f726e7e335f887ddfef5dae8e3f4963a663db29bc191c2613ff208679864dd1","observation_id":"14143dff-ff3b-403b-a571-16996e22651c","resolution":{"observed_at":"2026-08-15T23:13:02.832312Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2305.02884","last_updated":"2023-08-26T12:47:35Z","snapshot_observed_at":"2026-08-17T19:10:42.660192Z","submitted_at":"2023-05-04T14:47:27Z","title":"Carrollian conformal fields and flat holography","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2305.02884","snapshot_observed_at":"2026-08-15T23:13:02.836719Z","title":"Carrollian Conformal Fields and Flat Holography,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.836719Z"},"links":{"cited_paper":"/paper/2305.02884","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:bfafdb7deef15240c7ae86442aa964934144cadba18959425be3c0961f3d93d5","observation_id":"0d38ee2e-65bc-447d-a4a4-825556b4491f","resolution":{"observed_at":"2026-08-15T23:13:02.836719Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1509.01408","last_updated":"2015-09-04T11:25:24Z","snapshot_observed_at":"2026-08-20T05:18:11.727549Z","submitted_at":"2015-09-04T11:25:24Z","title":"Null to time-like infinity Green's functions for asymptotic symmetries in Minkowski spacetime","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1509.01408","snapshot_observed_at":"2026-08-15T23:13:02.840775Z","title":"Null to time-like infinity Green’s functions for asymptotic symmetries in Minkowski spacetime,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.840775Z"},"links":{"cited_paper":"/paper/1509.01408","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:1ae4036e9292325adc5cc70bbec4cafb45195e23b6a5bfcad0b854cc92e070c1","observation_id":"16398688-1a20-4a65-a041-686770a139af","resolution":{"observed_at":"2026-08-15T23:13:02.840775Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.05190","last_updated":"2024-07-08T13:35:56Z","snapshot_observed_at":"2026-08-18T00:06:24.926132Z","submitted_at":"2024-02-07T19:02:48Z","title":"Massive carrollian fields at timelike infinity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.05190","snapshot_observed_at":"2026-08-15T23:13:02.844324Z","title":"Massive carrollian fields at timelike infinity,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.844324Z"},"links":{"cited_paper":"/paper/2402.05190","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:6df23d209625a47485bc62ddeb867cceaccbf335eb763fee4b48dc70d85d4f02","observation_id":"cf116052-d1f6-48b0-8ccd-309de9f8419b","resolution":{"observed_at":"2026-08-15T23:13:02.844324Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.15996","last_updated":"2026-04-22T12:01:51Z","snapshot_observed_at":"2026-08-15T19:45:10.169105Z","submitted_at":"2024-12-20T15:45:24Z","title":"Ti and Spi, Carrollian extended boundaries at timelike and spatial infinity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.15996","snapshot_observed_at":"2026-08-15T23:13:02.848186Z","title":"Ti and Spi, Carrollian extended boundaries at timelike and spatial infinity,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.848186Z"},"links":{"cited_paper":"/paper/2412.15996","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:1a3e6f13501485a2e1fb20c63afd105e69655a1af417625ae16015bf7106bf51","observation_id":"d8090827-5b71-4354-9346-8c024e4577f0","resolution":{"observed_at":"2026-08-15T23:13:02.848186Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.750733Z","title":"Einstein’s equations near spatial infinity,","venue":null,"work_id":"8a4f3925-e05e-4e95-ba85-94d8603d0510","year":1982},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.851862Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:e96793cc0cbd4270d22af9d3513b0f18d683d3349b37eb39182b0b65bfd1e58e","observation_id":"0f5dea79-1999-499d-94fe-f4db271a17cf","resolution":{"observed_at":"2026-08-15T23:13:03.755964Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.03319","last_updated":"2024-04-30T13:06:47Z","snapshot_observed_at":"2026-08-16T17:36:38.984029Z","submitted_at":"2021-12-06T19:18:46Z","title":"Carrollian and celestial spaces at infinity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.03319","snapshot_observed_at":"2026-08-15T23:13:02.854847Z","title":"Carrollian and celestial spaces at infinity,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.854847Z"},"links":{"cited_paper":"/paper/2112.03319","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:f929cfb99c8ae549213b927d146de4a6aae320e5af68d791968bd67a18b2a2ec","observation_id":"d33b0870-a817-4678-b732-22fcfdf2dfaf","resolution":{"observed_at":"2026-08-15T23:13:02.854847Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.09962","last_updated":"2024-01-25T11:27:00Z","snapshot_observed_at":"2026-08-18T23:17:09.290704Z","submitted_at":"2023-09-18T17:38:10Z","title":"Asymptotic symmetries of projectively compact order one Einstein manifolds","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.09962","snapshot_observed_at":"2026-08-15T23:13:02.858131Z","title":"Asymptotic symmetries of projectively compact order one Einstein manifolds,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.858131Z"},"links":{"cited_paper":"/paper/2309.09962","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:c577dce9f9250fa32c86390d7a60e0bf0a11f42392d1cb71a1c43ebd5fed3b0d","observation_id":"17bc3ce3-2c2a-4342-b88f-3174a0d5b6e6","resolution":{"observed_at":"2026-08-15T23:13:02.858131Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.01800","last_updated":"2024-06-03T21:42:00Z","snapshot_observed_at":"2026-08-19T12:03:28.995701Z","submitted_at":"2024-06-03T21:42:00Z","title":"Projective and Carrollian geometry at time/space-like infinity on projectively compact Ricci flat Einstein manifolds","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.01800","snapshot_observed_at":"2026-08-15T23:13:02.861454Z","title":"Projective and Carrollian geometry at time/space-like infinity on projectively compact Ricci flat Einstein manifolds,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.861454Z"},"links":{"cited_paper":"/paper/2406.01800","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:291dfe00d5763d4d33bef1faeca57668dd01689bc55f0087dcda89b1bf10261b","observation_id":"d31e288b-314a-4fde-8bd1-139bbbc91b5c","resolution":{"observed_at":"2026-08-15T23:13:02.861454Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.739202Z","title":"A unified treatment of null and spatial infinity in general relativity. I - Universal structure, asymptotic symmetries, and conserved quantities at spatial infinity,","venue":null,"work_id":"c1325134-b9ec-40ad-95ec-163c4e31cd5b","year":1978},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.865447Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:ef2ef8b4e3175ad9b5cb210710f11a5895394e929bd2a23d0c47889ef9e2aeea","observation_id":"8d72308c-84b9-4283-a093-717993e137b9","resolution":{"observed_at":"2026-08-15T23:13:03.744029Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:02.868777Z","title":"Spatial infinity as a boundary of space-time,","venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.868777Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:9b4e50439fee5c7a32e3ae808c1f22cf7c53d302f2d61132c0ff883fc920a095","observation_id":"fcc7aa77-a7db-4d53-9201-f1e28df26fe3","resolution":{"observed_at":"2026-08-15T23:13:02.868777Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1704.06223","last_updated":"2018-03-07T11:07:19Z","snapshot_observed_at":"2026-08-14T21:05:45.656587Z","submitted_at":"2017-04-20T16:48:15Z","title":"The BMS4 algebra at spatial infinity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1704.06223","snapshot_observed_at":"2026-08-15T23:13:02.871983Z","title":"The BMS4 algebra at spatial infinity,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.871983Z"},"links":{"cited_paper":"/paper/1704.06223","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:e4e3584932e1a25c8deca578a782eb643a37d755ce0e6866f64014334662a562","observation_id":"66937e06-354d-4642-9c5e-40e717e9760e","resolution":{"observed_at":"2026-08-15T23:13:02.871983Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1805.11288","last_updated":"2018-05-29T08:04:14Z","snapshot_observed_at":"2026-08-17T05:00:59.336119Z","submitted_at":"2018-05-29T08:04:14Z","title":"Hamiltonian structure and asymptotic symmetries of the Einstein-Maxwell system at spatial infinity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1805.11288","snapshot_observed_at":"2026-08-15T23:13:02.875584Z","title":"Hamiltonian structure and asymptotic symmetries of the Einstein-Maxwell system at spatial infinity,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.875584Z"},"links":{"cited_paper":"/paper/1805.11288","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:203ac3c98da473181fef5385f941eef588d1140f451fbc1b8d1cf714d67aa0af","observation_id":"218fffd0-8788-48f7-8737-c7203caaf273","resolution":{"observed_at":"2026-08-15T23:13:02.875584Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.03718","last_updated":"2018-01-11T11:29:05Z","snapshot_observed_at":"2026-08-14T19:56:01.775165Z","submitted_at":"2018-01-11T11:29:05Z","title":"BMS Group at Spatial Infinity: the Hamiltonian (ADM) approach","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.03718","snapshot_observed_at":"2026-08-15T23:13:02.878926Z","title":"BMS Group at Spatial Infinity: the Hamiltonian (ADM) approach,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.878926Z"},"links":{"cited_paper":"/paper/1801.03718","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:5e1fa8b7986902892342f5c42421c4d6ca213482726ce4ce61c5582769ee36ea","observation_id":"29b79c26-4694-4763-b68f-9ba4e95e4228","resolution":{"observed_at":"2026-08-15T23:13:02.878926Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1904.04495","last_updated":"2019-08-22T14:31:00Z","snapshot_observed_at":"2026-08-16T12:07:34.311719Z","submitted_at":"2019-04-09T07:11:54Z","title":"The asymptotic structure of gravity at spatial infinity in four spacetime dimensions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1904.04495","snapshot_observed_at":"2026-08-15T23:13:02.882378Z","title":"The asymptotic structure of gravity at spatial infinity in four spacetime dimensions,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.882378Z"},"links":{"cited_paper":"/paper/1904.04495","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:e68b49e30f69f41f3a39d23bbce8fb2b7c894a3abea82f62695b27b356a74997","observation_id":"a119b349-dad6-4ab0-9e9e-7bc8f1584133","resolution":{"observed_at":"2026-08-15T23:13:02.882378Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.08907","last_updated":"2022-01-21T12:11:12Z","snapshot_observed_at":"2026-08-18T07:33:36.264147Z","submitted_at":"2021-11-17T05:03:32Z","title":"Supertranslations at Timelike Infinity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.08907","snapshot_observed_at":"2026-08-15T23:13:02.886713Z","title":"Supertranslations at timelike infinity,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.886713Z"},"links":{"cited_paper":"/paper/2111.08907","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:5d4dc0eddc5d8eba7b17a2bb9a41e95bc299a460bd7eaa6710e660f53b6c419c","observation_id":"9a5a51e1-1129-4baa-adc4-adb97ce02bf3","resolution":{"observed_at":"2026-08-15T23:13:02.886713Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.17124","last_updated":"2023-11-20T00:21:32Z","snapshot_observed_at":"2026-08-16T15:44:12.388597Z","submitted_at":"2023-03-30T03:21:18Z","title":"An asymptotic framework for gravitational scattering","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.17124","snapshot_observed_at":"2026-08-15T23:13:02.890118Z","title":"An asymptotic framework for gravitational scattering,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.890118Z"},"links":{"cited_paper":"/paper/2303.17124","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:a6a98c4cafb36463ebb7fdf4ccd11e76b097018ffec752aa03f2410f5de78341","observation_id":"378ffe89-ddbc-4b5a-8399-0f9f917b2ab2","resolution":{"observed_at":"2026-08-15T23:13:02.890118Z","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":"2026-08-15T23:13:02.893722Z","title":"Weinberg, The Quantum theory of fields","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.893722Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:3ef3f2b89eec8b6de817733cba46aee3cdc1e96ff746cab031429b0d07cae04e","observation_id":"dfba7381-5a1b-40fe-a9d6-f1460c414d30","resolution":{"observed_at":"2026-08-15T23:13:02.893722Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0611263","last_updated":"2021-06-13T13:47:57Z","snapshot_observed_at":"2026-08-18T23:09:19.602722Z","submitted_at":"2006-11-24T10:44:07Z","title":"The unitary representations of the Poincare group in any spacetime dimension","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0611263","snapshot_observed_at":"2026-08-15T23:13:02.897611Z","title":"The unitary representations of the Poincar \\’e group in any spacetime dimension,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.897611Z"},"links":{"cited_paper":"/paper/hep-th/0611263","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:2133697ac42ae07e4e25e4849c61acfab8e7dd034e9ff7af48b487be1a1bd0f4","observation_id":"e58cb38f-2d91-4434-98d9-d21857a4a2e3","resolution":{"observed_at":"2026-08-15T23:13:02.897611Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1708.01030","last_updated":"2017-08-18T10:06:48Z","snapshot_observed_at":"2026-08-14T20:43:29.991296Z","submitted_at":"2017-08-03T07:27:54Z","title":"Elementary particles with continuous spin","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1708.01030","snapshot_observed_at":"2026-08-15T23:13:02.900916Z","title":"Elementary particles with continuous spin,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.900916Z"},"links":{"cited_paper":"/paper/1708.01030","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:b8ab6265bb9aecab76a8dc689628a5aebe94ad8c129b4d2f812623b98e84b2bb","observation_id":"e2b6c0e0-35fb-4642-92a7-7b02ab21dbc4","resolution":{"observed_at":"2026-08-15T23:13:02.900916Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.14334","last_updated":"2022-09-09T13:40:51Z","snapshot_observed_at":"2026-08-20T02:58:39.144429Z","submitted_at":"2022-03-27T15:47:29Z","title":"Infrared Finite Scattering Theory in Quantum Field Theory and Quantum Gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.14334","snapshot_observed_at":"2026-08-15T23:13:02.904325Z","title":"Infrared finite scattering theory in quantum field theory and quantum gravity,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.904325Z"},"links":{"cited_paper":"/paper/2203.14334","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:a8712063722eea64058d7d3b8c830ff3523454a05ba0f0a1dda5fc61086eac3b","observation_id":"f213e1c4-f398-48b4-b8d8-bcfbce1577e7","resolution":{"observed_at":"2026-08-15T23:13:02.904325Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.00102","last_updated":"2024-08-07T15:28:51Z","snapshot_observed_at":"2026-08-16T14:22:45.317030Z","submitted_at":"2024-01-31T19:00:00Z","title":"Infrared finite scattering theory: Scattering states and representations of the BMS group","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.00102","snapshot_observed_at":"2026-08-15T23:13:02.907910Z","title":"Infrared finite scattering theory: scattering states and representations of the BMS group,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.907910Z"},"links":{"cited_paper":"/paper/2402.00102","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:385b7cc14446d510251d21865ed5f9dd662de04d8a6e7c036b10593beb3796bf","observation_id":"a272412d-5171-4107-abdd-4ca9048dbef0","resolution":{"observed_at":"2026-08-15T23:13:02.907910Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2303.04816","last_updated":"2023-04-05T22:16:06Z","snapshot_observed_at":"2026-08-16T15:49:43.896924Z","submitted_at":"2023-03-08T19:00:00Z","title":"Interactions of Particles with \"Continuous Spin\" Fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.04816","snapshot_observed_at":"2026-08-15T23:13:02.911354Z","title":"Interactions of Particles with","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.911354Z"},"links":{"cited_paper":"/paper/2303.04816","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:d1934c20b94ca9e11b9c8c3ec4d4670f785ba9351906b9a0aa854cb98070054f","observation_id":"b5ecdd21-47df-4bfc-812f-1c38746ba515","resolution":{"observed_at":"2026-08-15T23:13:02.911354Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.715760Z","title":"Tensor harmonics on the 3-sphere,","venue":null,"work_id":"890e9c9f-8e06-4e5c-b2f9-e8131be6a078","year":1978},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.914816Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:9e09c0f878c7ba88a62bb6ab48794a2817e46c02c04d8067e6aa3d8fdfe255c2","observation_id":"65c2cd0f-2cf0-4a79-bb8f-0d93ed8506ed","resolution":{"observed_at":"2026-08-15T23:13:03.718964Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.705317Z","title":"The peter–weyl theorem & harmonic analysis on sn,","venue":null,"work_id":"02fa1ba9-41e2-46bb-91de-873cade4d268","year":2024},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.917972Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:632f17feab129b892d88cd25899217095db4ab8e6c95ba6435a691c9d43dfd1c","observation_id":"bf774479-2f2f-43b4-b637-f780615e3604","resolution":{"observed_at":"2026-08-15T23:13:03.709534Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.693968Z","title":"Group theory and the hydrogen atom (i),","venue":null,"work_id":"8551753b-018e-4387-b98d-f747b0e6dd91","year":1966},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.921064Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:65f17d0dfe10a3f3a583b93ee109c511a5e0919ab164bcb700d141dcb711538c","observation_id":"2fa73b49-c1c6-4479-b58e-2de62035abc8","resolution":{"observed_at":"2026-08-15T23:13:03.698014Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1210.2518","last_updated":"2013-05-23T16:42:55Z","snapshot_observed_at":"2026-08-17T14:03:37.242182Z","submitted_at":"2012-10-09T07:59:46Z","title":"Probing the Early Universe with the CMB Scalar, Vector and Tensor Bispectrum","version":2},"cited_work":{"arxiv_id":"1210.2518","doi":null,"metadata_source":"pith","pith_arxiv_id":"1210.2518","snapshot_observed_at":"2026-08-15T23:13:03.097414Z","title":"Probing the Early Universe with the CMB Scalar, Vector and Tensor Bispectrum","venue":"astro-ph.CO","work_id":"e5a481d9-ac7f-498c-a314-a9fddc5e5789","year":2012},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.924674Z"},"links":{"cited_paper":"/paper/1210.2518","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:bc27bc36c42d1b9a118396ee9e4e7e8e37cb990d66a68e85c1cf6db2073f1ad7","observation_id":"72a257b2-0e77-4921-baed-80bcf373241a","resolution":{"observed_at":"2026-08-15T23:13:03.103281Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.682321Z","title":null,"venue":null,"work_id":"e407980e-a96c-4510-b189-50abd4564c20","year":1977},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.928286Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:83e1f39014fbe839efadc2f50b7ae50dcefa352351c10e1998173706e82cb11e","observation_id":"2131299f-0a6d-4b11-b33f-d4ad0ae3d6d2","resolution":{"observed_at":"2026-08-15T23:13:03.685844Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1409.1800","last_updated":"2015-04-28T14:06:24Z","snapshot_observed_at":"2026-08-17T19:29:27.390476Z","submitted_at":"2014-09-05T13:50:52Z","title":"Geometry and Physics of Null Infinity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.1800","snapshot_observed_at":"2026-08-15T23:13:02.931532Z","title":"Geometry and Physics of Null Infinity,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.931532Z"},"links":{"cited_paper":"/paper/1409.1800","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:94d09ea2ac2b2f4829ef4f734dc2de504e84c68a987463baede9ad548a73b299","observation_id":"e2b9bd41-e5b9-46da-9703-2dc91b155ac7","resolution":{"observed_at":"2026-08-15T23:13:02.931532Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.01281","last_updated":"2020-08-27T08:22:57Z","snapshot_observed_at":"2026-08-16T00:17:16.580753Z","submitted_at":"2020-01-05T18:08:59Z","title":"Asymptotic Shear and the Intrinsic Conformal Geometry of Null-Infinity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.01281","snapshot_observed_at":"2026-08-15T23:13:02.935136Z","title":"Asymptotic shear and the intrinsic conformal geometry of null-infinity,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.935136Z"},"links":{"cited_paper":"/paper/2001.01281","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:b8ed2ffab7e76ba1657c492374e0fb751615bb0cf3eed3a928e63a8c49f59be1","observation_id":"952c2d5b-677b-4e35-bed3-c5eb8d231a6e","resolution":{"observed_at":"2026-08-15T23:13:02.935136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2103.10405","last_updated":"2022-06-11T12:26:36Z","snapshot_observed_at":"2026-08-16T18:37:55.836676Z","submitted_at":"2021-03-18T17:40:54Z","title":"Tractor geometry of asymptotically flat spacetimes","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2103.10405","snapshot_observed_at":"2026-08-15T23:13:02.938474Z","title":"Tractor Geometry of Asymptotically Flat Spacetimes,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.938474Z"},"links":{"cited_paper":"/paper/2103.10405","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:f15507c01938aab009c17e99a7187c13f60660994eff3a5b2105e5bc731a240c","observation_id":"47213bfa-5934-4c4a-8fed-dacbe059dab8","resolution":{"observed_at":"2026-08-15T23:13:02.938474Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.09048","last_updated":"2022-09-09T14:46:49Z","snapshot_observed_at":"2026-08-19T00:34:08.379751Z","submitted_at":"2021-12-16T17:37:43Z","title":"Carrollian manifolds and null infinity: A view from Cartan geometry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.09048","snapshot_observed_at":"2026-08-15T23:13:02.942191Z","title":"Carrollian manifolds and null infinity: a view from Cartan geometry,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.942191Z"},"links":{"cited_paper":"/paper/2112.09048","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:6a1cc1d6bec6c87f9eba5c65ce94626c6a8329b8bdb73a8795f869d24210e069","observation_id":"2a227136-65a7-420b-967c-588e6e6a371e","resolution":{"observed_at":"2026-08-15T23:13:02.942191Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2109.00073","last_updated":"2021-08-31T20:47:13Z","snapshot_observed_at":"2026-08-16T17:59:40.385096Z","submitted_at":"2021-08-31T20:47:13Z","title":"Shadows and Soft Exchange in Celestial CFT","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2109.00073","snapshot_observed_at":"2026-08-15T23:13:02.945714Z","title":"Shadows and soft exchange in celestial CFT,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.945714Z"},"links":{"cited_paper":"/paper/2109.00073","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:ed4f50dac4a19feb77ff8a5cde104d8e050f02fa1ecf2d9cc41afc004c0249c4","observation_id":"ffdc06f5-007e-4927-b81f-c6ffaab732d0","resolution":{"observed_at":"2026-08-15T23:13:02.945714Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.10935","last_updated":"2022-05-22T21:37:33Z","snapshot_observed_at":"2026-08-16T16:58:34.171529Z","submitted_at":"2022-05-22T21:37:33Z","title":"Soft Scalars and the Geometry of the Space of Celestial CFTs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.10935","snapshot_observed_at":"2026-08-15T23:13:02.949466Z","title":"Soft scalars and the geometry of the space of celestial conformal field theories,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.949466Z"},"links":{"cited_paper":"/paper/2205.10935","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:8ebd25bbb099c8705b170676d9b48e9aa697410a94ae5b91ec41e2767247d837","observation_id":"36a4ba8f-4c83-4ceb-ab6d-d276111419a6","resolution":{"observed_at":"2026-08-15T23:13:02.949466Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.00606","last_updated":"2023-07-06T15:14:52Z","snapshot_observed_at":"2026-08-19T20:20:15.132756Z","submitted_at":"2022-10-02T19:27:44Z","title":"Soft Particles and Infinite-Dimensional Geometry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.00606","snapshot_observed_at":"2026-08-15T23:13:02.953202Z","title":"Soft particles and infinite-dimensional geometry,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.953202Z"},"links":{"cited_paper":"/paper/2210.00606","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:1088a6930448ef5fa6d8bdf65199d13599cf984ac3e9e6bc6eed69ed450e6294","observation_id":"18b0e482-63e7-4813-8850-d98a4598c196","resolution":{"observed_at":"2026-08-15T23:13:02.953202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.18637","last_updated":"2024-11-01T06:54:27Z","snapshot_observed_at":"2026-08-16T14:14:24.418298Z","submitted_at":"2024-02-28T19:00:02Z","title":"Infrared finite scattering theory: Amplitudes and soft theorems","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.18637","snapshot_observed_at":"2026-08-15T23:13:02.957725Z","title":"Infrared finite scattering theory: Amplitudes and soft theorems,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.957725Z"},"links":{"cited_paper":"/paper/2402.18637","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:794b6d13f10738286ac5bc95de5c069b281b0b2a54cf370d8a55d35e385de439","observation_id":"c799bf73-ebf8-4458-aa0e-065454ca2e37","resolution":{"observed_at":"2026-08-15T23:13:02.957725Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1808.07093","last_updated":"2018-09-18T23:19:12Z","snapshot_observed_at":"2026-08-15T09:34:58.292447Z","submitted_at":"2018-08-21T19:20:40Z","title":"Null infinity, the BMS group and infrared issues","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1808.07093","snapshot_observed_at":"2026-08-15T23:13:02.961349Z","title":"Null infinity, the BMS group and infrared issues,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.961349Z"},"links":{"cited_paper":"/paper/1808.07093","citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:cedbe0c53f235edb6a02716c358426784d5cbeadcba899124494d3c09a5d739e","observation_id":"599dc174-b8ba-4f81-a6a9-88e591e83a2f","resolution":{"observed_at":"2026-08-15T23:13:02.961349Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-15T23:13:03.670819Z","title":"Hungerford, Algebra","venue":null,"work_id":"cedf9bb2-c3ea-4e13-9457-e85fd4d28a12","year":2003},"citing_paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-15T23:13:02.964913Z"},"links":{"citing_paper":"/paper/2505.05368"},"observation_digest":"sha256:7ecd1b9976e4e5fadbf4ae53f406c3c23084b1a5fd8b1e3db800488f6c63c646","observation_id":"221f2446-1992-409a-a9d7-d07636a2bfec","resolution":{"observed_at":"2026-08-15T23:13:03.675200Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-21T06:32:19.484+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2505.05368","last_updated":"2025-05-08T16:05:13Z","latest_version":1,"primary_category":"hep-th","snapshot_observed_at":"2026-08-19T17:06:32.549266Z","submitted_at":"2025-05-08T16:05:13Z","title":"BMS representations for generic supermomentum"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":77,"verified_exact":3,"verified_fuzzy":20},"total_outbound_references":103},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-21T06:32:19.484+00:00","source":"crossref"},{"observed_at":"2026-08-21T06:32:16.066871+00:00","source":"retraction_watch"}],"thesis":"As of 21 August 2026, this Paper Citation Record lists 100 of 103 outbound references and 6 inbound Pith citation observations for arXiv:2505.05368."}