{"as_of":"2026-08-22T00:12:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:8b116796b21e004b1724213cbed043d3f1bf2e6b481ca5c76f8a50c4f0d463dd","coverage":[{"denominator":112,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":100,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T15:23:51.572310Z","state":"measured"},{"denominator":100,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":100,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-21T06:32:19.484+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2608.05324/citation-record","integrity":"/paper/2608.05324/integrity","json":"/paper/2608.05324/citation-record.json","paper":"/paper/2608.05324"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:23:51.230282Z","title":"Effective Lagrangians for Bound State Problems in QED, QCD, and Other Field Theories,","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.230282Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:97ec254e4a1645934a07d0a858cb6e1af75c3a57d581c3a36f245b927bc3b18a","observation_id":"2035bf35-bd9d-462a-86be-57d14f13513e","resolution":{"observed_at":"2026-08-08T15:23:51.230282Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0410047","last_updated":"2005-04-26T08:16:54Z","snapshot_observed_at":"2026-07-07T04:05:12.693563Z","submitted_at":"2004-10-04T08:23:56Z","title":"Effective field theories for heavy quarkonium","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0410047","snapshot_observed_at":"2026-08-08T15:23:51.234060Z","title":"Effective Field Theories for Heavy Quarkonium,","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.234060Z"},"links":{"cited_paper":"/paper/hep-ph/0410047","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:0997bf3b6b63200be49f2f57d679659093787bddb8727b51623e6993295e48f5","observation_id":"0e30737b-2c6b-42b5-88e8-a2a474ec0b3d","resolution":{"observed_at":"2026-08-08T15:23:51.234060Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"cond-mat/0509786","last_updated":"2006-01-14T23:59:09Z","snapshot_observed_at":"2026-08-17T16:14:35.067485Z","submitted_at":"2005-09-29T23:10:07Z","title":"General coordinate invariance and conformal invariance in nonrelativistic physics: Unitary Fermi gas","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"cond-mat/0509786","snapshot_observed_at":"2026-08-08T15:23:51.237886Z","title":"General coordinate invariance and conformal invariance in nonrelativistic physics: Unitary Fermi gas,","venue":null,"work_id":null,"year":2006},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.237886Z"},"links":{"cited_paper":"/paper/cond-mat/0509786","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:e39645fcbe2fd006a10e2aca0d90faa71ccb787e7ad072df0d87edaf19eadb3e","observation_id":"6f4c45b2-b52d-41c6-8c80-88cd71f5f718","resolution":{"observed_at":"2026-08-08T15:23:51.237886Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"nucl-th/0203055","last_updated":"2002-03-20T21:46:40Z","snapshot_observed_at":"2026-08-21T07:26:15.884767Z","submitted_at":"2002-03-20T21:46:40Z","title":"Effective Field Theory for Few-Nucleon Systems","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"nucl-th/0203055","snapshot_observed_at":"2026-08-08T15:23:51.241448Z","title":"Effective field theory for few nucleon systems,","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.241448Z"},"links":{"cited_paper":"/paper/nucl-th/0203055","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:0e496ec15976d37fd4687de4b4a014925972f656cf59ca9c070b6680031e5db0","observation_id":"d8ceeab0-9708-4970-b8b0-20c8e7ef9af6","resolution":{"observed_at":"2026-08-08T15:23:51.241448Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.1252","last_updated":"2014-09-06T11:36:14Z","snapshot_observed_at":"2026-08-15T02:07:15.589972Z","submitted_at":"2014-07-04T14:46:01Z","title":"Spacetime Symmetries of the Quantum Hall Effect","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.1252","snapshot_observed_at":"2026-08-08T15:23:51.245365Z","title":"Spacetime Symmetries of the Quantum Hall Effect,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.245365Z"},"links":{"cited_paper":"/paper/1407.1252","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:5771e9b99f45a397be1cf488a0d19cbbb8a024c732f25311c8fe0b553eb64170","observation_id":"26f88785-a06c-4920-bc0e-ccaddfa568e1","resolution":{"observed_at":"2026-08-08T15:23:51.245365Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.09142","last_updated":"2022-09-21T09:51:34Z","snapshot_observed_at":"2026-08-16T16:59:23.373088Z","submitted_at":"2022-05-18T18:01:04Z","title":"Relativistic Fluids, Hydrodynamic Frames and their Galilean versus Carrollian Avatars","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.09142","snapshot_observed_at":"2026-08-08T15:23:51.248998Z","title":"Relativistic fluids, hydrodynamic frames and their Galilean versus Carrollian avatars,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.248998Z"},"links":{"cited_paper":"/paper/2205.09142","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:e12e6755b342085584536925784cd8eecdbd555ca8141774c6e4f10e6fca1347","observation_id":"5c869c8f-f5b6-4317-9953-f07bb8b5c2e7","resolution":{"observed_at":"2026-08-08T15:23:51.248998Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.00027","last_updated":"2024-03-16T21:54:50Z","snapshot_observed_at":"2026-08-19T00:41:30.236624Z","submitted_at":"2023-10-31T18:00:01Z","title":"Aspects of Non-Relativistic Quantum Field Theories","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.00027","snapshot_observed_at":"2026-08-08T15:23:51.253102Z","title":"Aspects of non-relativistic quantum field theories,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.253102Z"},"links":{"cited_paper":"/paper/2311.00027","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:f9a3cc65da7d613dc6ba3843af7b78f095fc183e03bcc5949679bc345618bdf2","observation_id":"9961bdb1-6323-45e3-93e3-b565856ed48e","resolution":{"observed_at":"2026-08-08T15:23:51.253102Z","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":"2026-08-08T15:23:51.256826Z","title":"Une nouvelle limite non-relativiste du groupe de Poincar´ e,","venue":null,"work_id":null,"year":1965},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.256826Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:d3d3f19438993581eb5f0ce347ffb4cd296d164178ddffd67b9e051e6928bce2","observation_id":"e0bb8f9d-1131-480f-a298-09822dfa4cac","resolution":{"observed_at":"2026-08-08T15:23:51.256826Z","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":"2026-08-08T15:23:51.260011Z","title":"On an analogue of the Galilei group,","venue":null,"work_id":null,"year":1966},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.260011Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:3bf792feed76a8cec03aa26c9dc29fe3470674837f2e9d92d0669084e2e05c20","observation_id":"58ce3e22-b9a4-4810-af0f-6b2796cc184e","resolution":{"observed_at":"2026-08-08T15:23:51.260011Z","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":"2026-08-08T15:23:51.263236Z","title":"Possible kinematics,","venue":null,"work_id":null,"year":1968},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.263236Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:fff6b866cbf8230a14ba32d9ddeee0ca7c3f23657ff3133521d8b7e4c06b33e7","observation_id":"6484d4ef-b63a-4359-a0d9-3f13106f14e6","resolution":{"observed_at":"2026-08-08T15:23:51.263236Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1402.0657","last_updated":"2014-03-11T02:02:22Z","snapshot_observed_at":"2026-08-14T23:45:55.541594Z","submitted_at":"2014-02-04T08:43:18Z","title":"Carroll versus Newton and Galilei: two dual non-Einsteinian concepts of time","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1402.0657","snapshot_observed_at":"2026-08-08T15:23:51.266284Z","title":"Carroll versus Newton and Galilei: two dual non-Einsteinian concepts of time,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.266284Z"},"links":{"cited_paper":"/paper/1402.0657","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:89610d813dc9e8bf3890724be9bc5c13e95f5f6be663a876ba6f018afc42123d","observation_id":"69c611df-d6f2-4f67-8f4f-1edd83db81b6","resolution":{"observed_at":"2026-08-08T15:23:51.266284Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.02221","last_updated":"2019-05-06T18:03:30Z","snapshot_observed_at":"2026-08-14T16:36:31.672074Z","submitted_at":"2019-05-06T18:03:30Z","title":"Carroll Structures, Null Geometry and Conformal Isometries","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.02221","snapshot_observed_at":"2026-08-08T15:23:51.269735Z","title":"Carroll Structures, Null Geometry and Conformal Isometries,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.269735Z"},"links":{"cited_paper":"/paper/1905.02221","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:87019b9110dcc013459e420033305390e30672dd6ec3dd416f28232866afaff6","observation_id":"78fd6ec2-be37-4dcd-b0d4-4d42eb94e9ed","resolution":{"observed_at":"2026-08-08T15:23:51.269735Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2406.19343","last_updated":"2024-06-27T17:18:57Z","snapshot_observed_at":"2026-08-16T13:38:59.368840Z","submitted_at":"2024-06-27T17:18:57Z","title":"Carrollian Amplitudes from Holographic Correlators","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2406.19343","snapshot_observed_at":"2026-08-08T15:23:51.273044Z","title":"Carrollian amplitudes from holographic correlators,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.273044Z"},"links":{"cited_paper":"/paper/2406.19343","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:9d9ba4d07e6a52336a8bc5757a98dd9fce1167ccb655a618206713a83131ac5a","observation_id":"d7936359-7b4f-4ddc-9170-9de3b8e0acca","resolution":{"observed_at":"2026-08-08T15:23:51.273044Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2202.04702","last_updated":"2022-08-16T08:35:08Z","snapshot_observed_at":"2026-08-16T22:54:36.476415Z","submitted_at":"2022-02-09T19:52:15Z","title":"Carrollian Perspective on Celestial Holography","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2202.04702","snapshot_observed_at":"2026-08-08T15:23:51.276326Z","title":"Carrollian Perspective on Celestial Holography,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.276326Z"},"links":{"cited_paper":"/paper/2202.04702","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:0c8cf03a5dc004f35445ffd55c00c1d6734fc3da6b16c62400c0c4f93583309b","observation_id":"4578dc8b-ff12-4bd7-a1fe-524de1bdef2e","resolution":{"observed_at":"2026-08-08T15:23:51.276326Z","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":"2026-08-08T15:23:51.279730Z","title":"Carrollian physics and holography,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.279730Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:12a8f220748141776f4500a4e1904354afcf6ed3136ff26ba831d21f0d2a3d40","observation_id":"f4879d97-2323-4488-9682-32fa4b5f2ff2","resolution":{"observed_at":"2026-08-08T15:23:51.279730Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.10138","last_updated":"2023-12-15T19:00:00Z","snapshot_observed_at":"2026-08-20T01:21:06.395688Z","submitted_at":"2023-12-15T19:00:00Z","title":"Carrollian Amplitudes and Celestial Symmetries","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.10138","snapshot_observed_at":"2026-08-08T15:23:51.282754Z","title":"Carrollian amplitudes and celestial symmetries,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.282754Z"},"links":{"cited_paper":"/paper/2312.10138","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:a4ab428b442369663b2f3f6335dfe9a17cc35480e7f549180f62f055bd514cc9","observation_id":"f10a93c9-7a73-4cc1-81e7-38c44f8cf21d","resolution":{"observed_at":"2026-08-08T15:23:51.282754Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2211.13695","last_updated":"2023-03-25T17:12:05Z","snapshot_observed_at":"2026-08-20T11:02:14.196232Z","submitted_at":"2022-11-24T16:19:49Z","title":"Carrollian Motion in Magnetized Black Hole Horizons","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2211.13695","snapshot_observed_at":"2026-08-08T15:23:51.285882Z","title":"Carrollian motion in magnetized black hole horizons,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.285882Z"},"links":{"cited_paper":"/paper/2211.13695","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:394bbbbc077848416e5bf9eb6a71a98ad2b844d29746227ae3d3f6387a69ad6d","observation_id":"18e16173-0e82-4f62-9455-0c0eee042602","resolution":{"observed_at":"2026-08-08T15:23:51.285882Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1903.09654","last_updated":"2020-05-07T09:19:16Z","snapshot_observed_at":"2026-08-20T15:10:07.143035Z","submitted_at":"2019-03-22T18:03:22Z","title":"Carrollian Physics at the Black Hole Horizon","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1903.09654","snapshot_observed_at":"2026-08-08T15:23:51.289189Z","title":"Carrollian Physics at the Black Hole Horizon,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.289189Z"},"links":{"cited_paper":"/paper/1903.09654","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:c34d1080b330ccd29a7dcad2d2bc2075933c94bc9d81ccc22c8b9e1e8bcc1c7a","observation_id":"50f8449b-395a-40b4-8905-60a8e6ddcc7e","resolution":{"observed_at":"2026-08-08T15:23:51.289189Z","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":"2026-08-08T15:23:51.292473Z","title":"Carroll black holes,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.292473Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:817e25f1d8296e1ee533f28dce15a13653e4e144d740140f175fae2ec2114e65","observation_id":"e0b6469b-b0a3-4a43-b15b-9d3fe95ec706","resolution":{"observed_at":"2026-08-08T15:23:51.292473Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2605.15269","last_updated":"2026-06-02T18:21:13Z","snapshot_observed_at":"2026-08-14T01:36:38.922935Z","submitted_at":"2026-05-14T18:00:01Z","title":"Kerroll black holes","version":2},"cited_work":{"arxiv_id":"2605.15269","doi":null,"metadata_source":"pith","pith_arxiv_id":"2605.15269","snapshot_observed_at":"2026-08-08T15:23:52.720681Z","title":"Kerroll black holes","venue":"hep-th","work_id":"8f6a5271-d853-4acc-87e9-2a86c8279a60","year":2026},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.295414Z"},"links":{"cited_paper":"/paper/2605.15269","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:7fe33a42170ce1df34f0844d30d67db69df6f47287b119cb6bc0af53e0867847","observation_id":"1375330b-d678-433d-aad5-62eee6df159e","resolution":{"observed_at":"2026-08-08T15:23:52.724387Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:23:51.298995Z","title":"Sourced Carrollian fluids dual to black hole horizons,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.298995Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:5b37a2f4adcc907c26382f5462e3060070d3751565dda6292acfd9c0d9c62ac8","observation_id":"e0940fe1-be81-486a-9290-c7c1af68fe65","resolution":{"observed_at":"2026-08-08T15:23:51.298995Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.02360","last_updated":"2025-05-17T10:06:25Z","snapshot_observed_at":"2026-08-21T00:06:12.492514Z","submitted_at":"2022-12-05T15:45:09Z","title":"Hall effects in Carroll dynamics","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.02360","snapshot_observed_at":"2026-08-08T15:23:51.302073Z","title":"Hall effects in Carroll dynamics,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.302073Z"},"links":{"cited_paper":"/paper/2212.02360","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:e75585596e94b05c183a80a42d72003d2dc36d3ded4f58dd11c90450fcde7a40","observation_id":"30b5816e-8b76-425d-83b5-2879b8ad39ea","resolution":{"observed_at":"2026-08-08T15:23:51.302073Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2508.01446","last_updated":"2026-01-16T12:24:26Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-08-02T17:28:33Z","title":"Radiation in Fluid/Gravity and the Flat Limit","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2508.01446","snapshot_observed_at":"2026-08-08T15:23:51.305518Z","title":"Radiation in fluid/gravity and the flat limit,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.305518Z"},"links":{"cited_paper":"/paper/2508.01446","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:27d021b7cd4596765444c674b73db506366c716a0121d7b96bf04fc65d3b9e2f","observation_id":"22b36a83-e4b8-4b09-a0ae-e28aa2508f9f","resolution":{"observed_at":"2026-08-08T15:23:51.305518Z","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":"2026-08-08T15:23:51.308752Z","title":"Classical Null Strings,","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.308752Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:7a5a02b586c1f6030401be58bcd544fa5fa87ac760bc4afa06c454d6fff72970","observation_id":"9b8f22a9-6711-46fc-84aa-1d25a8f99da8","resolution":{"observed_at":"2026-08-08T15:23:51.308752Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9307108","last_updated":"1993-07-16T15:22:30Z","snapshot_observed_at":"2026-08-14T20:15:20.223681Z","submitted_at":"1993-07-16T15:22:30Z","title":"Classical and Quantized Tensionless Strings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9307108","snapshot_observed_at":"2026-08-08T15:23:51.311709Z","title":"Classical and quantized tensionless strings,","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.311709Z"},"links":{"cited_paper":"/paper/hep-th/9307108","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:5248daf4128f2789c2ceeec06da1e8f7948f177e727f5840bd24266c44f20791","observation_id":"a73ff924-bbec-42a1-b81b-7ff029b4418f","resolution":{"observed_at":"2026-08-08T15:23:51.311709Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1507.04361","last_updated":"2015-07-19T18:32:56Z","snapshot_observed_at":"2026-08-17T18:00:50.897612Z","submitted_at":"2015-07-15T20:01:30Z","title":"Tensionless Strings from Worldsheet Symmetries","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1507.04361","snapshot_observed_at":"2026-08-08T15:23:51.315138Z","title":"Tensionless Strings from Worldsheet Symmetries,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.315138Z"},"links":{"cited_paper":"/paper/1507.04361","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:1998b9f5534e0037db4172a9cee01c9e0f59c96dd91820b398ddc72fab9d2a63","observation_id":"946a38ec-ae15-4c80-aae7-bb7a75470fd8","resolution":{"observed_at":"2026-08-08T15:23:51.315138Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.11732","last_updated":"2019-05-28T10:45:00Z","snapshot_observed_at":"2026-08-21T08:08:59.051983Z","submitted_at":"2019-05-28T10:45:00Z","title":"The tensionless path from closed to open strings","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1905.11732","snapshot_observed_at":"2026-08-08T15:23:51.318385Z","title":"Tensionless Path from Closed to Open Strings,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.318385Z"},"links":{"cited_paper":"/paper/1905.11732","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:3d32e5ca939cd48b7afef3e2e5d33c2460dac9946af014ee8a30e6d02a62de12","observation_id":"0bb9c06e-4c60-4933-a5ee-0ebc542dea52","resolution":{"observed_at":"2026-08-08T15:23:51.318385Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.00354","last_updated":"2020-01-02T08:08:58Z","snapshot_observed_at":"2026-08-10T16:25:17.652414Z","submitted_at":"2020-01-02T08:08:58Z","title":"A Tale of Three. Tensionless strings and vacuum structure","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.00354","snapshot_observed_at":"2026-08-08T15:23:51.321623Z","title":"A tale of three — tensionless strings and vacuum structure,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.321623Z"},"links":{"cited_paper":"/paper/2001.00354","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:f86dafdf08799fc47c0a2d15679a150d07f6673efbd19ae79064c2673b8d6416","observation_id":"6a9cb795-0596-4582-aa99-fc94dbfc23f0","resolution":{"observed_at":"2026-08-08T15:23:51.321623Z","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":"2026-08-08T15:23:51.325117Z","title":"Scale and conformal transformations in galilean-covariant field theory,","venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.325117Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:8a019be4be24a19cb5aa5d9f04694ae2554a474d1d7311ddc8325be59bd46fe4","observation_id":"3b349ba5-28c6-4373-b9c3-fefac03a1dfd","resolution":{"observed_at":"2026-08-08T15:23:51.325117Z","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":"2026-08-08T15:23:51.328257Z","title":"Galilean invariant lee model for all spins and parities,","venue":null,"work_id":null,"year":1971},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.328257Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:f68504609edaa0ef165e8aab8bb8b197c68055ebd0e7038665409a3916e10fd2","observation_id":"5ad9c8ec-dd32-438c-94c7-2e43f4343837","resolution":{"observed_at":"2026-08-08T15:23:51.328257Z","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":"2026-08-08T15:23:51.331458Z","title":"Magnetic moment of a particle with arbitrary spin,","venue":null,"work_id":null,"year":1970},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.331458Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:961cc7e88d619d87b4306ba895ed68179b2859db026b6aaa1e63482c1fcb00f4","observation_id":"6281bad0-3411-4329-82ec-f9c468e495dc","resolution":{"observed_at":"2026-08-08T15:23:51.331458Z","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":"2026-08-08T15:23:51.334350Z","title":"A Pseudoclassical Description for a Nonrelativistic Spinning Particle. 1. The Levy-leblond Equation,","venue":null,"work_id":null,"year":1986},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.334350Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:0c4012adfb1065ac4c72db325f0bb032dfebca84b3971987a62214c8073d728d","observation_id":"431808ba-ba65-431a-9e9a-d2d84ae78002","resolution":{"observed_at":"2026-08-08T15:23:51.334350Z","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":"2026-08-08T15:23:51.337591Z","title":"Galilean Quantum Field Theories and a Ghostless Lee Model,","venue":null,"work_id":null,"year":1967},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.337591Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:718e6a935a4a8b4e34f2b7c2b70add5d481552d105d9b0c57c6db79124b33b74","observation_id":"8ccb410f-7119-42d8-9df8-341ab1cc7150","resolution":{"observed_at":"2026-08-08T15:23:51.337591Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0512188","last_updated":"2005-12-15T15:36:48Z","snapshot_observed_at":"2026-08-03T10:19:58.458880Z","submitted_at":"2005-12-15T15:36:48Z","title":"Celestial Mechanics, Conformal Structures, and Gravitational Waves","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0512188","snapshot_observed_at":"2026-08-08T15:23:51.340628Z","title":"Celestial mechanics, conformal structures and gravitational waves,","venue":null,"work_id":null,"year":1991},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.340628Z"},"links":{"cited_paper":"/paper/hep-th/0512188","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:f194e98123433a36389e3a25437110b97c747b217ded3b0b8635becfd56e6ec3","observation_id":"e304b4ff-4b65-483b-af94-60b5d1415187","resolution":{"observed_at":"2026-08-08T15:23:51.340628Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0903.1641","last_updated":"2009-03-09T20:07:44Z","snapshot_observed_at":"2026-08-15T05:53:18.421150Z","submitted_at":"2009-03-09T20:07:44Z","title":"Galilean Isometries","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0903.1641","snapshot_observed_at":"2026-08-08T15:23:51.343978Z","title":"On Galileian isometries,","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.343978Z"},"links":{"cited_paper":"/paper/0903.1641","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:2ed1b2652ea9812fdbcb3d3b57a63d0a5d6edbb0ab65183ae3e39bca7a3125e4","observation_id":"c8073d1f-2d56-4fff-86ee-a6166d758b0c","resolution":{"observed_at":"2026-08-08T15:23:51.343978Z","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":"2026-08-08T15:23:51.347132Z","title":"The maximal kinematical invariance group of the free Schrodinger equation.,","venue":null,"work_id":null,"year":1972},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.347132Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:b7adacd04df10178e453bb407608b498eeac2c2ff0835df3988db127cecaabf6","observation_id":"409e29eb-bb96-4f0a-975d-36791bbea0bb","resolution":{"observed_at":"2026-08-08T15:23:51.347132Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2403.20316","last_updated":"2025-05-19T00:43:36Z","snapshot_observed_at":"2026-08-18T13:30:20.165408Z","submitted_at":"2024-03-29T17:40:34Z","title":"Schr\\\"odinger symmetry: a historical review","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2403.20316","snapshot_observed_at":"2026-08-08T15:23:51.350329Z","title":"Schr¨ odinger Symmetry: A Historical Review,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.350329Z"},"links":{"cited_paper":"/paper/2403.20316","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:1add78b3648974f605b38fbc19e1a16e810ab1a18d1b6a7626e7b3832588ada2","observation_id":"9d676bc7-0564-4d7b-85ed-d755f7b75cc7","resolution":{"observed_at":"2026-08-08T15:23:51.350329Z","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":"2026-08-08T15:23:51.353866Z","title":"Ultralocal quantum field theory,","venue":null,"work_id":null,"year":1971},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.353866Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:68b2b6fcc214d49084ab096fadae79f0c7546ac934d933f8982a7cc426c38de2","observation_id":"10f19a73-1292-4ab9-a0ae-bfb9f2968cd8","resolution":{"observed_at":"2026-08-08T15:23:51.353866Z","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":"2026-08-08T15:23:51.357351Z","title":null,"venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.357351Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:3c9f9920a677b14ce553d4eec71165bc0a73a5773bbe1d275e0a5de30a6f7bf6","observation_id":"9f2ba934-bbb6-4b69-ae64-c30b98e86781","resolution":{"observed_at":"2026-08-08T15:23:51.357351Z","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":"2026-08-08T15:23:51.360542Z","title":"Ultralocal spinor field models,","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.360542Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:eeb091df87e025cffe826abbfe4c86ea423fc0455b25ef7878eaf1313f7e7e97","observation_id":"f79d21a8-e615-435f-92b5-c847f4e1d0bc","resolution":{"observed_at":"2026-08-08T15:23:51.360542Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1407.4275","last_updated":"2014-07-16T12:20:24Z","snapshot_observed_at":"2026-08-19T15:11:22.131106Z","submitted_at":"2014-07-16T12:20:24Z","title":"Asymptotic symmetries and dynamics of three-dimensional flat supergravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1407.4275","snapshot_observed_at":"2026-08-08T15:23:51.363682Z","title":"Asymptotic symmetries and dynamics of three-dimensional flat supergravity,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.363682Z"},"links":{"cited_paper":"/paper/1407.4275","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:59ff11a3b0a198a52c8aec80bd55af3bce81255529371a499c4c173690cb9992","observation_id":"4e2f3ecd-9ff0-4021-a0b5-3fabba9b7b7b","resolution":{"observed_at":"2026-08-08T15:23:51.363682Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.06064","last_updated":"2015-12-18T18:02:58Z","snapshot_observed_at":"2026-08-16T06:31:46.314299Z","submitted_at":"2015-12-18T18:02:58Z","title":"Non-relativistic fields from arbitrary contracting backgrounds","version":1},"cited_work":{"arxiv_id":"1512.06064","doi":null,"metadata_source":"pith","pith_arxiv_id":"1512.06064","snapshot_observed_at":"2026-08-08T15:23:52.505380Z","title":"Non-relativistic fields from arbitrary contracting backgrounds","venue":"hep-th","work_id":"a459795b-3b17-4061-a483-5b56068d8215","year":2015},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.367077Z"},"links":{"cited_paper":"/paper/1512.06064","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:5194bbca4422b32ea1425f13b4df52f87db692a515ea367ccbb70b01cdad06cf","observation_id":"3dc94e20-6b9e-4dfa-ac0d-8a07396c9dc4","resolution":{"observed_at":"2026-08-08T15:23:52.509271Z","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":"1609.06203","last_updated":"2016-09-20T14:37:38Z","snapshot_observed_at":"2026-08-14T21:39:00.708701Z","submitted_at":"2016-09-20T14:37:38Z","title":"Flat Holography: Aspects of the dual field theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1609.06203","snapshot_observed_at":"2026-08-08T15:23:51.370163Z","title":"Flat Holography: Aspects of the dual field theory,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.370163Z"},"links":{"cited_paper":"/paper/1609.06203","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:bc233adf3a775d8eb07952b14cc16e6609d4f3c5d82ed907022e8613911bc40e","observation_id":"ec1d1d7f-7b82-4e29-8a03-601c6ba7c587","resolution":{"observed_at":"2026-08-08T15:23:51.370163Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1701.06156","last_updated":"2017-02-16T21:21:48Z","snapshot_observed_at":"2026-08-14T21:20:06.801173Z","submitted_at":"2017-01-22T11:30:48Z","title":"Carroll versus Galilei Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1701.06156","snapshot_observed_at":"2026-08-08T15:23:51.373578Z","title":"Carroll versus Galilei Gravity,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.373578Z"},"links":{"cited_paper":"/paper/1701.06156","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:f1f59d17ee63cca77170e631b68b8092dd6718a993f73adc2386da4054a923e3","observation_id":"a6cd32c9-24a8-4e0a-bbd9-045b4d33642e","resolution":{"observed_at":"2026-08-08T15:23:51.373578Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.10277","last_updated":"2020-04-03T16:10:19Z","snapshot_observed_at":"2026-08-16T01:35:57.243238Z","submitted_at":"2020-01-28T11:47:30Z","title":"Non-Relativistic Gravity and its Coupling to Matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.10277","snapshot_observed_at":"2026-08-08T15:23:51.377220Z","title":"Non-Relativistic Gravity and its Coupling to Matter,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.377220Z"},"links":{"cited_paper":"/paper/2001.10277","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:4087a4df3d66851151bfbecfcc9cf19d37e4a09a6ff2b8965229a6ff9623d424","observation_id":"b60ed4f5-21c1-4f7a-a329-4a161652dccc","resolution":{"observed_at":"2026-08-08T15:23:51.377220Z","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":"2026-08-08T15:23:51.380541Z","title":"Galilean subdynamics and the dual resonance model,","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.380541Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:c3602d61dc972dfd4806b9699a3aa5dc03da8a99833048aea624cf743a15f872","observation_id":"0e77e0c0-cc1f-4eb8-a407-4df14b52c10c","resolution":{"observed_at":"2026-08-08T15:23:51.380541Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2301.06011","last_updated":"2023-09-08T15:31:07Z","snapshot_observed_at":"2026-08-20T04:26:59.827373Z","submitted_at":"2023-01-15T03:29:43Z","title":"Constructing Carrollian Field Theories from Null Reduction","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2301.06011","snapshot_observed_at":"2026-08-08T15:23:51.383929Z","title":"Constructing Carrollian field theories from null reduction,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.383929Z"},"links":{"cited_paper":"/paper/2301.06011","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:6f0ba815dd2a5c5e1c6cc7b37b35db104ab42fd546db42d31d933a8f51c64c45","observation_id":"aa69d985-4fc8-44fc-9ecf-55d2465f70ed","resolution":{"observed_at":"2026-08-08T15:23:51.383929Z","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":"2026-08-08T15:23:51.388026Z","title":"Galilean covariant Lagrangian models,","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.388026Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:70508cbe10598f79ee3810a1c483e5c241c53bcf130e97758c6a1011fabba65d","observation_id":"bbac3d31-0d6c-48c1-9e48-2a38e16472b0","resolution":{"observed_at":"2026-08-08T15:23:51.388026Z","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":"2026-08-08T15:23:51.391935Z","title":"Carroll theories from Lorentzian light-cone theories,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.391935Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:92a40f6e64ece1adf9b06eb67d70a31b2a25675b6eca320716ee9d4c72641707","observation_id":"115bbc44-23d3-426c-9a14-3613afa294ad","resolution":{"observed_at":"2026-08-08T15:23:51.391935Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2605.05334","last_updated":"2026-05-06T18:06:01Z","snapshot_observed_at":"2026-08-17T22:20:25.977563Z","submitted_at":"2026-05-06T18:06:01Z","title":"Carroll fermions from null reduction: A case of good and bad fermions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2605.05334","snapshot_observed_at":"2026-08-08T15:23:51.395954Z","title":"Carroll fermions from null reduction: A case of good and bad fermions,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.395954Z"},"links":{"cited_paper":"/paper/2605.05334","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:5bf30b99ad2fa1a7443dd94787f834dd63f2f5a04bfbbef56e8cf5c45555b98d","observation_id":"053f2048-7f53-4320-a79f-33e44da83792","resolution":{"observed_at":"2026-08-08T15:23:51.395954Z","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":"2026-08-08T15:23:51.400202Z","title":"Studies on Carrollian quantum field theories,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.400202Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:b7c9a92100dc40eedcac1e609ab5cbeae54ac6e52e5a997e5700d5c00e04541c","observation_id":"7ec378c2-c0d5-4c2b-8f7e-4ec780ed25ec","resolution":{"observed_at":"2026-08-08T15:23:51.400202Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2205.01918","last_updated":"2022-08-06T11:08:33Z","snapshot_observed_at":"2026-08-16T17:02:43.965018Z","submitted_at":"2022-05-04T07:06:03Z","title":"Quantization of Interacting Galilean Field theories","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2205.01918","snapshot_observed_at":"2026-08-08T15:23:51.403481Z","title":"Quantization of interacting Galilean field theories,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.403481Z"},"links":{"cited_paper":"/paper/2205.01918","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:0e36c82ba0e397f357a481ed4af8cc34ad782ef730534125f5ad43a1c9f0878c","observation_id":"bbe195e3-a4ac-440d-981a-0ca619d2667f","resolution":{"observed_at":"2026-08-08T15:23:51.403481Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2301.04538","last_updated":"2023-06-10T09:43:32Z","snapshot_observed_at":"2026-08-16T16:03:05.260568Z","submitted_at":"2023-01-11T16:02:10Z","title":"Galilean fermions: Classical and quantum aspects","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2301.04538","snapshot_observed_at":"2026-08-08T15:23:51.406789Z","title":"Galilean fermions: Classical and quantum aspects,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.406789Z"},"links":{"cited_paper":"/paper/2301.04538","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:801791cbea0a0fa32f5a6701dda2d8eda6af13825449fb7350c777308b6b0401","observation_id":"c4cef105-6357-46b6-899b-7e00d1cbe4c8","resolution":{"observed_at":"2026-08-08T15:23:51.406789Z","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":"2026-08-08T15:23:51.410187Z","title":"Null reduction and dynamical realization of Carrollian conformal symmetries,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.410187Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:6dd806fe7bf024f6ecd7dcae28971a9e29ca1681209ab4e0e8369d1bb8761451","observation_id":"3b73b391-9cc8-4db6-a332-b58a87f27c39","resolution":{"observed_at":"2026-08-08T15:23:51.410187Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2008.02829","last_updated":"2021-05-07T16:16:11Z","snapshot_observed_at":"2026-08-16T06:23:38.846790Z","submitted_at":"2020-08-06T18:26:52Z","title":"Interacting Conformal Carrollian Theories: Cues from Electrodynamics","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2008.02829","snapshot_observed_at":"2026-08-08T15:23:51.413555Z","title":"Interacting Conformal Carrollian Theories: Cues from Electrodynamics,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.413555Z"},"links":{"cited_paper":"/paper/2008.02829","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:621e090bf495505c649eac00489a5fe5b401d707688d2845a95ca6e8227f4492","observation_id":"e57c15a5-6043-4930-a54a-f8abd1a31dd2","resolution":{"observed_at":"2026-08-08T15:23:51.413555Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.03033","last_updated":"2021-03-15T20:46:55Z","snapshot_observed_at":"2026-08-18T18:45:13.701603Z","submitted_at":"2020-07-06T19:32:34Z","title":"Renormalization of Galilean Electrodynamics","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.03033","snapshot_observed_at":"2026-08-08T15:23:51.417592Z","title":"Renormalization of Galilean Electrodynamics,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.417592Z"},"links":{"cited_paper":"/paper/2007.03033","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:2563270130480bce9b5e29588780da41d0a323594d4cd5521700c2aa9bc51480","observation_id":"1a105cb2-b2cd-4760-89eb-4b1b1c133932","resolution":{"observed_at":"2026-08-08T15:23:51.417592Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2110.02319","last_updated":"2021-10-05T19:33:42Z","snapshot_observed_at":"2026-08-20T22:41:38.539117Z","submitted_at":"2021-10-05T19:33:42Z","title":"Carroll symmetry, dark energy and inflation","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2110.02319","snapshot_observed_at":"2026-08-08T15:23:51.421634Z","title":"Carroll Symmetry, Dark Energy and Inflation,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.421634Z"},"links":{"cited_paper":"/paper/2110.02319","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:19b8ba199291b77b2f4b033e1cce518ce264c6bd27b919123450e31cadd0704e","observation_id":"aa9a2e0f-c2f9-4b6e-b7dc-3b85e7523c5f","resolution":{"observed_at":"2026-08-08T15:23:51.421634Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.01647","last_updated":"2022-10-11T15:44:41Z","snapshot_observed_at":"2026-08-16T16:48:25.168944Z","submitted_at":"2022-07-04T18:00:37Z","title":"Revisiting the Carrollian Scalar Field","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.01647","snapshot_observed_at":"2026-08-08T15:23:51.425714Z","title":"Revisiting the Carrollian scalar field,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.425714Z"},"links":{"cited_paper":"/paper/2207.01647","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:02a437609e1af38fc0bace6ff2cba113ddc7a80f35fc1ad8fd1864af3fe2a3e2","observation_id":"1234d9fe-50f8-4c71-8de1-5cc23ecff40d","resolution":{"observed_at":"2026-08-08T15:23:51.425714Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2112.12684","last_updated":"2022-09-08T13:11:11Z","snapshot_observed_at":"2026-08-20T19:11:28.887915Z","submitted_at":"2021-12-23T16:26:16Z","title":"Carroll Expansion of General Relativity","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.12684","snapshot_observed_at":"2026-08-08T15:23:51.429556Z","title":"Carroll Expansion of General Relativity,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.429556Z"},"links":{"cited_paper":"/paper/2112.12684","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:599e203f35a3780f86b8f0c56572b8289b0e9b83d5232f8446e09f51ab809583","observation_id":"46edf678-9d72-47ed-a018-3323e346b5fe","resolution":{"observed_at":"2026-08-08T15:23:51.429556Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1905.13723","last_updated":"2020-01-29T09:20:38Z","snapshot_observed_at":"2026-08-14T19:28:01.463423Z","submitted_at":"2019-05-31T17:07:40Z","title":"Non-relativistic expansion of the Einstein-Hilbert Lagrangian","version":2},"cited_work":{"arxiv_id":"1905.13723","doi":null,"metadata_source":"pith","pith_arxiv_id":"1905.13723","snapshot_observed_at":"2026-08-08T15:23:52.186781Z","title":"Non-relativistic expansion of the Einstein-Hilbert Lagrangian","venue":"gr-qc","work_id":"cc8f4828-5b44-4d6b-be1a-662f5e22f318","year":2019},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.433903Z"},"links":{"cited_paper":"/paper/1905.13723","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:020575112bb1dde3f2cdcad7b959d9cddad476e4ef724d99e270c50d429e4dd4","observation_id":"8cf1f300-be8f-4276-aac1-8530c7705032","resolution":{"observed_at":"2026-08-08T15:23:52.190432Z","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":"2307.06367","last_updated":"2023-07-17T07:17:32Z","snapshot_observed_at":"2026-08-16T15:16:43.341152Z","submitted_at":"2023-07-12T18:00:03Z","title":"BMS$_{3}$ (Carrollian) field theories from a bound in the coupling of current-current deformations of CFT$_{2}$","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2307.06367","snapshot_observed_at":"2026-08-08T15:23:51.437761Z","title":"BMS 3 (Carrollian) field theories from a bound in the coupling of current-current deformations of CFT 2,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.437761Z"},"links":{"cited_paper":"/paper/2307.06367","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:e0309cfe4dab5a8f43db4711ba128296434d8446d439ca5075236383089e410a","observation_id":"ce3e4cd7-7d69-45eb-aa8d-f023f4e8b3a0","resolution":{"observed_at":"2026-08-08T15:23:51.437761Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2310.15245","last_updated":"2023-10-23T18:01:05Z","snapshot_observed_at":"2026-08-19T18:41:32.857719Z","submitted_at":"2023-10-23T18:01:05Z","title":"Non-Lorentzian expansions of the Lorentz force and kinematical algebras","version":1},"cited_work":{"arxiv_id":"2310.15245","doi":null,"metadata_source":"pith","pith_arxiv_id":"2310.15245","snapshot_observed_at":"2026-08-08T15:23:52.165446Z","title":"Non-Lorentzian expansions of the Lorentz force and kinematical algebras","venue":"hep-th","work_id":"ef1702f1-f859-4c53-9f15-4a899ca8b75b","year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.441485Z"},"links":{"cited_paper":"/paper/2310.15245","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:fe354697bcb4d118aa749e56f6d6a9b3e2bd2641fea32bc6d70b75014a4429ce","observation_id":"166caf6c-ecf4-41ae-a495-c37455655872","resolution":{"observed_at":"2026-08-08T15:23:52.168900Z","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":"2302.13257","last_updated":"2023-09-01T05:15:38Z","snapshot_observed_at":"2026-08-16T15:52:40.830907Z","submitted_at":"2023-02-26T08:07:11Z","title":"Towards Carrollian quantization: renormalization of Carrollian electrodynamics","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2302.13257","snapshot_observed_at":"2026-08-08T15:23:51.445638Z","title":"Toward Carrollian quantization: Renormalization of Carrollian electrodynamics,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.445638Z"},"links":{"cited_paper":"/paper/2302.13257","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:670687e2a3f8c4dad07d1b8654d109944b09b9e98d073ab70c499a763d4e10df","observation_id":"85f0f01c-d9aa-43cf-8126-583afadd8335","resolution":{"observed_at":"2026-08-08T15:23:51.445638Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2503.18818","last_updated":"2025-06-23T19:54:22Z","snapshot_observed_at":"2026-08-20T23:11:37.471488Z","submitted_at":"2025-03-24T16:00:36Z","title":"AdS$_3$ Carroll gravity: asymptotic symmetries and C-thermal configurations","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2503.18818","snapshot_observed_at":"2026-08-08T15:23:51.449280Z","title":"AdS3 Carroll gravity: asymptotic symmetries and C-thermal configurations,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.449280Z"},"links":{"cited_paper":"/paper/2503.18818","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:fa0c13e6dad71eed45ee04958a3bdf3e292c8b508051875514c4da130e2bb452","observation_id":"63be3225-babf-441b-800a-985257bb10ea","resolution":{"observed_at":"2026-08-08T15:23:51.449280Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2607.21124","last_updated":"2026-07-23T09:57:51Z","snapshot_observed_at":"2026-08-09T22:22:28.433885Z","submitted_at":"2026-07-23T09:57:51Z","title":"Carroll fermions of arbitrary spin","version":1},"cited_work":{"arxiv_id":"2607.21124","doi":null,"metadata_source":"pith","pith_arxiv_id":"2607.21124","snapshot_observed_at":"2026-08-08T15:23:52.135827Z","title":"Carroll fermions of arbitrary spin","venue":"hep-th","work_id":"ce035de4-6e37-4fa4-a184-16fa30bf6fe4","year":2026},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.452810Z"},"links":{"cited_paper":"/paper/2607.21124","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:6bb80bfde23ba89ebc28d9ff83299a299f791687c6a412b981b5970d3c7651cf","observation_id":"105f59c0-1390-4716-b66f-46c0e2ec0cf3","resolution":{"observed_at":"2026-08-08T15:23:52.139245Z","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":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:23:51.456579Z","title":"Galilean electromagnetism,","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.456579Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:2a290cdc98ff05d9d0d4a0da2882a3d6ccd48dc1c397f78a9eb224602e69dab4","observation_id":"6ab8ccbf-7dd9-4e35-86a1-336e953ef5cc","resolution":{"observed_at":"2026-08-08T15:23:51.456579Z","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":"2026-08-08T15:23:51.460317Z","title":"Forty years of galilean electromagnetism (1973–2013),","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.460317Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:6eb1544774ac4846b0f35cd4d1972db8ba179cc626e25d075f6ed2fa2563a348","observation_id":"95f82f97-f53f-476c-b141-b1efe92962eb","resolution":{"observed_at":"2026-08-08T15:23:51.460317Z","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":"2026-08-08T15:23:51.463275Z","title":"Gyromagnetic Ratio and Galilean Symmetries in the Light Cone Formulation. 1. Formulation Based on the Bargmann-Wigner Field Equations,","venue":null,"work_id":null,"year":1976},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.463275Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:04d86a0132e7a49cc4bc963fc53ba66eb5e810e991a3dddd5d97885609b4689f","observation_id":"73f5909d-05a4-476a-a50d-fb889b145955","resolution":{"observed_at":"2026-08-08T15:23:51.463275Z","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":"2026-08-08T15:23:51.466311Z","title":"Gyromagnetic Ratio and Galilean Symmetries in the Light Cone Formulation. 2. Galilean Invariant Equations for Several Spin Field Equations,","venue":null,"work_id":null,"year":1976},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.466311Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:a11ffe31fe09050ee3cbc833a01786a11ae8b4d9340a461695622e73ef407795","observation_id":"a7cdf981-a6c9-46ee-b42e-bc27d1d56d6b","resolution":{"observed_at":"2026-08-08T15:23:51.466311Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9412002","last_updated":"1994-12-01T13:11:14Z","snapshot_observed_at":"2026-07-07T05:07:03.317138Z","submitted_at":"1994-12-01T13:11:14Z","title":"Null Killing Vector Dimensional Reduction and Galilean Geometrodynamics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9412002","snapshot_observed_at":"2026-08-08T15:23:51.469407Z","title":"Null Killing vector dimensional reduction and Galilean geometrodynamics,","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.469407Z"},"links":{"cited_paper":"/paper/hep-th/9412002","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:4b48a9d1428b0aa7df3b430a9fccd5552466d1a385e0b1844fb57726d0d0f395","observation_id":"a8a544bf-0649-4d9d-b3ef-b157359b3228","resolution":{"observed_at":"2026-08-08T15:23:51.469407Z","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":"2026-08-08T15:23:51.472931Z","title":"Bargmann Structures and Newton-cartan Theory,","venue":null,"work_id":null,"year":1985},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.472931Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:510c4b973ed3c6f2a1593e3a0b09dfb7f8396f9704a205dc9f24c829e73ad060","observation_id":"a529332a-b41c-4b79-a184-41acc11e0ee3","resolution":{"observed_at":"2026-08-08T15:23:51.472931Z","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":"2026-08-08T15:23:51.476168Z","title":"THE DIRAC AND LEVY-LEBLOND EQUATIONS AND GEOMETRIC QUANTIZATION,","venue":null,"work_id":null,"year":1987},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.476168Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:bddf62363362cf844ca6665cf7476d580e795532c3474d83424c3fdf02c87688","observation_id":"e55385c2-a660-444f-9f6a-bd746adc436a","resolution":{"observed_at":"2026-08-08T15:23:51.476168Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2210.14848","last_updated":"2023-01-31T08:58:51Z","snapshot_observed_at":"2026-08-19T23:04:37.177212Z","submitted_at":"2022-10-26T16:48:49Z","title":"Non-Lorentzian theories with and without constraints","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2210.14848","snapshot_observed_at":"2026-08-08T15:23:51.479370Z","title":"Non-Lorentzian theories with and without constraints,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.479370Z"},"links":{"cited_paper":"/paper/2210.14848","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:e2f01ac6e92a2c81c611a34038d6a3226d5b618debe7c1cefbf7f52f40e57fd5","observation_id":"aded56a0-af64-4307-a8ec-cdb7856f06f9","resolution":{"observed_at":"2026-08-08T15:23:51.479370Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.16786","last_updated":"2023-12-23T19:54:02Z","snapshot_observed_at":"2026-08-18T05:16:17.406834Z","submitted_at":"2023-09-28T18:23:30Z","title":"Super-Carrollian and Super-Galilean Field Theories","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.16786","snapshot_observed_at":"2026-08-08T15:23:51.482519Z","title":"Super-Carrollian and Super-Galilean Field Theories,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.482519Z"},"links":{"cited_paper":"/paper/2309.16786","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:dab69071f81552c8ba4f74140a0472a484c00629e7ccba81dcbefdf69e730883","observation_id":"8a42a45f-ba33-4c67-8521-7960f382c89e","resolution":{"observed_at":"2026-08-08T15:23:51.482519Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.04113","last_updated":"2023-11-17T19:20:38Z","snapshot_observed_at":"2026-08-19T01:49:39.316202Z","submitted_at":"2023-11-07T16:33:24Z","title":"Dynamics of Carrollian Scalar Fields","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.04113","snapshot_observed_at":"2026-08-08T15:23:51.485778Z","title":"Dynamics of Carrollian scalar fields,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.485778Z"},"links":{"cited_paper":"/paper/2311.04113","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:32b99ad3260bbb964fbd640415ee4bb6a32dc56ec7d88261a27bbfd13381ed97","observation_id":"c18a6283-36d7-472e-9ec5-6ce0fe104058","resolution":{"observed_at":"2026-08-08T15:23:51.485778Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2001.03056","last_updated":"2020-01-09T15:19:05Z","snapshot_observed_at":"2026-08-13T23:47:30.215361Z","submitted_at":"2020-01-09T15:19:05Z","title":"Constructing Carrollian CFTs","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2001.03056","snapshot_observed_at":"2026-08-08T15:23:51.489075Z","title":"Constructing Carrollian CFTs,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.489075Z"},"links":{"cited_paper":"/paper/2001.03056","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:6f5729d19e54333c6f68b541ebe59c4ccc1bf9c5e75f39676081753fc4207c35","observation_id":"e88071a7-f994-4f08-a270-9c2bb3152201","resolution":{"observed_at":"2026-08-08T15:23:51.489075Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2203.13197","last_updated":"2023-01-14T13:11:09Z","snapshot_observed_at":"2026-08-19T01:49:37.695841Z","submitted_at":"2022-03-24T17:06:40Z","title":"Carroll covariant scalar fields in two dimensions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.13197","snapshot_observed_at":"2026-08-08T15:23:51.492430Z","title":"Carroll covariant scalar fields in two dimensions,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.492430Z"},"links":{"cited_paper":"/paper/2203.13197","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:87760bb430dd4a039e6139c667d69fad95b1c5f1b28f0891b84fcc478b78b0b4","observation_id":"c9278dc4-13e8-4ebf-95c1-4e3f292338c3","resolution":{"observed_at":"2026-08-08T15:23:51.492430Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.05890","last_updated":"2017-05-16T19:51:11Z","snapshot_observed_at":"2026-08-20T00:51:05.948230Z","submitted_at":"2017-05-16T19:51:11Z","title":"The nuts and bolts of the BMS Bootstrap","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.05890","snapshot_observed_at":"2026-08-08T15:23:51.495845Z","title":"The nuts and bolts of the BMS Bootstrap,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.495845Z"},"links":{"cited_paper":"/paper/1705.05890","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:30c8e91e4561cf79b28fdac5779adddd4190371602613c0b30cab3f457e795a2","observation_id":"76f7b3fe-c45e-4865-a296-56d9138888d0","resolution":{"observed_at":"2026-08-08T15:23:51.495845Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2011.11092","last_updated":"2021-05-02T21:56:46Z","snapshot_observed_at":"2026-08-16T19:04:06.647271Z","submitted_at":"2020-11-22T19:24:28Z","title":"On Galilean conformal bootstrap","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2011.11092","snapshot_observed_at":"2026-08-08T15:23:51.499312Z","title":"On Galilean conformal bootstrap,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.499312Z"},"links":{"cited_paper":"/paper/2011.11092","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:dfaeb21fccc7233992b9beeabffa62df5e8c02eb4508f1f5ed9be3cfd9afe467","observation_id":"c5718262-4998-4495-bd80-d9914c09d0d6","resolution":{"observed_at":"2026-08-08T15:23:51.499312Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.13574","last_updated":"2024-03-11T09:46:29Z","snapshot_observed_at":"2026-08-20T18:37:15.491364Z","submitted_at":"2023-12-21T04:43:33Z","title":"Bulk reconstruction in flat holography","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.13574","snapshot_observed_at":"2026-08-08T15:23:51.502765Z","title":"Bulk reconstruction in flat holography,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.502765Z"},"links":{"cited_paper":"/paper/2312.13574","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:463acfc1e240890aaaf49b2a959ce91df20706a40c95bc977de58eea5fd79ffe","observation_id":"641134dc-5458-4208-8338-50acc0583b1c","resolution":{"observed_at":"2026-08-08T15:23:51.502765Z","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":"2512.21733","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T15:23:52.043719Z","title":"Momentum Space Correlation Functions in 2D Galilean Conformal Algebra,","venue":null,"work_id":"2ed2b947-a41f-4670-a310-1bc873493d41","year":null},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.506243Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:87427921df4eb62304866724a7e57b8dc6bd6220f24ca17accdf69a53a344eb2","observation_id":"f74aea56-a62d-419a-913b-903899c4ffdd","resolution":{"observed_at":"2026-08-08T15:23:52.050313Z","resolver_source":"raw_fallback","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":"2207.01474","last_updated":"2022-07-04T15:08:51Z","snapshot_observed_at":"2026-08-19T19:41:33.335194Z","submitted_at":"2022-07-04T15:08:51Z","title":"On Galilean Conformal Bootstrap II: $\\xi=0$ sector","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.01474","snapshot_observed_at":"2026-08-08T15:23:51.509534Z","title":"On Galilean conformal bootstrap. Part II.ξ = 0 sector,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.509534Z"},"links":{"cited_paper":"/paper/2207.01474","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:38eb90bc78cab1bf93cb0e621b0bd2770d1128c5dd72675247d9912e3e6bb979","observation_id":"e3df63ed-91bb-4366-9834-03453bdea0df","resolution":{"observed_at":"2026-08-08T15:23:51.509534Z","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":"2026-08-08T15:23:51.512842Z","title":"Carrollian Conformal Theories in Momentum Space,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.512842Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:915a69f07916c7a84173da167df1436f2070295deff0beb4aeb95fa7f88a93f0","observation_id":"ff588d42-9ac0-4f41-b178-509ab082b446","resolution":{"observed_at":"2026-08-08T15:23:51.512842Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1011.1145","last_updated":"2011-05-25T13:30:07Z","snapshot_observed_at":"2026-08-15T05:03:55.313446Z","submitted_at":"2010-11-04T12:43:44Z","title":"Newtonian Gravity and the Bargmann Algebra","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1011.1145","snapshot_observed_at":"2026-08-08T15:23:51.516088Z","title":"Newtonian Gravity and the Bargmann Algebra,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.516088Z"},"links":{"cited_paper":"/paper/1011.1145","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:ca9a9a1660ed031b74e2b0feb99f5d9f02eac3a6b2eeca8c3f1407d713e7025b","observation_id":"c8b1c40a-91f4-41dc-a4c1-bb6f240d7c1b","resolution":{"observed_at":"2026-08-08T15:23:51.516088Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1305.6737","last_updated":"2013-06-19T16:39:49Z","snapshot_observed_at":"2026-08-15T00:16:14.855353Z","submitted_at":"2013-05-29T09:23:39Z","title":"Newton-Cartan Supergravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1305.6737","snapshot_observed_at":"2026-08-08T15:23:51.519380Z","title":"3D Newton–Cartan supergravity,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.519380Z"},"links":{"cited_paper":"/paper/1305.6737","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:cb8bfe56ed3dd54f523aa7e7eceebf7c97da95fb41aa95455499363709190e4e","observation_id":"aad228ee-d0a3-4c48-be5a-e1d7dcc7e6aa","resolution":{"observed_at":"2026-08-08T15:23:51.519380Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1409.5555","last_updated":"2014-10-27T17:27:57Z","snapshot_observed_at":"2026-08-14T23:18:53.241406Z","submitted_at":"2014-09-19T08:54:40Z","title":"Torsional Newton-Cartan Geometry and the Schr\\\"odinger Algebra","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1409.5555","snapshot_observed_at":"2026-08-08T15:23:51.522671Z","title":"Torsional Newton–Cartan geometry and the Schr¨ odinger algebra,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.522671Z"},"links":{"cited_paper":"/paper/1409.5555","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:5a43a647ba0b0060cf97a2a4e50a7e65e1587330f45dc55ab09644e1247ef12e","observation_id":"11b26515-496a-470e-b36b-6c8d3f496d69","resolution":{"observed_at":"2026-08-08T15:23:51.522671Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1504.07461","last_updated":"2015-04-28T13:20:57Z","snapshot_observed_at":"2026-08-20T05:57:33.880941Z","submitted_at":"2015-04-28T13:20:57Z","title":"Horava-Lifshitz Gravity From Dynamical Newton-Cartan Geometry","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1504.07461","snapshot_observed_at":"2026-08-08T15:23:51.526727Z","title":"Hoˇ rava-Lifshitz gravity from dynamical Newton-Cartan geometry,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.526727Z"},"links":{"cited_paper":"/paper/1504.07461","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:8199496f7db236c0e7bd4382253db351eef1797945b4e768a3ee77120612ecfc","observation_id":"0db84f5b-aae8-4776-8507-747d3436f5b5","resolution":{"observed_at":"2026-08-08T15:23:51.526727Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1512.06277","last_updated":"2015-12-19T19:14:45Z","snapshot_observed_at":"2026-08-19T11:20:56.435114Z","submitted_at":"2015-12-19T19:14:45Z","title":"A Schr\\\"odinger approach to Newton-Cartan and Ho\\v{r}ava-Lifshitz gravities","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1512.06277","snapshot_observed_at":"2026-08-08T15:23:51.530551Z","title":"A Schr¨ odinger approach to Newton-Cartan and Hoˇ rava-Lifshitz gravities,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.530551Z"},"links":{"cited_paper":"/paper/1512.06277","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:887499a2997f1d8429c1a44781dc910ffa1e1232c045926ac39984329e42e4d6","observation_id":"56ea7886-be2e-4f39-a647-4c166540ce10","resolution":{"observed_at":"2026-08-08T15:23:51.530551Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.02095","last_updated":"2015-09-28T15:05:49Z","snapshot_observed_at":"2026-08-14T22:49:18.988745Z","submitted_at":"2015-05-08T16:47:21Z","title":"Newton-Cartan (super)gravity as a non-relativistic limit","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.02095","snapshot_observed_at":"2026-08-08T15:23:51.533815Z","title":"Newton–Cartan (super)gravity as a non-relativistic limit,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.533815Z"},"links":{"cited_paper":"/paper/1505.02095","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:c3e36391ca124f30fe454c4ea5593642f84c5758fef63c793812903d131dc92d","observation_id":"0619512e-e98d-46d6-bfc6-6a4597134e07","resolution":{"observed_at":"2026-08-08T15:23:51.533815Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1904.08304","last_updated":"2019-05-15T21:54:45Z","snapshot_observed_at":"2026-08-19T08:09:16.024054Z","submitted_at":"2019-04-17T15:02:51Z","title":"Lie Algebra Expansions and Actions for Non-Relativistic Gravity","version":2},"cited_work":{"arxiv_id":"1904.08304","doi":null,"metadata_source":"pith","pith_arxiv_id":"1904.08304","snapshot_observed_at":"2026-08-08T15:23:51.815852Z","title":"Lie Algebra Expansions and Actions for Non-Relativistic Gravity","venue":"hep-th","work_id":"c66f8d59-8c34-48b8-b7b7-8d66d95e45e3","year":2019},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.537210Z"},"links":{"cited_paper":"/paper/1904.08304","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:7b056e4eee7518d9e4d4c16bfaa1d8bab837130322b39cc3f8197c12e09ee2ce","observation_id":"c1c10e75-b8de-458a-9cc1-6d3ee5fee799","resolution":{"observed_at":"2026-08-08T15:23:51.819707Z","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":"2206.12177","last_updated":"2023-05-06T09:03:45Z","snapshot_observed_at":"2026-08-20T17:41:43.326369Z","submitted_at":"2022-06-24T09:31:08Z","title":"A non-lorentzian primer","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2206.12177","snapshot_observed_at":"2026-08-08T15:23:51.540456Z","title":"A non-lorentzian primer,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.540456Z"},"links":{"cited_paper":"/paper/2206.12177","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:6b32dca522a7818ac0ed16de848f3c0a3217d773b80fa3cd470f9d6c5394f179","observation_id":"5322659e-ced6-497d-8ebc-33e1327f84ff","resolution":{"observed_at":"2026-08-08T15:23:51.540456Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2212.11309","last_updated":"2023-03-09T16:03:31Z","snapshot_observed_at":"2026-08-19T08:32:04.104351Z","submitted_at":"2022-12-21T19:08:24Z","title":"Review on Non-Relativistic Gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2212.11309","snapshot_observed_at":"2026-08-08T15:23:51.543671Z","title":"Review on Non-Relativistic Gravity,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.543671Z"},"links":{"cited_paper":"/paper/2212.11309","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:7d09333281b0ea599211a01861baa8f978e1838de9132d2f26c1461d9461fdf8","observation_id":"177159f9-6444-4d51-8bab-f6dbc15f73b2","resolution":{"observed_at":"2026-08-08T15:23:51.543671Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2207.14167","last_updated":"2022-07-28T15:27:51Z","snapshot_observed_at":"2026-08-16T16:42:40.364459Z","submitted_at":"2022-07-28T15:27:51Z","title":"Magnetic Carrollian gravity from the Carroll algebra","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2207.14167","snapshot_observed_at":"2026-08-08T15:23:51.547005Z","title":"Magnetic Carrollian gravity from the Carroll algebra,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.547005Z"},"links":{"cited_paper":"/paper/2207.14167","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:b2ee5099ec662dc3d8d0da4395078db1559f895b376546b932a572930d0531aa","observation_id":"70790f14-5627-464c-8ddf-ea60c555fcea","resolution":{"observed_at":"2026-08-08T15:23:51.547005Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1505.05011","last_updated":"2015-05-19T14:25:48Z","snapshot_observed_at":"2026-08-20T06:46:11.666627Z","submitted_at":"2015-05-19T14:25:48Z","title":"Gauging the Carroll Algebra and Ultra-Relativistic Gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1505.05011","snapshot_observed_at":"2026-08-08T15:23:51.550589Z","title":"Gauging the Carroll Algebra and Ultra-Relativistic Gravity,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.550589Z"},"links":{"cited_paper":"/paper/1505.05011","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:43d5346e841e9837a4c77806d9350616a1a1f5ef09e0ccee04faae9ea7ed30d6","observation_id":"cb8bf5cc-2c72-406c-b963-e5c4502afd8a","resolution":{"observed_at":"2026-08-08T15:23:51.550589Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1912.09388","last_updated":"2020-02-20T14:25:29Z","snapshot_observed_at":"2026-08-20T01:23:18.052376Z","submitted_at":"2019-12-19T17:06:02Z","title":"Field Theories on Null Manifolds","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1912.09388","snapshot_observed_at":"2026-08-08T15:23:51.554048Z","title":"Field Theories on Null Manifolds,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.554048Z"},"links":{"cited_paper":"/paper/1912.09388","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:eaddb942493a86a9d87e6f55a79e5a748450ac2be25fda52a56f1548e6140d06","observation_id":"914b3dde-a285-4d90-aa1b-1e502c70f1f2","resolution":{"observed_at":"2026-08-08T15:23:51.554048Z","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":"2026-08-08T15:23:51.557448Z","title":"Nonrelativistic particles and wave equations,","venue":null,"work_id":null,"year":1967},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.557448Z"},"links":{"citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:c92e50e937ce0ca41d80ca95d45528e37271e5045af3d3f1b7ffa2b75b14a22f","observation_id":"3d5c0b6b-8c63-4de7-a21a-b4080fae622a","resolution":{"observed_at":"2026-08-08T15:23:51.557448Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.00745","last_updated":"2024-06-14T08:32:03Z","snapshot_observed_at":"2026-08-18T20:48:02.850008Z","submitted_at":"2023-12-01T17:28:41Z","title":"Carroll Fermions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.00745","snapshot_observed_at":"2026-08-08T15:23:51.561340Z","title":"Carroll fermions,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.561340Z"},"links":{"cited_paper":"/paper/2312.00745","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:5613f3404e1cf1fdc765d25dc686c72a67357c51901d2d30db59cb1921588bd9","observation_id":"5cc72a42-7fac-4460-a1d0-5313a6223284","resolution":{"observed_at":"2026-08-08T15:23:51.561340Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.05645","last_updated":"2025-05-24T11:44:03Z","snapshot_observed_at":"2026-08-15T21:55:45.929092Z","submitted_at":"2025-02-08T17:18:50Z","title":"Quantization of Carrollian fermions","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2502.05645","snapshot_observed_at":"2026-08-08T15:23:51.565213Z","title":"Quantization of Carrollian fermions,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.565213Z"},"links":{"cited_paper":"/paper/2502.05645","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:032d94798656a40b0ca3675447a9fdbd300cdddc5db2c2cc1f6ae63a08a3108f","observation_id":"14355465-c736-4f1e-a004-a2827825e5e2","resolution":{"observed_at":"2026-08-08T15:23:51.565213Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2506.16164","last_updated":"2026-04-29T17:56:22Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-06-19T09:33:44Z","title":"The Carrollian Kaleidoscope","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2506.16164","snapshot_observed_at":"2026-08-08T15:23:51.568654Z","title":"The Carrollian kaleidoscope,","venue":null,"work_id":null,"year":2026},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":99,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.568654Z"},"links":{"cited_paper":"/paper/2506.16164","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:238be91ad883f65127507cf24964e7932761be1b6ff6e11ce59535532739b3ef","observation_id":"dfe17341-a446-42bf-bf2c-f3bc8aff3137","resolution":{"observed_at":"2026-08-08T15:23:51.568654Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2604.14301","last_updated":"2026-04-15T18:00:45Z","snapshot_observed_at":"2026-08-19T16:56:00.530833Z","submitted_at":"2026-04-15T18:00:45Z","title":"Carroll fermions, expansions and the lightcone","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2604.14301","snapshot_observed_at":"2026-08-08T15:23:51.572310Z","title":"Carroll fermions, expansions and the lightcone,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions","version":1},"reference_index":100,"source":"pdf_text","source_observed_at":"2026-08-08T15:23:51.572310Z"},"links":{"cited_paper":"/paper/2604.14301","citing_paper":"/paper/2608.05324"},"observation_digest":"sha256:5222da20b10ec43b6d9e3d39c6c947e193c67a59129f48e2d7bce9438f359da5","observation_id":"32b9fe23-fa45-4a2a-b8e4-b914c286ac04","resolution":{"observed_at":"2026-08-08T15:23:51.572310Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2608.05324","last_updated":"2026-08-05T18:28:55Z","latest_version":1,"primary_category":"hep-th","snapshot_observed_at":"2026-08-16T10:24:51.055449Z","submitted_at":"2026-08-05T18:28:55Z","title":"Interacting Galilean and Finite-Energy Carroll Fermions"},"reference_resolution":{"displayed":100,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":93,"verified_exact":7,"verified_fuzzy":0},"total_outbound_references":112},"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 22 August 2026, this Paper Citation Record lists 100 of 112 outbound references and 0 inbound Pith citation observations for arXiv:2608.05324."}