{"as_of":"2026-08-13T18:34:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:d923857ba258358f2f9721816be3ef17d4d78f52c6b34c70fd5a4810b917ff25","coverage":[{"denominator":50,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":50,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-11T10:43:30.727966Z","state":"measured"},{"denominator":53,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":53,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-13T06:32:02.005865+00:00","state":"measured"},{"denominator":3,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":3,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-02T06:16:06.313415Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-05-11T07:10:56.999170Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"cited_work":{"arxiv_id":"2412.16548","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2412.16548","snapshot_observed_at":"2026-06-05T21:23:00.469572Z","title":"Conformal geometry as a gauge theory of gravity: Covariant equations of motion & conservation laws","venue":null,"work_id":"e5699fe8-5bc5-4166-a316-57771ba397e7","year":2025},"citing_paper":{"arxiv_id":"2604.07508","last_updated":"2026-06-19T10:35:03Z","snapshot_observed_at":"2026-08-08T13:25:13.769753Z","submitted_at":"2026-04-08T18:47:05Z","title":"The fall and the rise of Weyl gauge theory","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-05-10T17:17:13.410170Z"},"links":{"cited_paper":"/paper/2412.16548","citing_paper":"/paper/2604.07508"},"observation_digest":"sha256:5464bbe649cd26fdc043ef5233ceec06419d6a4950d5cfcc0db059206dcd2e59","observation_id":"f19921bf-f538-4d01-820a-ce2e820e201f","resolution":{"observed_at":"2026-05-11T07:10:57.007912Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.16548","snapshot_observed_at":"2026-07-13T08:28:23.611896Z","title":"Conformal geometry as a gauge theory of gravity: Covariant equations of motion & conservation laws,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2604.07508","last_updated":"2026-06-19T10:35:03Z","snapshot_observed_at":"2026-08-08T13:25:13.769753Z","submitted_at":"2026-04-08T18:47:05Z","title":"The fall and the rise of Weyl gauge theory","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-07-13T08:28:23.611896Z"},"links":{"cited_paper":"/paper/2412.16548","citing_paper":"/paper/2604.07508"},"observation_digest":"sha256:6e6c67d4cdf5e9d0d3e48497bd08ed9e2104f79a11230b156d0f62ff1aad7da6","observation_id":"f53773e2-5d38-4fda-9893-08ab13f5e160","resolution":{"observed_at":"2026-07-13T08:28:23.611896Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2412.16548","snapshot_observed_at":"2026-08-02T06:16:06.313415Z","title":"Condeescu, D","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2607.13146","last_updated":"2026-08-11T18:03:05Z","snapshot_observed_at":"2026-08-13T17:31:15.098670Z","submitted_at":"2026-07-14T18:00:36Z","title":"Weyl gauge symmetry at LIGO-Virgo-KAGRA","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-02T06:16:06.313415Z"},"links":{"cited_paper":"/paper/2412.16548","citing_paper":"/paper/2607.13146"},"observation_digest":"sha256:437931c368b20cb7563983d3447d39f3b8f12bd0840e46b3cc71bce82e82590a","observation_id":"884262ef-1d9c-4b01-a24b-2e179d54e671","resolution":{"observed_at":"2026-08-02T06:16:06.313415Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2412.16548/citation-record","integrity":"/paper/2412.16548/integrity","json":"/paper/2412.16548/citation-record.json","paper":"/paper/2412.16548"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:32.096881Z","title":"(An English version by D","venue":null,"work_id":"360872f7-95cb-48f9-bc6f-932360574c03","year":1918},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.128208Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:7ab02a4228cf5a28ff9bbc36dd2a49a2ad65a47fc97cadbb866b4727da68290e","observation_id":"fcc17e8c-8c47-435e-a72a-d38ffcbbe35d","resolution":{"observed_at":"2026-08-11T10:43:32.101824Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:32.081648Z","title":"Eine neue Erweiterung der Relativit¨ atst heorie","venue":null,"work_id":"6f51896e-be75-4a63-9254-aa6585071717","year":1919},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.192213Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:170dc577f871564fb7bb283f3d0ecfa85e7165c9ddf1fea0871d42233a24148e","observation_id":"18fb4c4f-c8f7-4e91-a1f4-dc6d44418f07","resolution":{"observed_at":"2026-08-11T10:43:32.087208Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:32.043626Z","title":"Raum, Zeit, Materie","venue":null,"work_id":"4a904c17-5fc1-41d9-b63e-b025e3ff22f7","year":1921},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.267986Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:00b0c240b95c333ef9357f55ae9b1239fb8a4cb28062fc14dac8f48a1b5fbcc2","observation_id":"187cbad1-27a2-4eb6-8991-7214dc69e0c3","resolution":{"observed_at":"2026-08-11T10:43:32.049277Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07160","last_updated":"2025-06-04T00:59:20Z","snapshot_observed_at":"2026-08-12T23:04:04.167760Z","submitted_at":"2024-08-13T18:56:11Z","title":"Quantum gravity from Weyl conformal geometry","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07160","snapshot_observed_at":"2026-08-11T10:43:29.314552Z","title":"Quantum gravity from Weyl conformal ge ometry,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.314552Z"},"links":{"cited_paper":"/paper/2408.07160","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:6b1d4f1d8267c79595bd4a33cfc513c1fab0bb1aebe2579175785d54a5ddfe9c","observation_id":"db1a0d56-a51c-45a5-ab68-0ae9fa5bc23b","resolution":{"observed_at":"2026-08-11T10:43:29.314552Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"physics/0503066","last_updated":"2018-05-30T22:09:09Z","snapshot_observed_at":"2026-08-10T08:37:24.625490Z","submitted_at":"2005-03-08T22:21:40Z","title":"Invariant Variation Problems","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"physics/0503066","snapshot_observed_at":"2026-08-11T10:43:29.324329Z","title":"Invariant Variation Problems,","venue":null,"work_id":null,"year":1918},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.324329Z"},"links":{"cited_paper":"/paper/physics/0503066","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:3ce93204d2de457b01d25f2a95de721dc8767ea48ce80c47845a1c8341e95a82","observation_id":"1ac322ea-94af-45af-8aa5-556ac9601696","resolution":{"observed_at":"2026-08-11T10:43:29.324329Z","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":"2026-08-11T10:43:29.329083Z","title":"Invariant theoretical interpretation of i nteraction,","venue":null,"work_id":null,"year":1956},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.329083Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:a600cd65eb4e39f04f4bdba466e3c5f0bb1f9668296ed5a99433789737370c3b","observation_id":"c0036690-81cd-4969-89f0-f6942247576e","resolution":{"observed_at":"2026-08-11T10:43:29.329083Z","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":"2026-08-11T10:43:29.333562Z","title":"Lorentz invariance and the gravitation al field,","venue":null,"work_id":null,"year":1961},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.333562Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:9301dda9b904cc38cda822cf87afec663538ba3b12dc888784220c1f2e88e44d","observation_id":"96d8f9a5-3041-456b-9857-1edf2bcba918","resolution":{"observed_at":"2026-08-11T10:43:29.333562Z","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":"10.1143/ptp.49.667","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:30.882672Z","title":"Weyl transformations and poincare gauge in variance,","venue":null,"work_id":"c15e812d-5b8a-4516-bdad-6f99daf9f6f8","year":1973},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.400420Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:6511743c233548909e6b42945d256206a776231dd3a42c5f5dc2049217022824","observation_id":"8c4a9390-ec1c-403e-8c58-084671a04863","resolution":{"observed_at":"2026-08-11T10:43:30.888885Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+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":"2026-08-11T10:43:29.505546Z","title":"A gauge theory of the Weyl group,","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.505546Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:e41e366c04db7f5308675bc165a1af2301e20cf4cceb884f3347d12b2daecbbf","observation_id":"7e71a6a0-fb0f-481c-82a6-ffa1f301b39a","resolution":{"observed_at":"2026-08-11T10:43:29.505546Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.07159","last_updated":"2025-02-24T09:29:53Z","snapshot_observed_at":"2026-08-12T23:04:04.077000Z","submitted_at":"2024-08-13T18:55:55Z","title":"The Gauge Theory of Weyl Group and its Interpretation as Weyl Quadratic Gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.07159","snapshot_observed_at":"2026-08-11T10:43:29.624582Z","title":"The Gauge Theory of Weyl Group and its Interpretation as Weyl Quadratic Gravity,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.624582Z"},"links":{"cited_paper":"/paper/2408.07159","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:0b29f6886314106cdc7d41c3598f30a9668782384f67ab553025c535b3c68a02","observation_id":"8ffdec96-d4b6-408d-8f86-4d9391c3d2ed","resolution":{"observed_at":"2026-08-11T10:43:29.624582Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:32.024547Z","title":"Supergravity,","venue":null,"work_id":"41781693-39e2-43fa-bb2a-825ffdb4c5a2","year":2012},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.665344Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:836f29a2c5a1fc104c929aa69749c4052fa03edf95d2205d78d5d3ff73ae472b","observation_id":"0b225697-1547-41ee-9135-cad1a630c208","resolution":{"observed_at":"2026-08-11T10:43:32.030786Z","resolver_source":"raw_fallback","status":"malformed_identifier"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+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":"2026-08-11T10:43:29.686376Z","title":"Exact Vacuum Solution to Conformal Weyl Gravity and Galactic Rotation Curves,","venue":null,"work_id":null,"year":1989},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.686376Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:853da993a2edf2f54ef02c5232114636b648793a8b324f7eed068d1c196c2f46","observation_id":"ce75116c-833d-476e-9605-25988fa65e02","resolution":{"observed_at":"2026-08-11T10:43:29.686376Z","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":"2026-08-11T10:43:29.711328Z","title":"Gauge Theory of the Confor- mal and Superconformal Group,","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.711328Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:39d331a0d149c17550f240bde0de1248e501d40586f5403dd030c4685e582edf","observation_id":"9b51663c-28a1-4642-b906-6ac9cabd853f","resolution":{"observed_at":"2026-08-11T10:43:29.711328Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1703.03187","last_updated":"2017-03-09T09:17:47Z","snapshot_observed_at":"2026-08-09T05:52:16.890338Z","submitted_at":"2017-03-09T09:17:47Z","title":"The unexpected resurgence of Weyl geometry in late 20-th century physics","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1703.03187","snapshot_observed_at":"2026-08-11T10:43:29.728325Z","title":"The unexpected resurgence of Weyl geometry in the late 20-th cen- tury physics,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.728325Z"},"links":{"cited_paper":"/paper/1703.03187","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:9b87f0b067d253bbf6f688057e1d3e87c289c8baf61bb0667b7668b3cf83c59e","observation_id":"8b9f796e-56df-4dcf-a86d-b376bba88f6a","resolution":{"observed_at":"2026-08-11T10:43:29.728325Z","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":"2026-08-11T10:43:29.732312Z","title":"Long range forces and broken symmetries ,","venue":null,"work_id":null,"year":1973},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.732312Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:660ae2ef6fc3a0cb3e726977772b515c979faa79ce613a7d850f4b482d33675a","observation_id":"67af2797-8ba7-4f7f-b48d-5d0478a68fe6","resolution":{"observed_at":"2026-08-11T10:43:29.732312Z","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":"10.1016/0550-3213(79)90059-2","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:30.851101Z","title":"Towards a Theory of Space-Time Structure at Very Short Distances,","venue":null,"work_id":"0c7f8945-240f-4c3d-a4f7-561dedbf598f","year":1979},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.735850Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:b0f8882f4ddb8b9cfb32ab837c0123bf1b0de8c07eafb0a9dde9dbad98b92fbe","observation_id":"337b2a2c-8637-4b62-ae6f-6251bc2831ce","resolution":{"observed_at":"2026-08-11T10:43:30.856501Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1812.08613","last_updated":"2019-03-04T15:23:14Z","snapshot_observed_at":"2026-08-09T16:13:54.261785Z","submitted_at":"2018-12-20T14:45:39Z","title":"Spontaneous breaking of Weyl quadratic gravity to Einstein action and Higgs potential","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.08613","snapshot_observed_at":"2026-08-11T10:43:29.740082Z","title":"Spontaneous breaking of Weyl quadrat ic gravity to Einstein action and Higgs potential,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.740082Z"},"links":{"cited_paper":"/paper/1812.08613","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:9c52d98118c02e2036954af882223a8959ff9f221eafbf99190276e44fbd4a6c","observation_id":"11974a55-8809-4899-b1d6-ecdd3a161740","resolution":{"observed_at":"2026-08-11T10:43:29.740082Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:32.006440Z","title":"Interaction forces in electrod ynamics and in the field theory of nuclear forces,","venue":null,"work_id":"4277d205-77b4-471f-858a-f655b03bfc39","year":1938},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.744905Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:f3dd1411558b0d3ae0d7ce3851d2ecfa6e0a34cd62d62622cee7edd3823fa3a7","observation_id":"7a183ca5-8b67-4247-8715-16734517f405","resolution":{"observed_at":"2026-08-11T10:43:32.011950Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2312.1338","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:31.722921Z","title":"Weyl quadrat ic gravity as a gauge theory and non-metricity vs torsion duality,","venue":null,"work_id":"fb80abec-2560-4f32-be89-77d7896441e1","year":2024},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.748578Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:9cd713a58de2a907499bec3e99ce40f574c8f34c3ce2705fb556482f9af5beab","observation_id":"153d527f-9377-444e-a9f2-d8e4311452cf","resolution":{"observed_at":"2026-08-11T10:43:31.732729Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2203.05381","last_updated":"2024-01-18T16:54:43Z","snapshot_observed_at":"2026-08-13T16:25:32.899849Z","submitted_at":"2022-03-10T14:13:42Z","title":"Non-metric geometry as the origin of mass in gauge theories of scale invariance","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2203.05381","snapshot_observed_at":"2026-08-11T10:43:29.752464Z","title":"Non-metric geometry as the origin of m ass in gauge theories of scale invariance,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.752464Z"},"links":{"cited_paper":"/paper/2203.05381","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:15c25771f0c6fc4365a3c1832e398dc3b4e306b34390cfe6fe07d0e4e74b8356","observation_id":"b8b1657d-ed56-4fa3-97d8-7ff125f75a26","resolution":{"observed_at":"2026-08-11T10:43:29.752464Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2009.06407","last_updated":"2020-09-11T16:56:22Z","snapshot_observed_at":"2026-08-09T18:53:34.625046Z","submitted_at":"2020-09-11T16:56:22Z","title":"Weyl gauge theories of gravity do not predict a second clock effect","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2009.06407","snapshot_observed_at":"2026-08-11T10:43:29.789254Z","title":"Weyl gauge theories of gr avity do not predict a second clock effect,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.789254Z"},"links":{"cited_paper":"/paper/2009.06407","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:f05818b5bed540124c77a7c6b5e8566694a28016e92fe95c7623aa3600bd88cd","observation_id":"d1b081f9-fa9f-4337-b294-e28178a714e2","resolution":{"observed_at":"2026-08-11T10:43:29.789254Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2309.11372","last_updated":"2025-02-13T17:38:04Z","snapshot_observed_at":"2026-08-13T10:09:11.331301Z","submitted_at":"2023-09-20T14:54:37Z","title":"Weyl conformal geometry vs Weyl anomaly","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2309.11372","snapshot_observed_at":"2026-08-11T10:43:29.860811Z","title":"Weyl conformal geometry vs Weyl anoma ly,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.860811Z"},"links":{"cited_paper":"/paper/2309.11372","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:89949edd0e94c061045c8d5020dcfbcf2d828c65821a581718e84184938bffa0","observation_id":"294fa42d-c64c-413a-a9d0-b676ebf52b99","resolution":{"observed_at":"2026-08-11T10:43:29.860811Z","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":"10.1088/0264-9381/11/6/004","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:30.835062Z","title":"Twenty years of the Weyl anomaly,","venue":null,"work_id":"4c479de4-9638-4ed7-a102-0209e1a9c05f","year":1994},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.983828Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:22a9c199e0b7b5556ffab31f9c31ea71bf1ad9655fcbe979337f56b2fbd39ea8","observation_id":"61d81f5a-b785-41ee-95c8-298858a6db72","resolution":{"observed_at":"2026-08-11T10:43:30.841331Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+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":"2026-08-11T10:43:30.010731Z","title":"Photon correctio ns to the graviton prop- agator,","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.010731Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:4b8ab42cb9a3462c3757de061b14b139aa597262d8ed537f02a16ae11edd984f","observation_id":"36527e22-acb4-413d-8480-1ea527371a1e","resolution":{"observed_at":"2026-08-11T10:43:30.010731Z","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":"2026-08-11T10:43:30.038331Z","title":"Trace anomalies in dimensiona l regularization,","venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.038331Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:0c2650b133291ec657dd2fc0187533883664e1f539f20a7812c69564ff7d149b","observation_id":"f59efd20-317d-47a0-904e-b7d5935300e6","resolution":{"observed_at":"2026-08-11T10:43:30.038331Z","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":"10.1016/0550-3213(76)90480-6","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:30.801928Z","title":"Nonlocal Conformal A nomalies,","venue":null,"work_id":"0fb57740-a360-41d2-93ed-4347bfbb742b","year":1976},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.066342Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:8199c5e1fadae4832372702c62b92be4eaa1c5f7cb0a5ca6d478aa79e6ec4a73","observation_id":"83da75be-da6f-41c7-8499-8ad6b9294e02","resolution":{"observed_at":"2026-08-11T10:43:30.806681Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/9302047","last_updated":"1993-02-12T19:08:00Z","snapshot_observed_at":"2026-07-07T05:02:33.937337Z","submitted_at":"1993-02-12T19:08:00Z","title":"Geometric Classification of Conformal Anomalies in Arbitrary Dimensions","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/9302047","snapshot_observed_at":"2026-08-11T10:43:30.088862Z","title":"Geometric classification of conformal anomalies in arbi- trary dimensions,","venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.088862Z"},"links":{"cited_paper":"/paper/hep-th/9302047","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:31061a3bd9e318b11351a2bb12c75ea0fd8c4ac8a0756fe7edb49fd6d430fae0","observation_id":"b4610709-905d-4859-b430-04fb87f72aeb","resolution":{"observed_at":"2026-08-11T10:43:30.088862Z","resolver_source":null,"status":"malformed_identifier"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":"10.1016/0550-3213(76)90406-5","metadata_source":"doi_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:30.785681Z","title":"Conformal Invari ance in Quantum Gravity,","venue":null,"work_id":"9f1aaab1-a930-4495-b1d2-72258f5cd775","year":1976},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.094668Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:8c5e44b7e2185865758ca05218c779a6847b7d8dc8e1e006748e81b152a7a3ff","observation_id":"d561258b-5b20-47c6-9edf-4766e10dee06","resolution":{"observed_at":"2026-08-11T10:43:30.792101Z","resolver_source":"doi","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2104.15118","last_updated":"2022-11-22T20:45:56Z","snapshot_observed_at":"2026-08-10T17:32:25.505289Z","submitted_at":"2021-04-30T17:01:54Z","title":"Standard Model in Weyl conformal geometry","version":6},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2104.15118","snapshot_observed_at":"2026-08-11T10:43:30.101815Z","title":"Standard Model in Weyl conformal geom etry,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.101815Z"},"links":{"cited_paper":"/paper/2104.15118","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:19250d1ea86823eabaf60fea952902c84e840c425c3ac4392848687c9e12599e","observation_id":"9623c330-5b09-416c-abd5-23c5ff028590","resolution":{"observed_at":"2026-08-11T10:43:30.101815Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.03415","last_updated":"2019-07-19T06:05:00Z","snapshot_observed_at":"2026-08-02T22:03:56.784329Z","submitted_at":"2019-06-08T08:17:52Z","title":"Scale independent $R^2$ inflation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.03415","snapshot_observed_at":"2026-08-11T10:43:30.107765Z","title":"Scal e-independent R2 in- flation,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.107765Z"},"links":{"cited_paper":"/paper/1906.03415","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:9e30e328ffa0ec78c8c4bf0062d7c14e97f1196da977e70e689354f9adc9962a","observation_id":"1cdc2def-045e-4812-b5af-96caeff2a5aa","resolution":{"observed_at":"2026-08-11T10:43:30.107765Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1906.11572","last_updated":"2019-09-30T13:24:17Z","snapshot_observed_at":"2026-08-05T11:17:18.023925Z","submitted_at":"2019-06-27T11:58:21Z","title":"Weyl $R^2$ inflation with an emergent Planck scale","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1906.11572","snapshot_observed_at":"2026-08-11T10:43:30.112479Z","title":"Weyl R 2 inflation with an emergent Planck scale,","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.112479Z"},"links":{"cited_paper":"/paper/1906.11572","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:8d9c680eca9c7b3c97f729ef5e46c25fd7c49593fcf9ad9608b0718c0cd22326","observation_id":"e8da7301-cafe-4e1f-89ba-1ab5b8323b17","resolution":{"observed_at":"2026-08-11T10:43:30.112479Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.14733","last_updated":"2021-05-12T00:02:14Z","snapshot_observed_at":"2026-08-10T12:37:39.564762Z","submitted_at":"2020-07-29T10:43:38Z","title":"Gauging scale symmetry and inflation: Weyl versus Palatini gravity","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.14733","snapshot_observed_at":"2026-08-11T10:43:30.117185Z","title":"Gauging scale symmetry and inflation: Weyl versus Palatini gravity,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.117185Z"},"links":{"cited_paper":"/paper/2007.14733","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:1080c664f1b21f93100d2ef6cc5ea7397adbf13c02bc7899a863f29f6ef2bdcd","observation_id":"95e8360c-2b0a-47c3-88b6-6078ce7b7933","resolution":{"observed_at":"2026-08-11T10:43:30.117185Z","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":"2026-08-11T10:43:30.122758Z","title":"A New Type of Isotropic Cosmologica l Models Without Singular- ity,","venue":null,"work_id":null,"year":1980},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.122758Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:4b4bd2da833f18cb5d4824fee236d98244f4954f813943986fefa2c98c934441","observation_id":"8e2acc11-92d9-45dc-9707-b141ced42d3e","resolution":{"observed_at":"2026-08-11T10:43:30.122758Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2311.16893","last_updated":"2023-11-28T15:44:44Z","snapshot_observed_at":"2026-08-13T05:15:18.186414Z","submitted_at":"2023-11-28T15:44:44Z","title":"Testing Weyl geometric gravity with the SPARC galactic rotation curves database","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2311.16893","snapshot_observed_at":"2026-08-11T10:43:30.177802Z","title":"Testing Weyl geometric gravi ty with the SPARC galactic rotation curves database,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.177802Z"},"links":{"cited_paper":"/paper/2311.16893","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:b14979f97c5fad1e3f82ca44a329cf3a351394f390553770c1ef3989a566c958","observation_id":"dc0e0cb4-5be5-4f4b-bcc4-620909b45827","resolution":{"observed_at":"2026-08-11T10:43:30.177802Z","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":"2212.0554","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:31.427971Z","title":"Black hole solution s in the quadratic Weyl conformal geometric theory of gravity,","venue":null,"work_id":"89de71ca-b8e7-4065-b2a2-71836c33072d","year":2022},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.309304Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:0c94ecdce1f883b517fe4b3478d7384af776dce7cfcd14f417b4f7f3fc6fcfa0","observation_id":"3c7b2852-cba2-414a-abdb-667bb54aa8fa","resolution":{"observed_at":"2026-08-11T10:43:31.482505Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+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":"2026-08-11T10:43:30.384442Z","title":"Foundations of the new field theor y,","venue":null,"work_id":null,"year":1934},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.384442Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:d70ab9fd7f9cb7d5d07cc3642926ee8b297327a2fe545eb4b4c6d840fce382cf","observation_id":"11c84d15-6739-4736-987f-d1722bb544c3","resolution":{"observed_at":"2026-08-11T10:43:30.384442Z","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":"1962.0124","doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:31.193838Z","title":"An Extensible model of the electron,","venue":null,"work_id":"85d2b737-53b1-41e8-8f71-c709c32e5d10","year":1962},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.408908Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:3a4afbb9d0567c85a0bd1aaedf1d9a267d647fb809cf543e695bf43127a56567","observation_id":"6703e2a1-e246-4ea0-920d-b0edf4762c10","resolution":{"observed_at":"2026-08-11T10:43:31.237519Z","resolver_source":"raw_fallback","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2112.12118","last_updated":"2022-07-28T15:43:42Z","snapshot_observed_at":"2026-08-10T23:45:31.005130Z","submitted_at":"2021-12-22T18:30:32Z","title":"Introductory Notes on Non-linear Electrodynamics and its Applications","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2112.12118","snapshot_observed_at":"2026-08-11T10:43:30.413190Z","title":"Introductory Notes on N on-linear Elec- trodynamics and its Applications,","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.413190Z"},"links":{"cited_paper":"/paper/2112.12118","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:8e582924108cfea86af1a5f3592e5987b1c8f7be014a2fbf888afc5a471f5339","observation_id":"61147bf9-6e22-408c-ae20-825145e60b95","resolution":{"observed_at":"2026-08-11T10:43:30.413190Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0106059","last_updated":"2001-06-07T09:48:53Z","snapshot_observed_at":"2026-07-07T04:40:18.756605Z","submitted_at":"2001-06-07T09:48:53Z","title":"Aspects of Born-Infeld Theory and String/M-Theory","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0106059","snapshot_observed_at":"2026-08-11T10:43:30.417470Z","title":"Aspects of Born- Infeld theory and string / M theory,","venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.417470Z"},"links":{"cited_paper":"/paper/hep-th/0106059","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:6a6d9a2e0ea9f23746dcdae9f378796a42035ab1361999fea7b0244424901a57","observation_id":"b9eda923-0b74-42b2-bf27-61f2f7de2adc","resolution":{"observed_at":"2026-08-11T10:43:30.417470Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.18173","last_updated":"2025-03-07T19:54:18Z","snapshot_observed_at":"2026-08-13T17:46:10.110557Z","submitted_at":"2024-07-25T16:34:48Z","title":"Weyl gauge invariant DBI action in conformal geometry","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.18173","snapshot_observed_at":"2026-08-11T10:43:30.423062Z","title":"Weyl gauge invariant DBI action in con formal geometry,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.423062Z"},"links":{"cited_paper":"/paper/2407.18173","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:298f1af77216736e16e3b7ebc56907c765a3efe9a22a117c0999ad1e875c4257","observation_id":"41f72c67-d06c-4893-be59-5447fb1a9f79","resolution":{"observed_at":"2026-08-11T10:43:30.423062Z","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":"2026-08-11T10:43:30.428665Z","title":"Standard Model in confor mal geome- try: Local vs gauged scale invariance,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.428665Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:cf3d636f669b9b5763bcfee1ecd616508efeb0de492866667c8d98deeb35a1fa","observation_id":"ab7e3fb6-ee83-4802-8298-0956ff77f2af","resolution":{"observed_at":"2026-08-11T10:43:30.428665Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:31.991956Z","title":null,"venue":null,"work_id":"7de3be68-4720-40b0-9d2c-70fbc630bd26","year":2021},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.433575Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:02dfaead0f546c292edbd60a66d57e9ecfeefb2e0861622bac6ae0f5c05f60b5","observation_id":"e0fed4b9-e1f6-4805-a082-9dfb5eba5c88","resolution":{"observed_at":"2026-08-11T10:43:31.996375Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1603.05983","last_updated":"2016-10-27T20:53:15Z","snapshot_observed_at":"2026-07-06T04:50:00.997524Z","submitted_at":"2016-03-18T20:05:06Z","title":"Scale-Independent Inflation and Hierarchy Generation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1603.05983","snapshot_observed_at":"2026-08-11T10:43:30.437863Z","title":"Scale-Indepen dent Inflation and Hierarchy Generation,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.437863Z"},"links":{"cited_paper":"/paper/1603.05983","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:c2674daf51632ab285aaa58e334f409f4dfbfccd3ad0a3e8aff359174440229a","observation_id":"86a5ec83-2da4-4588-98a4-f0a92769d606","resolution":{"observed_at":"2026-08-11T10:43:30.437863Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1612.03157","last_updated":"2016-12-09T20:38:46Z","snapshot_observed_at":"2026-08-02T12:35:40.824422Z","submitted_at":"2016-12-09T20:38:46Z","title":"No fifth force in a scale invariant universe","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1612.03157","snapshot_observed_at":"2026-08-11T10:43:30.442914Z","title":"No fifth force in a scale invariant universe,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.442914Z"},"links":{"cited_paper":"/paper/1612.03157","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:29a4a55c68b43c2f67abd8c3b3d542d04e9c41611cfac3db7def34eefa397b1a","observation_id":"9a780736-02df-44ce-9ecd-a46d7933f517","resolution":{"observed_at":"2026-08-11T10:43:30.442914Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1801.07676","last_updated":"2018-10-31T06:32:33Z","snapshot_observed_at":"2026-07-06T06:19:55.917796Z","submitted_at":"2018-01-23T17:52:48Z","title":"Inertial Spontaneous Symmetry Breaking and Quantum Scale Invariance","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1801.07676","snapshot_observed_at":"2026-08-11T10:43:30.447817Z","title":"Inertial Spont aneous Symmetry Breaking and Quantum Scale Invariance,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.447817Z"},"links":{"cited_paper":"/paper/1801.07676","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:56bf9024bee3b082859358ddb602507c9a785d885e974018ae23406a1ce841ae","observation_id":"461cd14a-bd55-4251-a45d-d6167343da00","resolution":{"observed_at":"2026-08-11T10:43:30.447817Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1610.09243","last_updated":"2016-12-14T20:56:59Z","snapshot_observed_at":"2026-07-06T05:16:33.346094Z","submitted_at":"2016-10-28T14:42:22Z","title":"Weyl Current, Scale-Invariant Inflation and Planck Scale Generation","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1610.09243","snapshot_observed_at":"2026-08-11T10:43:30.501863Z","title":"Weyl Current, S cale-Invariant In- flation and Planck Scale Generation,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.501863Z"},"links":{"cited_paper":"/paper/1610.09243","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:22928e699b28a4669a2cf7a9b8656b86446b8145cba02ce2f0cd0e38ea04ac9c","observation_id":"489e6266-34e3-4432-83ab-ab450c9d6a53","resolution":{"observed_at":"2026-08-11T10:43:30.501863Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1107.2163","last_updated":"2011-07-11T23:11:59Z","snapshot_observed_at":"2026-08-02T22:33:57.704351Z","submitted_at":"2011-07-11T23:11:59Z","title":"Higgs-Dilaton Cosmology: From the Early to the Late Universe","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1107.2163","snapshot_observed_at":"2026-08-11T10:43:30.579343Z","title":"Higgs-Dilaton Cos- mology: From the Early to the Late Universe,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.579343Z"},"links":{"cited_paper":"/paper/1107.2163","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:8eea1c9734ee7f1de060b7e1ed5751c484f3986b92b6d34e9f6389c154a33148","observation_id":"1f8688b0-4d58-4db5-8fcd-2fb0a76ce2a4","resolution":{"observed_at":"2026-08-11T10:43:30.579343Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:31.977940Z","title":"Dimensionally dependent identities,","venue":null,"work_id":"8c245968-f4ab-4e1f-b4ec-87da27d05177","year":null},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.662411Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:d7b4205a0eee008a0d8ca707c8fd16769b37ad5b0d34bfb316188fdd57b6ddac","observation_id":"7b6c1132-0a54-4f33-824f-bae40850eb32","resolution":{"observed_at":"2026-08-11T10:43:31.982477Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1508.00595","last_updated":"2016-06-02T20:37:31Z","snapshot_observed_at":"2026-07-06T04:25:42.706754Z","submitted_at":"2015-08-03T20:42:51Z","title":"Manifestly scale-invariant regularization and quantum effective operators","version":5},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1508.00595","snapshot_observed_at":"2026-08-11T10:43:30.727966Z","title":"Manifestly scale-invariant regular ization and quantum effective operators,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:30.727966Z"},"links":{"cited_paper":"/paper/1508.00595","citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:e106513e16095ddddcf18ae02217055933f8477ad44dcebab437e531d47d77de","observation_id":"8e2b7d73-5692-4bb4-8aa0-1dc5b2dc9a93","resolution":{"observed_at":"2026-08-11T10:43:30.727966Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-11T10:43:32.059801Z","title":"Delphenich is currently ava ilable at this link: http://www.neo-classical-physics.info/spacetime-structure.html)","venue":null,"work_id":"303ec4a5-aea8-453f-bfa1-effe9fe909c1","year":null},"citing_paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws","version":3},"reference_index":133,"source":"pdf_text","source_observed_at":"2026-08-11T10:43:29.207038Z"},"links":{"citing_paper":"/paper/2412.16548"},"observation_digest":"sha256:36e98927b2586dbbdba701e2907d1240c148144ba0d575a4087953420402548a","observation_id":"755ba17c-a27b-4e89-b2e5-e4437c165f6e","resolution":{"observed_at":"2026-08-11T10:43:32.069964Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-13T06:32:02.005865+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2412.16548","last_updated":"2025-03-27T18:02:27Z","latest_version":3,"primary_category":"hep-th","snapshot_observed_at":"2026-08-11T18:12:33.573697Z","submitted_at":"2024-12-21T09:21:17Z","title":"Conformal geometry as a gauge theory of gravity: covariant equations of motion & conservation laws"},"reference_resolution":{"displayed":50,"state_counts":{"malformed_identifier":3,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":33,"verified_exact":8,"verified_fuzzy":6},"total_outbound_references":50},"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":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 50 of 50 outbound references and 3 inbound Pith citation observations for arXiv:2412.16548."}