{"as_of":"2026-08-20T09:42:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:45d7672e16d6fdea0f182b0fc545d8de85abfe8110643465183e9da362b402ef","coverage":[{"denominator":0,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":6,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":6,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-20T06:33:59.587034+00:00","state":"measured"},{"denominator":6,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":6,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T20:33:03.346246Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"arxiv_reference","source_observed_at":"2026-07-04T18:50:04.372814Z","state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2201.06558","last_updated":"2022-03-09T14:27:44Z","snapshot_observed_at":"2026-08-16T17:27:49.129183Z","submitted_at":"2022-01-17T18:25:38Z","title":"Singular Lagrangians, Constrained Hamiltonian Systems and Gauge Invariance: An Example of the Dirac-Bergmann Algorithm","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.06558","snapshot_observed_at":"2026-08-03T20:33:03.346246Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2511.20083","last_updated":"2026-06-09T03:37:54Z","snapshot_observed_at":"2026-08-15T12:32:42.143057Z","submitted_at":"2025-11-25T08:58:23Z","title":"Covariant equations of motion of massive spinning particles in a background Yang-Mills field","version":2},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-03T20:33:03.346246Z"},"links":{"cited_paper":"/paper/2201.06558","citing_paper":"/paper/2511.20083"},"observation_digest":"sha256:93c132b7366a72140a98101f53a6df995a5036e189292b5c0feec773fb4bbd21","observation_id":"825d017c-ee05-4be7-8fa0-0601ae004328","resolution":{"observed_at":"2026-08-03T20:33:03.346246Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.06558","last_updated":"2022-03-09T14:27:44Z","snapshot_observed_at":"2026-08-16T17:27:49.129183Z","submitted_at":"2022-01-17T18:25:38Z","title":"Singular Lagrangians, Constrained Hamiltonian Systems and Gauge Invariance: An Example of the Dirac-Bergmann Algorithm","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.06558","snapshot_observed_at":"2026-08-03T11:30:37.573041Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2601.06416","last_updated":"2026-07-19T15:37:42Z","snapshot_observed_at":"2026-08-18T16:26:02.478232Z","submitted_at":"2026-01-10T03:48:10Z","title":"Symplectic mechanics of relativistic spinning compact bodies. III. quadratic-in-spin integrability in Type-D Einstein spacetimes: persistence and breakdown","version":2},"reference_index":136,"source":"pdf_text","source_observed_at":"2026-08-03T11:30:37.573041Z"},"links":{"cited_paper":"/paper/2201.06558","citing_paper":"/paper/2601.06416"},"observation_digest":"sha256:ee551a702c498b278e33d12b4bb9e643b4a7a65730b16a048b86e63b23576ad9","observation_id":"9da2e280-a108-4a1e-b84c-76227b3ac7fa","resolution":{"observed_at":"2026-08-03T11:30:37.573041Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.06558","last_updated":"2022-03-09T14:27:44Z","snapshot_observed_at":"2026-08-16T17:27:49.129183Z","submitted_at":"2022-01-17T18:25:38Z","title":"Singular Lagrangians, Constrained Hamiltonian Systems and Gauge Invariance: An Example of the Dirac-Bergmann Algorithm","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.06558","snapshot_observed_at":"2026-07-12T15:56:07.930375Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2605.27046","last_updated":"2026-07-03T06:05:32Z","snapshot_observed_at":"2026-08-15T12:11:14.236385Z","submitted_at":"2026-05-26T14:00:10Z","title":"Learning to Balance Motor Thermal Safety and Quadrupedal Locomotion Performance with Residual Policy","version":3},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-07-12T15:56:07.930375Z"},"links":{"cited_paper":"/paper/2201.06558","citing_paper":"/paper/2605.27046"},"observation_digest":"sha256:8416a37eeb0837fe3e233f0136f4f211600e017675de93885ecd7468994c58b1","observation_id":"bf7acf3e-59d6-4d16-982d-24ce8d15a637","resolution":{"observed_at":"2026-07-12T15:56:07.930375Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.06558","last_updated":"2022-03-09T14:27:44Z","snapshot_observed_at":"2026-08-16T17:27:49.129183Z","submitted_at":"2022-01-17T18:25:38Z","title":"Singular Lagrangians, Constrained Hamiltonian Systems and Gauge Invariance: An Example of the Dirac-Bergmann Algorithm","version":3},"cited_work":{"arxiv_id":"2201.06558","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2201.06558","snapshot_observed_at":"2026-07-04T18:50:04.372814Z","title":null,"venue":null,"work_id":"a8b8c9c4-0408-4749-9017-0a4c2cf63a60","year":2022},"citing_paper":{"arxiv_id":"2605.27047","last_updated":"2026-05-26T14:00:27Z","snapshot_observed_at":"2026-08-13T19:29:24.979617Z","submitted_at":"2026-05-26T14:00:27Z","title":"Canonical quantization of massive vector field in Schwarzschild black hole background","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-06-29T16:11:41.210212Z"},"links":{"cited_paper":"/paper/2201.06558","citing_paper":"/paper/2605.27047"},"observation_digest":"sha256:20d8c2998ef0d7e05ea492cd20853dade85e75a26761e071078a907c329f3ced","observation_id":"145cbf8c-0a91-4e3f-a06b-f7a9a3bd55c1","resolution":{"observed_at":"2026-06-29T16:13:35.937203Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-20T06:33:59.587034+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2201.06558","last_updated":"2022-03-09T14:27:44Z","snapshot_observed_at":"2026-08-16T17:27:49.129183Z","submitted_at":"2022-01-17T18:25:38Z","title":"Singular Lagrangians, Constrained Hamiltonian Systems and Gauge Invariance: An Example of the Dirac-Bergmann Algorithm","version":3},"cited_work":{"arxiv_id":"2201.06558","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":"2201.06558","snapshot_observed_at":"2026-07-04T18:50:04.372814Z","title":null,"venue":null,"work_id":"a8b8c9c4-0408-4749-9017-0a4c2cf63a60","year":2022},"citing_paper":{"arxiv_id":"2606.24442","last_updated":"2026-07-03T01:45:19Z","snapshot_observed_at":"2026-08-05T11:53:37.197437Z","submitted_at":"2026-06-23T11:22:23Z","title":"Canonical quantization for effective theories with perturbations altering degrees of freedom: a covariant phase space approach","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-06-25T22:32:20.450539Z"},"links":{"cited_paper":"/paper/2201.06558","citing_paper":"/paper/2606.24442"},"observation_digest":"sha256:5bba3e1ef197cb73dfb0fdd1b5079c106dc16eed7fa859510a5f116f0c520a49","observation_id":"753e0357-9298-46cb-98ab-827226969027","resolution":{"observed_at":"2026-07-04T18:50:04.374327Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-20T06:33:59.587034+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2201.06558","last_updated":"2022-03-09T14:27:44Z","snapshot_observed_at":"2026-08-16T17:27:49.129183Z","submitted_at":"2022-01-17T18:25:38Z","title":"Singular Lagrangians, Constrained Hamiltonian Systems and Gauge Invariance: An Example of the Dirac-Bergmann Algorithm","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2201.06558","snapshot_observed_at":"2026-07-12T12:32:01.913058Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2606.24442","last_updated":"2026-07-03T01:45:19Z","snapshot_observed_at":"2026-08-05T11:53:37.197437Z","submitted_at":"2026-06-23T11:22:23Z","title":"Canonical quantization for effective theories with perturbations altering degrees of freedom: a covariant phase space approach","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-07-12T12:32:01.913058Z"},"links":{"cited_paper":"/paper/2201.06558","citing_paper":"/paper/2606.24442"},"observation_digest":"sha256:e996bfe532c6dbd61a939e2547ea20f911e638b9a9667861a125c35f132ab3a5","observation_id":"46c9dcd5-66fb-42b4-baca-94af21c5c43b","resolution":{"observed_at":"2026-07-12T12:32:01.913058Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2201.06558/citation-record","integrity":"/paper/2201.06558/integrity","json":"/paper/2201.06558/citation-record.json","paper":"/paper/2201.06558"},"outbound":[],"paper":{"arxiv_id":"2201.06558","last_updated":"2022-03-09T14:27:44Z","latest_version":3,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-16T17:27:49.129183Z","submitted_at":"2022-01-17T18:25:38Z","title":"Singular Lagrangians, Constrained Hamiltonian Systems and Gauge Invariance: An Example of the Dirac-Bergmann Algorithm"},"reference_resolution":{"displayed":0,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":0,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":0},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-20T06:33:59.587034+00:00","source":"crossref"},{"observed_at":"2026-08-20T06:33:54.927442+00:00","source":"retraction_watch"}],"thesis":"As of 20 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 6 inbound Pith citation observations for arXiv:2201.06558."}