Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links
Paper Citation Record · LEDGER
Lagrangian and Hamiltonian formulations of asymmetric rigid body, considered as a constrained system
As of 16 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 5 inbound Pith citation observations for arXiv:2301.10741.
A citation records a reference. It does not transfer a finding from one paper to another.
Coverage vector
One-hop event checks from named stored sources.
Source: scholarly_work_events, retraction_status_cache, observed 2026-08-16T06:30:59.297886+00:00
Pith citing papers itemized under the disclosed page cap.
Source: paper_references, paper_reference_links, observed 2026-08-15T18:39:50.754534Z
A source-named dated measurement, never combined with another source.
Source: arxiv_reference, observed 2026-05-20T23:03:50.500758Z
Reference resolution
0 of 0 outbound references displayed
- verified exact0
- verified fuzzy0
- unresolved0
- parse uncertain0
- malformed identifier0
- metadata mismatch0
External citation measurements
No source-named external measurement is stored.
Outbound references
No outbound reference observations are available for this paper version.
Pith citing papers
Observation 4ded1c9b-3f79-4b7a-8208-451ccb662881 · inbound
An alternative interpretation of the Grioli gyroscope suspension points cites this paper.
An alternative interpretation of the Grioli gyroscope suspension points Lagrangian and Hamiltonian formulations of asymmetric rigid body, considered as a constrained system
Reference 39
- Resolution
- unresolved
- no resolver link, observed 2026-08-15T18:39:50.754534Z
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation b912be4c-d66a-46bf-b9e5-f8092ecf69d6 · inbound
Dynamics of a relativistic discrete body: rigidity conditions, and covariant equations of motion cites this paper.
Dynamics of a relativistic discrete body: rigidity conditions, and covariant equations of motion Lagrangian and Hamiltonian formulations of asymmetric rigid body, considered as a constrained system
Reference 11
- Resolution
- verified exact
- arxiv_id, observed 2026-05-13T02:17:06.204962Z
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.
Observation eb2c2388-9311-4658-b35f-2d563cbf0835 · inbound
Dynamics of a relativistic discrete body: rigidity conditions, and covariant equations of motion cites this paper.
Dynamics of a relativistic discrete body: rigidity conditions, and covariant equations of motion Lagrangian and Hamiltonian formulations of asymmetric rigid body, considered as a constrained system
Reference 3
- Resolution
- verified exact
- arxiv_id, observed 2026-05-14T21:02:58.957696Z
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.
Observation 34c78416-e64d-4732-99f1-3cf41a1dd4b9 · inbound
Dynamics of a relativistic discrete body: rigidity conditions, and covariant equations of motion cites this paper.
Dynamics of a relativistic discrete body: rigidity conditions, and covariant equations of motion Lagrangian and Hamiltonian formulations of asymmetric rigid body, considered as a constrained system
Reference 3
- Resolution
- verified exact
- arxiv_id, observed 2026-05-20T23:03:50.503695Z
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-16T06:30:59.297886+00:00.
Observation b71e74df-2e05-44ce-89a4-fc4a558eb7ed · inbound
Dynamics of a relativistic discrete body: rigidity conditions, and covariant equations of motion cites this paper.
Dynamics of a relativistic discrete body: rigidity conditions, and covariant equations of motion Lagrangian and Hamiltonian formulations of asymmetric rigid body, considered as a constrained system
Reference 3
- Resolution
- unresolved
- no resolver link, observed 2026-08-04T05:22:08.714645Z
Source-reported events for the cited work
Unavailable: canonical work link unavailable.