Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links
Paper Citation Record · LEDGER
As of 12 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 3 inbound Pith citation observations for arXiv:1507.00922.
A citation records a reference. It does not transfer a finding from one paper to another.
Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links
One-hop event checks from named stored sources.
Source: scholarly_work_events, retraction_status_cache, observed 2026-08-12T06:34:41.77262+00:00
Pith citing papers itemized under the disclosed page cap.
Source: paper_references, paper_reference_links, observed 2026-08-11T10:59:05.862316Z
A source-named dated measurement, never combined with another source.
Source: arxiv_reference, observed 2026-05-11T23:01:14.822647Z
0 of 0 outbound references displayed
External citation measurements
No source-named external measurement is stored.
No outbound reference observations are available for this paper version.
Observation 32ab92db-0726-4e7b-abee-1a8baca817e7 · inbound
Discriminating between different modified dispersion relations from gamma-ray observations Hamilton geometry: Phase space geometry from modified dispersion relations
Reference 32
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 1e1e5cc9-738e-4ea8-81ef-5851c3720ab3 · inbound
Fermi Acceleration Mechanisms Beyond Lorentz Symmetry Hamilton geometry: Phase space geometry from modified dispersion relations
Reference 34
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation db7afca5-31f1-4520-a9b2-6c72a5785647 · inbound
Hawking radiation with dispersion: reconciling the Bogoliubov and tunneling approaches Hamilton geometry: Phase space geometry from modified dispersion relations
Reference 41
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.