Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links
Paper Citation Record · LEDGER
Resurgence in Liouville Theory
As of 19 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 2 inbound Pith citation observations for arXiv:2408.14574.
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 2026-08-19T06:32:44.657259+00:00
Pith citing papers itemized under the disclosed page cap.
Source: paper_references, paper_reference_links, observed 2026-08-11T21:40:32.542533Z
A source-named dated measurement, never combined with another source.
Source: pith, observed 2026-08-05T16:09:16.779884Z
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 35a02b36-a0e3-469c-8078-88425017122f · inbound
On the $1/c$ expansion in $2d$ CFTs with degenerate operators cites this paper.
On the $1/c$ expansion in $2d$ CFTs with degenerate operators Resurgence in Liouville Theory
Reference 49
- Resolution
- unresolved
- no resolver link, observed 2026-08-11T21:40:32.542533Z
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation afe26744-5449-488e-a127-2d925f50bf91 · inbound
Resurgence for large $c$ expansion in Coulomb gas formalism cites this paper.
Resurgence for large $c$ expansion in Coulomb gas formalism Resurgence in Liouville Theory
Reference 17
- Resolution
- verified exact
- local_arxiv, observed 2026-08-05T16:09:16.940232Z
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-19T06:32:44.657259+00:00.