Typed states for the displayed outbound observations.
Source: paper_references, paper_reference_links
Paper Citation Record · LEDGER
As of 15 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 3 inbound Pith citation observations for arXiv:1709.00921.
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 2026-08-15T06:32:42.880941+00:00
Pith citing papers itemized under the disclosed page cap.
Source: paper_references, paper_reference_links, observed 2026-08-14T14:16:23.294509Z
A source-named dated measurement, never combined with another source.
Source: arxiv_reference, observed 2026-05-11T03:15:55.477829Z
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 637f2fe7-357e-49aa-bf09-c9cc5a4176ef · inbound
Complexity measures in QFT and constrained geometric actions A Complexity for Quantum Field Theory States and Application in Thermofield Double States
Reference 14
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 2e9e3f4c-229f-42d5-aa11-589019c2ac9a · inbound
Reflections on Virasoro circuit complexity and Berry phase A Complexity for Quantum Field Theory States and Application in Thermofield Double States
Reference 62
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation bfefb7f1-2d65-44fd-b015-cfad8f4e5388 · inbound
Bridging Krylov Complexity and Universal Analog Quantum Simulator A Complexity for Quantum Field Theory States and Application in Thermofield Double States
Reference 3
Source-reported events for the cited work
No event found in the named queried sources as of 2026-08-15T06:32:42.880941+00:00.