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:1711.05755.
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 2026-08-11T19:25:00.769336Z
A source-named dated measurement, never combined with another source.
Source: pith, observed 2026-08-07T05:02:23.499747Z
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 d5a307be-a695-449a-bbb8-40bbeace5275 · inbound
Three-loop jet function for boosted heavy quarks Bottom and Charm Mass determinations from global fits to $Q\bar{Q}$ bound states at N$^3$LO
Reference 66
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation c99c4777-cb4b-474d-94bd-0564018edba8 · inbound
On Determining $\alpha_s(m_Z)$ from Dijets in $e^+e^-$ Thrust Bottom and Charm Mass determinations from global fits to $Q\bar{Q}$ bound states at N$^3$LO
Reference 79
Source-reported events for the cited work
Unavailable: canonical work link unavailable.
Observation 00954a09-f16a-4f04-8620-aa64b8bc350a · inbound
Precision $e^+e^-$ Hemisphere Masses in the Dijet Region with Power Corrections Bottom and Charm Mass determinations from global fits to $Q\bar{Q}$ bound states at N$^3$LO
Reference 131
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.