Pith. sign in

Paper Citation Record · LEDGER

Chiral Effective Field Theories for Strong and Weak Dynamics

As of 7 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 1 inbound Pith citation observation for arXiv:2501.14018.

A citation records a reference. It does not transfer a finding from one paper to another.

pith.paper-citation-record.v1
2501.14018 v1

Coverage vector

measured 0 of 0 reference resolution

Typed states for the displayed outbound observations.

Source: paper_references, paper_reference_links

measured 1 of 1 standing notices

One-hop event checks from named stored sources.

Source: scholarly_work_events, retraction_status_cache, observed 2026-08-07T06:34:17.273281+00:00

measured 1 of 1 inbound itemization

Pith citing papers itemized under the disclosed page cap.

Source: paper_references, paper_reference_links, observed 2026-05-08T18:24:51.004930Z

measured 0 of 1 external citation measurements

A source-named dated measurement, never combined with another source.

Source: arxiv_reference, observed 2026-05-09T06:30:39.619805Z

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 19298720-b3f4-4420-a405-f5b44f64f579 · inbound

Finite-temperature operator basis on $\mathbb{R}^3 \times S^1$ for SMEFT cites this paper.

Finite-temperature operator basis on $\mathbb{R}^3 \times S^1$ for SMEFT Chiral Effective Field Theories for Strong and Weak Dynamics

Reference 58

Resolution
verified exact
arxiv_id, observed 2026-05-09T06:30:39.622082Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-07T06:34:17.273281+00:00.

source=pdf_text observed=2026-05-08T18:24:51.004930Z digest=sha256:ddd2abf296c04dcec244156dd67eac865cd61fafa51ff937ed4252eb96effc1b