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Paper Citation Record · LEDGER

$SU(2)$ principal chiral model with tensor renormalization group on a cubic lattice

As of 18 August 2026, this Paper Citation Record lists 0 of 0 outbound references and 4 inbound Pith citation observations for arXiv:2406.10081.

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

pith.paper-citation-record.v1
2406.10081 v1

Coverage vector

measured 0 of 0 reference resolution

Typed states for the displayed outbound observations.

Source: paper_references, paper_reference_links

measured 4 of 4 standing notices

One-hop event checks from named stored sources.

Source: scholarly_work_events, retraction_status_cache, observed 2026-08-18T06:34:40.430872+00:00

measured 4 of 4 inbound itemization

Pith citing papers itemized under the disclosed page cap.

Source: paper_references, paper_reference_links, observed 2026-08-11T12:32:45.304616Z

measured 0 of 1 external citation measurements

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

Source: arxiv_reference, observed 2026-05-16T17:38:10.728401Z

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 4f4e8e63-b461-41a7-9363-46d1bc7b23eb · inbound

Applying the Triad network representation to four-dimensional ATRG method cites this paper.

Applying the Triad network representation to four-dimensional ATRG method $SU(2)$ principal chiral model with tensor renormalization group on a cubic lattice

Reference 12

Resolution
unresolved
no resolver link, observed 2026-08-11T12:32:45.304616Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-11T12:32:45.304616Z digest=sha256:549fd3e7afb0100fe0b0034904120a611b98f07ceda5ee8636b24a6c77eb6eee

Observation 4a06717c-b4f9-497b-951c-dd1cf62c5c43 · inbound

Twisted Partition Functions as Order Parameters cites this paper.

Twisted Partition Functions as Order Parameters $SU(2)$ principal chiral model with tensor renormalization group on a cubic lattice

Reference 73

Resolution
unresolved
no resolver link, observed 2026-08-07T15:09:37.983458Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-07T15:09:37.983458Z digest=sha256:0737efeb865a90b83d48d145dc397e4d0b71455fd5137a71d2623897cb7fd904

Observation aeb867f4-7fb4-4b63-9f27-b8eb0a713dd5 · inbound

Tensor renormalization group approach to critical phenomena via symmetry-twisted partition functions cites this paper.

Tensor renormalization group approach to critical phenomena via symmetry-twisted partition functions $SU(2)$ principal chiral model with tensor renormalization group on a cubic lattice

Reference 26

Resolution
verified exact
arxiv_id, observed 2026-05-16T17:38:10.730494Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-18T06:34:40.430872+00:00.

source=pdf_text observed=2026-05-16T17:34:54.910650Z digest=sha256:2f32cd5c60f74dc98d3985cf441efdea91a0d23d16da56ee2f9c675b8e3ea9ca

Observation bc435010-9de2-48d5-a3ed-c08077c37442 · inbound

Forward-mode automatic differentiation for the tensor renormalization group and its relation to the impurity method cites this paper.

Forward-mode automatic differentiation for the tensor renormalization group and its relation to the impurity method $SU(2)$ principal chiral model with tensor renormalization group on a cubic lattice

Reference 44

Resolution
unresolved
no resolver link, observed 2026-08-03T03:08:17.597261Z

Source-reported events for the cited work

Unavailable: canonical work link unavailable.

source=pdf_text observed=2026-08-03T03:08:17.597261Z digest=sha256:29da68011dabe8a404fb6daa80c50815d0306f489a08f5e55c8327ed47782af0