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PreprintCC BY 4.0arXiv

Fluctuations in the Potts spin glass model at high temperature

Abstract

We study the fluctuations of the free energy of the Potts spin glass with κ colors at high temperature. The disorder is symmetric with unit variance and finite fourth moment. For configurations with a balanced, or nearly balanced, color profile, the log-partition function satisfies a central limit theorem whenever β2<αc(κ). Here καc(κ) is the critical inverse temperature of the Curie-Weiss-Potts model. A comparison of color profiles transfers this limit to the unconstrained model for β<βmax(κ), an explicit threshold. In the same range, the magnetizations of two replicas and their overlap matrix satisfy a joint quenched central limit theorem with independent Gaussian limits. The fourth cumulant of the disorder enters the limiting mean and variance explicitly.

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BibTeX
@misc{dey2026fluctuations,
  title = {{Fluctuations in the Potts spin glass model at high temperature}},
  author = {Partha S. Dey and Taegu Kang},
  howpublished = {arXiv},
  year = {2026},
  month = oct,
  doi = {10.48550/arxiv.2610.19356},
  eprint = {2610.19356},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2610.19356},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Fluctuations in the Potts spin glass model at high temperature
AU  - Partha S. Dey
AU  - Taegu Kang
PY  - 2026
DA  - 2026/10/14
PB  - arXiv
DO  - 10.48550/arxiv.2610.19356
UR  - https://arxiv.org/abs/2610.19356
AB  - We study the fluctuations of the free energy of the Potts spin glass with κ colors at high temperature. The disorder is symmetric with unit variance and finite fourth moment. For configurations with a balanced, or nearly balanced, color profile, the log-partition function satisfies a central limit theorem whenever β^2<α_c(κ). Here κα_c(κ) is the critical inverse temperature of the Curie-Weiss-Potts model. A comparison of color profiles transfers this limit to the unconstrained model for β<β_max(κ), an explicit threshold. In the same range, the magnetizations of two replicas and their overlap matrix satisfy a joint quenched central limit theorem with independent Gaussian limits. The fourth cumulant of the disorder enters the limiting mean and variance explicitly.
ER  -