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Fluctuations for the Sherrington--Kirkpatrick spin glass model near the critical temperature

Probability 2026-03-09 v1

Abstract

We consider the Sherrington--Kirkpatrick spin glass model with zero external field and at inverse temperature β>0\beta>0. Let FN(β)F_N(\beta) be the corresponding log-partition function. Under the assumption that cN:=N1/3(1βN2)c_N:=N^{1/3}(1-\beta_N^2) is bounded away from 00, we prove that Var(FN(βN))=12log(1βN2)βN2/2+O(cN3/2).(F_N(\beta_N)) = - \frac{1}{2} \log (1-\beta_N^2) -{\beta_N^2}/{2} + O( c_N^{-3/2}). As a consequence, we obtain Var(FN(1cN1/3))=16logN+O(1)(F_N(1-c N^{-1/3})) = \frac16\log N + O(1) for any fixed constant c(0,)c\in(0,\infty). We also prove a Gaussian central limit theorem for the centered and scaled FN(βN)F_N(\beta_N).

Keywords

Cite

@article{arxiv.2603.05636,
  title  = {Fluctuations for the Sherrington--Kirkpatrick spin glass model near the critical temperature},
  author = {Partha S. Dey and Taegu Kang},
  journal= {arXiv preprint arXiv:2603.05636},
  year   = {2026}
}

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14 pages