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

Partha S. Dey, Taegu Kang

Abstract

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

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

Abstract

We consider the Sherrington--Kirkpatrick spin glass model with zero external field and at inverse temperature . Let be the corresponding log-partition function. Under the assumption that is bounded away from , we prove that Var As a consequence, we obtain Var for any fixed constant . We also prove a Gaussian central limit theorem for the centered and scaled .
Paper Structure (11 sections, 15 theorems, 95 equations)

This paper contains 11 sections, 15 theorems, 95 equations.

Key Result

Theorem 1.1

Assume that the inverse temperature sequence $(\beta_N)_{N \geqslant 1}$ satisfies $\lim_{N\to\infty}\beta_N=1$ and Define the function for $\beta<1$. Then, the variance satisfies Moreover, we have the following distributional convergence for the free energy Here, $L$ is a finite constant depending on the sequence $(\beta_N)_{N \geqslant 1}$, $g\sim\mathop{\mathrm{N}}\nolimits(0,1)$ and $\math

Theorems & Definitions (26)

  • Theorem 1.1
  • Corollary 1.2
  • Remark 1
  • Remark 2
  • Lemma 1.3: Cha09
  • Lemma 1.4
  • Lemma 1.5: Tal1
  • Proposition 1.6
  • Corollary 2.1
  • proof
  • ...and 16 more