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

Published 5 Mar 2026 in math.PR | (2603.05636v1)

Abstract: We consider the Sherrington--Kirkpatrick spin glass model with zero external field and at inverse temperature $β&gt;0$. Let FN(β)F_N(β) be the corresponding log-partition function. Under the assumption that cN:=N<sup>1/3(1βN<sup>2)c_N:=N<sup>{1/3}(1-β_N<sup>2) is bounded away from $0$, we prove that Var(FN(βN))=12log(1βN<sup>2)</sup>βN<sup>2/2</sup>+O(cN<sup>3/2).(F_N(β_N)) = - \frac{1}{2} \log (1-β_N<sup>2)</sup> -{β_N<sup>2}/{2}</sup> + O( c_N<sup>{-3/2}). As a consequence, we obtain Var(FN(1cN<sup>1/3))</sup>=16logN+O(1)(F_N(1-c N<sup>{-1/3}))</sup> = \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(β_N).

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