Spin Covariance Fluctuations in the SK Model at High Temperature

Fuente: arXiv
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Auteurs principaux: Brennecke, Christian, Schertzer, Adrien, Van Dam, Chen
Format: Preprint
Publié: 2024
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_version_ 1866913335762485248
author Brennecke, Christian
Schertzer, Adrien
Van Dam, Chen
author_facet Brennecke, Christian
Schertzer, Adrien
Van Dam, Chen
contents Based on \cite{H}, it is well known that the rescaled two point correlation functions \[ \sqrt{N} \langle σ_i ; σ_j\rangle = \sqrt{N} \big( \langle σ_i σ_j\rangle -\langle σ_i\rangle \langle σ_j\rangle\big) \] in the Sherrington-Kirkpatrick spin glass model with non-zero external field admit at sufficiently high temperature an explicit non-Gaussian distributional limit as $N\to \infty$. Inspired by recent results from \cite{ABSY, BSXY, BXY}, we provide a novel proof of the distributional convergence which is based on expanding $\langle σ_i ; σ_j\rangle$ into a sum over suitable weights of self-avoiding paths from vertex $i$ to $j$. Compared to \cite{H}, our key observation is that the path representation of $\langle σ_i ; σ_j\rangle$ provides a direct explanation of the specific form of the limiting distribution of $\sqrt{N} \langle σ_i ; σ_j\rangle$.
format Preprint
id arxiv_https___arxiv_org_abs_2404_19122
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Spin Covariance Fluctuations in the SK Model at High Temperature
Brennecke, Christian
Schertzer, Adrien
Van Dam, Chen
Probability
Mathematical Physics
82D30, 60F05
Based on \cite{H}, it is well known that the rescaled two point correlation functions \[ \sqrt{N} \langle σ_i ; σ_j\rangle = \sqrt{N} \big( \langle σ_i σ_j\rangle -\langle σ_i\rangle \langle σ_j\rangle\big) \] in the Sherrington-Kirkpatrick spin glass model with non-zero external field admit at sufficiently high temperature an explicit non-Gaussian distributional limit as $N\to \infty$. Inspired by recent results from \cite{ABSY, BSXY, BXY}, we provide a novel proof of the distributional convergence which is based on expanding $\langle σ_i ; σ_j\rangle$ into a sum over suitable weights of self-avoiding paths from vertex $i$ to $j$. Compared to \cite{H}, our key observation is that the path representation of $\langle σ_i ; σ_j\rangle$ provides a direct explanation of the specific form of the limiting distribution of $\sqrt{N} \langle σ_i ; σ_j\rangle$.
title Spin Covariance Fluctuations in the SK Model at High Temperature
topic Probability
Mathematical Physics
82D30, 60F05
url https://arxiv.org/abs/2404.19122