Toward mean-field bound for critical temperature on Nishimori line

Fuente: arXiv
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Main Authors: Okuyama, Manaka, Ohzeki, Masayuki
Format: Preprint
Published: 2024
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author Okuyama, Manaka
Ohzeki, Masayuki
author_facet Okuyama, Manaka
Ohzeki, Masayuki
contents The critical inverse temperature of the mean-field approximation establishes a lower bound of the true critical inverse temperature in a broad class of ferromagnetic spin models. This is referred to as the mean-field bound for the critical temperature. In this study, we explored the possibility of a corresponding mean-field bound for the critical temperature in Ising spin glass models with Gaussian randomness on the Nishimori line. On this line, the critical inverse temperature of the mean-field approximation is given by $β_{MF}^{NL}=\sqrt{1/z}$, where $z$ is the coordination number. Using the Griffiths inequalities on the Nishimori line, we proved that there is zero spontaneous magnetization in the high-temperature region $β< β_{MF}^{NL}/2$. In other words, the true critical inverse temperature $β_c^{NL}$ on the Nishimori line is always bounded by $β_c^{NL} \ge β_{MF}^{NL}/2$. Unfortunately, we have not succeeded in obtaining the corresponding mean-field bound $β_c^{NL} \ge β_{MF}^{NL}$ on the Nishimori line.
format Preprint
id arxiv_https___arxiv_org_abs_2406_12728
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Toward mean-field bound for critical temperature on Nishimori line
Okuyama, Manaka
Ohzeki, Masayuki
Disordered Systems and Neural Networks
Statistical Mechanics
The critical inverse temperature of the mean-field approximation establishes a lower bound of the true critical inverse temperature in a broad class of ferromagnetic spin models. This is referred to as the mean-field bound for the critical temperature. In this study, we explored the possibility of a corresponding mean-field bound for the critical temperature in Ising spin glass models with Gaussian randomness on the Nishimori line. On this line, the critical inverse temperature of the mean-field approximation is given by $β_{MF}^{NL}=\sqrt{1/z}$, where $z$ is the coordination number. Using the Griffiths inequalities on the Nishimori line, we proved that there is zero spontaneous magnetization in the high-temperature region $β< β_{MF}^{NL}/2$. In other words, the true critical inverse temperature $β_c^{NL}$ on the Nishimori line is always bounded by $β_c^{NL} \ge β_{MF}^{NL}/2$. Unfortunately, we have not succeeded in obtaining the corresponding mean-field bound $β_c^{NL} \ge β_{MF}^{NL}$ on the Nishimori line.
title Toward mean-field bound for critical temperature on Nishimori line
topic Disordered Systems and Neural Networks
Statistical Mechanics
url https://arxiv.org/abs/2406.12728