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自旋玻璃中的小场混沌:来自超度量树的通用预测及与数值模拟的比较。

Small field chaos in spin glasses: Universal predictions from the ultrametric tree and comparison with numerical simulations.

作者信息

Aguilar-Janita Miguel, Franz Silvio, Martin-Mayor Victor, Moreno-Gordo Javier, Parisi Giorgio, Ricci-Tersenghi Federico, Ruiz-Lorenzo Juan J

机构信息

Departamento de Matematica Aplicada, Ciencia e Ingeniería de los Materiales y Tecnológia Electrónica, Complex Systems Group, Universidad Rey Juan Carlos, Móstoles, Madrid 28933, Spain.

Laboratoire de Physique Théorique et Modèles Statistiques, CNRS, Université Paris-Sud, Université Paris-Saclay, 91405 Orsay, France.

出版信息

Proc Natl Acad Sci U S A. 2024 Oct;121(40):e2404973121. doi: 10.1073/pnas.2404973121. Epub 2024 Sep 20.

DOI:10.1073/pnas.2404973121
PMID:39302998
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11459185/
Abstract

Replica symmetry breaking (RSB) for spin glasses predicts that the equilibrium configuration at two different magnetic fields are maximally decorrelated. We show that this theory presents quantitative predictions for this chaotic behavior under the application of a external magnetic field, in the crossover region where the field intensity scales proportionally to [Formula: see text], being the system size. We show that RSB theory provides universal predictions for chaotic behavior: They depend only on the zero-field overlap probability function [Formula: see text] and are independent of other system features. In the infinite volume limit, each spin-glass sample is characterized by an infinite number of states that have a tree-like structure. We generate the corresponding probability distribution through efficient sampling using a representation based on the Bolthausen-Sznitman coalescent. Using solely [Formula: see text] as input we can analytically compute the statistics of the states in the region of vanishing magnetic field. In this way, we can compute the overlap probability distribution in the presence of a small vanishing field and the increase of chaoticity when increasing the field. To test our computations, we have simulated the Bethe lattice spin glass and the 4D Edwards-Anderson model, finding in both cases excellent agreement with the universal predictions.

摘要

自旋玻璃的副本对称性破缺(RSB)预测,在两个不同磁场下的平衡构型是最大程度不相关的。我们表明,该理论针对外部磁场作用下这种混沌行为给出了定量预测,该磁场处于场强与[公式:见原文]成比例缩放的交叉区域,其中[公式:见原文]为系统大小。我们表明,RSB理论为混沌行为提供了通用预测:它们仅取决于零场重叠概率函数[公式:见原文],且与其他系统特征无关。在无限体积极限下,每个自旋玻璃样本由具有树状结构的无限多个状态表征。我们通过基于博尔托豪森 - 斯尼曼合并的表示法进行高效采样来生成相应的概率分布。仅将[公式:见原文]作为输入,我们就可以解析计算零磁场区域内状态的统计量。通过这种方式,我们可以计算存在小的消失场时的重叠概率分布以及场增加时混沌性的增强。为了检验我们的计算结果,我们模拟了贝塞晶格自旋玻璃和四维爱德华兹 - 安德森模型,在这两种情况下都发现与通用预测有极好的一致性。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/c274d3b02b69/pnas.2404973121fig07.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/4cc13effb2ef/pnas.2404973121fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/3c646d8e9808/pnas.2404973121fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/cc41ac2028b5/pnas.2404973121fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/ff2d2206776b/pnas.2404973121fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/6cd3d4ac4f76/pnas.2404973121fig05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/9707d42c8947/pnas.2404973121fig06.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/c274d3b02b69/pnas.2404973121fig07.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/4cc13effb2ef/pnas.2404973121fig01.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/3c646d8e9808/pnas.2404973121fig02.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/cc41ac2028b5/pnas.2404973121fig03.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/ff2d2206776b/pnas.2404973121fig04.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/6cd3d4ac4f76/pnas.2404973121fig05.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/9707d42c8947/pnas.2404973121fig06.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1ce1/11459185/c274d3b02b69/pnas.2404973121fig07.jpg

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