{"title":"Parisi Formula for Balanced Potts Spin Glass","authors":"Erik Bates, Youngtak Sohn","doi":"10.1007/s00220-024-05100-9","DOIUrl":null,"url":null,"abstract":"<div><p>The Potts spin glass is a generalization of the Sherrington–Kirkpatrick (SK) model that allows for spins to take more than two values. Based on a novel synchronization mechanism, Panchenko (Ann Probab 46(2):829–864, 2018) showed that the limiting free energy is given by a Parisi-type variational formula. The functional order parameter in this formula is a probability measure on a monotone path in the space of positive-semidefinite matrices. By comparison, the order parameter for the SK model is much simpler: a probability measure on the unit interval. Nevertheless, a longstanding prediction by Elderfield and Sherrington (J Phys C Solid State Phys 16(15):L497–L503, 1983) is that the order parameter for the Potts spin glass can be reduced to that of the SK model. We prove this prediction for the balanced Potts spin glass, where the model is constrained so that the fraction of spins taking each value is asymptotically the same. It is generally believed that the limiting free energy of the balanced model is the same as that of the unconstrained model, in which case our results reduce the functional order parameter of Panchenko’s variational formula to probability measures on the unit interval. The intuitive reason—for both this belief and the Elderfield–Sherrington prediction—is that no spin value is a priori preferred over another, and the order parameter should reflect this inherent symmetry. This paper rigorously demonstrates how symmetry, when combined with synchronization, acts as the desired reduction mechanism. Our proof requires that we introduce a generalized Potts spin glass model with mixed higher-order interactions, which is interesting it its own right. We prove that the Parisi formula for this model is differentiable with respect to inverse temperatures. This is a key ingredient for guaranteeing the Ghirlanda–Guerra identities without perturbation, which then allow us to exploit symmetry and synchronization simultaneously.</p></div>","PeriodicalId":522,"journal":{"name":"Communications in Mathematical Physics","volume":"405 10","pages":""},"PeriodicalIF":2.2000,"publicationDate":"2024-09-13","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Communications in Mathematical Physics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s00220-024-05100-9","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
引用次数: 0
Abstract
The Potts spin glass is a generalization of the Sherrington–Kirkpatrick (SK) model that allows for spins to take more than two values. Based on a novel synchronization mechanism, Panchenko (Ann Probab 46(2):829–864, 2018) showed that the limiting free energy is given by a Parisi-type variational formula. The functional order parameter in this formula is a probability measure on a monotone path in the space of positive-semidefinite matrices. By comparison, the order parameter for the SK model is much simpler: a probability measure on the unit interval. Nevertheless, a longstanding prediction by Elderfield and Sherrington (J Phys C Solid State Phys 16(15):L497–L503, 1983) is that the order parameter for the Potts spin glass can be reduced to that of the SK model. We prove this prediction for the balanced Potts spin glass, where the model is constrained so that the fraction of spins taking each value is asymptotically the same. It is generally believed that the limiting free energy of the balanced model is the same as that of the unconstrained model, in which case our results reduce the functional order parameter of Panchenko’s variational formula to probability measures on the unit interval. The intuitive reason—for both this belief and the Elderfield–Sherrington prediction—is that no spin value is a priori preferred over another, and the order parameter should reflect this inherent symmetry. This paper rigorously demonstrates how symmetry, when combined with synchronization, acts as the desired reduction mechanism. Our proof requires that we introduce a generalized Potts spin glass model with mixed higher-order interactions, which is interesting it its own right. We prove that the Parisi formula for this model is differentiable with respect to inverse temperatures. This is a key ingredient for guaranteeing the Ghirlanda–Guerra identities without perturbation, which then allow us to exploit symmetry and synchronization simultaneously.
波茨自旋玻璃是谢林顿-柯克帕特里克(SK)模型的广义化,允许自旋取两个以上的值。基于一种新颖的同步机制,潘琴科(Ann Probab 46(2):829-864, 2018)证明,极限自由能是由一个巴黎式变分公式给出的。该公式中的函数阶参数是正半无限矩阵空间中单调路径上的概率度量。相比之下,SK 模型的阶次参数要简单得多:是单位区间上的概率度量。尽管如此,埃尔德菲尔德和谢林顿(J Phys C Solid State Phys 16(15):L497-L503, 1983)长期以来一直预言,波茨自旋玻璃的阶次参数可以简化为 SK 模型的阶次参数。我们为平衡波茨自旋玻璃证明了这一预言,在平衡波茨自旋玻璃中,模型受到约束,因此每个值的自旋分数渐近相同。一般认为,平衡模型的极限自由能与无约束模型的极限自由能相同,在这种情况下,我们的结果将潘琴科变分公式的功能阶参数简化为单位区间上的概率度量。这种观点和埃尔德菲尔德-谢林顿预言的直观原因是,没有任何自旋值是先验地优于另一个自旋值的,而阶参数应该反映这种固有的对称性。本文严谨地证明了对称性与同步性相结合是如何成为理想的还原机制的。我们的证明需要引入一个具有混合高阶相互作用的广义波茨自旋玻璃模型,这本身就很有趣。我们证明了该模型的帕里西公式在反温度方面是可微分的。这是保证吉尔兰达-格拉(Ghirlanda-Guerra)等式无扰动的关键要素,从而使我们能够同时利用对称性和同步性。
期刊介绍:
The mission of Communications in Mathematical Physics is to offer a high forum for works which are motivated by the vision and the challenges of modern physics and which at the same time meet the highest mathematical standards.