Slow Convergence of Ising and Spin Glass Models with Well-Separated Frustrated Vertices

D. Gillman, Dana Randall
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Abstract

Many physical models undergo phase transitions as some parameter of the system is varied. This phenomenon has bearing on the convergence times for local Markov chains walking among the configurations of the physical system. One of the most basic examples of this phenomenon is the ferromagnetic Ising model on an n× n square lattice region Λ with mixed boundary conditions. For this spin system, if we fix the spins on the top and bottom sides of the square to be + and the left and right sides to be −, a standard Peierls argument based on energy shows that below some critical temperature tc, any local Markov chainM requires time exponential in n to mix. Spin glasses are magnetic alloys that generalize the Ising model by specifying the strength of nearest neighbor interactions on the lattice, including whether they are ferromagnetic or antiferromagnetic. Whenever a face of the lattice is bounded by an odd number of edges with ferromagnetic interactions, the face is considered frustrated because the local competing objectives cannot be simultaneously satisfied. We consider spin glasses with exactly four well-separated frustrated faces that are symmetric around the center of the lattice region under 90 degree rotations. We show that local Markov chains require exponential time for all spin glasses in this class. This class includes the ferromagnetic Ising model with mixed boundary conditions described above, where the frustrated faces are on the boundary. The standard Peierls argument breaks down when the frustrated faces are on the interior of Λ and yields weaker results when they are on the boundary of Λ but not near the corners. We show that there is a universal temperature T below which M will be slow for all spin glasses with four well-separated frustrated faces. Our argument shows that there is an exponentially small cut indicated by the free energy, carefully exploiting both entropy and energy to establish a small bottleneck in the state space to establish slow mixing. 2012 ACM Subject Classification Theory of computation→ Random walks and Markov chains
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具有良好分离挫折顶点的Ising和Spin Glass模型的慢收敛性
随着系统某些参数的变化,许多物理模型都会发生相变。这一现象与局部马尔可夫链在物理系统各构型间行走的收敛时间有关。这种现象的一个最基本的例子是在nxn方形晶格区域Λ上具有混合边界条件的铁磁Ising模型。对于这个自旋系统,如果我们将正方形的上下两侧的自旋固定为+,左右两侧固定为-,基于能量的标准佩尔斯论证表明,在某个临界温度tc以下,任何局部马尔可夫链m都需要n的时间指数才能混合。自旋玻璃是一种磁性合金,它通过指定晶格上最近邻相互作用的强度来推广Ising模型,包括它们是铁磁的还是反铁磁的。当晶格的一个面被奇数个具有铁磁相互作用的边所包围时,由于局部竞争目标不能同时得到满足,该面被认为是受挫面。我们考虑在90度旋转下,具有四个完全分开的受挫面围绕晶格区域中心对称的自旋玻璃。我们证明了局部马尔可夫链对所有自旋玻璃都需要指数时间。这一类包括上述具有混合边界条件的铁磁Ising模型,其中受挫面位于边界上。当挫折面位于Λ的内部时,标准的佩尔斯论证就失效了,当挫折面位于Λ的边界但不靠近拐角时,得出的结果较弱。我们证明存在一个通用温度T,低于此温度M对于所有具有四个分离良好的受挫面的自旋玻璃都是缓慢的。我们的论证表明,存在一个指数级的小切割,由自由能表示,仔细利用熵和能量在状态空间中建立一个小瓶颈,以建立缓慢混合。2012 ACM学科分类计算理论→随机行走与马尔可夫链
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