一维非周期基态的非稳定性

IF 1.2 3区 物理与天体物理 Q3 PHYSICS, MATHEMATICAL
Damian Głodkowski, Jacek Miȩkisz
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引用次数: 0

摘要

我们讨论了经典晶格-气体模型中一维非周期基态构型在有限范围相互作用扰动下的稳定性问题。我们证明了在这种情况下基态构型的一个相关性质是它们的同质性。所谓严格边界条件是指在晶格的任何有限子集中,一个构型的有限模式的数目具有均匀的有界起伏 \(\mathbb Z\). 我们证明,如果不满足严格的边界条件,粒子之间的相互作用衰减速度至少与 \(1/r^{\alpha }\) 有 \(\alpha >2\),那么基态构型就不稳定。在Thue-Morse基态中,有限模式的数量波动可能与晶格子集长度的对数一样大。我们证明了在任何情况下都是不稳定的 \(\alpha >1\) 对于任意小的两体相互作用,倾向于由两个相邻的上下自旋组成的分子的存在。我们还研究了由圆上的非理性旋转所定义的Sturmian系统。它们满足严格的边界条件,但不稳定 \(\alpha >3\).
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On Non-stability of One-Dimensional Non-periodic Ground States

We address the problem of stability of one-dimensional non-periodic ground-state configurations in classical lattice-gas models with respect to finite-range perturbations of interactions. We show that a relevant property of ground-state configurations in this context is their homogeneity. The so-called strict boundary condition says that the number of finite patterns of a configuration has bounded fluctuations uniform in any finite subset of the lattice \(\mathbb Z\). We show that if the strict boundary condition is not satisfied and interactions between particles decay at least as fast as \(1/r^{\alpha }\) with \(\alpha >2\), then ground-state configurations are not stable. In the Thue–Morse ground state, the number of finite patterns may fluctuate as much as the logarithm of the length of a lattice subset. We show that the Thue–Morse ground state is unstable for any \(\alpha >1\) with respect to arbitrarily small two-body interactions favoring the presence of molecules consisting of two neighboring up or down spins. We also investigate Sturmian systems defined by irrational rotations on the circle. They satisfy the strict boundary condition but nevertheless they are unstable for \(\alpha >3\).

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来源期刊
Journal of Statistical Physics
Journal of Statistical Physics 物理-物理:数学物理
CiteScore
3.10
自引率
12.50%
发文量
152
审稿时长
3-6 weeks
期刊介绍: The Journal of Statistical Physics publishes original and invited review papers in all areas of statistical physics as well as in related fields concerned with collective phenomena in physical systems.
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