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首页> 外文期刊>Journal of Statistical Physics >LOW-TEMPERATURE PHASE DIAGRAMS OF QUANTUM LATTICE SYSTEMS .1. STABILITY FOR QUANTUM PERTURBATIONS OF CLASSICAL SYSTEMS WITH FINITELY-MANY GROUND STATES
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LOW-TEMPERATURE PHASE DIAGRAMS OF QUANTUM LATTICE SYSTEMS .1. STABILITY FOR QUANTUM PERTURBATIONS OF CLASSICAL SYSTEMS WITH FINITELY-MANY GROUND STATES

机译:量子晶格系统的低温相位图.1。具有有限多个基态的经典系统的量子扰动的稳定性

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摘要

Starting from classical lattice systems in d greater than or equal to 2 dimensions with a regular zero-temperature phase diagram, involving a finite number of periodic ground states, we prove that adding a small quantum perturbation and/or increasing the temperature produce only smooth deformations of their phase diagrams. The quantum perturbations can involve bosons or fermions and can be of infinite range but decaying exponentially fast with the size of the bonds. For fermions, the interactions must be given by monomials of even degree in creation and annihilation operators. Our methods can be applied to some anyonic systems as well. Our analysis is based on an extension of Pirogov-Sinai theory to contour expansions in d + 1 dimensions obtained by iteration of the Duhamel formula. [References: 37]
机译:从具有大于或等于2维的d的经典晶格系统开始,使用规则的零温度相图,涉及有限数量的周期性基态,我们证明,添加小的量子扰动和/或增加温度只会产生平滑的变形他们的相图。量子扰动可能涉及玻色子或费米子,并且可能处于无限范围,但随着键的大小呈指数衰减。对于费米子,相互作用必须由创造和an灭算子中均匀度的单项式给出。我们的方法也可以应用于某些非离子系统。我们的分析是基于Pirogov-Sinai理论的扩展,以通过Duhamel公式的迭代获得的d + 1维轮廓的扩展。 [参考:37]

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