Ising链中的量子和热涨落:以自旋二系为例

S. Ehika, O. Ataman, S. Iyayi
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引用次数: 1

摘要

对于一个处于绝对零度的系统,所有的热涨落都被冻结了,而量子涨落则占上风。当两个相互竞争的能量项的相对强度在一个临界值上变化时,这些微观量子涨落可以在多体系统的基态中诱导量子相变(QPT)。本文详细、定量地研究了伊辛双自旋系统在零温度下,在纵向场、横向场和混合场以及有限温度下的磁性能。在临界纵向磁场下,发现系统经历了QPT到铁磁状态。对于该系统,发现横向场与零的无穷小偏差可以触发QPT,并且可以消除即使在纵向场存在的情况下仍然存在的简并。这些量子涨落导致QPT在混合场中比纵向场和横向场的单独效应更为明显。在有限温度下,由于热波动,该系统在零温度下观察到的量子效应被完全消除。温度升高有利于自旋的反铁磁排列,而温度降低有利于铁磁排列。
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Quantum and Thermal Fluctuations in the Ising Chains: A Case Study of Spin-Two System
For a system at absolute zero temperature, all thermal fluctuations are frozen out, while quantum fluctuations prevail. These microscopic quantum fluctuations can induce a quantum phase transition (QPT) in the ground state of a many-body system when the relative strength of two competing energy terms is varied across a critical value. This paper presents a detailed and quantitative study of the magnetic properties of Ising two-spin system at zero temperature in the presence of longitudinal, transverse and mixed fields, and also at finite temperatures. At the critical longitudinal magnetic field, the system is found to undergo a QPT to a ferromagnetic state. For this system, an infinitesimal departure from zero transverse field is found to trigger off QPT and also remove the degeneracies that persisted even in the presence of longitudinal field. These quantum fluctuations, leading to QPT are more evident in the mixed field than the separate effect of longitudinal and transverse fields. The observed quantum effects at zero temperature for this system are found to be completely wiped out at finite temperatures due to thermal fluctuations. A temperature increase favours antiferromagnetic alignment of spins, while a decrease in temperature favours ferromagnetic alignment.
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