二维ising方形晶格中的反相现象

Y. B. Sitamtze, S. Zekeng, J. Ndjaka, S. Domngang
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引用次数: 0

摘要

对二维Ising模型进行了蒙特卡罗模拟,以确定反相边界(APBs)对系统某些热力学函数的影响。我们考虑了几种晶格尺寸,有时在同一晶格中铁磁(FM)和反铁磁(AFM)相互作用。对所得曲线的分析表明,apb只出现在AFM相互作用中,其作用是产生能隙,阻止系统达到基态。这只发生在线性大小为奇数L (L = 9,15,31…)的格中。然而,这些边界并没有改变反铁磁/顺磁(AFM/PARA)相变的临界温度,大约保持在2.26(单位J/kB)。然而,它们在比热曲线上施加了一种作为温度函数的抖动行为,并且没有明显的峰值,这与均匀L (L = 16,20,48,…)的情况相反,其中有一个明显的峰值和光滑的曲线。在低温(AFM相位)时,在零值附近也存在波动的磁化强度。我们表明,这个能隙与1/L成正比,其中L是晶格的线性大小,因此,如果L变高,这个能隙应该消失。在一些晶体结构中,特别是在由Ising模型描述的二元合金中,APB所起的作用与之相似。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Antiphase phenomena in 2d ising square lattice
Monte Carlo simulations of the two dimensional Ising model were carried out to determine the impact of Antiphase Boundaries (APBs) in some thermodynamic functions of the system. We considered several lattice sizes and sometimes both Ferromagnetic (FM) and Antiferromagnetic (AFM) interactions for the same lattice. The analysis of the curves obtained shows that APBs appears only in AFM interaction and their effect is the creation of an energy gap that prevents the system from reaching the ground state. This happens only in lattices with odd linear size L (L = 9, 15, 31 …). However, these boundaries do not change the critical temperature of the Antiferromagnetic/Paramagnetic (AFM/PARA) phase transition which remains approximately at 2.26 (in unit of J/kB). Nevertheless, they impose on the curve of the specific heat a jittery behaviour as a function of the temperature and with no clear peak as opposed to the case of even L (L = 16 ,20, 48,…) where there is a clear peak and a smooth curve. There is also a fluctuating magnetization around the value zero at low temperature (AFM phase). We show that this energy gap is proportional to 1/L where L is the linear size of the lattice, thus this gap should vanish if L becomes high. A similarity has been established with the role played by APB in some crystal structures and more especially in the binary alloys that are moreover described by the Ising model.
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