Monte-Carlo simulation of phase transition in 2D and 3D ising model

Rajendra Neupane, Hari Ram Krishna Gauli, K. B. Rai, Karan Giri
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Abstract

In this work, Markov Chain-Monte Carlo technique was used to study the phase transition in two and three dimensional Ising Model (IM) in a square and cubic lattice. The study of temperature dependence of average magnetization and specific heat in different magnetic fields has been carried out in the 3x3 and 3x3x3 lattice with periodic boundary. Critical temperature point kBTc / J for 2D and 3D Ising Model has been observed at around 2.2 and 4.3 respectively at zero field. Our work satisfies Onsager’s critical value in 2D IM. The simulation suggests bifurcation in average magnetization below critical temperature Tc. Temperature plays the role of increasing randomness of spins. We found that Ising Model in small lattice size still retains interesting features like spontaneous magnetization and symmetry breaking below Tc at B = 0. At a non-zero field, the likelihood of spins to prefer certain alignment depends on the direction of the external field and magnitude of magnetization depends on magnitude of field ±B. Specific heat Cv, which gives us fluctuation of energy at particular temperature, has been found to attain maximum value at critical regions.
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二维和三维ising模型中相变的蒙特卡罗模拟
本文采用马尔可夫链-蒙特卡罗方法研究了二维和三维二维伊辛模型(IM)在方形和立方晶格中的相变。在具有周期边界的3x3和3x3x3晶格中,研究了不同磁场下平均磁化强度和比热的温度依赖性。在零场条件下,二维和三维Ising模型的临界温度点kBTc / J分别约为2.2和4.3。我们的工作满足了Onsager在2D IM中的临界值。模拟结果表明,在临界温度Tc以下,平均磁化强度出现分叉。温度起着增加自旋随机性的作用。我们发现小晶格尺寸的Ising模型在B = 0时仍然保留了自发磁化和对称性破缺等有趣特征。在非零场中,自旋倾向于某种排列的可能性取决于外场的方向,磁化强度取决于场的大小±B。比热Cv是指在特定温度下能量的波动,它在临界区域达到最大值。
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