论文标题

在棋盘方面结构上混合自旋-1和自旋1/2 ising模型的磁性和相图:蒙特卡洛研究

Magnetic properties and phase diagrams of mixed spin-1 and spin-1/2 Ising model on a checkerboard square structure: A Monte Carlo study

论文作者

Gharaibeh, Maen, Badarneh, Mohammad H. A., Alqaiem, Samah, Obeidat, Abdalla, Qaseer, Mohammad-Khair

论文摘要

使用基于Metropolis更新协议的蒙特卡洛模拟研究了Checkboard Square结构上混合Spin-1和Spin-1/2 ISING模型的磁性和相图。该系统由替代旋转配置的四个四重奏组成。已经研究了交换相互作用J和晶体场D对磁性特性,临界和补偿温度,易感性以及系统的比热的影响。已经检查了用于交换相互作用和晶体场的不同值的相图T-J和T-D。我们发现,Spin-1组件的J1 <0.6的补偿温度开始演变,而J2> 1.6对于Spin-1/2。另一方面,铁磁耦合的效果不会显示任何阈值。在这种情况下,补偿温度是恒定的。关于晶体场强度,已经观察到d> -0.8的阈值。我们在系统中获得N-,Q-和P型补偿行为。我们已经观察到相图仅表现出二阶相变为顺磁相。因此,该系统没有显示三义点。已经发现了与交换相互作用,温度和晶体场的不同值的混合自旋-1和自旋1/2的磁性磁滞循环。最后,该系统表现出对温度和晶体场的固定值的超级磁性行为。

The magnetic properties and phase diagrams of the mixed spin-1 and spin-1/2 Ising model on a checkerboard square structure have been studied using the Monte Carlo simulations based on the Metropolis update protocol. The system consists of four quartets of alternative spin configuration. The effect of the exchange interactions J and crystal field D on the magnetic properties, critical and compensation temperatures, susceptibility, and specific heat of the system have been investigated. The phase diagrams, T-J and T-D, for different values of the exchange interactions and crystal field have been examined. We found that the compensation temperature starts to evolve for J1 < 0.6 of the spin-1 assembly and for J2 > 1.6 for spin-1/2. On the other hand, the effect of ferrimagnetic coupling does not show any threshold value; in this case, the compensation temperature is constant. Regarding the crystal field strength, the threshold value of D > -0.8 has been observed. We obtain the N-, Q- and P-type compensation behaviors in the system. We have observed that the phase diagrams exhibit only a second-order phase transition to a paramagnetic phase; hence, the system does not show the tricritical point. The magnetic hysteresis cycles of the mixed spin-1 and spin-1/2 on a checkerboard square structure for different values of the exchange interactions, temperatures, and crystal fields have been found. Finally, the system exhibits the superparamagnetism behavior for a fixed value of the temperature and crystal field.

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