高温下混合自旋铁磁体的相变

Intesar A Obaid, Shakir D. Al-Saeedi, H. Mohamad
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引用次数: 0

摘要

本文基于具有不同磁场的铁磁混合自旋-3和自旋-5/2 Blume-Capel模型的Gibbs-Bogoliubov自由能函数,研究了分子平均场理论(MMFT)。利用试哈密顿算符计算了所提出的铁磁体的自由能。将自由能最小化,可以分别在低温范围内诱导出纵向磁化、相变和自旋补偿温度的特征。特别地,我们研究了晶体场域对所提出模型的关键现象的影响。讨论了自由能函数与亚晶格磁化强度的关系。我们的结果预测了简单立方晶格的无序Blume-Capel - Ising系统中存在多个自旋补偿位。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Phase transitions of a mixed spin ferrimagnet in high temperatures
In this research paper molecular mean field theory (MMFT) has been investigated based on Gibbs-Bogoliubov free energy function of a ferromagnetic mixed spin-3 and spin-5/2 Blume-Capel model with different magnetic crystal fields. The free energy of the proposed ferrimagnet has been evaluated depending on the trial Hamiltonian operator. Minimizing the free energy, one may induce characteristic features of the longitudinal magnetizations, phase transitions and spin compensation temperatures, in the ranges of low temperatures, respectively. In particular, we study the effect of crystal field domains on the critical phenomena for the proposed model. The sublattice magnetization dependence of freerenergy function has been discussed as well. Our results predict the existence of multiple spin compensation sites in the disordered Blume-Capel Ising system for a simple cubic lattice.
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