E. M. Jalal, H. Saadi, A. Hasnaoui, A. Lafhal, N. Hachem, M. El Bouziani
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引用次数: 0
摘要
摘要利用基于自由能波哥留波夫不等式的均场近似,我们研究了双二次交换相互作用对混合自旋(1,2)布卢姆-埃默里-格里菲斯模型的临界行为和相图的影响。我们首先关注模型的一种特殊情况:当相互作用参数 (K=0\)时,与布卢姆-卡佩尔模型相对应。对于有吸引力的布卢姆-埃默里-格里菲斯模型,我们给出了温度-晶体场平面上的相图。在 K 值较小的情况下,与 Blume-Capel 模型类似,相图呈现出一阶和二阶相变线,将有序相和无序相分开,三临界点标志着这些区域的边界。图文摘要在混合自旋-1 和自旋-2 布卢姆-卡佩尔模型上存在双四次方相互作用会产生一些重要现象;系统呈现不同的相变,即一阶、二阶和重入现象;确定了单离子各向异性和双四次方相互作用对磁化的影响;并与其他近似结果进行了讨论。
Critical and reentrant phenomena in the Blume–Emery–Griffiths model with attractive biquadratic interaction
Using the mean field approximation based on the Bogoliubov inequality for free energy, we investigate the effects of the biquadratic exchange interaction on the critical behavior and phase diagram of the mixed spin (1,2) Blume–Emery–Griffiths model. We first focus on a specific case of the model: when the interaction parameter \(K=0\), corresponding to the Blume–Capel model. For the attractive Blume–Emery–Griffiths model, we present the phase diagram in the temperature-crystal field plane. The phase diagram is significantly influenced by the value of the biquadratic exchange interaction K. For small values of K, similar to the Blume–Capel model, the phase diagram exhibits first and second order phase transition lines separating ordered and disordered phases, with a tricritical point marking the boundary between these regions. As K increases, the phase diagram changes significantly, with the appearance of reentrant and double reentrant phenomena.