未屏蔽Anderson晶格模型的竞争反铁磁相(应邀)

A. C. Lausmann, E. Calegari, S. Magalhães, P. Riseborough
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引用次数: 0

摘要

我们研究了近半填充5f带的下屏蔽安德森晶格模型(UALM)的磁相,并发现了两个不同磁相之间的竞争。我们考虑的UALM版本由两个相关的5f带组成,在顺磁状态下,它们与单个导带杂交。在nsamel温度下,顺磁态经历了向反铁磁有序态的二阶跃迁,其中nsamel序参量引起了具有不同5f特征的态之间的混合。当施加压力时,有一条一阶转换线将两个nsamel阶段分开。此外,随着压力的增加,nsamel温度降低,就好像系统被推向量子临界点一样。然而,在尼尔温度达到绝对零度之前,顺磁不稳定性的性质由二阶变为一阶。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Competing antiferromagnetic phases of the under-screened Anderson lattice model (INVITED)
We investigate the magnetic phases of the Under-screened Anderson Lattice Model (UALM) for nearly half-filled 5f bands and find a competition between two distinct magnetic phases. The version of the UALM that we consider consists of two correlated 5f bands that, in the paramagnetic state, hybridize with a single conduction band. At the Néel temperature, the paramagnetic state undergoes a second-order transition to antiferromagnetically ordered states, in which the Néel order parameter induces a mixing between the states with different 5f characters. As pressure is applied, there is a line of first-order transitions that separates two Néel phases. Furthermore, as the pressure is increased, the Néel temperature decreases as if the system is being driven towards a quantum critical point. However, the nature of the paramagnetic instability changes from second-order to first-order before the Neel temperature reaches absolute zero.
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