自旋冰

M. Gingras
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引用次数: 86

摘要

几何挫折通常出现在包含磁矩(自旋)的系统中,这些磁矩(自旋)位于由基本三角形或四面体单元组成的晶格的位置上,并通过反铁磁最近邻交换相互作用。尽管不太常见,但几何挫折也可能出现在具有强非共线单离子易轴各向异性和铁磁耦合自旋的系统中。这是发生在一些焦绿盐氧化物材料中的情况,其中类似伊辛的磁性稀土矩(Ho, Dy)位于角共享四面体的晶格上,并通过有效的铁磁(偶极)相互作用耦合。这些系统具有宏观数量的准简并经典基态,并显示出与普通水冰中质子无序熵密切相关的广泛低温熵。由于这个原因,这些磁系统被称为自旋冰。本章综述了磁性焦绿盐氧化物中自旋冰现象学的基本成分。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
SPIN ICE
Geometric frustration usually arises in systems that comprise magnetic moments (spins) which reside on the sites of a lattice made up of elementary triangular or tetrahedral units and which interact via antiferromagnetic nearest-neighbor exchange. Albeit much less common, geometric frustration can also arise in systems with strong non-collinear single-ion easy-axis (Ising-like) anisotropy and ferromagnetically coupled spins. This is what happens in some pyrochlore oxide materials where Ising-like magnetic rare earth moments (Ho, Dy) sit on a lattice of corner-shared tetrahedra and are coupled via effectively ferromagnetic (dipolar) interactions. These systems possess a macroscopic number of quasi-degenerate classical ground states and display an extensive low-temperature entropy closely related to the extensive proton disorder entropy in common water ice. For this reason, these magnetic systems are called spin ice. This chapter reviews the essential ingredients of spin ice phenomenology in magnetic pyrochlore oxides.
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