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Effects of Crystal Structure and the On-Site Coulomb Interactions on the Electronic and Magnetic Structure of Pyrochlores $A_2$Mo$_2$O$_7$ (A= Y, Gd, and Nd)

机译:晶体结构和现场库仑相互作用对晶体的影响   pyrochlores的电子和磁性结构$ a_2 $ mo $ _2 $ O $ _7 $(a = Y,Gd,   和Nd)

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摘要

Being motivated by recent experimental studies, we investigate magneticstructures of the Mo pyrochlores $A_2$Mo$_2$O$_7$ ($A$= Y, Nd, and Gd) andtheir impact on the electronic properties. The latter are closely related withthe behavior of twelve Mo($t_{2g}$) bands, located near the Fermi level andwell separated from the rest of the spectrum. We use a mean-field Hartree-Fockapproach, which combines fine details of the electronic structure for thesebands, extracted from the conventional calculations in the local-densityapproximation, the spin-orbit interaction, and the on-site Coulomb interactionsamongst the Mo(4d) electrons, treated in the most general rotationallyinvariant form. The Coulomb repulsion U plays a very important role in theproblem, and the semi-empirical value U$\sim$1.5-2.5 eV accounts simultaneouslyfor the metal-insulator (M-I) transition, the ferromagnetic (FM) - spin-glass(SG) transition, and for the observed enhancement of the anomalous Hall effect(AHE). The M-I transition is mainly controlled by $U$. The magnetic structureat the metallic side is nearly collinear FM, due to the double exchangemechanism. The transition into the insulating state is accompanied by the largecanting of spin and orbital magnetic moments. The sign of exchange interactionsin the insulating state is controlled by the Mo-Mo distances. Smaller distancesfavor the antiferromagnetic coupling, which preludes the SG behavior in thefrustrated pyrochlore lattice. Large AHE is expected in the nearly collinear FMstate, near the point of M-I transition, and is related with the unquenchedorbital magnetization at the Mo sites. We also predict large magneto-opticaleffect in the same FM compounds.
机译:受近期实验研究的启发,我们研究了烧绿钼MoA的磁性结构$ A_2 $ Mo $ _2 $ O $ _7 $($ A $ = Y,Nd和Gd)及其对电子性能的影响。后者与十二个Mo($ t_ {2g} $)的行为密切相关,这些Mo($ t_ {2g} $)位于费米能级附近,并且与其余光谱区分开。我们使用平均场Hartree-Fockapproach方法,该方法结合了这些波段电子结构的精细细节,这些细节是从Mo(4d)之间的局部密度近似,自旋轨道相互作用和库仑相互作用的常规计算中提取的电子,以最一般的旋转不变形式处理。库仑斥力U在此问题中起着非常重要的作用,半经验值U $ \ sim $ 1.5-2.5 eV同时解释了金属-绝缘体(MI)过渡,铁磁(FM)-自旋玻璃(SG)过渡,并观察到异常霍尔效应(AHE)的增强。 M-I过渡主要由$ U $控制。由于双重交换机制,金属侧的磁性结构几乎是共线FM。向绝缘状态的过渡伴随着自旋和轨道磁矩的大幅度倾斜。绝缘状态下交换相互作用的符号由Mo-Mo距离控制。较小的距离有利于反铁磁耦合,从而阻止了在受阻的烧绿石晶格中的SG行为。在接近共线的FM态中,在M-1跃迁点附近,预计会有较大的AHE,这与Mo位置的非猝灭轨道磁化有关。我们还预测了相同FM化合物中的大磁光效应。

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    Solovyev, I. V.;

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  • 年度 2002
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