无序BCC FeCo合金LCAO-CPA的自旋极化电子结构

R. Richter, H. Eschrig
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引用次数: 39

摘要

将LCAO-CPA理论应用于取代无序铁磁BCC FeCo合金。计算是基于在局部自旋密度泛函理论下确定的纯组分金属的电荷和自旋自洽LCAO参数。对电荷和自旋一致性对合金磁化性能的影响进行了研究。解释了局部磁矩浓度依赖性的决定机制。讨论了磁矩形成与局部电荷中性保持的关系。在Fe位点上,自旋子带内杂化驱动的局部重占增强了交换分裂。这导致观察到的铁矩增加了约30%。给出了饱和磁化强度、局部磁矩、d带密度和比热系数随浓度变化的数值结果。定性结果与现有实验数据一致。给出了态的总密度和组分密度与浓度关系的数值结果。这两种自旋态的无序程度大不相同。大多数自旋态为典型的刚性带状,而合金无序性对少数自旋态的影响较大。这导致了少数自旋布洛赫谱函数和费米表面的强烈展宽。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Spin-polarised electronic structure of disordered BCC FeCo alloys from LCAO-CPA
LCAO-CPA theory is applied to substitutionally disordered ferromagnetic BCC FeCo alloys. Calculations are based on charge and spin self-consistent LCAO parameters determined for the pure component metals within the local spin density functional theory. Effects of charge and spin self-consistency on the alloy magnetisation are treated in an ad hoc manner. Mechanisms determining the concentration dependence of the local magnetic moments are explained. The correlation of magnetic moment formation and maintenance of local charge neutrality is discussed. At Fe sites the exchange splitting is enhanced by a hybridisation-driven local reoccupation within the spin sub-bands. This causes the observed increase of the Fe moment by about 30%. Numerical results are presented for the saturation magnetisation, local magnetic moments, d-band population and specific heat coefficient as functions of concentration. Qualitative agreement was obtained with available experimental data. Numerical results for the concentration dependence of the total and component density of states are shown. Quite different degrees of disorder are found for both spin states. The majority spin states are typical rigid-band-like, whereas a strong influence of alloy disorder on the minority spin states is observed. This causes a strong broadening of the minority spin Bloch spectral functions and Fermi surface.
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