从ab-initio型计算中得出的磁隧效应的各个方面

P. Weinberger, V. Drchal, J. Kudrnovský, I. Turek, H. Herper, L. Szunyogh, C. Sommers
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引用次数: 3

摘要

利用完全相对论性自旋极化屏蔽Korringa-Kohn-Rostoker方法和非相对论性自旋极化紧密结合线性松松锡轨道方法,在ab-initio水平上对真空分离的两个半无限铁磁电极之间的隧穿现象进行了理论研究。采用Kubo-Greenwood方程计算非局部电导率和层分解片材电阻;然后用传输矩阵公式来计算电导。我们表明,薄片电阻对费米能量虚部的依赖使我们能够区分电子传递的隧穿和导电机制。我们对bcc Fe(100)/真空/bcc Fe(100)体系的数值研究表明,真空区静电势的变化非常剧烈,并且随着真空势垒厚度的增加,隧道势垒逐渐发展。改变真空屏障内部的马德隆电位,使我们能够模拟由半导体或绝缘材料制成的间隔层,并讨论在这种多层材料中存在磁阻的条件。对于真空势垒厚度,用传输矩阵法计算fee Co(001)/vacuum/fee Co(001)的结果与Kubo-Greenwood方程计算bcc Fe(100)/vacuum/bcc Fe(100)的结果具有相似的趋势;渐近地,即随着真空势垒厚度的增加,磁电阻趋于零。
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Aspects of magnetotunnelling drawn from ab-initio-type calculations
Abstract Tunnelling between two semi-infinite ferromagnetic electrodes separated by vacuum is studied theoretically on an ab-initio level by using the fully relativistic spin-polarized screened Korringa-Kohn-Rostoker and the spin-polarized non-relativistic tight-binding linear muffin-tin orbital method. The Kubo-Greenwood equation is employed to calculate the non-local conductivity and layer-resolved sheet resistances; the transmission matrix formulation in turn is used to evaluate the conductance. We show that the dependence of sheet resistance on the imaginary part of the Fermi energy allows us to distinguish between the tunnelling and conductive regimes of electron transport. Our numerical studies of the system bcc Fe(100)/vacuum/bcc Fe(100) show quite dramatic variations in the electrostatic potential in the vacuum region and a gradual development of the tunnelling barrier with increasing thickness of the vacuum barrier. Varying the Madelung potential in the interior of the vacuum barrier allowed us to simulate spacers made of semiconducting or insulating material and to discuss the conditions for the presence of a magnetoresistance in such multilayers. As far as the thickness of the vacuum barrier is concerned the results obtained with the transmission matrix approach for fee Co(001)/vacuum/fee Co(001) show a similar tendency to those obtained within the Kubo-Greenwood equation for bcc Fe(100)/vacuum/bcc Fe(100); asymptotically, that is with increasing thickness of the vacuum barrier, the magnetoresistance tends to zero.
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