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首页> 外文期刊>The journal of physical chemistry, A. Molecules, spectroscopy, kinetics, environment, & general theory >Spin-Polarized Structural, Electronic, and Magnetic Properties of Diluted Magnetic Semiconductors Cd1-xMnxS and Cd1-xMnxSe in Zinc Blende Phase
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Spin-Polarized Structural, Electronic, and Magnetic Properties of Diluted Magnetic Semiconductors Cd1-xMnxS and Cd1-xMnxSe in Zinc Blende Phase

机译:锌共混相稀磁半导体Cd1-xMnxS和Cd1-xMnxSe的自旋极化结构,电子和磁性

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摘要

We studied the structural, spin-polarized electronic band structures, density of states, and magnetic properties of the diluted magnetic semiconductors (DMSs) Cd1-xMnxS and Cd1-xMnxSe in zinc blende phase (B3) with 25% Mn by using the ab initio method. The calculations were performed by using the full potential linearized augmented plane wave plus local orbitals (FP-L/APW+lo) method within the spin-polarized density functional theory and the local spin density approximation (LSDA). Calculated electronic band structures and the density of states of these DMSs are discussed in terms of the contribution of Mn 3d54s2, Cd 4d105s2, S 3s23p4, and Se 4s24p4 partial density of states and we also compute the local magnetic moments. We estimated the spinexchange splitting energies, Δx(d) and Δx(p-d), produced by the Mn 3d states, and we found that the effective potential for the minority spin is more attractive than that for the majority spin. We determine the s-d exchange constant N0R and p-d exchange constant N0, which resembles a typical magneto-optical experiment. The calculated total magnetic moment is found to be 5.0020 and 5.00013 μB for Cd1-xMnxS and Cd1-xMnxSe, respectively. These values indicate that every Mn impurity adds no hole carriers to the perfect CdS and CdSe crystals. Moreover, we found that p-d hybridization reduces the local magnetic moment of Mn from its free space charge value of 5.0μB and produces small local magnetic moments on the nonmagnetic Cd and S sites.
机译:我们使用从头算方法研究了含25%Mn的锌混合相(B3)中的稀磁半导体(DMS)Cd1-xMnxS和Cd1-xMnxSe的结构,自旋极化电子带结构,态密度和磁性能。方法。通过在自旋极化密度泛函理论和局部自旋密度近似(LSDA)中使用全势线性化增强平面波加局部轨道(FP-L / APW + lo)方法进行计算。根据Mn 3d54s2,Cd 4d105s2,S 3s23p4和Se 4s24p4的部分态态密度的贡献,讨论了这些DMS的计算出的电子能带结构和态密度。我们还计算了局部磁矩。我们估计了Mn 3d态产生的自旋交换分裂能Δx(d)和Δx(p-d),并且我们发现少数自旋的有效电势比多数自旋的有效电势更具吸引力。我们确定s-d交换常数N0R和p-d交换常数N0,这与典型的磁光实验相似。对于Cd1-xMnxS和Cd1-xMnxSe,计算出的总磁矩分别为5.0020和5.00013μB。这些值表明,每种Mn杂质均不会在理想的CdS和CdSe晶体中添加任何空穴载流子。此外,我们发现p-d杂化从Mn的自由空间电荷值5.0μB降低了Mn的局部磁矩,并在非磁性Cd和S位点产生了较小的局部磁矩。

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