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Carrier-mediated ferromagnetism in N co-doped (Zn, Mn)O-based diluted magnetic semiconductors

机译:N共掺杂的(Zn,Mn)O基稀磁半导体中的载流子介导的铁磁性

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摘要

Mn-doped ZnO is anti-ferromagnetic spin glass state, however, it becomes half-metallic ferromagnets upon hole doping. In this Letter we report a theoretical study of (Zn, Mn)O system codoped with N, and show that this codoping can change the ground state from anti-ferromagnetic to ferromagnetic. We have carried out the first-principles electronic structure calculations and report total energy to estimate whether the ferromagnetic state was stable or not. Our approach is based on the spin-polarized relativistic Korringa–Kohn–Rostoker (SPR–KKR) density functional theoretical (DFT) method, within the coherent potential approximation (CPA). Self-consistent electronic structure calculations were performed within the local density approximation, using the Vosko–Wilk–Nusair parameterization of the exchange-correlation energy functional. Our results for energy difference between ferromagnetic sate and spin glass state as well as their dependence on concentrations were presented and discussed.
机译:Mn掺杂的ZnO是反铁磁性的自旋玻璃态,但是,在掺杂空穴后它变成半金属铁磁体。在这封信中,我们报告了与N共掺杂的(Zn,Mn)O体系的理论研究,并表明这种共掺杂可以将基态从反铁磁变为铁磁。我们已经进行了第一性原理电子结构计算,并报告了总能量以估计铁磁状态是否稳定。我们的方法基于自旋极化的相对论性Korringa-Kohn-Rostoker(SPR-KKR)密度泛函理论(DFT)方法,并且处于相干势近似(CPA)之内。使用交换相关能量函数的Vosko-Wilk-Nusair参数化,在局部密度近似值范围内执行了自洽电子结构计算。提出并讨论了我们关于铁磁态和自旋玻璃态之间的能量差以及它们对浓度的依赖性的结果。

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