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首页> 外文期刊>Physical Review, B. Condensed Matter >Electronic structure, magnetic ordering, and optical properties of GaN and GaAs doped with Mn - art. no. 045203
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Electronic structure, magnetic ordering, and optical properties of GaN and GaAs doped with Mn - art. no. 045203

机译:掺杂Mn的GaN和GaAs的电子结构,磁有序性和光学性质-艺术。没有。 045203

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摘要

The electronic structure and the properties of superdoped GaN(As):Mn (a concentration of Mn from 1.56% to 12.5%) are studied by using the tight-binding linear-muffin-tin-orbital method. Calculations show that the ferromagnetic state is lower in energy than the paramagnetic and antiferromagnetic states for both materials GaN:Mn and GaAs:Mn with all Mn concentrations. At the Fermi energy electronic states are 100% spin polarized, excluding GaAs:Mn with 12.5% of Mn. The most important difference between two materials concerns the energy position and localization of the Mn spin-majority states. In GaN these impurity states lie inside the fundamental gap and are well localized. In GaAs they are positioned near the top of the valence band and are strongly hybridized with it. This difference is clearly seen in the calculated magnetic, optical and, especially, kinetic properties of these materials, which are significantly different. Our investigation of codoping in GaN:Mn (substitution of O for N or Zn for Ga) shows that the atoms of O and Zn change the occupation of Mn bands and strongly affect both magnetic moments and conductivity. [References: 23]
机译:采用紧密结合的线性松饼-锡-轨道法研究了GaN(As):Mn(Mn的浓度为1.56%至12.5%)的电子结构和性能。计算表明,对于具有所有Mn浓度的GaN:Mn和GaAs:Mn两种材料,铁磁态的能量均低于顺磁和反铁磁态。在费米能量处,电子状态为100%自旋极化,不包括具有12.5%Mn的GaAs:Mn。两种材料之间最重要的区别在于Mn自旋多数状态的能量位置和局部化。在GaN中,这些杂质态位于基极间隙内,并且位置很好。在砷化镓中,它们位于价带的顶部附近并与之强烈杂交。在计算得出的这些材料的磁,光学,尤其是动力学特性中,可以明显看出这种差异,它们之间存在显着差异。我们对GaN:Mn(N取代O或Ga取代锌)的共掺杂研究表明,O和Zn原子改变了Mn带的占有率,并强烈影响磁矩和电导率。 [参考:23]

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