首页> 外文期刊>Journal of Applied Physics >Subband characteristics of Si δ-doped pseudomorphic In_(0.2)Ga_(0.8)As/GaAs heterostructures
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Subband characteristics of Si δ-doped pseudomorphic In_(0.2)Ga_(0.8)As/GaAs heterostructures

机译:Si δ掺杂假晶In_(0.2)Ga_(0.8)As/GaAs异质结构的子带特性

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摘要

Subband properties of Si δ-doped pseudomorphic In_(0.2)Ga_(0.8)As/GaAs heterostructures have been investigated by solving the Schrodinger-Kohn-Sham equation and the Poission equation self-consistently, and by the density-density dynamical response function. Different δ-doping configurations, in which the same Si δ-doped layer is placed at different positions with respect to the In_(0.2)Ga_(0.8)As well, have been studied to find their effect on subband electron densities and mobilities. High electron densities of greater than 3.6×10~(12) cm~(-2) are obtained when a δ-doping density of 4.5×10~(12)cm~(-2) is placed at the well center or at the well-barrier interface. However, the electron density in the well for Si δ-modulation-doped In_(0.2)Ga_(0.8)As/GaAs heterostructure is only about 1.3×10~(12)cm~(-2). The change of the position of a Si δ-doped layer from the well center to the barrier does not change the mobility of electrons in the lowest subband significantly. The Si δ doping in both barriers leads to an increase of the electron density by almost a factor of 2. The mobilities in the well for the modulation-doped structures are always much greater than those for the well-doped structures. The calculated results are also compared to the corresponding experimental data.
机译:通过自洽求解薛定谔-Kohn-Sham方程和泊松方程,利用密度-密度动态响应函数,研究了Si掺杂δ假晶In_(0.2)Ga_(0.8)As/GaAs异质结构的子带性质.研究了不同的δ掺杂构型,其中相同的Si δ掺杂层相对于In_(0.2)Ga_(0.8)放置在不同的位置,以发现它们对子带电子密度和迁移率的影响。当δ掺杂密度为4.5×10~(12)cm~(-2)时,在阱中心或阱势界面处放置掺杂密度大于3.610~(12)cm~(-2)时,电子密度大于3.6×10~(12) cm~(-2)。然而,Si δ调制掺杂In_(0.2)Ga_(0.8)As/GaAs异质结阱内的电子密度仅为约1.3×10~(12)cm~(-2)。Si掺δ层的位置从阱中心到势垒的变化不会显着改变电子在最低子带中的迁移率。两个势垒中的Si δ掺杂导致电子密度增加近2倍。调制掺杂结构在阱中的迁移率总是远大于掺杂良好结构的迁移率。计算结果还与相应的实验数据进行了比较。

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