首页> 外文期刊>Applied Physics A: Materials Science & Processing >The influence of the 1st AlN and the 2nd GaN layers on properties of AlGaN/2nd AlN/2nd GaN/1st AlN/1st GaN structure
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The influence of the 1st AlN and the 2nd GaN layers on properties of AlGaN/2nd AlN/2nd GaN/1st AlN/1st GaN structure

机译:第一AlN和第二GaN层对AlGaN / 2ndAlN / 2ndGaN / 1stAlN / 1stGaN结构的性能的影响

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This is a theoretical study of the 1st AlN interlayer and the 2nd GaN layer on properties of the Al0.3Ga0.7N/2nd AlN/2nd GaN/1st AlN/1st GaN HEMT structure by self-consistently solving coupled Schrödinger and Poisson equations. Our calculation shows that by increasing the 1st AlN thickness from 1.0 nm to 3.0 nm, the 2DEG, which is originally confined totally in the 2nd channel, gradually decreases, begins to turn up and eventually concentrates in the 1st one. The total 2DEG (2DEG in both channels) sheet density increases nearly linearly with the increasing 1st AlN thickness. And the slope of the potential profile of the AlGaN changes with the 1st AlN thickness, causing the unusual dependence of the total 2DEG sheet density on the thickness of the AlGaN barrier. The variations of 2DEG distribution, the total 2DEG sheet density and the conduction band profiles as a function of the 2nd GaN thickness also have been discussed. Their physical mechanisms have been investigated on the basis of the surface state theory. And the confinement of 2DEG can be further enhanced by the double-AlN interlayer, compared with the InGaN back-barrier.
机译:这是关于Al 0.3 Ga 0.7 N / 2nd AlN / 2nd GaN / 1st AlN / 1st GaN性能的第一AlN中间层和第二GaN层的理论研究通过自洽地求解耦合的Schrödinger和Poisson方程来构造HEMT结构。我们的计算表明,通过将第一AlN厚度从1.0 nm增加到3.0 nm,最初完全限制在第二通道中的2DEG逐渐减小,开始出现并最终集中在第一通道中。总的2DEG(两个通道中均为2DEG)片材密度几乎随着第一AlN厚度的增加而线性增加。并且,AlGaN的电势轮廓的斜率随第一AlN厚度而变化,从而导致总的2DEG片密度与AlGaN势垒的厚度不寻常地相关。还讨论了2DEG分布,总2DEG片密度和导带分布随第二GaN厚度的变化。在表面状态理论的基础上研究了它们的物理机理。与InGaN背势垒相比,双AlN中间层可以进一步增强2DEG的限制。

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