III-V型半导体的选择性面积生长:从基本方面到器件结构

M. Sugiyama
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引用次数: 4

摘要

本文介绍了III-V型半导体的选择性区金属-有机气相外延(MOVPE)的基本方面,重点介绍了iii族前驱体的气相扩散的作用,它在更宽(>100 μm)掩膜周围的有效带隙的实质调制中起主导作用,并且是MOVPE在接近大气压下工作的一个特征。一个参数D/ks(气相质量扩散系数/表面掺入率系数)决定了层的厚度和组成的调制。D/ks值可以看作是iii族前驱体的有效横向扩散长度,ks值可以与D/ks解耦,为研究MOVPE的表面反应动力学提供依据。与反应器尺度分布的耦合为综合反应机理的讨论提供了独特的依据。对于组成InGaAsP系统的基本材料,将给出k的值。基于简单的扩散/反应模型,可以精确地模拟给定掩模图案周围的多个量子阱(mqw)的发光波长,并且适用于使用ingaasp相关材料的选择性面积生长的单片集成器件。同样的框架可以应用于iii -氮化物材料,并获得了GaN生长的ks值。在有图案的GaN模板上,InGaN/GaN mqw发出的可见光根据掩膜宽度发生红移,其中只有InGaN阱的厚度调制被认为是控制机制。
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Selective area growth of III-V semiconductors: From fundamental aspects to device structures
Fundamental aspects in the selective-area metal-organic vapor-phase epitaxy (MOVPE) of III-V semiconductors are presented in this paper, with an emphasis on the role of vapor-phase diffusion of a group-III precursor, which plays the dominant role for substantial modulation of an effective bandgap around wider (>100 μm) masks and is a characteristic of MOVPE that is operated close to atmospheric pressure. A single parameter, D/ks (vapor-phase mass diffusivity / surface incorporation rate coefficient), determines modulation of both thickness and composition of a layer. The value of D/ks can be regarded as an effective lateral diffusion length of a group-III precursor, and the value of ks can be decoupled from D/ks, providing insight to surface reaction kinetics of MOVPE. Coupling with reactor-scale distributions provides unique basis for the discussion of comprehensive reaction mechanism. The values of ks will be presented for basic materials composing InGaAsP system. Luminescence wavelength from multiple quantum wells (MQWs) around a given mask pattern can be simulated precisely based on a simple diffusion/reaction model and it is applicable to monolithic integration of devices using selective-area growth of InGaAsP-related materials. The same framework can be applied to III-nitride materials, and ks values for GaN growth have been obtained. Visible luminescence from InGaN/GaN MQWs on a patterned GaN template was red-shifted according to the mask width, for which only the thickness modulation of the InGaN wells has been suggested to be the governing mechanism.
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