in /sub 0.66/Ga/sub 0.33/As/ in /sub 0.66/Ga/sub 0.33/As/sub 0.7/P/sub 0.3/量子阱结构中的V族相互扩散

W. Gillin, I. Bradley, W. L. Foo, K. Homewood, S. Perrin, P.C. Spurdens
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引用次数: 0

摘要

利用n = 1电子到重空穴跃迁的光致发光,测定了in /sub 0.66/Ga/sub 0.33/ as / in /sub 0.66/Ga/sub 0.33/ as /sub 0.7/P/sub 0.3/应变量子阱中砷和磷的相互扩散系数随温度的变化。作者利用in /sub 0.66/Ga/sub 0.33/As在in /sub 0.66/Ga/sub 0.33/As/sub 0.7/P/sub 0.3/势垒中100/spl Aring/单量子阱的光致发光位移与退火来监测相互扩散。在该体系中,没有浓度梯度驱动III族相互扩散,因此光致发光跃迁能的变化仅使用模型中的磷/砷相互扩散来建模。通过对单个样品进行多次退火并测量每次退火后光致发光的位移,监测相互扩散作为时间的函数。在900和700之间,扩散系数D可以用关系式D = D/sub o/exp(-E/sub A//kT)来描述,其中D/sub o/ = 507 cm/sup 2//s, E/sub A/ = 3.9 eV。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Group V interdiffusion in In/sub 0.66/Ga/sub 0.33/As/ In/sub 0.66/Ga/sub 0.33/As/sub 0.7/P/sub 0.3/ quantum well structures
The diffusion coefficient for arsenic and phosphorous interdiffusion has been measured as a function of temperature in In/sub 0.66/Ga/sub 0.33/As/ In/sub 0.66/Ga/sub 0.33/As/sub 0.7/P/sub 0.3/ strained quantum wells, using the photoluminescence from the n = 1 electron to heavy hole transition. The authors have used the shift in the photoluminescence from a 100/spl Aring/ single quantum well of In/sub 0.66/Ga/sub 0.33/As in In/sub 0.66/Ga/sub 0.33/As/sub 0.7/P/sub 0.3/ barriers with annealing to monitor the interdiffusion. In this system there is no concentration gradient to drive group III interdiffusion and therefore the variation in the photoluminescence transition energy was modeled using only phosphorous/arsenic interdiffusion in the model. By performing several anneals to a single sample and measuring the shift in the photoluminescence after each anneal the interdiffusion was monitored as a function of time. Between temperatures of 900/spl deg/C and 700/spl deg/C the diffusion coefficient, D, can be described using the relationship D = D/sub o/exp(-E/sub A//kT) where D/sub o/ = 507 cm/sup 2//s and E/sub A/ = 3.9 eV.<>
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