室温约束与HgCdTe多量子阱的光致发光

C. L. César, M.N. Islam, R. Feldman, R. Spitzer, R. F. Austin, A. DiGiovanni, J. Shah, J. Orenstein
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引用次数: 0

摘要

我们已经生长出了最低跃迁在3µm附近的HgCdTe/CdTe多量子阱(MQW),并且我们已经观察到室温约束和光致发光。不同成分的HgCdTe/CdTe MOW可以在整个红外范围内使用,因为材料在0到1.5 eV范围内是晶格匹配的。3µm区域的重要性来自于使用氟化物光纤运行的通信系统的可能性。用MBE生长MQW,用100 A的Hg0.15Cd0.85Te势垒和50 A的Hg0.73Cd0.27Te势垒生长50个周期(1)。透射电子显微镜(TEM)和x射线数据证实,层厚的互扩散很小,重现性很高。为了实现强约束,特别是对光孔,厚屏障是必要的。因此,我们可以看到重孔和轻孔到导带的转变。这两个跃迁之间的分离主要取决于HgTe/CdTe之间的价带偏移(VBO)的值,这是一个有争议的参数,报道的值从40到400 meV不等(2),并且建议与温度有关。我们的数据支持接近400 mev的值,它很少或没有温度依赖性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Room Temperature Confinement and Photoluminescence in HgCdTe Multiple Quantum Wells
We have grown HgCdTe/CdTe Multiple Quantum Wells (MQW) with the lowest transition near 3 µm, and we have observed room temperature confinement and photoluminescence. HgCdTe/CdTe MOW’S of different compositions can be used over the entire infrared range, since the material is lattice matched from 0 to 1.5 eV. The importance of the 3 µm region comes from the possibility of a communications system operating with fluoride fibers. The MQW was grown by MBE with 50 periods of 100 A of Hg0.15Cd0.85Te barriers and 50 A of Hg0.73Cd0.27Te wells (1). Transmission Electron Microscopy (TEM) and X-ray data confirm very little interdiffusion and high reproducibility of layer thickness. The thick barriers are necessary for strong confinement, especially for the light hole. Therefore we can see the heavy and light hole to conduction band transitions. The separation between these two transitions is mainly determined by the value of the valence band offset (VBO) between HgTe/CdTe, a controversial parameter with reported values ranging from 40 to 400 meV (2), and suggestions of being temperature dependent. Our data support a value near 400 mev which has little or no temperature dependence.
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