首页> 外文期刊>Journal of Crystal Growth >Relaxation study of In_xGa_(1-x)As/GaAs quantum-well structures grown by MBE on (0 0 1) and (1 1 1)B GaAs for long wavelength applications
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Relaxation study of In_xGa_(1-x)As/GaAs quantum-well structures grown by MBE on (0 0 1) and (1 1 1)B GaAs for long wavelength applications

机译:MBE在(0 0 1)和(1 1 1)B GaAs上通过MBE生长的In_xGa_(1-x)As / GaAs量子阱结构的弛豫研究,用于长波长应用

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摘要

A comparative study of the relaxation mechanisms of thin. single In_xGa_(1-x) As/GaAs quantum wells (QWs) grown simultaneously on (0 0 1) and (1 1 1)B GaAs substrates is presented. Transmission electron microscopy (TEM) studies indicate that the primary relaxation mechanism for high-indium content (0 0 1 ) samples is the formation of 3D islands. For the growth conditions used, this occurs at an indium content above 0.24 in our samples. Although initially coherent with the substrate. above a certain critical thickness catastrophic relaxation occurs through a very high density of edge dislocations (> 10~12 cm~-2) as the islands coalesce. A similar relaxation mechanism is not observed in the (1 1 1) orientation. Here. 3D islanding is suppressed and instead a novel configuration of misfit dislocations (MD) appears at x > 0.24. This new MD configuration presents an additional misfit-rc1ieving component not taken into account in the previous theoretical analysis of the critical layer thickness (CLT) for (1 1 1)B. However, the mechanism is relatively inefficient when compared to the catastrophic relaxation in the (0 0 1) case, and therefore, the (1 1 1)B substrate still offers considerable advantages. This is illustrated by photoluminescence results, which show that (1 1 1)B In_xGa_(1-x)As QWs are able to reach wavelengths as long as 1.1 μm at room temperature.
机译:薄层松弛机制的比较研究。提出了在(0 0 1)和(1 1 1)B GaAs衬底上同时生长的单个In_xGa_(1-x)As / GaAs量子阱(QW)。透射电子显微镜(TEM)研究表明,高铟含量(0 0 1)样品的主要弛豫机理是3D岛的形成。对于所用的生长条件,在我们的样品中铟含量高于0.24时会发生这种情况。尽管起初与基底是连贯的。当超过一定的临界厚度时,随着岛的合并,边缘脱位的密度很高(> 10〜12 cm〜-2),发生灾难性的松弛。在(1 1 1)方向上未观察到类似的松弛机制。这里。 3D孤岛被抑制,取而代之的是新的错配位错(MD)配置出现在x> 0.24处。这种新的MD构造提供了一个额外的失配分量,在以前的(1 1 1)B临界层厚度(CLT)的理论分析中没有考虑。但是,与(0 0 1)情况下的灾难性弛豫相比,该机制效率相对较低,因此(1 1 1)B衬底仍然具有相当大的优势。这由光致发光结果说明,该结果表明(1 1 1)B In_xGa_(1-x)As QW在室温下能够达到长达1.1μm的波长。

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