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Carrier Redistribution Between Two Kinds of Localized States in the InGaN/GaN Quantum Wells Studied by Photoluminescence

机译:用光致发光研究InGaN / GaN量子阱中两种局部状态之间的载流子重分布

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摘要

The InGaN/GaN multi-quantum wells (MQWs) are prepared at the same condition by metal-organic chemical vapor deposition (MOCVD) except the thickness of cap layers additionally grown on each InGaN well layer. The photoluminescence (PL) intensity of the thin cap layer sample is much stronger than that of thicker cap layer sample. Interestingly, the thick cap layer sample has two photoluminescence peaks under high excitation power, and the PL peak energy-temperature curves show an anomalous transition from reversed V-shaped to regular S-shaped with increasing excitation power. Meanwhile, it exhibits a poorer thermal stability of thick cap layer sample under higher excitation power than that under lower excitation power. Such an untypical phenomenon is attributed to carrier redistribution between the two kinds of localized states which is induced by the inhomogeneous distribution of indium composition in thick cap layer sample. Furthermore, the luminescence of deep localized states has a better thermal stability, and the luminescence of shallow localized states has a poor thermal stability. In fact, such a severer inhomogeneous indium distribution may be caused by the degradation of subsequent epitaxial growth of InGaN/GaN MQWs region due to longer low-temperature GaN cap layer growth time.
机译:通过金属有机化学气相沉积(MOCVD)在相同条件下制备InGaN / GaN多量子阱(MQW),除了在每个InGaN阱层上另外生长的盖层的厚度。薄覆盖层样品的光致发光(PL)强度比厚覆盖层样品的光致发光(PL)强度要强得多。有趣的是,厚的盖层样品在高激发功率下具有两个光致发光峰,并且PL峰的能量-温度曲线显示出随着激发功率的增加从反V形到规则S形的异常转变。同时,与较低激发功率相比,厚覆盖层样品在较高激发功率下的热稳定性较差。这种不典型的现象归因于两种局部状态之间的载流子重新分布,这是由厚覆盖层样品中铟成分的不均匀分布引起的。此外,深局部态的发光具有更好的热稳定性,而浅局部态的发光具有较差的热稳定性。实际上,由于更长的低温GaN盖层生长时间导致InGaN / GaN MQWs区域随后的外延生长变差,可能导致这种更严重的不均匀铟分布。

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