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Optical characteristics of MOCVD-grown InGaN/GaN multiple quantum wells investigated by excitation energy dependent PL and PLE spectroscopy

机译:通过依赖于激发能量的PL和PLE光谱研究了MOCVD生长的InGaN / GaN多量子阱的光学特性

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We have systematiclaly studied the optical properties of InGaN/GaN multiple quantum wells (MQWs) at 10K under different excitation conditions using photoluminescence (PL) and PL excitation (PLE) spectroscopy. The MQWs were grown on 1.8-#mu#m-thick GaN on c-plane sapphire films by metal-organic chemical vapor deposition. Structures consist of 12 MQWs with 3-nm-thick In_(0.2)Ga_(0.8)N wells, 4.5-nm-thick GaN barriers, and a 100-nm-thick Al_(0.07)Ga_(0.93)N capping layers. We found that the PL emission consists of a strong main peak at 2.80 eV and a much weaker and broader secondary peak at approx 2.25 eV. We observed that both the peak position and the spectral width of the main peak vary with the excitation energy. The PL peak blueshifts and narrows when the excitation energies are varied from 3.81 eV (above the bandgap of the AlGaN capping layer) to 2.99 eV (below the bandgap of the GaN barrier layers). The intensity ratio of the main peak to the secondary peak also varied with excitation energy. The PLE studies, combined with the excitation dependent PL emission studies, reveal that the two observed emission peaks originate from different layers of the MQWs. In addition, we found that the InGaN-related spontaneous emission processes are strongly affected by different carrier generation conditions with further complications associated with compositional fluctuations and possible carrier localization. The differences in the observed emission processes under varying excitation conditions can be explained by considering the transfer of carriers between the different layers of the MQW structures.
机译:我们使用光致发光(PL)和PL激发(PLE)光谱系统地研究了在不同激发条件下10K下InGaN / GaN多量子阱(MQWs)的光学性质。通过金属有机化学气相沉积法,在c面蓝宝石膜上的1.8微米厚的GaN上生长MQW。结构由12个MQW组成,具有3纳米厚的In_(0.2)Ga_(0.8)N阱,4.5纳米厚的GaN势垒和100纳米厚的Al_(0.07)Ga_(0.93)N覆盖层。我们发现,PL发射包括一个在2.80 eV处的强主峰和一个在约2.25 eV处更弱和更宽的次级峰。我们观察到主峰的峰位置和光谱宽度均随激发能而变化。当激发能从3.81 eV(在AlGaN覆盖层的带隙以上)到2.99 eV(在GaN阻挡层的带隙以下)变化时,PL峰蓝移并变窄。主峰与次峰的强度比也随激发能而变化。 PLE研究与激发相关的PL发射研究相结合,发现两个观察到的发射峰源自MQW的不同层。此外,我们发现与InGaN有关的自发发射过程受到不同载流子产生条件的强烈影响,并伴随着与成分波动和可能的载流子局部化有关的进一步复杂化。通过考虑MQW结构不同层之间载流子的转移,可以解释在变化的激发条件下观察到的发射过程中的差异。

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