横断面电子束诱导电流成像研究了InGaN/GaN激光二极管的降解

H. Xiu, E. Thrush, L. Zhao, A. Phillips, C. Humphreys
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引用次数: 0

摘要

本研究采用截面电子束感应电流(EBIC)成像技术,结合扫描电子显微镜(SEM)研究了InGaN/GaN激光二极管的降解机理。通过对同一激光棒中未测试和降级激光器的EBIC图像的比较,我们发现降级激光器的pn结位置已经向n掺杂区域移动,并且降级激光器pn结p侧的载流子界面比原始激光二极管中的载流子界面变得不那么尖锐。这种p-n结的位置移位导致了有源区和n掺杂区载流子的补偿,从而导致了有源区空穴和电子浓度的不平衡以及InGaN量子阱发射效率的降低。这是因为p-n结的位移,从其最佳位置,导致少数载流子损失,因为后者在通往有源区域的途中具有更高的非辐射重组概率。用两种不同的理论模型计算了少数载流子的扩散长度。结果表明,降解激光中p掺杂区域的电子扩散长度比未测试激光长。其原因也可能与补偿效应或退化激光中复合率的降低有关,这将导致激光阈值电流的增加和激光的退化。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Degradation of InGaN/GaN laser diodes investigated by cross-sectional electron beam induced current imaging
In this study, the degradation mechanism of InGaN/GaN laser diodes has been investigated using cross-sectional electron beam induced current (EBIC) imaging, combined with scanning electron microscopy (SEM). By comparing the EBIC images of an untested and a degraded laser from the same laser bar, we show that the p-n junction position of the degraded laser has shifted towards the n-doped region and the carrier interface at the p-side of the p-n junction of the degraded laser became less sharp than in the original laser diode. This p-n junction position shift leads to carrier compensation in the active and the n-doped regions, which subsequently leads to an imbalance in the hole and electron concentrations in the active region and a reduction in the emission efficiency of InGaN quantum wells. This occurs because a displacement of the p-n junction, from its optimal position, results in a minority carrier loss, as the latter has a higher probability of recombining non-radiatively en-route to the active region. The minority carrier diffusion lengths were also calculated using two different theoretical models. The results show that the electron diffusion length in the p-doped region in the degraded laser is longer than that in the untested laser. The reason may also be related to the compensation effect or the reduced recombination rate in the degraded laser, which will result in an increase in the threshold current of the laser and the degradation of the laser.
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