980 nm光纤泵浦激光器的光谱特性研究

I. Avrutsky, R. Gordon, J.M. Xu, R. Clayton
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引用次数: 0

摘要

Al,,58Gao,42波导,其总厚度为500nm。NSOM系统如图2.13所示,使用分辨率为-100 nm的悬臂光学元件。扫描和控制的原理已在参考文献3和4中描述。悬臂式光纤的输出通过单色仪,并使用敏感的硅APD进行检测。图3a14描述了用放置在导线中心的高分辨率光纤测量的空间分辨L-I曲线。我们注意到一个清晰的阈值在100毫安和线性响应高达约1.5倍的阈值。在图3b中,我们显示了在驱动电流为140 mA时,从导线区域收集的光的光谱,以2纳米分辨率测量。我们基本上观察到806 nm的单模发射,在100 mA到150 mA的驱动电流下没有变化。图3c显示了基本心形激光模式的详细图像,在低于和高于阈值的几个驱动电流下测量,单色器设置为806 nm。在150毫安时测量的图案,在图3d中突出显示,以惊人的精度证实了预测的形状。除了对导线区域进行高分辨率扫描外,我们还对整个激光截面进行了扫描,并记录了在几个驱动电流下的空间分辨光谱。这些测量揭示了倾斜区域以及结构顶角的发射,从而获得了这些复杂器件中电流和注入载流子泄漏路径的重要信息。总之,我们使用NSOM技术对QWR二极管激光器的光电流特性、发射光谱和近场强度分布进行了高空间分辨率的测量。我们的结果为这些装置的设计提供了重要的信息。以色列耶路撒冷的Nanonics有限公司因提供这些实验中使用的悬臂光纤而受到认可。*以色列哈卡理工学院电气工程系*瑞士洛桑联邦理工学院物理系E. Kapon et al.,光电。发展和技术,8,429(1993)。2. E. Kapon et al., superlattice and Microstructures, 12491(1992)。3.S. Shalom, K. Lieberman, A. Lewis, S. R. Cohen, Rev. Sci。乐器。63,4061(1992)。4. U. Ben-Ami, N. Ben-Ami, G. Fish, N. Tessler, R. Nagar, G. Eisenstein, A. Lewis, J. M. Nielsen, A. Moller-Larson, apple。理论物理。页65 648(1994)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Investigations of the spectral characteristics of 980-nm fiber pump lasers
Al,,58Gao,42 waveguide whose total thickness is 500 nm. The NSOM system, described schematically in Fig. 2,13 uses cantilevered optical elements3 with a resolution of -100 nm. The principles of scanning and control have been described in Refs. 3 and 4. The output from the cantilevered optical fibers passed through a monochromator and was detected by use of a sensitive silicon APD. Figure 3a14 describes a spatially resolved L-I curve measured with the high-resolution fiber placed at the wire center. We note a clear threshold at 100 mA and a linear response up to about one and a half times threshold. In Fig. 3b we show the optical spectrum, measured with a 2-nm resolution, of the light collected from the wire region at a drive current of 140 mA. We observe essentially a single-moded emission at 806 nm that did not change for drive currents of 100 mA to 150 mA. Figure 3c shows a detailed image of the fundamental heart-shaped lasing mode, measured at several drive currents below and above threshold with the monochromator set to 806 nm. The measured pattern at 150 mA, which is highlighted in Fig. 3d, confirms the predicted shape’ with a remarkable accuracy. In addition to the high resolution scans of the wire region, we have also scanned the complete laser cross section and recorded the spatially resolved spectra at several drive currents. These measurements revealed emission from the sloped areas as well as the top corners ofthe structure yielding important information on current and injected carrier leakage paths in these complex devices. In conclusion, we have performed high spatial resolution measurements of light-current characteristics, emission spectra, and nearfield intensity distributions of QWR diode lasers using NSOM techniques. Our results provide important information relevant to the design of these devices. Nanonics Ltd., Jerusalem, Israel is acknowledged for providing the cantilevered optical fibers used in these experiments. *Electrical Engineering Department, Technion, Haqa, Israel **Physics Department, Swiss Federal Institute of Technology, Lausanne, Switzerland 1. E. Kapon et al., Optoelectron. Dev. and Technol. 8,429 (1993). 2. E. Kapon et al., Superlattices and Microstructures 12,491 (1992). 3. S. Shalom, K. Lieberman, A. Lewis, S. R. Cohen, Rev. Sci. Instrum. 63,4061 (1992). 4. U. Ben-Ami, N. Ben-Ami, G. Fish, N. Tessler, R. Nagar, G. Eisenstein, A. Lewis, J. M. Nielsen, A. Moller-Larson, Appl. Phys. Lett. 65,648 (1994).
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