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基于反向游标效应的耦合微盘中的单模激光发射。

Inversed Vernier effect based single-mode laser emission in coupled microdisks.

作者信息

Li Meng, Zhang Nan, Wang Kaiyang, Li Jiankai, Xiao Shumin, Song Qinghai

机构信息

Integrated Nanoscience Lab, Department of Electrical and Information Engineering, Harbin Institute of Technology, Shenzhen, 518055, China.

Department of Material Science and Engineering, Harbin Institute of Technology, Shenzhen, 518055, China.

出版信息

Sci Rep. 2015 Sep 2;5:13682. doi: 10.1038/srep13682.

Abstract

Recently, on-chip single-mode laser emissions in coupled microdisks have attracted considerable research attention due to their wide applications. While most of single-mode lasers in coupled microdisks or microrings have been qualitatively explained by either Vernier effect or inversed Vernier effect, none of them have been experimentally confirmed. Here, we studied the mechanism of single-mode laser operation in coupled microdisks. We found that the mode numbers had been significantly reduced to nearly single-mode within a large pumping power range from threshold to gain saturation. The detail laser spectra showed that the largest gain and the first lasing peak were mainly generated by one disk and the laser intensity was proportional to the wavelength detuning of two set of modes. The corresponding theoretical analysis showed that the experimental observations were dominated by internal coupling within one cavity, which was similar to the recently explored inversed Vernier effect in two coupled microrings. We believe our finding will be important for understanding the previous experimental findings and the development of on-chip single-mode laser.

摘要

近年来,耦合微盘中的片上单模激光发射因其广泛的应用而备受研究关注。虽然耦合微盘或微环中的大多数单模激光器已通过游标效应或反游标效应进行了定性解释,但均未得到实验证实。在此,我们研究了耦合微盘中单模激光运行的机制。我们发现,在从阈值到增益饱和的大泵浦功率范围内,模式数量已显著减少至近单模。详细的激光光谱表明,最大增益和首个激射峰主要由一个微盘产生,且激光强度与两组模式的波长失谐成正比。相应的理论分析表明,实验观测结果主要受一个腔内的内部耦合支配,这与最近在两个耦合微环中探索的反游标效应类似。我们相信我们的发现对于理解先前的实验结果以及片上单模激光器的发展将具有重要意义。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1352/4557034/a181355109eb/srep13682-f1.jpg

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