王婷 1,2吴冀亮 1,2马春光 1,2黄勇涛 1,2[ ... ]黄永箴 1,2,*
作者单位
摘要
1 中国科学院半导体研究所 集成光电子学国家重点实验室,北京 100083
2 中国科学院大学 材料科学与光电工程中心,北京 100049
针对双波长激光器间距精细调谐的需求,基于正方形微腔的模场分布,设计了中心及四个角区电流注入窗口的正方形微腔激光器。利用有限元法对提出的结构进行分析,发现改变腔体折射率分布差,可以调控基横模和一阶横模的波长间距。基于半导体平面加工工艺成功制备了边长为30 μm的非均匀注入正方形微腔激光器。当注入电流从42 mA增加到53 mA时,该激光器的波长间隔从0.18 nm减小到0.1 nm,强度比小于4 dB。除此之外,继续增加电流,由于双模间隔的进一步减小,出现了明显的单周期振荡现象。
激光器 半导体激光器 微腔 双波长 正方形谐振腔 Laser Semiconductor laser Microcavity Dual wavelength Square microcavity 
光子学报
2022, 51(2): 0251202
Author Affiliations
Abstract
1 State Key Laboratory of Integrated Optoelectronics, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
2 Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
We propose and demonstrate the generation of wideband chaos based on a dual-mode microsquare semiconductor laser with optical feedback. By adjusting the dual-mode intensity ratio and the feedback strength, wideband chaos covering more than 50 GHz in the RF spectrum is achieved. The standard and effective bandwidths of the chaotic signal are 31.3 GHz and 30.7 GHz with the flatness of 8.3 dB and 6.1 dB, respectively.
dual-mode laser micro laser chaos optical feedback 
Chinese Optics Letters
2021, 19(11): 111401
Author Affiliations
Abstract
1 State Key Laboratory of Integrated Optoelectronics, Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China
2 Center of Materials Science and Opto-Electronic Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
3 State Key Laboratory of Integrated Optoelectronics, College of Electronic Science & Engineering, Jilin University, Changchun 130012, China
4 National Key Laboratory of Science and Technology on Electronic Test and Measurement, the 41st Research Institute, China Electronics Technology Group Corporation, Qingdao 266555, China
The generation of high-repetition rate (frep ≥ 10 GHz) ultra-broadband optical frequency combs (OFCs) at 1550 nm and 1310 nm is investigated by seeding two types of highly nonlinear fibers (HNLFs) with 10 GHz picosecond pulses at the pump wavelength of 1550 nm. When pumped near the zero dispersion wavelength (ZDW) in the normal dispersion region of a HNLF, 10 GHz flat-topped OFC with 43 nm bandwidth within 5 dB power variation is generated by self-phase modulation (SPM)-based OFC spectral broadening at 26.5 dBm pump power, and 291 fs pulse trains with 10 GHz repetition rate are obtained at 18 dBm pump power without complicated pulse shaping methods. Furthermore, when pumped in the abnormal dispersion region of a HNLF, OFCs with dispersive waves around 1310 nm are studied using a common HNLF and fluorotellurite fibers, which maintain the good coherence of the pump light at 1550 nm. At the same time, sufficient tunability of the generated dispersive waves is achieved when tuning the pump power or ZDW.
optical comb electro-optic devices ultrafast optics optical pulses nonlinear optics 
Opto-Electronic Advances
2020, 3(7): 07190033

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