• Acta Physica Sinica
  • Vol. 68, Issue 11, 110501-1 (2019)
Kun-Ying Li1、2, Pu Li1、2、3、4、5、*, Xiao-Min Guo1、2, Yan-Qiang Guo1、2, Jian-Guo Zhang1、2, Yi-Ming Liu4、5, Bing-Jie Xu4、5, and Yun-Cai Wang1、2
Author Affiliations
  • 1Key Laboratory of Advanced Transducers and Intelligent Control System, Ministry of Education and Shanxi Province, Taiyuan University of Technology, Taiyuan 030024, China
  • 2College of Physics and Optoelectronics, Taiyuan University of Technology, Taiyuan 030024, China
  • 3Key Laboratory of Specialty Fiber Optics and Optical Access Networks, Shanghai University, Shanghai 200444, China
  • 4No.30 Institute of China Electronic Technology Corporation, Chengdu 610041, China
  • 5Science and Technology on Communication Laboratory, Institute of Southwestern Communication, Chengdu 610041, China
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    DOI: 10.7498/aps.68.20190171 Cite this Article
    Kun-Ying Li, Pu Li, Xiao-Min Guo, Yan-Qiang Guo, Jian-Guo Zhang, Yi-Ming Liu, Bing-Jie Xu, Yun-Cai Wang. Flat chaos generated by optical feedback multi-mode laser with filter[J]. Acta Physica Sinica, 2019, 68(11): 110501-1 Copy Citation Text show less
    Experimental setup for the RF spectrum analysis of optical feedback FP laser (FP-LD, Fabry-Perot laser diode; PC, polarization controller; VOA, variable optical attenuator; FM, fiber mirror; EDFA, erbium-doped fiber amplifier; BPF, optical bandpass filter; PD, photodetector; ESA, electrical spectrum analyzer; OSA, optical spectrum analyzer).基于光反馈FP激光器混沌频谱特性分析实验装置(FP-LD, 法布里-珀罗激光二极管; PC, 偏振控制器; VOA, 可调光衰减器; FM, 光纤反射镜; EDFA, 掺铒光纤放大器; BPF, 可调光滤波器; PD, 光电探测器; ESA, 频谱仪; OSA, 光谱仪)
    Fig. 1. Experimental setup for the RF spectrum analysis of optical feedback FP laser (FP-LD, Fabry-Perot laser diode; PC, polarization controller; VOA, variable optical attenuator; FM, fiber mirror; EDFA, erbium-doped fiber amplifier; BPF, optical bandpass filter; PD, photodetector; ESA, electrical spectrum analyzer; OSA, optical spectrum analyzer).基于光反馈FP激光器混沌频谱特性分析实验装置(FP-LD, 法布里-珀罗激光二极管; PC, 偏振控制器; VOA, 可调光衰减器; FM, 光纤反射镜; EDFA, 掺铒光纤放大器; BPF, 可调光滤波器; PD, 光电探测器; ESA, 频谱仪; OSA, 光谱仪)
    Characteristics of the multi-mode chaos: (a) Optical spectrum; (b) RF spectrum.多模混沌激光特性实验结果 (a)光谱; (b)频谱
    Fig. 2. Characteristics of the multi-mode chaos: (a) Optical spectrum; (b) RF spectrum.多模混沌激光特性实验结果 (a)光谱; (b)频谱
    Characteristics of single-mode chaotic signals (m = –1, 0, +1): (a1)−(a3) Optical spectra; (b1)−(b3) RF spectra.m = –1, 0, +1模式下的单模混沌信号特性实验结果 (a1)—(a3)光谱; (b1)—(b3)频谱
    Fig. 3. Characteristics of single-mode chaotic signals (m = –1, 0, +1): (a1)−(a3) Optical spectra; (b1)−(b3) RF spectra. m = –1, 0, +1模式下的单模混沌信号特性实验结果 (a1)—(a3)光谱; (b1)—(b3)频谱
    Numerical results of multi-mode FP-LD with optical feedback: (a) Optical spectrum (M = 15); (b) power spectrum.多纵模光反馈FP激光器数值仿真结果 (a) 光谱(M = 15); (b) 频谱
    Fig. 4. Numerical results of multi-mode FP-LD with optical feedback: (a) Optical spectrum (M = 15); (b) power spectrum. 多纵模光反馈FP激光器数值仿真结果 (a) 光谱(M = 15); (b) 频谱
    Simulation results of single-mode chaotic signals (m = –1, 0, +1): (a1)−(a3) Power spectra; (b1)−(b3) time series; (c1)−(c3) cross-correlations.光反馈多模激光器在3个模式(m = –1, 0, +1)下单模混沌信号的模拟结果 (a1)—(a3) 频谱; (b1)—(b3) 时序; (c1)—(c3) 互相关函数
    Fig. 5. Simulation results of single-mode chaotic signals (m = –1, 0, +1): (a1)−(a3) Power spectra; (b1)−(b3) time series; (c1)−(c3) cross-correlations. 光反馈多模激光器在3个模式(m = –1, 0, +1)下单模混沌信号的模拟结果 (a1)—(a3) 频谱; (b1)—(b3) 时序; (c1)—(c3) 互相关函数
    参数符号参考值
    模式总数目M15
    线宽增强因子α3.5
    内腔损耗系数γ0.283 ps–1
    载流子损耗系数γe6.21 × 10-4 ps–1
    归一化电流系数C1.5
    内腔环行时间τ7.3 ps
    增益峰值频率ωc$2{\text{π}} \times 193.7$ THz
    增益宽度Δωg$2{\text{π}} \times 10$ THz
    增益饱和系数s1 × 10–7
    微分增益系数gc3.2 × 10–9
    透明载流子数N01.25 × 108
    反馈系数kt0.020 ps–1
    反馈延时τt2 ns
    自发辐射率β5 ps–1
    Table 1. Simulation parameters of FP-LD with optical feedback.
    Kun-Ying Li, Pu Li, Xiao-Min Guo, Yan-Qiang Guo, Jian-Guo Zhang, Yi-Ming Liu, Bing-Jie Xu, Yun-Cai Wang. Flat chaos generated by optical feedback multi-mode laser with filter[J]. Acta Physica Sinica, 2019, 68(11): 110501-1
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