• Photonics Research
  • Vol. 7, Issue 2, 187 (2019)
Guangwei Chen1、2, Wenlei Li1、2, Guomei Wang1、2, Wenfu Zhang1、2, Chao Zeng1、2、3、*, and Wei Zhao1、2、4、*
Author Affiliations
  • 1State Key Laboratory of Transient Optics and Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China
  • 2University of Chinese Academy of Sciences (UCAS), Beijing 100049, China
  • 3e-mail: zengchao@opt.cn
  • 4e-mail: weiz@opt.ac.cn
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    DOI: 10.1364/PRJ.7.000187 Cite this Article Set citation alerts
    Guangwei Chen, Wenlei Li, Guomei Wang, Wenfu Zhang, Chao Zeng, Wei Zhao. Generation of coexisting high-energy pulses in a mode-locked all-fiber laser with a nonlinear multimodal interference technique[J]. Photonics Research, 2019, 7(2): 187 Copy Citation Text show less
    Schematic structure of SMF–GIMF–SMF. Blue and red lines denote light under a linear (low power) and a nonlinear (high power) case, respectively.
    Fig. 1. Schematic structure of SMF–GIMF–SMF. Blue and red lines denote light under a linear (low power) and a nonlinear (high power) case, respectively.
    (a) Transmission is plotted as a function of peak power with the GIMF-length of 30 cm; (b) a relative metric for pulse power discrimination with the length of GIMF LGIMF=30 cm+δL.
    Fig. 2. (a) Transmission is plotted as a function of peak power with the GIMF-length of 30 cm; (b) a relative metric for pulse power discrimination with the length of GIMF LGIMF=30  cm+δL.
    Experimental setup of the passively mode-locked fiber laser. Inset: nonlinear power-dependent transmission (left) and microscopy image of a GIMF-based modulator.
    Fig. 3. Experimental setup of the passively mode-locked fiber laser. Inset: nonlinear power-dependent transmission (left) and microscopy image of a GIMF-based modulator.
    Characterizations of a CS and a SP. Output spectra of (a) a CS and (b) a SP plot in linear and logarithmic coordinates (insets); temporal information and RF spectra of (c) a CS and (d) a SP.
    Fig. 4. Characterizations of a CS and a SP. Output spectra of (a) a CS and (b) a SP plot in linear and logarithmic coordinates (insets); temporal information and RF spectra of (c) a CS and (d) a SP.
    Output power (blue) and pulse energy (red) as functions of launched pump power. A, B, C, and D denote the regions of the laser operations for generating a CS, the multipulse state of the CS, a SP, and the multipulse state of the SP, respectively. The slope efficiencies of the laser in regions A and C are ∼1.8% and ∼3.1%, respectively.
    Fig. 5. Output power (blue) and pulse energy (red) as functions of launched pump power. A, B, C, and D denote the regions of the laser operations for generating a CS, the multipulse state of the CS, a SP, and the multipulse state of the SP, respectively. The slope efficiencies of the laser in regions A and C are 1.8% and 3.1%, respectively.
    Real-time observations of spectral dynamics of (a) a CS and (b) a SP. Inset: continuous real-time spectra measured by the DFT.
    Fig. 6. Real-time observations of spectral dynamics of (a) a CS and (b) a SP. Inset: continuous real-time spectra measured by the DFT.
    Statistical information and the dynamics process of a rogue wave.
    Fig. 7. Statistical information and the dynamics process of a rogue wave.
    Numerical simulation results. Temporal and spectral profiles of (a) a CS and (b) a SP; the spectral evolution of (c) CS and (d) SP pulses.
    Fig. 8. Numerical simulation results. Temporal and spectral profiles of (a) a CS and (b) a SP; the spectral evolution of (c) CS and (d) SP pulses.
    Guangwei Chen, Wenlei Li, Guomei Wang, Wenfu Zhang, Chao Zeng, Wei Zhao. Generation of coexisting high-energy pulses in a mode-locked all-fiber laser with a nonlinear multimodal interference technique[J]. Photonics Research, 2019, 7(2): 187
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