Photonics Research, Volume. 7, Issue 2, 187(2019)
Generation of coexisting high-energy pulses in a mode-locked all-fiber laser with a nonlinear multimodal interference technique
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.
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
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.
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.
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
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.
Fig. 7. Statistical information and the dynamics process of a rogue wave.
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.
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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," Photonics Res. 7, 187 (2019)
Category: Nonlinear Optics
Received: Oct. 30, 2018
Accepted: Dec. 17, 2018
Published Online: Feb. 19, 2019
The Author Email: Chao Zeng (zengchao@opt.cn), Wei Zhao (weiz@opt.ac.cn)