• Chinese Journal of Lasers
  • Vol. 49, Issue 1, 0101012 (2022)
Weiyi Sun1、5, Jiapeng Huang1、2、4、*, Liming Chen2, Zhiyuan Huang1, Wenbin He2, Xin Jiang2、3, Meng Pang1、2、3、**, and Yuxin Leng1、3、***
Author Affiliations
  • 1State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China;
  • 2Innovation and Integration Center of New Laser Technology, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China;
  • 3School of Physics and Opto-Electronic Engineering, Hangzhou Institute for Advanced Study, Chinese Academy of Sciences, Hangzhou, Zhejiang 310013, China;
  • 4Department of Electrical Engineering, Hong Kong Polytechnic University, Hong Kong, China;
  • 5School of Physical Science and Technology, Shanghai Tech University, Shanghai 201210, China
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    DOI: 10.3788/CJL202249.0101012 Cite this Article Set citation alerts
    Weiyi Sun, Jiapeng Huang, Liming Chen, Zhiyuan Huang, Wenbin He, Xin Jiang, Meng Pang, Yuxin Leng. Design of a 10 W Level Dispersion-Managed High-Power Ultrafast Mid-Infrared Fiber Laser System[J]. Chinese Journal of Lasers, 2022, 49(1): 0101012 Copy Citation Text show less
    Design of high-power ultrafast fiber laser system at 2.8 μm using dispersion-management and CPA techniques
    Fig. 1. Design of high-power ultrafast fiber laser system at 2.8 μm using dispersion-management and CPA techniques
    Wave shape transformation of the pulse in time domain and frequency domain in seed oscillator. (a) Time and (b) frequency domain wave shapes of input Gaussian pulse; (c) time (top) and frequency (below) transformation; (d)time and (e) frequency domain wave shapes of output pulse
    Fig. 2. Wave shape transformation of the pulse in time domain and frequency domain in seed oscillator. (a) Time and (b) frequency domain wave shapes of input Gaussian pulse; (c) time (top) and frequency (below) transformation;   (d)time and (e) frequency domain wave shapes of output pulse
    After forming a stable pulse in seed oscillator cavity, transmission process of a single round pulse in time and frequency domain and pulse widths. (a) Transformation process of pulse shape and spectral shape;(b)the largest pulse width; (c) the smallest pulse width
    Fig. 3. After forming a stable pulse in seed oscillator cavity, transmission process of a single round pulse in time and frequency domain and pulse widths. (a) Transformation process of pulse shape and spectral shape;(b)the largest   pulse width; (c) the smallest pulse width
    Output pulse from the pre-amplifier. (a) Pulse shape;(b) pulse spectrum;(c) transformation process in time and frequency domain
    Fig. 4. Output pulse from the pre-amplifier. (a) Pulse shape;(b) pulse spectrum;(c) transformation process in time and frequency domain
    Output pulse in the main amplifier without compressor when positive chirp provided by pulse stretcher is balanced by negative chirp provided by gain fiber. (a) Pulse shape;(b) pulse spectrum;(c) transformation process in time and frequency domain
    Fig. 5. Output pulse in the main amplifier without compressor when positive chirp provided by pulse stretcher is balanced by negative chirp provided by gain fiber. (a) Pulse shape;(b) pulse spectrum;(c) transformation process in time and frequency domain
    Change of fiber output pulse width and the proportion of central pulse energy with normal dispersion provided by stretcher
    Fig. 6. Change of fiber output pulse width and the proportion of central pulse energy with normal dispersion provided by stretcher
    Output pulse in the main amplifier with two different groups dispersion values
    Fig. 7. Output pulse in the main amplifier with two different groups dispersion values
    DeviceLength /mβ2 /(ps2·km-1)β3 /(ps3·km-1)γ /(W-1·km-1)Core diameter /μmConcentration
    Fiber4-83.50.640.24150.07
    Stretcher1415-3.370
    Table 1. Parameters in the simulation of seed oscillator
    DeviceLength / mβ2 / (ps2·km-1)β3 / (ps3·km-1)γ / (W-1·km-1)
    Fiber5.5-83.50.640.24
    Stretcher1800-6.50
    Table 2. Parameters in the simulation of per-amplifier
    DeviceGDD /ps2β2/(ps2·km-1)β3/(ps3·km-1)
    Stretcher+0.730850-6.91
    Compressor-1200.98
    Stretcher+0.6321250-10.16
    Compressor-6185.02
    Table 3. Two different groups of parameters of main amplifier chosen for the simulation
    Weiyi Sun, Jiapeng Huang, Liming Chen, Zhiyuan Huang, Wenbin He, Xin Jiang, Meng Pang, Yuxin Leng. Design of a 10 W Level Dispersion-Managed High-Power Ultrafast Mid-Infrared Fiber Laser System[J]. Chinese Journal of Lasers, 2022, 49(1): 0101012
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