• Chinese Journal of Lasers
  • Vol. 50, Issue 6, 0601004 (2023)
Yuyang Yin1、3, Hui Ye2、3, Xuewu Cheng1、*, Kaijun Ji1、3, Jiqin Wang1、3, Jiaming Liang1、3, Kaijie Ji1, Xin Lin1, Yong Yang1, Linmei Liu1, and Faquan Li1
Author Affiliations
  • 1State Key Laboratory of Magnetic Resonance and Atomic and Molecular Physics, Innovation Academy for Precision Measurement Science and Technology, Chinese Academy of Sciences, Wuhan 430071, Hubei, China
  • 2Shanghai Institution of Satellite Engineering, Shanghai 201109, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.3788/CJL220734 Cite this Article Set citation alerts
    Yuyang Yin, Hui Ye, Xuewu Cheng, Kaijun Ji, Jiqin Wang, Jiaming Liang, Kaijie Ji, Xin Lin, Yong Yang, Linmei Liu, Faquan Li. Research on Adjustment Method of Pulsed Laser Waveform Based on Beam Splitting and Delay[J]. Chinese Journal of Lasers, 2023, 50(6): 0601004 Copy Citation Text show less
    Principle of beam splitting and delay superimposition
    Fig. 1. Principle of beam splitting and delay superimposition
    Experimental setup
    Fig. 2. Experimental setup
    Numerical simulation results of rectangular pulsed laser. (a) Rectangular pulsed lasers under different α; (b) simulated u
    Fig. 3. Numerical simulation results of rectangular pulsed laser. (a) Rectangular pulsed lasers under different α; (b) simulated u
    Numerical simulation results of pulsed laser with special waveform. (a) Rectangular pulsed laser; (b) triangular pulsed laser; (c) hump-shaped pulsed laser; (d) dual-peak pulsed laser
    Fig. 4. Numerical simulation results of pulsed laser with special waveform. (a) Rectangular pulsed laser; (b) triangular pulsed laser; (c) hump-shaped pulsed laser; (d) dual-peak pulsed laser
    Waveforms stored by oscilloscope
    Fig. 5. Waveforms stored by oscilloscope
    Experimental results. (a) Rectangular pulsed laser; (b) triangular pulsed laser; (c) hump-shaped pulsed laser; (d) dual-peak pulsed laser
    Fig. 6. Experimental results. (a) Rectangular pulsed laser; (b) triangular pulsed laser; (c) hump-shaped pulsed laser; (d) dual-peak pulsed laser
    Comparison between experimental results and numerical simulation results. (a) Comparison between original pulsed laser waveform and Gaussian waveform; (b) comparison between modified simulation result and experimental result
    Fig. 7. Comparison between experimental results and numerical simulation results. (a) Comparison between original pulsed laser waveform and Gaussian waveform; (b) comparison between modified simulation result and experimental result
    DeviceParameter
    Laser

    Wavelength:532 nm

    Output frequency:30 Hz

    Full width at half maximum:7 ns

    Maximum output energy:800 mJ

    High-speed photodetector

    Response bandwidth:>1.2 GHz

    Rising edge:<500 ps

    Polarizing beam splitter

    Polarization extinction ratio:>1000∶1

    Transmittance:>90%

    Damage threshold:2 J/cm2 at 532 nm wavelength,10 ns FWHM,and 10 Hz laser output frequency

    Oscilloscope

    Bandwidth:350 MHz

    Sampling rate:6.25 GHz

    Sampling resolution:12

    Table 1. Parameters of device used in experiment
    WaveformSplitting ratioDelay
    Beam splitter 1Beam splitter 2α1α2
    Rectangular50∶5050∶500.691.38
    Triangular80∶2070∶300.430.80
    Hump-shaped50∶5050∶500.371.40
    Dual-peak50∶5050∶500.102.50
    Table 2. Splitting ratio and delay in simulation of laser waveform
    Yuyang Yin, Hui Ye, Xuewu Cheng, Kaijun Ji, Jiqin Wang, Jiaming Liang, Kaijie Ji, Xin Lin, Yong Yang, Linmei Liu, Faquan Li. Research on Adjustment Method of Pulsed Laser Waveform Based on Beam Splitting and Delay[J]. Chinese Journal of Lasers, 2023, 50(6): 0601004
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