High Power Laser Science and Engineering, Volume. 13, Issue 1, 010000e5(2025)

Passive spherical aberration compensation in laser diode side-pumped master oscillator power amplifier laser systems

Pengfei Li1,2, Yulei Wang1,2、*, Fei Zhang1,2, Yan Li1,2, Hao Zheng1,2, Chen Cao1,2, Kai Li1,2, Mengyu Jia1,2, Bingzheng Yan1,2, Zhenxu Bai1,2, Yu Yu1,2, and Zhiwei Lv1,2
Author Affiliations
  • 1Center for Advanced Laser Technology, Hebei University of Technology, Tianjin, China
  • 2Hebei Key Laboratory of Advanced Laser Technology and Equipment, Tianjin, China
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    Figures & Tables(11)
    Under varying pump powers: (a) the variation in single-pass and double-pass amplified laser energy; (b) the variation in the upper-state particle extraction efficiency of the Nd:YAG crystal for both single-pass and double-pass amplifications.
    Variation of the thermal focal length of the Nd:YAG crystal rod at different pump power levels.
    Relationship graph between the dimensionless aberration coefficient for a lens as a function of the lens-shape factor and the imaging parameter .
    The diagram showing the variation in the optical field diameter of the single-pass amplified laser output from amplifier.
    High beam quality, high-efficiency MOPA laser system.
    At varying pump power levels, the laser beam quality factors are assessed for single-pass amplification through the side-pump amplifier LD2, double-pass amplification with M5 positioned at location A and ordinary double-pass amplification without the 4f system.
    The single-pulse energy of the double-pass amplified laser, with mirror M5 positioned at location A under varying pump powers, is compared to the single-pulse energy of the ordinary double-pass amplified laser without the 4f system.
    At varying pump power levels, the beam quality factors for the LD2 amplified laser in single-pass configuration and for the amplified laser with M5 placed in positions A, B and C in double-pass configuration.
    Under a pump power of 60.7 W, when the mirror M5 is positioned at locations A, B and C, the laser undergoes double-pass amplification through the side-pumped amplifier LD2. The distribution of the optical field shape is measured at distances of 25 and 120 cm from the output aperture.
    When M5 is positioned at A, B and C, the amplified laser reflected by M5 reaches the focal points at SF (positions 3, 1 and 2, respectively).
    When the laser undergoes single-pass and double-pass amplification through the side-pumped amplifier LD2: (a) the relationship between the pump power and amplified laser energy; (b) the relationship between the pump power and optical-to-optical conversion efficiency.
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    Pengfei Li, Yulei Wang, Fei Zhang, Yan Li, Hao Zheng, Chen Cao, Kai Li, Mengyu Jia, Bingzheng Yan, Zhenxu Bai, Yu Yu, Zhiwei Lv. Passive spherical aberration compensation in laser diode side-pumped master oscillator power amplifier laser systems[J]. High Power Laser Science and Engineering, 2025, 13(1): 010000e5

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    Paper Information

    Category: Research Articles

    Received: Aug. 17, 2024

    Accepted: Dec. 5, 2024

    Published Online: Mar. 18, 2025

    The Author Email: Yulei Wang (wyl@hebut.edu.cn)

    DOI:10.1017/hpl.2024.88

    CSTR:32185.14.hpl.2024.88

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