Laser & Optoelectronics Progress, Volume. 61, Issue 15, 1514004(2024)

Optimization of SPGD Algorithm Based on Adaptive Random Perturbation Voltages in Coherent Beam Combining

Jiaqin Qi1,2,3, Wenhui Zheng1,2,3, Wenjun Jiang1,2,3, Guiyuan Tan1,2,3, Liyun Zhong1,2,3, Jianglei Di1,2,3、*, Xiaoyan Wu4、**, Guodong Liu4, and Yuwen Qin1,2,3
Author Affiliations
  • 1Institute of Advanced Photon Technology, School of Information Engineering, Guangdong University of Technology, Guangzhou 510006, Guangdong, China
  • 2Key Laboratory of Synsensory Fusion Photonics Technology, Ministry of Education, Guangzhou 510006, Guangdong, China
  • 3Guangdong Provincial Key Laboratory of Information Photonics Technology, Guangzhou 510006, Guangdong, China
  • 4Institute of Fluid Physics, China Academy of Engineering Physics, Mianyang 621900, Sichuan, China
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    Figures & Tables(12)
    Flow chart for executing SPGD algorithm
    Interaction diagram between variables in the J-Based SPGD algorithm
    Flow chart of data acquisition and statistics
    Values of p1 and η1 under different perturbation voltage amplitudes
    Iteration curves of each variable after optimization. (a) γ; (b) δu; (c) δJ; (d) u; (e) ΔJ; (f) J
    Iteration curves of the evaluation function of Piecewise SPGD, AdmSPGD, ExpSPGD, and SPGD
    Iteration curves of the evaluation function of each algorithm. (a) 3 beams; (b) 19 beams
    Distribution of the iteration number when each algorithm converges. (a) Piecewise SPGD; (b) AdmSPGD; (c) ExpSPGD; (d) SPGD
    • Table 1. The process of Piecewise SPGD algorithm

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      Table 1. The process of Piecewise SPGD algorithm

      Piecewise SPGD algorithm
      1)Setinitial control voltages u(0)=0,,0,gain coefficient γ0=4.5,and measure the initial value of the evaluation function J(0)
      2)Forn=0,1,2,,N do
      3)generate a set of random perturbation voltages that obey the amplitude of δu(n)=π×(1-0.7×J(n))/3
      4)apply forward perturbation voltages:u(n)+δu(n)
      5)obtain performance evaluation functions:J+(n)
      6)apply negative perturbation voltages:u(n)-δu(n)
      7)obtain performance evaluation functions:J-(n)
      8)obtain the change of the evaluation function:δJ(n)=J+(n)-J-(n)
      9)determine if max(J+(n),J-(n)) is greater than J(n),if yes or J(n) is convergent then execute 9.1,if no then execute 9.2

      9.1:update the control voltages,γ=1J+(n)-J-(n)u(n+1)=u(n)+γδJ(n)δu(n),

      9.2:update the control voltages,u(n+1)=u(n)+γ0δu(n)δJ(n)

      10)obtain the performance evaluation function J(n+1) and determine whether J(n+1) meets the end of algorithm condition
      11)End For
    • Table 2. Simulation parameter setting

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      Table 2. Simulation parameter setting

      ParameterValue
      Distance:L /m2
      Wavelength:λ /10-9 m1064
      Beam waist:ω /10-3 m4
      Beam spacing:d /10-2 m1
      Working modeSingle-mode
    • Table 3. Initial parameter setting of each algorithm

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      Table 3. Initial parameter setting of each algorithm

      AlgorithmParameter
      SPGDγ=1,amplitude of δu=π/3
      ExpSPGDγ0=1.6α=0,amplitude of δu=π/3
      AdmSPGDγ=0.8p=0.3ρ=1,amplitude of δu=π/3
      Piecewise SPGDγ=4.5,amplitude of δu(0)=π/3
    • Table 4. Iteration number for algorithm convergence

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      Table 4. Iteration number for algorithm convergence

      AlgorithmIteration number of J=0.9Iteration number of J=0.95
      Piecewise SPGD17.523.5
      AdmSPGD20.526.0
      ExpSPGD23.129.0
      SPGD27.534.0
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    Jiaqin Qi, Wenhui Zheng, Wenjun Jiang, Guiyuan Tan, Liyun Zhong, Jianglei Di, Xiaoyan Wu, Guodong Liu, Yuwen Qin. Optimization of SPGD Algorithm Based on Adaptive Random Perturbation Voltages in Coherent Beam Combining[J]. Laser & Optoelectronics Progress, 2024, 61(15): 1514004

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    Paper Information

    Category: Lasers and Laser Optics

    Received: Jun. 30, 2023

    Accepted: Aug. 8, 2023

    Published Online: Aug. 12, 2024

    The Author Email: Jianglei Di (jiangleidi@gdut.edu.cn), Xiaoyan Wu (wuxiaoyan1219@sina.cn)

    DOI:10.3788/LOP231638

    CSTR:32186.14.LOP231638

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