• High Power Laser and Particle Beams
  • Vol. 35, Issue 4, 041003 (2023)
Jiaying Liu1、2、3, Ziqiang Li1、2, Ran Yang1、2、3, Fan Zou1、2、3, Xu Yang1、2, Xin Zhou1、2、3, Ziting Pan1、2、3, Likang Pan1、2、3, Yuting Li1、2、3, Jiali Jiang1、2, Feng Li1、2, Chao Geng1、2、*, and Xinyang Li1、2
Author Affiliations
  • 1Key Laboratory on Adaptive Optics, Chinese Academy of Sciences, Chengdu 610209, China
  • 2Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.11884/HPLPB202335.220323 Cite this Article
    Jiaying Liu, Ziqiang Li, Ran Yang, Fan Zou, Xu Yang, Xin Zhou, Ziting Pan, Likang Pan, Yuting Li, Jiali Jiang, Feng Li, Chao Geng, Xinyang Li. Research progress of coherent beam combining technique of phased fiber laser array[J]. High Power Laser and Particle Beams, 2023, 35(4): 041003 Copy Citation Text show less
    Schematic diagram and real picture of the emissive hexagon array plane of a 19-element PFLA
    Fig. 1. Schematic diagram and real picture of the emissive hexagon array plane of a 19-element PFLA
    Simulation results of combined beam’s metrics characteristics of 19 Gaussian beamlets in the far-field with different Tr
    Fig. 2. Simulation results of combined beam’s metrics characteristics of 19 Gaussian beamlets in the far-field with different Tr
    Experimental results of combined beam’s metrics characteristics of 19 Gaussian beamlets in the far-field with different Tr
    Fig. 3. Experimental results of combined beam’s metrics characteristics of 19 Gaussian beamlets in the far-field with different Tr
    Bidirectional CBC scheme based on 19-element PFLA
    Fig. 4. Bidirectional CBC scheme based on 19-element PFLA
    Curves of normalized optical intensity coupled by the AFOC array
    Fig. 5. Curves of normalized optical intensity coupled by the AFOC array
    Long exposure patterns in far field (frame averaged) at different stages in the closed loop control processes
    Fig. 6. Long exposure patterns in far field (frame averaged) at different stages in the closed loop control processes
    Experimental setup and block diagram for CBC and pointing of a 19-element PFLA under 2 km turbulence conditions
    Fig. 7. Experimental setup and block diagram for CBC and pointing of a 19-element PFLA under 2 km turbulence conditions
    Variation of the reflected optical intensity metircs of the combined beam under different turbulence intensities at the stages of OP, PL, PLTT of SPGD algorithm
    Fig. 8. Variation of the reflected optical intensity metircs of the combined beam under different turbulence intensities at the stages of OP, PL, PLTT of SPGD algorithm
    Experimental principle and real device diagram of CBC and pointing of 57-element PFLA in 2.1 km transmission
    Fig. 9. Experimental principle and real device diagram of CBC and pointing of 57-element PFLA in 2.1 km transmission
    Metric curve of back-reflected signals from the target of different stages in the closed-loop control process
    Fig. 10. Metric curve of back-reflected signals from the target of different stages in the closed-loop control process
    Long exposure patterns on the target of different stages in the closed-loop control process
    Fig. 11. Long exposure patterns on the target of different stages in the closed-loop control process
    CBC Receiving system diagram of a 19-element PFLA array within 2.1 km horizontal turbulence
    Fig. 12. CBC Receiving system diagram of a 19-element PFLA array within 2.1 km horizontal turbulence
    Metrics characteristics of 19-element CBC receiving in 2.1 km horizontal turbulence
    Fig. 13. Metrics characteristics of 19-element CBC receiving in 2.1 km horizontal turbulence
    Scheme of the wavefront sensor based on AFOC array
    Fig. 14. Scheme of the wavefront sensor based on AFOC array
    Wavefront recovery results
    Fig. 15. Wavefront recovery results
    Experimental setup of PFLA based on active wavefront measurement and external aberration pre-compensation
    Fig. 16. Experimental setup of PFLA based on active wavefront measurement and external aberration pre-compensation
    Far-field spot distribution at different stages of the pre-compensation process
    Fig. 17. Far-field spot distribution at different stages of the pre-compensation process
    Schematic diagram of the optical arrangement of the continuous beam scanning system
    Fig. 18. Schematic diagram of the optical arrangement of the continuous beam scanning system
    Principle of continuous scanning based on AFOC and MLAS
    Fig. 19. Principle of continuous scanning based on AFOC and MLAS
    Experimental structure of beam scanning with two-stage modulation of AFOC and MLAS
    Fig. 20. Experimental structure of beam scanning with two-stage modulation of AFOC and MLAS
    Long-exposure pictures of the linear scanning of MLAS alone and AFOC+MLAS
    Fig. 21. Long-exposure pictures of the linear scanning of MLAS alone and AFOC+MLAS
    Jiaying Liu, Ziqiang Li, Ran Yang, Fan Zou, Xu Yang, Xin Zhou, Ziting Pan, Likang Pan, Yuting Li, Jiali Jiang, Feng Li, Chao Geng, Xinyang Li. Research progress of coherent beam combining technique of phased fiber laser array[J]. High Power Laser and Particle Beams, 2023, 35(4): 041003
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