• High Power Laser and Particle Beams
  • Vol. 33, Issue 8, 081001 (2021)
Ziqiang Li1、2, Xinyang Li1、2、*, Zeyu Gao1、2, and Qiwang Jia1、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
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    DOI: 10.11884/HPLPB202133.210158 Cite this Article
    Ziqiang Li, Xinyang Li, Zeyu Gao, Qiwang Jia. Review of wavefront sensing technology in adaptive optics based on deep learning[J]. High Power Laser and Particle Beams, 2021, 33(8): 081001 Copy Citation Text show less
    Development of Deep Learning
    Fig. 1. Development of Deep Learning
    ANN and the basic operation of a neuron
    Fig. 2. ANN and the basic operation of a neuron
    Optical path of using wavefront sensor based on ANN to correct the aberration of two independent mirrors of MMT
    Fig. 3. Optical path of using wavefront sensor based on ANN to correct the aberration of two independent mirrors of MMT
    Architecture of wavefront sensor based on ANN
    Fig. 4. Architecture of wavefront sensor based on ANN
    Result of the PD model of PD-CNN
    Fig. 5. Result of the PD model of PD-CNN
    Sketch (a) and physical map (b) of the optical system used in the experiment
    Fig. 6. Sketch (a) and physical map (b) of the optical system used in the experiment
    Elongation of spots in the SHWFS. Here, r is the distance of the subaperture in the SHWFS from the center (as projected on to the primary mirror), h0 is the average altitude of the sodium layer, σNA is the thickness of the sodium layer and z is the zenith angle
    Fig. 7. Elongation of spots in the SHWFS. Here, r is the distance of the subaperture in the SHWFS from the center (as projected on to the primary mirror), h0 is the average altitude of the sodium layer, σNA is the thickness of the sodium layer and z is the zenith angle
    Experimental result of centroid computation for Shack-Hartmann wavefront sensor in extreme situations based on the SHNN
    Fig. 8. Experimental result of centroid computation for Shack-Hartmann wavefront sensor in extreme situations based on the SHNN
    Wavefront sensing by using multiple laser guide stars
    Fig. 9. Wavefront sensing by using multiple laser guide stars
    CARMEN with MLP
    Fig. 10. CARMEN with MLP
    Example of the topology of CARMEN with CNN
    Fig. 11. Example of the topology of CARMEN with CNN
    ISNet architecture
    Fig. 12. ISNet architecture
    Statistical results of the RMS wavefront error of five methods in wavefront detection. Each kind of phase screen contains 100 datasets
    Fig. 13. Statistical results of the RMS wavefront error of five methods in wavefront detection. Each kind of phase screen contains 100 datasets
    Physical process and flow chart of the CS-WFS method
    Fig. 14. Physical process and flow chart of the CS-WFS method
    MethodsPerformances
    CEE/pixelFalse RatePV/umRMS/um
    TCoG4.595895.31%2.65930.5349
    SHNN-500.52501.17%0.31070.0651
    Table 1. Results of experiments
    Ziqiang Li, Xinyang Li, Zeyu Gao, Qiwang Jia. Review of wavefront sensing technology in adaptive optics based on deep learning[J]. High Power Laser and Particle Beams, 2021, 33(8): 081001
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