• Acta Optica Sinica
  • Vol. 38, Issue 9, 0901005 (2018)
Boqing Pang1、2、3、*, Shuai Wang1、3, and Ping Yang1、3、*
Author Affiliations
  • 1 Key Laboratory of Adaptive Optics, Chinese Academy of Sciences, Chengdu, Sichuan 610209, China
  • 2 University of Chinese Academy of Sciences, Beijing 100049, China
  • 3 Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu, Sichuan 610209, China
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    DOI: 10.3788/AOS201838.0901005 Cite this Article Set citation alerts
    Boqing Pang, Shuai Wang, Ping Yang. Wavefront Reconstruction Based on Truncated Modulation Modes[J]. Acta Optica Sinica, 2018, 38(9): 0901005 Copy Citation Text show less
    Optical setup for wavefront measurement
    Fig. 1. Optical setup for wavefront measurement
    Walsh functions. (a) Segments formed by divided unit circle; (b) Walsh functions in polar coordinates (Black areas are assigned value of 1, white areas are assigned value of -1)
    Fig. 2. Walsh functions. (a) Segments formed by divided unit circle; (b) Walsh functions in polar coordinates (Black areas are assigned value of 1, white areas are assigned value of -1)
    Equivalent matrix of wavefront
    Fig. 3. Equivalent matrix of wavefront
    Mean value of absolute value of Walsh function coefficient
    Fig. 4. Mean value of absolute value of Walsh function coefficient
    Incident wavefront (PV is 1.43λ,RMS is 0.31λ)
    Fig. 5. Incident wavefront (PV is 1.43λ,RMS is 0.31λ)
    RMS of residual wavefront reconstructed with different number of Walsh functions
    Fig. 6. RMS of residual wavefront reconstructed with different number of Walsh functions
    Reconstructed real part of optical field
    Fig. 7. Reconstructed real part of optical field
    Reconstructed imaginary part of optical field with selected 64 Walsh functions. (a) Absolute value of reconstructed imaginary part of optical field; (b) reconstructed imaginary part of optical field
    Fig. 8. Reconstructed imaginary part of optical field with selected 64 Walsh functions. (a) Absolute value of reconstructed imaginary part of optical field; (b) reconstructed imaginary part of optical field
    Reconstructed discrete wavefront. (a) Wrapped wavefront; (b) unwrapped wavefront
    Fig. 9. Reconstructed discrete wavefront. (a) Wrapped wavefront; (b) unwrapped wavefront
    (a) Wavefront after smoothing; (b) residual wavefront (PV is 0.074λ,RMS is 0.0086λ)
    Fig. 10. (a) Wavefront after smoothing; (b) residual wavefront (PV is 0.074λ,RMS is 0.0086λ)
    Wavefront reconstructed with the first 256 Walsh functions. (a) Reconstructed wavefront; (b) residual wavefront (PV is 2.30×10-3λ,RMS is 1.58×10-4λ)
    Fig. 11. Wavefront reconstructed with the first 256 Walsh functions. (a) Reconstructed wavefront; (b) residual wavefront (PV is 2.30×10-3λ,RMS is 1.58×10-4λ)
    Wavefront reconstructed results when signal-to-noise ratio of thermal noise is 30 dB. (a) Unwrapped discrete wavefront; (b) reconstructed wavefront; (c) residual wavefront between unwrapped discrete wavefront and incident wavefront; (d) residual wavefront of reconstructed wavefront (PV is 0.47λ,RMS is 0.045λ)
    Fig. 12. Wavefront reconstructed results when signal-to-noise ratio of thermal noise is 30 dB. (a) Unwrapped discrete wavefront; (b) reconstructed wavefront; (c) residual wavefront between unwrapped discrete wavefront and incident wavefront; (d) residual wavefront of reconstructed wavefront (PV is 0.47λ,RMS is 0.045λ)
    Boqing Pang, Shuai Wang, Ping Yang. Wavefront Reconstruction Based on Truncated Modulation Modes[J]. Acta Optica Sinica, 2018, 38(9): 0901005
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