• Acta Optica Sinica
  • Vol. 40, Issue 18, 1811001 (2020)
Xingchen Pan1、2, Cheng Liu1、2、*, and Jianqiang Zhu1、2
Author Affiliations
  • 1Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2National Laboratory on High Power Laser and Physics, China Academy of Engineering Physics, Chinese Academy of Sciences, Shanghai 201800, China
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    DOI: 10.3788/AOS202040.1811001 Cite this Article Set citation alerts
    Xingchen Pan, Cheng Liu, Jianqiang Zhu. Iterative Convergence and Reconstruction Uniqueness of Coherent Modulation Imaging[J]. Acta Optica Sinica, 2020, 40(18): 1811001 Copy Citation Text show less
    Basic optical path of CMI algorithm, phase distribution of adopted binary random phase plate, and representative diffraction pattern. (a) Basic optical path of CMI algorithm; (b) phase distribution of adopted binary random phase plate; (c) representative diffraction pattern
    Fig. 1. Basic optical path of CMI algorithm, phase distribution of adopted binary random phase plate, and representative diffraction pattern. (a) Basic optical path of CMI algorithm; (b) phase distribution of adopted binary random phase plate; (c) representative diffraction pattern
    Relationship between B and φ(x) varying with increasing iterations
    Fig. 2. Relationship between B and φ(x) varying with increasing iterations
    Matrix representation of CMI pattern generation
    Fig. 3. Matrix representation of CMI pattern generation
    Scheme of convolution
    Fig. 4. Scheme of convolution
    Basic optical path and simulation results. (a) Amplitude and phase of sample; (b) incident light of modulation plate; (c) spectrum and phase map of modulation plate; (d) pattern recorded by detector without modulation plate (image of sample); (e) diffraction pattern with modulation plate; (f) basic optical path
    Fig. 5. Basic optical path and simulation results. (a) Amplitude and phase of sample; (b) incident light of modulation plate; (c) spectrum and phase map of modulation plate; (d) pattern recorded by detector without modulation plate (image of sample); (e) diffraction pattern with modulation plate; (f) basic optical path
    Reconstructed results with different number of equations. (a) Complete diffraction pattern; (b)--(e) pattern random sampling when Nratio is 0.2, 1, 2, and 5, respectively; (f)--(j) reconstructed results corresponding to Figs. 6(a)--(e)
    Fig. 6. Reconstructed results with different number of equations. (a) Complete diffraction pattern; (b)--(e) pattern random sampling when Nratio is 0.2, 1, 2, and 5, respectively; (f)--(j) reconstructed results corresponding to Figs. 6(a)--(e)
    Error curve and corresponding error gradient curve under different number of equations
    Fig. 7. Error curve and corresponding error gradient curve under different number of equations
    Reconstructed results under different spectral width of modulation plate. (a)--(e) Spectra of different modulators and corresponding phase maps; (f)--(j) diffraction patterns corresponding to Figs. 8(a)--(e); (k)--(o) reconstructed results corresponding to Figs. 8(a)--(e)
    Fig. 8. Reconstructed results under different spectral width of modulation plate. (a)--(e) Spectra of different modulators and corresponding phase maps; (f)--(j) diffraction patterns corresponding to Figs. 8(a)--(e); (k)--(o) reconstructed results corresponding to Figs. 8(a)--(e)
    Error curves and corresponding error gradient curves of reconstructed results with different spectral width of modulation plate
    Fig. 9. Error curves and corresponding error gradient curves of reconstructed results with different spectral width of modulation plate
    Reconstruction results of light to be measured with different sparsity characteristics and same spectrum of modulation plate. (a)--(d) Diffraction patterns under different N″; (e)--(h) reconstructed results corresponding to Figs. 10(a)--(d)
    Fig. 10. Reconstruction results of light to be measured with different sparsity characteristics and same spectrum of modulation plate. (a)--(d) Diffraction patterns under different N″; (e)--(h) reconstructed results corresponding to Figs. 10(a)--(d)
    Reconstructed error under different spot width of light to be measured, without modulation plate. Green dashed line represents critical width
    Fig. 11. Reconstructed error under different spot width of light to be measured, without modulation plate. Green dashed line represents critical width
    Xingchen Pan, Cheng Liu, Jianqiang Zhu. Iterative Convergence and Reconstruction Uniqueness of Coherent Modulation Imaging[J]. Acta Optica Sinica, 2020, 40(18): 1811001
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