• Collection Of theses on high power laser and plasma physics
  • Vol. 14, Issue 1, 71203 (2016)
Hua Tao1,2, Suhas P. Veetil3, Xingchen Pan1,2, Cheng Liu1, and Jianqiang Zhu1,*
Author Affiliations
  • 1Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2University of Chinese academy of sciences, Beijing 100049, China
  • 3Department of Engineering Technology and Science, Higher Colleges of Technology, Fujairah 4114, United Arab Emirates
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    DOI: 10.3788/col201614.071203 Cite this Article
    Hua Tao, Suhas P. Veetil, Xingchen Pan, Cheng Liu, Jianqiang Zhu. Lens-free coherent modulation imaging with collimated illumination[J]. Collection Of theses on high power laser and plasma physics, 2016, 14(1): 71203 Copy Citation Text show less
    Schematic of lens-free CMI method.
    Fig. 1. Schematic of lens-free CMI method.
    Flowchart of the proposed method.
    Fig. 2. Flowchart of the proposed method.
    (a) The amplitude and (b) phase distribution of O(x,y) of the RPP obtained with the ePIE algorithm.
    Fig. 3. (a) The amplitude and (b) phase distribution of O(x,y) of the RPP obtained with the ePIE algorithm.
    Recorded diffraction pattern and field reconstructions for the incident beam. (a) The diffraction pattern recorded by CCD, (b) the Fourier components of the exit incident beam, (c) reconstructed amplitude and (d) phase distribution of illumination on the RPP plane. (e) Obtained amplitude and (f) phase distribution of the incident beam.
    Fig. 4. Recorded diffraction pattern and field reconstructions for the incident beam. (a) The diffraction pattern recorded by CCD, (b) the Fourier components of the exit incident beam, (c) reconstructed amplitude and (d) phase distribution of illumination on the RPP plane. (e) Obtained amplitude and (f) phase distribution of the incident beam.
    Recorded diffraction pattern and reconstructed fields when a biological specimen (a pumpkin stem) is used as the sample. (a) The diffraction pattern recorded by CCD, (b) the Fourier components of the exit wave field of the sample, (c) the reconstructed amplitude, and (d) the phase distribution of illumination on the RPP. The reconstructed (e) amplitude and (f) phase distribution of the sample.
    Fig. 5. Recorded diffraction pattern and reconstructed fields when a biological specimen (a pumpkin stem) is used as the sample. (a) The diffraction pattern recorded by CCD, (b) the Fourier components of the exit wave field of the sample, (c) the reconstructed amplitude, and (d) the phase distribution of illumination on the RPP. The reconstructed (e) amplitude and (f) phase distribution of the sample.
    Convergence curves obtained as a function of the number of iterations with different parameters of rn, α, and β.
    Fig. 6. Convergence curves obtained as a function of the number of iterations with different parameters of rn, α, and β.
    USAF 1951 target is placed at the sample plane. The reconstructed (a) amplitude and (b) phase distribution of the transmitted field of the USAF 1951 target.
    Fig. 7. USAF 1951 target is placed at the sample plane. The reconstructed (a) amplitude and (b) phase distribution of the transmitted field of the USAF 1951 target.
    Hua Tao, Suhas P. Veetil, Xingchen Pan, Cheng Liu, Jianqiang Zhu. Lens-free coherent modulation imaging with collimated illumination[J]. Collection Of theses on high power laser and plasma physics, 2016, 14(1): 71203
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