• Chinese Optics Letters
  • Vol. 16, Issue 4, 041102 (2018)
Bin Zhuang1、2, Chengfang Xu1、2、3, Yi Geng1、2, Guangzhi Zhao1、2, Hui Chen1、2, Zhengquan He1, Zhaoxin Wu3, and Liyong Ren1、*
Author Affiliations
  • 1Research Department of Information Photonics, Xi’an Institute of Optics and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Department of Electronics Science and Technology, School of Electronic & Information Engineering, Xi’an Jiaotong University, Xi’an 710049, China
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    DOI: 10.3788/COL201816.041102 Cite this Article Set citation alerts
    Bin Zhuang, Chengfang Xu, Yi Geng, Guangzhi Zhao, Hui Chen, Zhengquan He, Zhaoxin Wu, Liyong Ren. Round-trip imaging through scattering media based on optical transmission matrix[J]. Chinese Optics Letters, 2018, 16(4): 041102 Copy Citation Text show less
    Schematic of the round-trip imaging through a scattering medium.
    Fig. 1. Schematic of the round-trip imaging through a scattering medium.
    Experimental setup. Scattering medium (Thorlabs Optics 220 grit ground-glass diffuser); DMD, digital micromirror devices (ViALUX, V-7001VIS, 1024 pixel×768 pixel); SLM, spatial light modulator (Meadowlark Optics, P1920-0635-HDMI); CCD (Hamamatsu, C13440-20CU, 2048 pixel×2048 pixel, the central 2048 pixel×1536 pixel area is used for imaging); L, lens; P, polarizer; BS, beam splitter; A, attenuation film.
    Fig. 2. Experimental setup. Scattering medium (Thorlabs Optics 220 grit ground-glass diffuser); DMD, digital micromirror devices (ViALUX, V-7001VIS, 1024pixel×768pixel); SLM, spatial light modulator (Meadowlark Optics, P1920-0635-HDMI); CCD (Hamamatsu, C13440-20CU, 2048pixel×2048pixel, the central 2048pixel×1536pixel area is used for imaging); L, lens; P, polarizer; BS, beam splitter; A, attenuation film.
    Typical measured T(x,y;ξ,η) elements. (a) Amplitude and (b) corresponding phase, respectively. Scale bars: 4000 μm; color bar: phase in radian.
    Fig. 3. Typical measured T(x,y;ξ,η) elements. (a) Amplitude and (b) corresponding phase, respectively. Scale bars: 4000 μm; color bar: phase in radian.
    Reconstruction of the object constructed by DMD. (a) A binary amplitude object constructed by using DMD. (b) Output speckle image of the object captured by CCD. (c) Interference image of the object wave and the reference wave. (d), (e) Amplitude and phase of E(x,y), respectively. (f) Recovered object. Scale bars indicate 1000 μm in (a), (f) and 2000 μm in (b), (c), (d), (e). Color bar: phase in radian.
    Fig. 4. Reconstruction of the object constructed by DMD. (a) A binary amplitude object constructed by using DMD. (b) Output speckle image of the object captured by CCD. (c) Interference image of the object wave and the reference wave. (d), (e) Amplitude and phase of E(x,y), respectively. (f) Recovered object. Scale bars indicate 1000 μm in (a), (f) and 2000 μm in (b), (c), (d), (e). Color bar: phase in radian.
    Reconstruction of the real target object. (a) USAF 1951 test pattern. (b) Output speckle image of the object. (c) Recovered object. Scale bars indicate 300 μm in (a), (c) and 2000 μm in (b).
    Fig. 5. Reconstruction of the real target object. (a) USAF 1951 test pattern. (b) Output speckle image of the object. (c) Recovered object. Scale bars indicate 300 μm in (a), (c) and 2000 μm in (b).
    (a) Speckle pattern of the illumination wave. (b) Object constructed using the DMD. (c) Intensity of the reflected wave of the object. Scale bar: 1000 μm.
    Fig. 6. (a) Speckle pattern of the illumination wave. (b) Object constructed using the DMD. (c) Intensity of the reflected wave of the object. Scale bar: 1000 μm.
    Bin Zhuang, Chengfang Xu, Yi Geng, Guangzhi Zhao, Hui Chen, Zhengquan He, Zhaoxin Wu, Liyong Ren. Round-trip imaging through scattering media based on optical transmission matrix[J]. Chinese Optics Letters, 2018, 16(4): 041102
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