• Chinese Optics Letters
  • Vol. 20, Issue 9, 091102 (2022)
Pengwei Wang1、2, Zhentao Liu1、2、*, Jianrong Wu1, Xia Shen1, and Shensheng Han1、2、3
Author Affiliations
  • 1Key Laboratory of Quantum Optics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou 310024, China
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    DOI: 10.3788/COL202220.091102 Cite this Article Set citation alerts
    Pengwei Wang, Zhentao Liu, Jianrong Wu, Xia Shen, Shensheng Han. Dispersion control of broadband super-Rayleigh speckles for snapshot spectral ghost imaging[J]. Chinese Optics Letters, 2022, 20(9): 091102 Copy Citation Text show less
    Schematic of snapshot spectral ghost imaging with broadband super-Rayleigh speckles. (a) is the object plane; (b) is the first imaging plane; (c) is the virtual speckle plane; (d) is the speckle plane.
    Fig. 1. Schematic of snapshot spectral ghost imaging with broadband super-Rayleigh speckles. (a) is the object plane; (b) is the first imaging plane; (c) is the virtual speckle plane; (d) is the speckle plane.
    Numerical simulation results for the speckle contrast varied with the system parameters z1, z2′, and λ. (a) The simulation results of the speckle contrast varied with the system parameters z1 and λ. Here, z2′ = 10.6 mm. (b) The simulation results of the speckle contrast varied with the system parameters z2′ and λ. Here, z1 = 60 mm. The solid black line is the theoretical curve based on Eq. (4).
    Fig. 2. Numerical simulation results for the speckle contrast varied with the system parameters z1, z2′, and λ. (a) The simulation results of the speckle contrast varied with the system parameters z1 and λ. Here, z2′ = 10.6 mm. (b) The simulation results of the speckle contrast varied with the system parameters z2′ and λ. Here, z1 = 60 mm. The solid black line is the theoretical curve based on Eq. (4).
    (a) Simulation speckles of different wavelengths on the detection plane. AP: the amplitude and phase of Uslm (r0, λ0) were extracted to the SLM. P: the phase-only of Uslm (r0, λ0) was extracted to the SLM. (b) Probability distribution of the normalized intensity of the speckles. (c) Simulation results of the speckle contrast when the dispersion of the lens satisfied Eq. (7) (marked as designed lens), and the lens of focal length f was achromatic (marked as achromatic lens). The theoretical curve, according to Eq. (5), is also represented with the black line. (d) Theoretical curve and simulated curve of the correlation function for speckles generated by two points at the same wavelength and different positions with a distance Δro. (e) Theoretical and simulated curves of the correlation function of the speckles generated by two points at the same position and different wavelengths with a gap Δλ.
    Fig. 3. (a) Simulation speckles of different wavelengths on the detection plane. AP: the amplitude and phase of Uslm (r0, λ0) were extracted to the SLM. P: the phase-only of Uslm (r0, λ0) was extracted to the SLM. (b) Probability distribution of the normalized intensity of the speckles. (c) Simulation results of the speckle contrast when the dispersion of the lens satisfied Eq. (7) (marked as designed lens), and the lens of focal length f was achromatic (marked as achromatic lens). The theoretical curve, according to Eq. (5), is also represented with the black line. (d) Theoretical curve and simulated curve of the correlation function for speckles generated by two points at the same wavelength and different positions with a distance Δro. (e) Theoretical and simulated curves of the correlation function of the speckles generated by two points at the same position and different wavelengths with a gap Δλ.
    (a) Experimental setup of the snapshot spectral ghost imaging with broadband super-Rayleigh speckles. The calibration setup shown in the bottom box was adopted instead of the object in the black box when calibrating. The SCL was a supercontinuum laser. (b) Dispersion curves of lenses used in the experiment.
    Fig. 4. (a) Experimental setup of the snapshot spectral ghost imaging with broadband super-Rayleigh speckles. The calibration setup shown in the bottom box was adopted instead of the object in the black box when calibrating. The SCL was a supercontinuum laser. (b) Dispersion curves of lenses used in the experiment.
    (a) Curve of the correlation function of the experimental speckles generated by two points at the same wavelength and different positions with a distance Δro. (b) Curve of the correlation function of the experimental speckles generated by two points at the same position and different wavelengths with a gap Δλ. (c) The experimental speckles of snapshot spectral ghost imaging with broadband super-Rayleigh speckles at different wavelengths. (d) The contrast of speckles of the corresponding groups.
    Fig. 5. (a) Curve of the correlation function of the experimental speckles generated by two points at the same wavelength and different positions with a distance Δro. (b) Curve of the correlation function of the experimental speckles generated by two points at the same position and different wavelengths with a gap Δλ. (c) The experimental speckles of snapshot spectral ghost imaging with broadband super-Rayleigh speckles at different wavelengths. (d) The contrast of speckles of the corresponding groups.
    Experimental imaging results with different exposure times, while the sampling rate remained at 40%. The mPSNR and mSSIM are also shown. (a) Exposure time of 50 ms. (b) Exposure time of 10 ms.
    Fig. 6. Experimental imaging results with different exposure times, while the sampling rate remained at 40%. The mPSNR and mSSIM are also shown. (a) Exposure time of 50 ms. (b) Exposure time of 10 ms.
    Pengwei Wang, Zhentao Liu, Jianrong Wu, Xia Shen, Shensheng Han. Dispersion control of broadband super-Rayleigh speckles for snapshot spectral ghost imaging[J]. Chinese Optics Letters, 2022, 20(9): 091102
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