• Infrared and Laser Engineering
  • Vol. 50, Issue 12, 20211059 (2021)
Zhentao Liu1, Chenyu Hu1、2, Zhishen Tong1, Chunyan Chu3, and Shensheng Han1、2、*
Author Affiliations
  • 1Key Laboratory for Quantum Optics of CAS, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou 310024, China
  • 3Beijing Key Laboratory for Precision Optoelectronic Measurement Instrument and Technology, School of Optics and Photonics, Beijing Institute of Technology, Beijing 100081, China
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    DOI: 10.3788/IRLA20211059 Cite this Article
    Zhentao Liu, Chenyu Hu, Zhishen Tong, Chunyan Chu, Shensheng Han. Some research progress on the theoretical study of ghost imaging in Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences (Invited)[J]. Infrared and Laser Engineering, 2021, 50(12): 20211059 Copy Citation Text show less
    Schematic diagram of the apparatus in HBT experiment[1]
    Fig. 1. Schematic diagram of the apparatus in HBT experiment[1]
    Diagram of classical ghost imaging with two arms[41]
    Fig. 2. Diagram of classical ghost imaging with two arms[41]
    Diagram of ghost imaging based on time-domain ensemble statistics
    Fig. 3. Diagram of ghost imaging based on time-domain ensemble statistics
    Diagram of ghost imaging camera[18]
    Fig. 4. Diagram of ghost imaging camera[18]
    Simulation target image of real-space ghost imaging
    Fig. 5. Simulation target image of real-space ghost imaging
    Comparison of variance distribution of simulated results in real-space ghost imaging with theoretical results at different SNRs in object light path. (a) ; (b) 不同物光路探测信噪比下,实空间鬼成像关联结果的仿真方差分布与理论比较。(a)信噪比;(b)信噪比
    Fig. 6. Comparison of variance distribution of simulated results in real-space ghost imaging with theoretical results at different SNRs in object light path. (a) ; (b) 不同物光路探测信噪比下,实空间鬼成像关联结果的仿真方差分布与理论比较。(a)信噪比 ;(b)信噪比
    Simulated target in Fourier diffraction ghost imaging (a) and its Fourier spectrum (b)
    Fig. 7. Simulated target in Fourier diffraction ghost imaging (a) and its Fourier spectrum (b)
    Comparison of variance distribution of simulated results in Fourier diffraction ghost imaging with theoretical results at different SNRs. (a) ;(b) 不同物光路探测信噪比下,傅里叶衍射鬼成像关联结果的仿真方差分布与理论比较。 (a)信噪比;(b)信噪比
    Fig. 8. Comparison of variance distribution of simulated results in Fourier diffraction ghost imaging with theoretical results at different SNRs. (a) ;(b) 不同物光路探测信噪比下,傅里叶衍射鬼成像关联结果的仿真方差分布与理论比较。 (a)信噪比 ;(b)信噪比
    Fisher information of different ranges of values of as a function of relative intensity [77]不同取值范围的的Fisher信息与相对强度系数的关系曲线[77]
    Fig. 9. Fisher information of different ranges of values of as a function of relative intensity [77]不同取值范围的 的Fisher信息与相对强度系数 的关系曲线[77]
    Diffraction spectrum images obtained via conditional averaging on two equally-divided parts. (a) Positive image; (b) Negative image; (c) Subtraction image of positive images and negative images; (d) Diffraction spectrum image of reference object[77]
    Fig. 10. Diffraction spectrum images obtained via conditional averaging on two equally-divided parts. (a) Positive image; (b) Negative image; (c) Subtraction image of positive images and negative images; (d) Diffraction spectrum image of reference object[77]
    Simulation results. (a) Retrieved image via conditional average; (b) Retrieved image via original fluctuation relation[77]
    Fig. 11. Simulation results. (a) Retrieved image via conditional average; (b) Retrieved image via original fluctuation relation[77]
    Experiment results. (a) Retrieved image via conditional average; (b) Retrieved image via original fluctuation correlation[77]
    Fig. 12. Experiment results. (a) Retrieved image via conditional average; (b) Retrieved image via original fluctuation correlation[77]
    Statistical resolution limit of ghost imaging camera in (x, λ) light-field space[10], and are the nearest resolved spatial distance and spectral distance among K points, respectively, with K=2,3,5,7. is Rayleigh’s spatial resolution criterion, and is the spectral resolution of ghost imaging camera鬼成像相机在高维空间(x ,λ)中的统计分辨率极限[10],其中和分别为在高维空间中个点能分辨的最近空间距离和光谱距离,分别取=2,3,5,7。为空间分辨率瑞利判据,为鬼成像相机的光谱分辨率
    Fig. 13. Statistical resolution limit of ghost imaging camera in (x, λ) light-field space[10], and are the nearest resolved spatial distance and spectral distance among K points, respectively, with K=2,3,5,7. is Rayleigh’s spatial resolution criterion, and is the spectral resolution of ghost imaging camera 鬼成像相机在高维空间(x ,λ)中的统计分辨率极限[10],其中 和 分别为在高维空间中 个点能分辨的最近空间距离和光谱距离,分别取 =2,3,5,7。 为空间分辨率瑞利判据, 为鬼成像相机的光谱分辨率
    Zhentao Liu, Chenyu Hu, Zhishen Tong, Chunyan Chu, Shensheng Han. Some research progress on the theoretical study of ghost imaging in Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences (Invited)[J]. Infrared and Laser Engineering, 2021, 50(12): 20211059
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