• Chinese Optics Letters
  • Vol. 22, Issue 11, 111101 (2024)
Weitao Liu1,2,3,*, Wenlin Gong4,5,**, Zhentao Liu6,7,8,***, Shuai Sun1,2,3, and Zhenwu Nie1,2,3
Author Affiliations
  • 1Institute for Quantum Science and Technology, College of Science, National University of Defense Technology, Changsha 410073, China
  • 2Interdisciplinary Center of Quantum Information, National University of Defense Technology, Changsha 410073, China
  • 3Hunan Key Laboratory of Mechanism and Technology of Quantum Information, Changsha 410073, China
  • 4School of Optoelectronic Science and Engineering, Soochow University, Suzhou 215006, China
  • 5Key Laboratory of Advanced Optical Manufacturing Technologies of Jiangsu Province, Soochow University, Suzhou 215006, China
  • 6Key Laboratory of Quantum Optics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 7Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of Sciences, Beijing 100049, China
  • 8Wangzhijiang Innovation Center for Laser, Aerospace Laser Technology and System Department, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
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    DOI: 10.3788/COL202422.111101 Cite this Article Set citation alerts
    Weitao Liu, Wenlin Gong, Zhentao Liu, Shuai Sun, Zhenwu Nie, "Progress and applications of ghost imaging with classical sources: a brief review [Invited]," Chin. Opt. Lett. 22, 111101 (2024) Copy Citation Text show less

    Abstract

    Study on optical correlation function initiates the development of many quantum techniques, with ghost imaging (GI) being one of the great achievements. Upon the first demonstration with entangled sources, the physics and improvements of GI attracted much interest. Among existing studies, GI with classical sources provoked debates and ideas to the most extent. Toward better understanding and practical applications of GI, fundamental theory, various designs of illumination patterns as well as reconstruction algorithms, demonstrations and field tests have been reported, with the topic of GI very much enriched. In this paper, we try to sketch the evolution of GI, focusing mainly on the basic idea, the properties and superiority, progress toward applications of GI with classical sources, and provide our discussion looking into the future.
    G(2)(x,x)=Ir(x)Io(x)Ir(x)Io(x),

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    ho(x;xi)=O(x)hr(x;xr),

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    G(2)(x)=BIr(x)BIr(x)=dxO(x)Ir(x)Ir(x)dxO(x)Ir(x)Ir(x)=1αO(x)g(2)(x,x),

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    g(2)(x,x)=Ir(x)Ir(x)Ir(x)Ir(x)

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    g(2)(x0,x0)={δ(x0x0),entangled1+δ(x0x0),classical.

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    ΔG(x)=BIr(x)BIr(x)BIr(x)=ΔBΔIr(x)BIr(x),

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    B=AO.

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    O^GI=ATB=ATAO,

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    g(2)(x,x=0)=I(x)I(x=0)I(x)I(x=0),

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    Mc=(AIsA¯)TA,

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    SNRGI=[ΔOGI(x)]min2ΔOGI2(x)=NΔTmin2ns,

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    Weitao Liu, Wenlin Gong, Zhentao Liu, Shuai Sun, Zhenwu Nie, "Progress and applications of ghost imaging with classical sources: a brief review [Invited]," Chin. Opt. Lett. 22, 111101 (2024)
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