• Chinese Optics Letters
  • Vol. 18, Issue 7, 071101 (2020)
Zijie Li1, Qing Zhao1、*, and Wenlin Gong2、**
Author Affiliations
  • 1Center for Quantum Technology Research, School of Physics, Beijing Institute of Technology, Beijing 100081, China
  • 2Key Laboratory for Quantum Optics and Center for Cold Atom Physics of CAS, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
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    DOI: 10.3788/COL202018.071101 Cite this Article Set citation alerts
    Zijie Li, Qing Zhao, Wenlin Gong. Performance comparison of ghost imaging versus conventional imaging in photon shot noise cases[J]. Chinese Optics Letters, 2020, 18(7): 071101 Copy Citation Text show less

    Abstract

    The performances of ghost imaging and conventional imaging in photon shot noise cases are investigated. We define an imaging signal-to-noise ratio called SNRtran where only the object’s transmission region is used to evaluate the imaging quality and it can be applied to ghost imaging (GI) with any random pattern. Both the values SNRGItran of GI and SNRCItran of conventional imaging in photon shot noise cases are deduced from a simple statistical analysis. The analytical results, which are backed up by numerical simulations, demonstrate that the value SNRGItran is related to the ratio between the object’s transmission area Ao and the number density of photons illuminating the object plane Io, which is similar to the theoretical results based on the first principle of GI with a Gaussian speckle field deduced by B. I. Erkmen and J. H. Shapiro [in Adv. Opt. Photonics 2, 405–450 (2010)]. In addition, we also show that the value SNRCItran will be larger than SNRGItran when Ao is beyond a threshold value.
    OGI(x,y)=1Ks=1K[Irs(x,y)Irs(x,y)]IBs=1Ks=1KΔIrs(x,y)IBs,(1)

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    IBs=Isignals+Inoises,s=1,2,...,K,(2)

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    DSNRGI=10×log10[Isignalsstd(Inoises)]10×log10(Isignals)=10×log10(IoAo),(3)

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    OGI(x,y)=1Ks=1KΔIrs(x,y)(Isignals+Inoises)=1Ks=1KΔIrs(x,y)ΔIsignals+1Ks=1KIrs(x,y)ΔInoises=Io2[O(x,y)μ(x,y)+AoKs=1KIrs(x,y)Iostd(Inoises)Isignalsfs]Io2[O(x,y)μ(x,y)+AoKIos=1KIrs(x,y)Iofs]=Io2[O(x,y)μ(x,y)+AoIoN(x,y)],(4)

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    SNRGItran=10×log10[O¯GItranδ(OGItran)],(5)

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    DSNRCI=SNRCItran=10×log10(Iphoton),(6)

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    Zijie Li, Qing Zhao, Wenlin Gong. Performance comparison of ghost imaging versus conventional imaging in photon shot noise cases[J]. Chinese Optics Letters, 2020, 18(7): 071101
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