• Photonics Research
  • Vol. 10, Issue 9, 2157 (2022)
Wenjie Jiang1, Yongkai Yin1, Junpeng Jiao2, Xian Zhao2、3, and Baoqing Sun1、*
Author Affiliations
  • 1School of Information Science and Engineering, Shandong Universityhttps://ror.org/0207yh398https://ror.org/0207yh398, Qingdao 266237, China
  • 2Key Laboratory of Laser & Infrared System, Ministry of Education, Qingdao 266237, China
  • 3Center for Optics Research and Engineering, Shandong University, Qingdao 266237, China
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    DOI: 10.1364/PRJ.461064 Cite this Article Set citation alerts
    Wenjie Jiang, Yongkai Yin, Junpeng Jiao, Xian Zhao, Baoqing Sun. 2,000,000 fps 2D and 3D imaging of periodic or reproducible scenes with single-pixel detectors[J]. Photonics Research, 2022, 10(9): 2157 Copy Citation Text show less

    Abstract

    Single-pixel imaging (SPI) can capture 2D images of the target with only a nonpixelated detector, showing promising application potential in nonvisible spectral imaging, low-photon imaging, lidar, and other extreme imaging fields. However, the imaging mechanism of traditional SPI makes it difficult to achieve high imaging speed, which is a primary barrier for its widespread application. To address this issue, in this work, we propose and demonstrate a novel high-speed 2D and 3D imaging scheme based on traditional SPI, termed time-resolved single-pixel imaging (TRSPI). Previous SPI works mainly utilize correlation between a stable target and iterative illumination masks to reconstruct a single image. In TRSPI, by further exploiting correlation information between a dynamic scene and every static mask, we can reconstruct a series of time-varying images of the dynamic scene, given the dynamic scene is repetitive or reproducible. Experimentally, we conducted 2D and 3D imaging on a rotating chopper with a speed of 4800 revolutions per minute (rpm), and imaging speeds up to 2,000,000 fps. It is believed that this technology not only opens up a novel application direction for SPI, but also will provide a powerful solution for high-speed imaging.
    Y=AX,

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    ym=p=1Pamp·xp.

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    X^=AY.

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    X^=argminX12YAX22+λΨ(X),

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    ymt=p=1Pamp·xpt.

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    X^(ti)=AY(ti),

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    X^(ti)=argminX(ti)12Y(ti)AX(ti)22+λΨ[X(ti)].

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    I0(x,y)=a0+b0cos[φ0(x,y)].

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    Id(x,y)=a(x,y)+b(x,y)cos[φ(x,y)].

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    Id(x,y)=a(x,y)+b(x,y)2[eiφ(x,y)+eiφ(x,y)].

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    If(x,y)=b(x,y)2eiφ(x,y).

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    φ(x,y)=arctan{Im[If{x,y}]Re[If{x,y}]}.

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    h(x,y)=S[φ(x,y)φ0(x,y)]=S[Δφ(x,y)].

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    Wenjie Jiang, Yongkai Yin, Junpeng Jiao, Xian Zhao, Baoqing Sun. 2,000,000 fps 2D and 3D imaging of periodic or reproducible scenes with single-pixel detectors[J]. Photonics Research, 2022, 10(9): 2157
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