• Advanced Photonics
  • Vol. 2, Issue 1, 014003 (2020)
Dalong Qi1, Shian Zhang1、2、*, Chengshuai Yang1, Yilin He1, Fengyan Cao1, Jiali Yao1, Pengpeng Ding1, Liang Gao3, Tianqing Jia1, Jinyang Liang4, Zhenrong Sun1、*, and Lihong V. Wang5、*
Author Affiliations
  • 1East China Normal University, School of Physics and Electric Science, State Key Laboratory of Precision Spectroscopy, Shanghai, China
  • 2Shanxi University, Collaborative Innovation Center of Extreme Optics, Taiyuan, China
  • 3University of Illinois at Urbana-Champaign, Department of Electrical and Computer Engineering, Urbana, Illinois, United States
  • 4Institut National de la Recherche Scientifique, Centre Énergie Matériaux Télécommunications, Laboratory of Applied Computational Imaging, Varennes, Québec, Canada
  • 5California Institute of Technology, Andrew and Peggy Cherng Department of Medical Engineering, Department of Electrical Engineering, Caltech Optical Imaging Laboratory, Pasadena, California, United States
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    DOI: 10.1117/1.AP.2.1.014003 Cite this Article Set citation alerts
    Dalong Qi, Shian Zhang, Chengshuai Yang, Yilin He, Fengyan Cao, Jiali Yao, Pengpeng Ding, Liang Gao, Tianqing Jia, Jinyang Liang, Zhenrong Sun, Lihong V. Wang. Single-shot compressed ultrafast photography: a review[J]. Advanced Photonics, 2020, 2(1): 014003 Copy Citation Text show less
    CUP system configuration. CCD, charge-coupled device; DMD, digital micromirror device; V, sweeping voltage; t, time; x and y, spatial coordinates of the dynamic scene; x′ and y′, spatial coordinates of the streak camera. Since each micromirror (72 mm×72 mm) of the DMD is much larger than the light wavelength, the diffraction angle is small (∼4 deg). With a collecting objective of numerical aperture NA=0.16, the throughput loss caused by the DMD’s diffraction is negligible. Equipment details: camera lens, Fujinon CF75HA-1; DMD, Texas Instruments DLP LightCrafter; microscope objective, Olympus UPLSAPO 4X; tube lens, Thorlabs AC254-150-A; streak camera, Hamamatsu C7700; CCD, Hamamatsu ORCA-R2. Figure reprinted from Ref. 19.
    Fig. 1. CUP system configuration. CCD, charge-coupled device; DMD, digital micromirror device; V, sweeping voltage; t, time; x and y, spatial coordinates of the dynamic scene; x and y, spatial coordinates of the streak camera. Since each micromirror (72  mm×72  mm) of the DMD is much larger than the light wavelength, the diffraction angle is small (4  deg). With a collecting objective of numerical aperture NA=0.16, the throughput loss caused by the DMD’s diffraction is negligible. Equipment details: camera lens, Fujinon CF75HA-1; DMD, Texas Instruments DLP LightCrafter; microscope objective, Olympus UPLSAPO 4X; tube lens, Thorlabs AC254-150-A; streak camera, Hamamatsu C7700; CCD, Hamamatsu ORCA-R2. Figure reprinted from Ref. 19.
    Data flow of CUP in (a) data acquisition and (b) image reconstruction.
    Fig. 2. Data flow of CUP in (a) data acquisition and (b) image reconstruction.
    (a) Flow chart for optimizing the encoding mask in a CUP system based on GA. (b), (c) The experimental results for a spatially modulated picosecond laser pulse evolution obtained by (b) optimal codes and (c) random codes. TwIST: two-step iterative shrinkage/thresholding.28" target="_self" style="display: inline;">28 Figures reprinted from Ref. 29.
    Fig. 3. (a) Flow chart for optimizing the encoding mask in a CUP system based on GA. (b), (c) The experimental results for a spatially modulated picosecond laser pulse evolution obtained by (b) optimal codes and (c) random codes. TwIST: two-step iterative shrinkage/thresholding.28 Figures reprinted from Ref. 29.
    A schematic diagram of data acquisition in multiencoding CUP. Here, t and t′ are time; Ck is the spatial encoding operator; S is the temporal shearing operator; T is the spatiotemporal integration operator. Figure reprinted from Ref. 29.
    Fig. 4. A schematic diagram of data acquisition in multiencoding CUP. Here, t and t are time; Ck is the spatial encoding operator; S is the temporal shearing operator; T is the spatiotemporal integration operator. Figure reprinted from Ref. 29.
    Schematic diagram of the T-CUP system. Inset (black dashed box): detailed illustration of the streak tube. MCP, microchannel plate. Figure reprinted from Ref. 34.
    Fig. 5. Schematic diagram of the T-CUP system. Inset (black dashed box): detailed illustration of the streak tube. MCP, microchannel plate. Figure reprinted from Ref. 34.
    (a) An experimental diagram of imaging a superluminal propagation, showing experimental results obtained by the (b) AL algorithm and (c) TwIST algorithm. Figures reprinted from Ref. 36.
    Fig. 6. (a) An experimental diagram of imaging a superluminal propagation, showing experimental results obtained by the (b) AL algorithm and (c) TwIST algorithm. Figures reprinted from Ref. 36.
    The experimental results of imaging a picosecond laser pulse propagation. The frame at t=170 ps is shown as reconstructed by the (a) TwIST and (b) SIC algorithms; (c) image profiles along the blue lines indicated in (a) and (b). Figures reprinted from Ref. 37.
    Fig. 7. The experimental results of imaging a picosecond laser pulse propagation. The frame at t=170  ps is shown as reconstructed by the (a) TwIST and (b) SIC algorithms; (c) image profiles along the blue lines indicated in (a) and (b). Figures reprinted from Ref. 37.
    A schematic diagram of the CUST technique. Figure reprinted with permission from Ref. 43.
    Fig. 8. A schematic diagram of the CUST technique. Figure reprinted with permission from Ref. 43.
    The theoretical designs of (a) CUEDI, (b) CUTEM, and (c) dual-shearing CUTEM. Figures reprinted from Refs. 44 and 45.
    Fig. 9. The theoretical designs of (a) CUEDI, (b) CUTEM, and (c) dual-shearing CUTEM. Figures reprinted from Refs. 44 and 45.
    The experimental setup of COSUP. Figure reprinted from Ref. 46.
    Fig. 10. The experimental setup of COSUP. Figure reprinted from Ref. 46.
    (a) Spectral separation unit of the dual-color CUP system; (b) an ultrafast laser-induced fluorescence process revealed by dual-color CUP; (c) the photonic Mach cone dynamics obtained by LLE-CUP. Figures reprinted from Refs. 19 and 33.
    Fig. 11. (a) Spectral separation unit of the dual-color CUP system; (b) an ultrafast laser-induced fluorescence process revealed by dual-color CUP; (c) the photonic Mach cone dynamics obtained by LLE-CUP. Figures reprinted from Refs. 19 and 33.
    3-D images of (a) static targets and (b) two-ball rotation, obtained by CUP. Figures reprinted from Ref. 35.
    Fig. 12. 3-D images of (a) static targets and (b) two-ball rotation, obtained by CUP. Figures reprinted from Ref. 35.
    Spatiotemporal evolutions of (a) a dual-color picosecond laser field and (b) the temporal focusing of a femtosecond laser pulse. Figures reprinted from Refs. 34 and 87.
    Fig. 13. Spatiotemporal evolutions of (a) a dual-color picosecond laser field and (b) the temporal focusing of a femtosecond laser pulse. Figures reprinted from Refs. 34 and 87.
    A schematic diagram of the experimental design of compressed 3-D image information secure communication. Figure reprinted from Ref. 107.
    Fig. 14. A schematic diagram of the experimental design of compressed 3-D image information secure communication. Figure reprinted from Ref. 107.
    Dalong Qi, Shian Zhang, Chengshuai Yang, Yilin He, Fengyan Cao, Jiali Yao, Pengpeng Ding, Liang Gao, Tianqing Jia, Jinyang Liang, Zhenrong Sun, Lihong V. Wang. Single-shot compressed ultrafast photography: a review[J]. Advanced Photonics, 2020, 2(1): 014003
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