Chinese Optics Letters, Volume. 22, Issue 8, 080501(2024)

Autofocus by Lissajous scanning in time reversal optical scanning holography

Jie Liu1, Haiyan Ou1,2、*, Hua Wang1, Lin Peng3, and Wei Shao2
Author Affiliations
  • 1Shenzhen Institute for Advanced Study, University of Electronic Science and Technology of China, Shenzhen 518000, China
  • 2School of Physics, University of Electronic Science and Technology of China, Chengdu 611731, China
  • 3Key Laboratory of Cognitive Radio and Information Processing, Guilin University of Electronic Technology, Guilin 541004, China
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    Figures & Tables(21)
    OSH system. BS, beam splitter; AOFS, acousto-optic frequency shifter; M, mirror; p(x,y), pupil; L, lens; PD, photodetector; BPF, bandpass filter; LPF, low-pass filter.
    The Lissajous curve and the selected test positions.
    (a) The generated hologram; (b) the first 50 eigenvalues.
    The sum of the pseudo-spectrum along the z axis, with target at (a) (10,6) and (b) (30,10).
    The sum of the pseudo-spectrum along the z axis. (a) Frequency ratio p∶q = 13∶21 or p∶q = 23∶11; (b) phase difference ϕ = 0 or ϕ = π.
    (a) The first 50 eigenvalues of TR matrix; (b) the sum of the pseudo-spectrum along the z axis.
    (a) The first 50 eigenvalues of TR matrix; (b) the sum of pseudo-spectrum of each layer along the z axis.
    The sum of pseudo-spectrum of each layer along the z axis.
    The sum of pseudo-spectrum along the z axis. (a) z1 = 30 mm, z2 = 31.5 mm, (b) z1 = 50 mm, z2 = 51.5 mm, (c) z1 = 70 mm, z2 = 71.5 mm.
    The sum of pseudo-spectrum along the z axis. (a) λ = 405 nm, (b) λ = 780 nm, (c) λ = 980 nm.
    The relationship between SNR and resolution.
    Complex objects (a) at z1 = 30 mm and (b) at z2 = 35 mm.
    (a) The generated hologram; (b) the eigenvalues of TR matrix.
    The proposed method is compared with various positioning methods. (a) Entropy minimization; (b) TR-MUSIC based on diagonal elements.
    The recorded hologram. (a) Real part; (b) imaginary part.
    (a) Eigenvalues of TR matrix; (b) parameters calculated along the z axis obtained by different methods.
    Reconstructed image at (a) z1 and (b) z2.
    • Table 1. Calculation Time and FWHM with Different Frequency Ratios in Lissajous Curve

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      Table 1. Calculation Time and FWHM with Different Frequency Ratios in Lissajous Curve

      pq3∶24∶59∶813∶2119∶2323∶11
      Time (s)33.6935.2435.8731.0934.9131.13
      FWHM0.010.010.010.010.010.01
    • Table 2. Calculation Time and FWHM with Different Phase Differences in Lissajous Curve

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      Table 2. Calculation Time and FWHM with Different Phase Differences in Lissajous Curve

      ϕ0π/4π/23π/4π3π/2
      Time (s)31.2541.5941.6942.2331.2241.24
      FWHM0.010.010.010.010.010.01
    • Table 3. Performance Comparison in Simulation

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      Table 3. Performance Comparison in Simulation

      MethodEntropyDiagonal scanLissajous scan
      Time (s)0.33.835.5
      PPFailed1.471.96
    • Table 4. Performance Comparison in Experiment

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      Table 4. Performance Comparison in Experiment

      MethodEntropyDiagonal scanLissajous scan
      Time (s)1.1218.52281.7
      PPFailed0.210.34
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    Jie Liu, Haiyan Ou, Hua Wang, Lin Peng, Wei Shao, "Autofocus by Lissajous scanning in time reversal optical scanning holography," Chin. Opt. Lett. 22, 080501 (2024)

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    Paper Information

    Category: Diffraction, Gratings, and Holography

    Received: Jan. 20, 2024

    Accepted: Apr. 17, 2024

    Published Online: Aug. 21, 2024

    The Author Email: Haiyan Ou (ouhaiyan@uestc.edu.cn)

    DOI:10.3788/COL202422.080501

    CSTR:32184.14.COL202422.080501

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