Chinese Journal of Quantum Electronics, Volume. 41, Issue 1, 67(2024)

Aberration optimization method for aspherical catadioptric imaging system with large acceptance aperture based on sixth-order wave aberration theory

CAO Yiqing1、*, SHEN Zhijuan1, and LYU Lijun2
Author Affiliations
  • 1School of Mechanical, Electrical & Information Engineering, Putian University, Putian 351100, China
  • 2Department of Precision Mechanical Engineering, Shanghai University, Shanghai 200072, China
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    Figures & Tables(12)
    Propagation diagram of the chief ray at a quadrics of revolution
    Optical scheme of the chief ray passing the gth optical surface of optical system
    Flow chart for aberration optimization of catadioptric imaging system with large acceptance aperture
    Initial structure and optical scheme of catadioptric imaging system with large accptance aperture
    MTF curves of catadioptric imaging system with large acceptance aperture in the case of initial structure
    Spot diagram with field angles at 5°, 25°, 45° and 60° of catadioptric imaging system with large acceptance aperture in the case of initial structure
    MTF curves of catadioptric imaging system with large acceptance aperture obtained using proposed aberration optimization method
    Spot diagram with field angles at 5°, 25°, 45° and 60° of catadioptric imaging system with large acceptance aperture obtained using proposed optimization method
    • Table 1. Initial structure parameters of catadioptric imaging system with large acceptance aperture

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      Table 1. Initial structure parameters of catadioptric imaging system with large acceptance aperture

      Optical surfaceRadius/mmSpacing/mmMaterial
      122.35-35.25MIRROR
      2-25.66-7.89N-PSK53A
      3-50.23-15.43
      445.25-6.24N-PSK53A
      5-18.56-14.14
      6-75.62-5.12N-PSK53A
      7-22.78-14.29
      Aperture stopInfinite-1.50
      8800.23-4.76BK7
      9-10.42-6.11PSK52
      1014.39-0.41
      11-50.21-1.20PSK54
      1240.29-0.25
      13-65.26-1.52PSK54
      1448.96-4.58
      15-7.89-4.56PSK54
      1618.75-2.78
      Image planeInfinite
    • Table 2. Optical structure parameters of catadioptric imaging system with large acceptance aperture obtained using proposed aberration optimization method

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      Table 2. Optical structure parameters of catadioptric imaging system with large acceptance aperture obtained using proposed aberration optimization method

      Optical surfaceRadius/mmSpacing/mmMaterial
      116.84-50.12MIRROR
      2-20.45-6.79N-PSK53A
      3-66.24-9.96
      434.54-8.21N-PSK53A
      5-10.01-10.56
      6-53.61- 6.78N-PSK53A
      7-15.60-10.81
      Aperture stopInfinite-1.20
      8570.10-3.26BK7
      9-14.40-4.56PSK52
      1018.37-0.51
      11-65.60-1.50PSK54
      1243.55-0.37
      13-75.39-2.03PSK54
      1443.40-3.79
      15-10.16-3.49PSK54
      1617.65-4.92
      Image planeInfinite
    • Table 3. RMS of the spot diagram given in Fig. 6

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      Table 3. RMS of the spot diagram given in Fig. 6

      ParameterValue
      Field angle/(°)5254560
      RMS/μm112.42112.55112.81113.06
    • Table 4. RMS of the spot diagram given in Fig. 8

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      Table 4. RMS of the spot diagram given in Fig. 8

      ParameterValue
      Field angle/(°)5254560
      RMS/μm7.868.068.468.81
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    Yiqing CAO, Zhijuan SHEN, Lijun LYU. Aberration optimization method for aspherical catadioptric imaging system with large acceptance aperture based on sixth-order wave aberration theory[J]. Chinese Journal of Quantum Electronics, 2024, 41(1): 67

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    Paper Information

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    Received: Jul. 20, 2022

    Accepted: --

    Published Online: Mar. 19, 2024

    The Author Email: CAO Yiqing (caoyiqing1987@163.com)

    DOI:10.3969/j.issn.1007-5461.2024.01.006

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