• Chinese Journal of Quantum Electronics
  • Vol. 41, Issue 1, 67 (2024)
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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    DOI: 10.3969/j.issn.1007-5461.2024.01.006 Cite this Article
    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 Copy Citation Text show less
    Propagation diagram of the chief ray at a quadrics of revolution
    Fig. 1. 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
    Fig. 2. 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
    Fig. 3. 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
    Fig. 4. 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
    Fig. 5. 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
    Fig. 6. 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
    Fig. 7. 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
    Fig. 8. Spot diagram with field angles at 5°, 25°, 45° and 60° of catadioptric imaging system with large acceptance aperture obtained using proposed optimization method
    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 1. Initial structure parameters of catadioptric imaging system with large acceptance aperture
    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 2. Optical structure parameters of catadioptric imaging system with large acceptance aperture obtained using proposed aberration optimization method
    ParameterValue
    Field angle/(°)5254560
    RMS/μm112.42112.55112.81113.06
    Table 3. RMS of the spot diagram given in Fig. 6
    ParameterValue
    Field angle/(°)5254560
    RMS/μm7.868.068.468.81
    Table 4. RMS of the spot diagram given in Fig. 8
    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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