Infrared and Laser Engineering, Volume. 50, Issue 6, 20200523(2021)

Solving initial structure of bifocal system according to theory of paraxial optics

Xiao Liang1, Huilin Jiang2, Hao Sun1, Chunyan Wang1, and Huan Liu1
Author Affiliations
  • 1School of Opto-Electronic Engineering, Changchun University of Science and Thchnology, Changchun 130022, China
  • 2Institute of Space Photoelectric Technology, Changchun University of Science and Technology, Changchun 130022, China
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    Figures & Tables(12)
    Structure diagram of axial bifocal optical system
    Light path of paraxial optical system
    Light path after the first step optimization
    Light path after the second step optimization
    Light path diagram after the third step optimization
    Light path and aberration diagram. (a) Light path; (b) Spot diagram; (c) MTF; (d) Field curvature and distortion; (e) Lateral color
    [in Chinese]
    • Table 1. Design index of optical system

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      Table 1. Design index of optical system

      ParameterValue
      Wavelength486-656 nm
      Field of view8.6°/2.9°
      Focal length40 (WFOV) mm 120 (NFOV) mm
      Spot diagram<0.5 pixel@0-0.707 fields <0.7 pixel@0.707-1 fields
      MTF100 lp/mm>0.3
      Temperature−20-45 ℃
      CCD pixel5 μm
    • Table 2. Lens parameters after the first step optimization

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      Table 2. Lens parameters after the first step optimization

      Radius/mmThickness/mmGlass
      75.1834.46Zk13
      −23.1741.063
      −20.4561.977Sf6
      −43.44311.686
      914.6722.267Sk11
      −39.32150.766
    • Table 3. Lens parameters after the second step optimization

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      Table 3. Lens parameters after the second step optimization

      Radius/mmThickness/mmGlass
      −53.0121.999P-sf68
      −33.6810.998
      −35.3821.999N-lak33b
      69.94856.318/1.357
      128.8813.276Zk13
      −34.6621.524
      −26.7161.999Sf6
      −60.5430.999
      117.3078.127Sk11
      −44.07864.357
    • Table 4. Lens parameters after the third step optimization

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      Table 4. Lens parameters after the third step optimization

      SurfaceRadius/mmThickness/mmGlass
      157.87010Zk12
      2−77.1062Kzfs8
      3193.41913.083/59.282
      4−42.4194.997P-sf68
      5−28.5451
      6−27.7892N-lak33b
      777.38547.197/0.997
      878.6316.895Zk13
      9−26.741.612
      10−24.3162Sf6
      11−62.5781
      1260.4292.496Sk11
      13−80.59555.744
    • Table 5. The size of aberration during optimization

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      Table 5. The size of aberration during optimization

      FieldAberrationFirst stepSecond stepThird step
      WFOVS10.0398410.0289050.009558
      S2−0.001334−0.0021040.000991
      S30.0036870.001254−0.001397
      S40.0047530.0006640.001780
      S50.0008350.0066410.008469
      CL−0.002214−0.001471−0.001162
      CT−0.001464−0.001599−0.000406
      Maximum RMS radius/μm25.20311.0115.852
      Minimum RMS radius/μm21.08110.0543.684
      NFOVS10.039844−0.0264490.000056
      S2−0.0013330.001632−0.000895
      S30.003687−0.0009910.000350
      S40.0047530.0006640.001780
      S50.0008350.0006430.000416
      CL−0.0022150.003065−0.001473
      CT−0.001464−0.0007740.000831
      Maximum RMS radius/μm25.36811.7118.691
      Minimum RMS radius/μm20.5648.9844.626
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    Xiao Liang, Huilin Jiang, Hao Sun, Chunyan Wang, Huan Liu. Solving initial structure of bifocal system according to theory of paraxial optics[J]. Infrared and Laser Engineering, 2021, 50(6): 20200523

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    Paper Information

    Category: Optical design

    Received: Dec. 21, 2020

    Accepted: --

    Published Online: Aug. 19, 2021

    The Author Email:

    DOI:10.3788/IRLA20200523

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