• Infrared and Laser Engineering
  • Vol. 50, Issue 9, 20210090 (2021)
Rui Qu1,2, Huinan Guo1, Jianzhong Cao1, and Jianfeng Yang1
Author Affiliations
  • 1Xi’an Institute of Optical and Precision Mechanics, Chinese Academy of Sciences, Xi’an 710119, China
  • 2Univisity of Chinese Academy of Sciences, Beijing 100049, China
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    DOI: 10.3788/IRLA20210090 Cite this Article
    Rui Qu, Huinan Guo, Jianzhong Cao, Jianfeng Yang. Design of visible-near infrared athermal continuous zoom optical system[J]. Infrared and Laser Engineering, 2021, 50(9): 20210090 Copy Citation Text show less

    Abstract

    The primary aberration of each lens group will be changed with their movement, and the change of environment temperature will also lead to defocus, both of which will cause a lot of difficulties in the zoom lens design process. To solve this problem, aberration functions do depend and not depend on group movement were introduced based on optical aberration theory, and lens power distribution and material selection method were discussed with the achromatic and athermal design model futher. A visible-near infrared (Vis-Nir) optical system under the requirements of F/5, focal length of 8-120 mm, focal plane diameter of 6.2 mm, work waveband of 0.48-0.68 μm and 0.7-0.9 μm was designed with mechanically compensated method and optical passive athermal technology. The proposed zoom lens system, which used 7 kinds of common optical glass, consists of 12 groups 16 lenses, total length of only 90 mm, has good image quality and tolerance character among the zoom range within -40~60 ℃.
    $ W\left(\mathop H\limits^{\rightharpoonup},\mathop {\rho }\limits^{\rightharpoonup},\gamma \right)={W}_{P}\left(\mathop H\limits^{\rightharpoonup},\mathop {\rho }\limits^{\rightharpoonup}\right)+{W}_{K}\left(\mathop H\limits^{\rightharpoonup},\mathop {\rho }\limits^{\rightharpoonup}\right)+{W}_{K}\left(\mathop H\limits^{\rightharpoonup},\mathop {\rho }\limits^{\rightharpoonup},\gamma \right) $()

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    $ WK(H,ρ,γ)=(WK1111+WK1112γ2+WK113γ3)(Hρ)+(WK0201+WK0202γ2+WK0203γ3)(ρρ)+(WK0401+WK0402γ2+WK0403γ3)(ρρ)2+(WK1311+WK1312γ2+WK1313γ3)(Hρ)(ρρ)+(WK2221+WK2222γ2+WK2223γ3)(Hρ)2+(WK2201+WK2202γ2+WK2203γ3)(HH)(ρρ)+(WK3111+WK3112γ2+WK3113γ3)(HH)(Hρ) $()

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    $ \;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\left\{f1m2m3m4=f(1)1m22m22f2dm2+1m32m32f3dm3=0(2)\right. $()

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    $ Δfc=Δf1cm2m3m4+f1Δm2m3m4+f1m2Δm3m4+f1m2m3Δm4 $(3)

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    $ Δfcf=Δf1cf1+Δf2cf2+Δf3cf3+Δf4cf4m2Δf1cf2m22m3Δf1cf3m22m32m4Δf1cf4 $(4)

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    $ ΔfTf=Δf1Tf1+Δf2Tf2+Δf3Tf3+Δf4Tf4m2Δf1Tf2m22m3Δf1Tf3m22m32m4Δf1Tf4 $(5)

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    Rui Qu, Huinan Guo, Jianzhong Cao, Jianfeng Yang. Design of visible-near infrared athermal continuous zoom optical system[J]. Infrared and Laser Engineering, 2021, 50(9): 20210090
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