基于Alvarez透镜的短行程红外变焦镜头

Application of Alvarez lens in small movement infrared zoom lens

  • 摘要: 变焦镜头可通过改变系统焦距,实现从大视场观察到小视场高分辨成像的连续观测,在各种场景都有广泛的应用。Alvarez透镜较小径向位移即可实现较大倍率焦距变化,有利于缩短变焦行程,其应用难点在于具有非旋转对称像差,难以通过其他透镜校正。首先通过薄透镜模型及波像差理论给出了Alvarez透镜各项像差与自由曲面系数对应关系,得出口径、移动行程和空气间隔是影响轴上像差大小及像差对称中心偏移的关键因素,将面型扩展为高阶xy多项式可校正轴上的球差、彗差等像差。其次,根据Alvarez透镜像差特性和变焦行程最小化原则提出一种五组元变焦镜头,利用高斯括号法给出变焦方程。最后,依据上述理论设计出一款中波焦距100~600 mm连续变焦镜头,变焦最大行程8.6 mm,成像质量良好,验证了理论正确性,为Alvarez透镜应用提供了理论基础。

     

    Abstract:
    Objective Zoom lens is widely used, it can achieve both wide field of view to observe and narrow field of view to get high resolution image. Alvarez lens (AL) is used in zoom lens to achieve continuous change of focal length in a large range through small lateral movements. However, AL has asymmetric aberrations and the aberrations are difficult to be compensated by other lenses. Firstly, in order to correct on-axial aberrations, the relationship between aberrations in AL and the coefficients of free-form surfaces is analyzed by using wave aberration theory, the factors that affect the decentration of the symmetry center of aberration field is also analyzed. Secondly, a five-group zoom lens is proposed based on the aberration characteristics in AL and the principle of minimizing lateral movement. Finally, using the above theory, a medium-wave infrared continuous zoom lens is designed. The zoom lens has good imaging quality and small lateral movements, verifying the correctness of the above theory.
    Methods Fringe Zernike polynomial wave aberration is used in present study to analysis the aberration in AL. Firstly, the relationship between the wave aberrations of each order on-axis and the lateral movement, spacing, and aperture of AL are analyzed. According to thin-element approximation of AL, its surface needs to extend to higher-order polynomials, and the relationship between the coefficients of free-form surfaces and the Fringe Zernike wave aberration coefficient is given. Secondly, the relationship between off-axis aberrations, lateral movement, spacing, and aperture of AL are analyzed, and their effects on the decentration of aberrations field center are given. Finally, according to the aberration of AL and the principle of minimizing movement, a five-component zoom lens is proposed. The zoom equation is given with Gaussian Brackets, and a design example is provided.
    Results and Discussions Through theoretical calculations and simulations, it is found that aperture, lateral movement, and spacing are the main factors affecting the aberration of AL. When the focal length is fixed, the aberration of AL on-axis and the decentration of the AL aberration field center is smaller with smaller aperture, larger lateral movement, and smaller spacing. The decentration of the AL aberration field center is related to the asymmetric air gap of the AL. The larger lateral movement is, the smaller the polynomial coefficient is, and the less asymmetric it is. At the same time, reducing the spacing can also minimize the impact of asymmetry. Most importantly, the asymmetric aberration of AL on-axis such as primary and secondary coma, trefoil and tetrafoil can’t be corrected by other lenses. These aberrations will be directly added to the optical system, so they must be corrected by AL itself. With the lager aperture and smaller lateral movement, the value and order of aberration will be larger and higher, so it is necessary to extend the free-form to higher order xy polynomials. In most cases, the aberrations on-axis can be corrected effectively by increasing the order of polynomial to seventh order. At this point, the center of coma moves to the central field of view, meanwhile, astigmatism and field curvature decreases slightly, with no significant change in the symmetry center. The designed five-element zoom lens places two pairs of AL in the middle of three groups, with the front-fixed group and the middle-fixed group reducing the AL aperture in order to reduce the aberrations of AL. A continuous zoom lens with a focal length of 100 mm to 600 mm and a maximum lateral movement of 8.6 mm for AL has been designed, the max aperture of zoom lens is 150 mm, F number is 4, and the optical length is 349 mm.
    Conclusions Through theoretical calculations and simulation analysis, the relationship between the on-axis aberration of AL and the xy polynomial coefficients of the AL is given. It is found that the aperture, lateral movement, and spacing are the main factors affecting the decentration of the AL aberration field center. Expanding the AL surface to a high-order xy polynomial to correct the aberration in the central field of view, the coma center moves to the center of the field, and there is no significant change in the symmetry centers of astigmatism and field curvature. Based on the characteristics of the aberration field center of AL and the principle of minimizing lateral movement, a five-component zoom lens is proposed, and the zoom equation is derived using the Gaussian bracket. A design example is given, with compact size and good imaging quality. The maximum lateral movement is 8.6 mm, allowing for a continuous zoom range from 100 mm to 600 mm, the small lateral movements are enabling fast zoom.

     

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