CN102368114A - Optical system surface shape compensation adjustment method based on wave aberration detection - Google Patents
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Abstract
Description
技术领域 technical field
本发明属光学工程领域,涉及一种光学系统的装调方法,尤其涉及一种基于波像差检测的光学系统面形补偿装调方法。The invention belongs to the field of optical engineering, and relates to an optical system installation and adjustment method, in particular to an optical system surface shape compensation installation and adjustment method based on wave aberration detection.
背景技术 Background technique
影响光学系统象质的误差主要来自光学、机械两方面。光学方面的误差主要是由于受加工工艺水平的限制,引起的曲率半径、厚度、偏心等偏差。这些偏差在元件加工完成后就不可更改,但通过计量检测可以知道其确定的偏差值。机械方面的误差主要是机械零件加工同轴度、垂直度等低于设计要求,而使装配进去的光学元件面形精度降低,产生位移、偏心、倾斜等。光机加工、装调中的误差可以概括为元件的厚度偏差、位移、偏心、倾斜等。它们对光学系统像质的影响作用是不相同的。当光学元件存在位移、厚度偏差时,主要影响对称性像差,使像点的弥散增大。系统存在偏心、倾斜则导致非对称性的像差,对于轴上点而言,有中心慧差和垂轴色差,使得像点的衍射环失去对称性,而且带有非对称性颜色。在偏心较严重的情况下,还会在视场的中心看到两条分开的焦线,即中心像散。同时,轴外像点出现像散和非对称性的畸变。所有这些加工、装配带来的误差对光学系统象质的综合影响表现为分辨率降低、畸变增大、像点的弥散斑增大、传递函数降低等。此时,通过对各光学元件的空间相对位置的微调,可以补偿由于制造误差引进的像差,提高实际系统装配后的成像质量。经典的补偿调整方法是基于光学、机械零件的几何计量与检测的补偿调整方法,该方法盲目性强,需要反复多次操作,而且需要有丰富经验的技术人员进行操作,使用非常不方便,同时,该方法并未涉及大口径光学元件和系统经常进行的波像差检测以及由此带来的可能的基于等光程原理的波面补偿调整方法。The errors that affect the image quality of the optical system mainly come from two aspects: optics and mechanics. The optical error is mainly due to the limitation of the processing technology level, which causes the deviation of the radius of curvature, thickness, eccentricity and so on. These deviations cannot be changed after the component processing is completed, but the determined deviation value can be known through metrological inspection. Mechanical errors are mainly due to the fact that the coaxiality and verticality of the mechanical parts are lower than the design requirements, which reduces the surface accuracy of the assembled optical components, resulting in displacement, eccentricity, and tilt. Errors in optical machining and assembly can be summarized as component thickness deviation, displacement, eccentricity, inclination, etc. They have different effects on the image quality of the optical system. When the optical element has displacement and thickness deviation, it mainly affects the symmetrical aberration and increases the dispersion of the image point. The eccentricity and inclination of the system will lead to asymmetrical aberrations. For the on-axis point, there are central coma and vertical axis chromatic aberration, which make the diffraction ring of the image point lose symmetry and have asymmetrical color. In the case of severe decentering, two separate focal lines can also be seen in the center of the field of view, that is, central astigmatism. At the same time, astigmatism and asymmetric distortion appear in off-axis image points. The comprehensive impact of all these processing and assembly errors on the image quality of the optical system is manifested in the reduction of resolution, the increase of distortion, the increase of diffuse spot of the image point, and the decrease of transfer function. At this time, by fine-tuning the spatial relative position of each optical element, the aberration introduced by the manufacturing error can be compensated, and the imaging quality of the actual system after assembly can be improved. The classic compensation adjustment method is based on the geometric measurement and detection of optical and mechanical parts. This method is blind, requires repeated operations, and requires experienced technicians to operate. It is very inconvenient to use. At the same time , this method does not involve the wave aberration detection often performed by large-aperture optical elements and systems and the resulting possible wave surface compensation adjustment method based on the principle of equal optical path.
发明内容 Contents of the invention
为了解决背景技术中存在的上述技术问题,本发明提供了一种针对性强、实现迅捷、操作简便以及实用性强的基于波像差检测的光学系统面形补偿装调方法。In order to solve the above-mentioned technical problems in the background technology, the present invention provides an optical system surface compensation and adjustment method based on wave aberration detection, which is highly targeted, quick to implement, easy to operate and highly practical.
本发明的技术解决方案是:本发明提供了一种基于波像差检测的光学系统面形补偿装调方法,其特殊之处在于:所述基于波像差检测的光学系统面形补偿装调方法包括以下步骤:The technical solution of the present invention is: the present invention provides an optical system surface shape compensation adjustment method based on wave aberration detection, which is special in that: the optical system surface shape compensation adjustment method based on wave aberration detection The method includes the following steps:
1)检测待装调光学系统各光学元件的面形波像差;1) Detect the surface wave aberration of each optical element of the optical system to be adjusted;
2)根据等光程原则,判断待装调光学系统的各光学元件的面形是否存在互补,若是,则直接退出待装调光学系统的装调过程;若否,则进行步骤3);2) According to the principle of equal optical path, judge whether the surface shape of each optical element of the optical system to be adjusted is complementary, if yes, then directly exit the adjustment process of the optical system to be adjusted; if not, proceed to step 3);
3)对待装调光学系统各光学元件的空间位置进行调整,使其实现元件面形波像差互补。3) The spatial position of each optical element of the optical system to be adjusted is adjusted so that the surface wave aberration of the elements can be complemented.
上述步骤2)中面形互补的判断方式是:In the above step 2), the judgment method of surface shape complementarity is:
2.1)将步骤1)中已经得到的待装调光学系统各光学元件的面形波像差进行矢量叠加,并得到叠加后的各光学元件的面形波像差矢量和;2.1) Carry out vector superposition of the surface wave aberration of each optical element of the optical system to be adjusted which has been obtained in step 1), and obtain the surface wave aberration vector sum of each optical element after superimposition;
2.2)若叠加后的各光学元件的面形波像差矢量和的绝对值减小,则待装调光学系统各光学元件的面形是互补;若叠加后的各光学元件的面形波像差矢量和的绝对值增大,则待装调光学系统各光学元件的面形是非互补的。2.2) If the absolute value of the surface wave aberration vector sum of the superimposed optical elements decreases, the surface shapes of the optical elements of the optical system to be adjusted are complementary; if the surface wave images of the superimposed optical elements As the absolute value of the difference vector sum increases, the surface shapes of the optical elements of the optical system to be adjusted are non-complementary.
上述步骤3)中对待装调光学系统各光学元件的空间位置进行调整的方式是:对待装调光学系统各光学元件进行平移、旋转或倾斜。The way to adjust the spatial position of each optical element of the optical system to be adjusted in the above step 3) is: to translate, rotate or tilt each optical element of the optical system to be adjusted.
本发明的优点是:The advantages of the present invention are:
本发明提供了一种基于波像差检测的光学系统面形补偿装调方法,该方法采用当系统中各光学元件的几何失调量为零时,如果仅存在光学元件的面形误差,则系统最终像面的波像差将由各光学元件的面形波像差唯一决定的原理,在不改变光学系统其它结构关系的前提下,通过旋转等简单调整操作,可以将光学系统内光学零件面形误差调整达到相互间的波像差互补关系,从而达到优化系统波像差从而提高系统成像质量的目的,其装调过程简单可控,操作简单,实用性强。The invention provides a surface compensation and adjustment method of optical system based on wave aberration detection. The method adopts that when the geometric misalignment of each optical element in the system is zero, if only the surface error of the optical element exists, the system The principle that the wave aberration of the final image plane will be uniquely determined by the surface wave aberration of each optical element, without changing other structural relations of the optical system, through simple adjustment operations such as rotation, the surface shape of the optical parts in the optical system can be adjusted The error adjustment achieves the mutual wave aberration complementary relationship, so as to achieve the purpose of optimizing the system wave aberration and improving the system imaging quality. The installation and adjustment process is simple and controllable, the operation is simple, and the practicability is strong.
附图说明 Description of drawings
图1是本发明提供的装调方法的装调过程示意图。Fig. 1 is a schematic diagram of the assembly and adjustment process of the assembly and adjustment method provided by the present invention.
具体实施方式 Detailed ways
本发明的原理是:光在任意介质中从一点传播到另一点时,沿所需时间最短的路径传播,该原理又称最小时间原理或极短光程原理,这是法国数学家费马(Pierre de Fermat)于1657年首先提出的费马原理(Fermat′s Principle)。费马原理是几何光学中的一条重要原理,由此原理可证明光在均匀介质中传播时遵从的直线传播定律、反射和折射定律,以及傍轴条件下光学系统的等光程性等。因此所有的成像光学系统的设计过程都遵循等光程性原则。The principle of the present invention is: when light propagates from one point to another in any medium, it propagates along the path with the shortest required time. This principle is also called the principle of minimum time or the principle of extremely short optical path. Pierre de Fermat first proposed Fermat's Principle in 1657. Fermat's principle is an important principle in geometric optics, which can prove the law of straight line propagation, the law of reflection and refraction that light obeys when propagating in a homogeneous medium, and the equal optical path length of optical systems under paraxial conditions. Therefore, the design process of all imaging optical systems follows the principle of equal optical path length.
依据上述原理,本发明提供了一种基于波像差检测的光学系统面形补偿装调方法,该方法包括以下步骤:According to the above principles, the present invention provides a method for adjusting and adjusting the surface shape of an optical system based on wave aberration detection. The method includes the following steps:
1)检测待装调光学系统各光学元件的面形波像差;1) Detect the surface wave aberration of each optical element of the optical system to be adjusted;
2)根据等光程原则,判断待装调光学系统的各光学元件的面形是否存在互补,若是,则直接退出待装调光学系统的装调过程;若否,则进行步骤3):2) According to the principle of equal optical path, judge whether the surface shape of each optical element of the optical system to be adjusted is complementary, if yes, directly exit the adjustment process of the optical system to be adjusted; if not, proceed to step 3):
其互补的判断过程是:The complementary judgment process is:
2.1)将步骤1)中已经得到的待装调光学系统各光学元件的面形波像差进行叠加,并得到叠加后的各光学元件的面形波像差矢量和;2.1) Superimpose the surface wave aberrations of the optical elements of the optical system to be adjusted that have been obtained in step 1), and obtain the surface wave aberration vector sum of the superimposed optical elements;
2.2)若叠加后的各光学元件的面形波像差矢量和之绝对值减小,则待装调光学系统各光学元件的面形是互补;若叠加后的各光学元件的面形波像差矢量和之绝对值增大,则待装调光学系统各光学元件的面形是非互补的。2.2) If the absolute value of the surface wave aberration vector sum of the superimposed optical elements decreases, the surface shapes of the optical elements of the optical system to be adjusted are complementary; if the surface wave images of the superimposed optical elements When the absolute value of the difference vector sum increases, the surface shape of each optical element of the optical system to be adjusted is non-complementary.
3)对待装调光学系统各光学元件的空间位置进行平移、旋转和/或倾斜等的调整,使待装调光学系统的各光学元件的面形达到互补。3) The spatial position of each optical element of the optical system to be adjusted is adjusted by translation, rotation and/or tilt, etc., so that the surface shape of each optical element of the optical system to be adjusted is complementary.
参见图1,本发明以图1所示的光学系统为例对本发明所提供的基于波像差检测的光学系统面形补偿装调方法进行详细的说明。在图1中,该光学系统包括主镜、次镜、物点O以及像点I,其中,实线表示理想状态下各光学元件的面形结构示意图;虚线表示实际得到的各光学元件的实测面形结构示意图;当主镜的面形波像差为Wmain(也就是虚线所表示的面形波像差),次镜面形波像差为Wsec(也就是虚线所表示的面形波像差)时,物点O发出的球面波WO与像点I处的波像差WI可表达为:Referring to FIG. 1 , the present invention takes the optical system shown in FIG. 1 as an example to describe in detail the surface shape compensation and adjustment method of the optical system based on wave aberration detection provided by the present invention. In Fig. 1, the optical system includes a primary mirror, a secondary mirror, an object point O, and an image point I, wherein the solid line represents a schematic diagram of the surface structure of each optical element in an ideal state; the dotted line represents the actual measurement of each optical element obtained in practice. Schematic diagram of the surface structure; when the surface wave aberration of the primary mirror is W main (that is, the surface wave aberration represented by the dotted line), the surface wave aberration of the secondary mirror is W sec (that is, the surface wave aberration represented by the dotted line difference), the spherical wave W O emitted by the object point O and the wave aberration W I at the image point I can be expressed as:
WI=WO+kmWmain+ksWsec W I =W O +k m W main +k s W sec
其中km为主镜面到次镜面的光瞳放大倍率,ks为次镜面到像面的光瞳放大倍率,均由系统结构参数决定,则根据等光程设计原则,主镜和次镜的面形误差存在互补关系。也就是说,假设当系统中各光学元件的几何失调量为零时,如果仅存在光学元件的面形误差,则系统最终像面的波像差将由各光学元件的面形波像差唯一决定。Among them, k m is the pupil magnification from the primary mirror to the secondary mirror, and k s is the pupil magnification from the secondary mirror to the image plane, both of which are determined by the system structure parameters. According to the principle of equal optical path design, the primary mirror and secondary mirror There is a complementary relationship between surface shape errors. That is to say, assuming that the geometric misalignment of each optical element in the system is zero, if only the surface error of the optical element exists, the wave aberration of the final image plane of the system will be uniquely determined by the surface wave aberration of each optical element .
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Application publication date: 20120307 |