CN114185144B - A Method for Mounting and Adjusting a Large-Aperture Optical System Based on a Small-Aperture Plane Mirror - Google Patents
A Method for Mounting and Adjusting a Large-Aperture Optical System Based on a Small-Aperture Plane Mirror Download PDFInfo
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Abstract
Description
技术领域technical field
本发明属于天文望远镜技术领域,涉及一种光学系统装调方法及系统,具体为一种基于小口径平面镜装调大口径光学系统的装调方法。The invention belongs to the technical field of astronomical telescopes, and relates to an optical system installation and adjustment method and system, in particular to an installation and adjustment method for a large-diameter optical system based on a small-diameter plane mirror.
背景技术Background technique
为了满足更高的成像分辨率,光学系统的有效通光口径越来越大,同时也对系统装调提出了更高的要求。基于平面反射镜的干涉装调是一种典型的光学系统装调方法,因其装调精度高被广泛应用于各种类型的光学系统装调中。该装调方法通常使用一块与待装调光学系统相同口径的平面反射镜与待装调光学系统组成干涉光路进行系统装调。干涉仪放置在光学系统焦点处,发出点光源,经光学系统后形成平行光入射在标准平面反射镜上,平行光经平面反射镜反射后进入光学系统,反射的平行光经光学系统后汇聚在系统焦点处,与干涉仪出射点光源形成干涉。装调光路见附图1。平面反射镜是干涉装调中的基准元器件,其面型精度决定了光学系统的最高装调精度。为了满足高精度的系统装调,平面反射镜的面型精度RMS值需≤λ/50(λ为装调波长)。In order to meet higher imaging resolution, the effective light aperture of the optical system is getting larger and larger, which also puts forward higher requirements for system assembly and adjustment. Interferometric adjustment based on plane mirror is a typical optical system adjustment method, which is widely used in various types of optical system adjustment because of its high adjustment accuracy. This adjustment method usually uses a flat mirror with the same diameter as the optical system to be adjusted to form an interference optical path with the optical system to be adjusted for system adjustment. The interferometer is placed at the focal point of the optical system, emits a point light source, passes through the optical system to form parallel light incident on the standard plane mirror, the parallel light enters the optical system after being reflected by the plane mirror, and the reflected parallel light converges on the At the focal point of the system, it interferes with the point light source emitted by the interferometer. See attached drawing 1 for the installation and adjustment optical path. The plane mirror is the reference component in the interference adjustment, and its surface shape accuracy determines the highest adjustment accuracy of the optical system. In order to meet the high-precision system installation and adjustment, the surface accuracy RMS value of the plane reflector must be ≤λ/50 (λ is the installation wavelength).
但是,大口径标准平面镜制造成本很高,作为检测元件无疑会大大增加研制成本。另外,针对处于特殊姿态下(倾斜)的大口径光学系统,大口径平面反射镜因其自身重力和支撑结构,很难在特殊姿态下(倾斜)保证其面型精度。因此大口径平面反射镜越来越不适于大口径光学系统的装调。However, the manufacturing cost of a large-diameter standard flat mirror is very high, and it will undoubtedly greatly increase the development cost as a detection element. In addition, for the large-aperture optical system in a special posture (tilted), it is difficult to ensure the surface accuracy of the large-aperture flat mirror due to its own gravity and support structure in a special posture (tilted). Therefore, large-aperture flat mirrors are more and more unsuitable for the adjustment of large-aperture optical systems.
发明内容Contents of the invention
本发明的目的是提供一种基于小口径平面镜装调大口径光学系统的装调方法。该方法解决了大口径平面反射镜不适于大口径光学系统干涉装调的技术问题。小口径平面反射镜与大口径平面反射镜相比造价低,降低了装调设备成本,且小口径平面反射镜质量轻且易于机械支撑,可以用于在倾斜状态下保持其面型精度的装调要求。本发明提出一种基于小口径平面镜装调大口径光学系统的评价方法,实现利用小口径平面反射镜装调大口径光学系统。The purpose of the present invention is to provide a method for assembling and adjusting a large-diameter optical system based on a small-diameter plane mirror. The method solves the technical problem that the large-aperture plane mirror is not suitable for the interference adjustment of the large-aperture optical system. Compared with the large-diameter plane mirror, the small-diameter plane mirror has a lower cost, which reduces the cost of assembly and adjustment equipment, and the small-diameter plane mirror is light in weight and easy to support mechanically, and can be used to maintain its surface accuracy in an inclined state. call request. The invention proposes an evaluation method for installing and adjusting a large-diameter optical system based on a small-diameter plane mirror, and realizes the installation and adjustment of a large-diameter optical system by using a small-diameter plane mirror.
本发明包括一个待装调光学系统、一块小口径平面反射镜和一台干涉仪。将平面反射镜放置在待装调的光学系统前。光学系统、小口径平面反射镜和干涉仪构成干涉光路。通过干涉仪得到系统成像波像差均方根值(Root Mean Square:RMS)和各项泽尼克(Zernike)多项式系数值后,使用光学软件进行逆向优化,得到光学元件的失调量,从而进行系统装调。The invention includes an optical system to be adjusted, a small-diameter flat mirror and an interferometer. Place the flat mirror in front of the optical system to be adjusted. An optical system, a small-diameter plane mirror and an interferometer constitute an interference optical path. After obtaining the root mean square value (Root Mean Square: RMS) of the imaging wave aberration of the system and the values of the Zernike polynomial coefficients through the interferometer, use the optical software to perform reverse optimization to obtain the misalignment of the optical components, so as to carry out the system Adjustment.
本发明的工作原理:Working principle of the present invention:
光学系统在系统焦面处的波像差可以由Zernike多项式进行表示,具体形式如式(1)所示:The wave aberration of the optical system at the focal plane of the system can be expressed by Zernike polynomials, and the specific form is shown in formula (1):
其中Ai为Zernike多项式第i项的系数,Zi(ρ,θ)为Zernike多项式的第i项,ρ为归一化的径向距离(0≤ρ≤1),θ为方位角(0≤θ≤2π),n为Zernike多项式的项数。Among them, A i is the coefficient of the i-th item of the Zernike polynomial, Z i (ρ,θ) is the i-th item of the Zernike polynomial, ρ is the normalized radial distance (0≤ρ≤1), and θ is the azimuth (0 ≤θ≤2π), n is the number of items of the Zernike polynomial.
在单位圆内,Zernike多项式各项连续正交。利用Zernike多项式的正交性,从全口径中单独取任一位置的小口径圆形区域的Zernike多项式系数具有唯一性,因此可以使用小口径圆形区域的Zernike多项式系数表征全口径波像差,指导系统装调。Within the unit circle, the terms of the Zernike polynomials are continuous and orthogonal. Using the orthogonality of the Zernike polynomials, the Zernike polynomial coefficients of the small-aperture circular area taken from any position in the full-aperture are unique, so the Zernike polynomial coefficients of the small-aperture circular area can be used to characterize the full-aperture wave aberration, Guide system setup and adjustment.
Zernike多项式的第1-4项表征位置、倾斜和离焦,Zernike多项式的第5-11项表征像散、慧差、球差和三叶像散,Zernike多项式的第12项及以后表征高阶像差。在实际装调中,光学元件的位置误差对5-11项的低阶像差的影响较大,对12项及以后的高阶像差影响较小,一般认为12项及以后的高阶像差由光学元件的面型造成,无法通过调整光学元件的位置进行消除。因此装调过程中,使用5-11项低阶像差做为优化目标进行光学元件位置误差的计算。Zernike多项式的第5-11项见式(2)。Items 1-4 of the Zernike polynomial represent position, tilt, and defocus, items 5-11 of the Zernike polynomial represent astigmatism, coma, spherical aberration, and trefoil astigmatism, and items 12 and later of the Zernike polynomial represent high-order aberrations. In actual installation and adjustment, the position error of optical components has a greater impact on the low-order aberrations of items 5-11, and has little impact on the high-order aberrations of items 12 and later. It is generally believed that the high-order aberrations of items 12 and later The difference is caused by the surface shape of the optical element and cannot be eliminated by adjusting the position of the optical element. Therefore, during the adjustment process, use the 5-11 low-order aberrations as the optimization target to calculate the position error of the optical components. Items 5-11 of the Zernike polynomial are shown in formula (2).
本发明的技术方案为:Technical scheme of the present invention is:
一种基于小口径平面镜装调大口径光学系统的装调方法,其步骤包括:A method for assembling and adjusting a large-diameter optical system based on a small-diameter plane mirror, the steps of which include:
1)将待装调的光学系统中各光学元件的实测参数信息输入光学仿真软件,建立光学系统模型,得到光学系统在焦点处的波像差RMS值和Zernike多项式各项系数值;1) Input the measured parameter information of each optical element in the optical system to be adjusted into the optical simulation software, establish the optical system model, and obtain the wave aberration RMS value of the optical system at the focal point and the coefficient values of the Zernike polynomial;
2)在所述光学系统模型中截取一小口径圆形区域,获得光学系统焦点处在该小口径圆形区域内的波像差RMS值和Zernike多项式各项系数值;2) intercept a small-diameter circular area in the optical system model, and obtain the wave aberration RMS value and Zernike polynomial coefficient values of the optical system focus in the small-diameter circular area;
3)所述光学系统中的各光学元件完成粗定位后,将干涉仪放置在所述光学系统的焦点处,将一小口径平面反射镜放置在粗装调所得光学系统前,所述光学系统、小口径平面反射镜和干涉仪构成干涉光路;其中所述小口径平面反射镜的口径和对准区域与所选小口径圆形区域对应一致;3) After the rough positioning of each optical element in the optical system is completed, the interferometer is placed at the focal point of the optical system, and a small-diameter plane mirror is placed in front of the optical system obtained by rough assembly and adjustment, and the optical system , the small-diameter plane mirror and the interferometer constitute an interference optical path; wherein the aperture and alignment area of the small-diameter plane mirror correspond to the selected small-diameter circular area;
4)使用干涉仪测量当前所述光学系统焦点处在该小口径圆形区域内的波像差RMS值和Zernike多项式各项系数值;4) using an interferometer to measure the wave aberration RMS value and the Zernike polynomial coefficient values of the current optical system focus in the small-diameter circular area;
5)将步骤4)测量得到的低阶像差作为优化目标值输入到所述光学系统模型中进行逆向优化,得到所述光学系统各光学元件的位置失调量;5) inputting the low-order aberration obtained from the measurement in step 4) into the optical system model as an optimization target value for reverse optimization to obtain the positional misalignment of each optical element of the optical system;
6)根据步骤5)计算所得的各光学元件位置失调量对各光学元件进行装调到位后,使用干涉仪获得装调完成后光学系统焦点处该小口径圆形区域内的波像差RMS值和Zernike多项式各项系数值,与步骤2)所得理论波像差RMS值和Zernike多项式各项系数值进行核对;6) After adjusting each optical element according to the positional misalignment of each optical element calculated in step 5), use an interferometer to obtain the wave aberration RMS value in the small-diameter circular area at the focal point of the optical system after the adjustment is completed and Zernike polynomial each coefficient value, check with step 2) gained theoretical wave aberration RMS value and Zernike polynomial each coefficient value;
7)步骤6)核对一致后,及完成系统装调;否则返回步骤4)。7) After checking in step 6), the system installation and adjustment is completed; otherwise, return to step 4).
进一步的,所述光学元件的实测参数信息包括:光学元件的曲率、非球面系数以及面型;如果所述光学元件为折射光学元件,所述参数信息还包括光学元件的厚度、面偏心和面倾斜。Further, the measured parameter information of the optical element includes: the curvature, aspheric coefficient, and surface shape of the optical element; if the optical element is a refractive optical element, the parameter information also includes the thickness of the optical element, surface eccentricity, and surface shape. tilt.
进一步的,所述低阶像差为Zernike多项式的第5-11项系数,即像散、慧差、球差和三叶像散。Further, the low-order aberrations are coefficients 5-11 of Zernike polynomials, namely astigmatism, coma, spherical aberration and trefoil astigmatism.
进一步的,步骤7)中,小口径圆形区域内Zernike多项式的5-11项与理论值一致,则判定符合装调要求,完成系统装调。Further, in step 7), if the 5-11 terms of the Zernike polynomial in the small-diameter circular area are consistent with the theoretical value, it is determined that the installation and adjustment requirements are met, and the system installation and adjustment is completed.
进一步的,所述全口径区域为所述光学系统的有效口径。Further, the full aperture area is the effective aperture of the optical system.
一种基于小口径平面镜装调大口径光学系统的装调系统,其特征在于,包括小口径平面反射镜、干涉仪和一数据处理单元;其中An installation and adjustment system for adjusting a large-diameter optical system based on a small-diameter plane mirror, characterized in that it includes a small-diameter plane mirror, an interferometer, and a data processing unit; wherein
所述数据处理单元,用于根据待装调的光学系统中各光学元件的实测参数信息建立一光学系统模型,得到光学系统在焦点处的波像差RMS值和Zernike多项式各项系数值;并在所述光学系统模型中截取一小口径圆形区域,获得光学系统焦点处在该子孔径区域内的波像差RMS值和Zernike多项式各项系数值;其中所述小口径平面反射镜的口径和对准区域与所选小口径圆形区域对应一致;The data processing unit is used to establish an optical system model according to the measured parameter information of each optical element in the optical system to be adjusted, and obtain the wave aberration RMS value of the optical system at the focal point and the coefficient values of Zernike polynomials; and A small-diameter circular area is intercepted in the optical system model, and the wave aberration RMS value and the Zernike polynomial coefficient values of the optical system focal point in the sub-aperture area are obtained; wherein the aperture of the small-diameter plane reflector The alignment area corresponds to the selected small-diameter circular area;
所述小口径平面反射镜放置在粗装调后所得光学系统前;所述光学系统、小口径平面反射镜和干涉仪构成干涉光路;The small-diameter plane reflector is placed in front of the optical system obtained after rough assembly and adjustment; the optical system, the small-diameter plane reflector and the interferometer form an interference optical path;
所述小口径平面反射镜,用于依次扫描所述光学系统的全口径区域,得到光学系统焦点处各子孔径区域的波前数据并发送给所述数据处理单元;The small-aperture plane mirror is used to sequentially scan the full-aperture area of the optical system to obtain wavefront data of each sub-aperture area at the focal point of the optical system and send it to the data processing unit;
所述干涉仪,用于测量当前所述光学系统焦点处在该小口径圆形区域内的波像差RMS值和Zernike多项式各项系数值,发送给所述数据处理单元;The interferometer is used to measure the wave aberration RMS value and Zernike polynomial coefficient values of the current focus of the optical system in the small-aperture circular area, and send it to the data processing unit;
所述数据处理单元根据测量得到的低阶像差作为优化目标值输入到所述光学系统模型中进行逆向优化,得到所述光学系统各光学元件的位置失调量。The data processing unit inputs the measured low-order aberrations as optimization target values into the optical system model for reverse optimization, and obtains the positional misalignment of each optical element of the optical system.
与现有技术相比,本发明的积极效果为:Compared with prior art, positive effect of the present invention is:
与传统的大口径平面反射镜干涉装调方法相比,小口径平面反射镜造价低,支撑结构较为简单,大大降低装调设备的成本。并且,小口径平面反射镜在特殊姿态下能较好的保证其面型精度,适用于特殊姿态的光学系统装调Compared with the traditional method of interference assembly and adjustment of large-diameter flat mirrors, the cost of small-diameter flat mirrors is low, and the supporting structure is relatively simple, which greatly reduces the cost of installation and adjustment equipment. In addition, the small-aperture flat mirror can better guarantee its surface accuracy in a special posture, and is suitable for the installation and adjustment of an optical system with a special posture
附图说明Description of drawings
图1为平面反射镜干涉装调示意图。Figure 1 is a schematic diagram of interference adjustment of a plane mirror.
图2为小口径平面反射镜干涉装调示意图。Figure 2 is a schematic diagram of the interference adjustment of a small-aperture plane mirror.
图3为小口径平面反射镜口径示意图。Fig. 3 is a schematic diagram of the aperture of a small-aperture plane mirror.
具体实施方式Detailed ways
下面结合附图对本发明进行进一步详细描述。The present invention will be described in further detail below in conjunction with the accompanying drawings.
如图2所示,本发明的具体装调方案如下:As shown in Figure 2, the concrete adjustment scheme of the present invention is as follows:
步骤一:测量待装调的光学系统中每个光学元件的曲率、非球面系数以及面型(折射光学元件还需测量每个元件的厚度、面偏心、面倾斜),将所测量数据输入光学仿真软件,建立光学系统模型,得到光学系统带有实际加工误差和面型情况下的系统焦点处的波像差RMS值和Zernike多项式各项系数值。Step 1: Measure the curvature, aspheric coefficient, and surface shape of each optical element in the optical system to be adjusted (refractive optical elements also need to measure the thickness, surface eccentricity, and surface inclination of each element), and input the measured data into the optical The simulation software establishes the optical system model, and obtains the RMS value of the wave aberration at the focal point of the system and the coefficient values of the Zernike polynomial under the condition of the actual processing error and surface shape of the optical system.
步骤二:在光学模型中截取所需使用的小口径圆形区域,获得光学系统焦点处在该小口径圆形区域内的波像差RMS值和Zernike多项式各项系数值。理论上任意大小的子孔径都可以进行装调;在可以保证面型精度的条件下,选取口径尽可能大的小口径圆形区域进行装调会更加方便。Step 2: Intercept the required small-diameter circular area in the optical model, and obtain the wave aberration RMS value and Zernike polynomial coefficient values of the focal point of the optical system in the small-diameter circular area. Theoretically, sub-apertures of any size can be adjusted; under the condition that the surface accuracy can be guaranteed, it is more convenient to select a small-diameter circular area with as large a diameter as possible for adjustment.
步骤三:光学系统中的各光学元件完成粗装调后,将干涉仪放置在光学系统的焦点处,小口径平面反射镜放置在待装调光学系统前,待装调光学系统、小口径平面反射镜和干涉仪组成干涉光路。小口径平面反射镜口径示意图如图3所示,小口径平面反射镜的口径和对准区域与所选小口径圆形区域对应一致。Step 3: After the rough assembly and adjustment of each optical element in the optical system is completed, the interferometer is placed at the focus of the optical system, and the small-diameter plane mirror is placed in front of the optical system to be installed and adjusted. Mirrors and interferometers form an interference optical path. The schematic diagram of the aperture of the small-aperture plane mirror is shown in Figure 3, and the aperture and alignment area of the small-aperture plane mirror correspond to the selected small-aperture circular area.
步骤四:使用干涉仪测量此时光学系统焦点处小口径圆形区域的波像差RMS值和各项Zernike多项式系数值。Step 4: Use an interferometer to measure the wave aberration RMS value and various Zernike polynomial coefficient values of the small-aperture circular area at the focal point of the optical system at this time.
步骤五:将步骤四测量得到的5-11项Zernike系数作为优化目标值输入到步骤一所建立的光学模型中进行逆向优化,得到光学系统各元件的位置失调量。Step 5: Input the 5-11 Zernike coefficients measured in step 4 as the optimization target value into the optical model established in step 1 for reverse optimization to obtain the positional misalignment of each component of the optical system.
步骤六:根据步骤五计算所得的各元件位置失调量进行系统装调,各元件装调到位后,使用干涉仪获得装调完成后光学系统焦点处子口径的波像差RMS值和各项Zernike多项式系数值,与步骤二中的理论波像差RMS值和各项Zernike多项式系数值进行核对。Step 6: Perform system adjustment according to the positional misalignment of each component calculated in step 5. After each component is adjusted in place, use the interferometer to obtain the wave aberration RMS value of the sub-aperture at the focal point of the optical system after the adjustment is completed and various Zernike polynomials The coefficient value is checked with the theoretical wave aberration RMS value and various Zernike polynomial coefficient values in step 2.
步骤七:步骤六核对一致后,完成系统装调。Step 7: After checking in step 6, the system installation and adjustment is completed.
以上所述仅为本发明的较佳实施例而已,并不用以限制本发明,凡在本发明的精神和原则之内所作的任何修改、等同替换和改进等,均应包含在本发明的保护范围之内。The above descriptions are only preferred embodiments of the present invention, and are not intended to limit the present invention. Any modifications, equivalent replacements and improvements made within the spirit and principles of the present invention should be included in the protection of the present invention. within range.
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