CN118372174B - Optical performance measurement and compensating polishing method for multi-reflective optical system - Google Patents
Optical performance measurement and compensating polishing method for multi-reflective optical system Download PDFInfo
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Abstract
Description
技术领域Technical Field
本发明涉及光学技术领域,尤其涉及一种多反光学系统的光学性能测量及补偿抛光方法。The invention relates to the field of optical technology, and in particular to an optical performance measurement and compensating polishing method for a multi-reflection optical system.
背景技术Background Art
一般来说,仅仅通过制造精度无法满足多反光学系统的精度需求,因此在制造后都需要进行测量以避免不合格品投入使用。然而,多反光学系统的测量往往存在两种方式。第一种方式是对每个反射镜单独切削加工后,分别对面形测量并补偿抛光加工,最后将反射镜安装和调整形成多反光学系统;另一种方式是在切削加工和装调后,采用激光干涉仪等仪器进行离线测量,然后进行补偿加工。这两种方式均存在一定的不足。第一种方式仅保证了单个反射镜的面形,但光学装调引入的位姿误差将完全地影响到最终的光学性能;第二种方式虽然对整体的光学性能进行了评估且通过加工来改善,但离线测量降低了这一过程的效率,并且测量结果无法准确地指导补偿加工。Generally speaking, the precision requirements of multi-reflection optical systems cannot be met by manufacturing accuracy alone, so measurements are required after manufacturing to avoid unqualified products from being put into use. However, there are usually two ways to measure multi-reflection optical systems. The first way is to cut each reflector separately, measure the surface shape and perform compensatory polishing, and finally install and adjust the reflector to form a multi-reflection optical system; the other way is to use instruments such as laser interferometers for offline measurement after cutting and adjustment, and then perform compensation processing. Both methods have certain shortcomings. The first method only guarantees the surface shape of a single reflector, but the posture error introduced by optical adjustment will completely affect the final optical performance; although the second method evaluates the overall optical performance and improves it through processing, offline measurement reduces the efficiency of this process, and the measurement results cannot accurately guide the compensation processing.
发明内容Summary of the invention
鉴于现有技术中的上述缺陷或不足,期望提供一种多反光学系统的光学性能测量及补偿抛光方法,将多反光学系统中各镜面的面形偏差和位姿偏差归结到了一个镜面上进行评估和补偿,对装调引入的位姿偏差进行补偿,在确保多反光学系统的整体性能的基础上,极大的提高了补偿抛光效率。In view of the above-mentioned defects or deficiencies in the prior art, it is desired to provide a method for measuring the optical performance and compensatory polishing of a multi-reflective optical system, which can attribute the surface shape deviation and posture deviation of each mirror in the multi-reflective optical system to one mirror for evaluation and compensation, and compensate for the posture deviation introduced by the installation, thereby greatly improving the compensatory polishing efficiency while ensuring the overall performance of the multi-reflective optical system.
本发明提供的一种多反光学系统的光学性能测量及补偿抛光方法,包括如下步骤:The present invention provides a method for measuring the optical performance of a multi-reflection optical system and for compensating for polishing, comprising the following steps:
1)确定待修面,首先根据多反光学系统的参数设计相应的光线追踪模型,计算所述光线追踪模型的出射波前像差Wi,然后分别对所述光线追踪模型的各反射表面添加相同大小的面形偏差或位姿偏差,得到使所述出射波前像差Wi变化最大的反射表面,将其定义为待修面,获取所述待修面的理想面型参数Mi;1) determining a surface to be repaired, first designing a corresponding ray tracing model according to the parameters of the multi-reflection optical system, calculating the outgoing wavefront aberration Wi of the ray tracing model, then adding the same size of surface shape deviation or posture deviation to each reflective surface of the ray tracing model, obtaining a reflective surface that makes the outgoing wavefront aberration Wi change the most, defining it as the surface to be repaired, and obtaining the ideal surface shape parameter Mi of the surface to be repaired;
2)波前像差测量,对所述多反光学系统进行出射波前测量,并计算当前出射波前像差Wr;2) wavefront aberration measurement, measuring the outgoing wavefront of the multi-reflection optical system and calculating the current outgoing wavefront aberration W r ;
3)待修面面形解算,将所述Wr代入所述光线追踪模型,获得所述待修面的优化面形参数Mr,进而得到去除函数H;3) Calculating the surface shape of the surface to be trimmed, substituting the W r into the ray tracing model to obtain the optimized surface shape parameter Mr of the surface to be trimmed, and then obtaining the removal function H;
H=λ(Mr-Mi);H = λ(M r -M i );
Mr=arcmin(||f(Wr,Mr)-Wi||);M r = arcmin(||f(W r ,M r )-W i ||);
其中,λ为缩放比例系数;f为Mr作用下所述多反光学系统对于输入波前的整形函数;Wherein, λ is the scaling factor; f is the shaping function of the multi-reflection optical system for the input wavefront under the action of Mr ;
4)补偿抛光路径规划,根据抛光装置的工艺参数进行驻留点布置并拟合得到驻留函数R,结合所述去除函数H采用迭代优化过程计算各驻留点处的驻留时间T,生成一系列含驻留点坐标和驻留时间的补偿抛光路径;4) Compensation polishing path planning, arranging the dwell points according to the process parameters of the polishing device and fitting to obtain the dwell function R, combining the removal function H with an iterative optimization process to calculate the dwell time T at each dwell point, and generating a series of compensation polishing paths containing the dwell point coordinates and the dwell time;
5)补偿抛光,根据所述补偿抛光路径对所述多反光学系统的对应所述待修面的反射面进行抛光,然后重复步骤2)-5),直到步骤2)中的出射波前像差Wr满足应用需求,完成所述多反光学系统的补偿抛光。5) Compensation polishing: polish the reflective surface of the multi-reflection optical system corresponding to the surface to be repaired according to the compensation polishing path, and then repeat steps 2)-5) until the output wavefront aberration W r in step 2) meets the application requirements, and the compensation polishing of the multi-reflection optical system is completed.
进一步的,所述步骤1)中,物方入射光线的方向向量依次与所述光线追踪模型的各个反射表面求交点,然后根据反射定律计算出射光线,再计算所述光线追踪模型的出射波前像差Wi。Furthermore, in step 1), the direction vector of the incident light from the object side intersects with each reflection surface of the ray tracing model in turn, and then the outgoing light is calculated according to the law of reflection, and then the outgoing wavefront aberration W i of the ray tracing model is calculated.
进一步的,所述步骤2)中,将待抛光的所述多反光学系统和原位测量装置安装到抛光装置中,原位测量装置对准所述多反光学系统;所述抛光装置对所述多反光学系统的各反射表面进行抛光后,将所述多反光学系统的各反射表面擦拭干净,通过所述原位测量装置对所述多反光学系统进行出射波前测量,计算所述当前出射波前像差Wr。Furthermore, in the step 2), the multi-reflection optical system to be polished and the in-situ measuring device are installed in a polishing device, and the in-situ measuring device is aligned with the multi-reflection optical system; after the polishing device polishes each reflective surface of the multi-reflection optical system, each reflective surface of the multi-reflection optical system is wiped clean, and the multi-reflection optical system is measured for an outgoing wavefront by the in-situ measuring device, and the current outgoing wavefront aberration W r is calculated.
进一步的,所述步骤3)中,将所述光线追踪模型中无像差的平行入射光设置为带有所述当前出射波前像差Wr的平行光,以多起点全局最优算法求解所述待修面的优化面型参数Mr,所述优化面型参数Mr为使出射波前像差最接近0的面型参数;Furthermore, in the step 3), the parallel incident light without aberration in the ray tracing model is set as the parallel light with the current outgoing wavefront aberration W r , and the optimized surface parameter Mr of the surface to be repaired is solved by a multi-starting point global optimal algorithm, and the optimized surface parameter Mr is the surface parameter that makes the outgoing wavefront aberration closest to 0;
进一步的,所述迭代优化过程为:Furthermore, the iterative optimization process is:
根据所述待修面生成一系列合适间隔的驻留点,结合驻留函数R计算初始驻留时间T0:A series of dwell points with appropriate intervals are generated according to the surface to be trimmed, and the initial dwell time T 0 is calculated in combination with the dwell function R:
T0=H/R;T 0 =H/R;
初始残余误差E0为:The initial residual error E0 is:
E0=H-T0*R;E 0 = HT 0 * R;
对残余误差进一步逼近,第i次迭代求残余时间ti为:To further approximate the residual error, the residual time ti of the i-th iteration is:
ti=Ei-1/R;t i =E i-1 /R;
经过此次迭代后的新的驻留时间Ti和残余误差Ei为:The new dwell time Ti and residual error Ei after this iteration are:
Ti=Ti-1+λti; Ti = Ti -1 + λt i ;
Ei=H-(Ti+λti)*R;E i =H-(T i +λt i )*R;
通过迭代优化过程一步步精确求解T的值,直到残余误差的RMS小于预设的阈值为止,从而得到各驻留点的驻留时间T。The value of T is accurately solved step by step through the iterative optimization process until the RMS of the residual error is less than the preset threshold, thereby obtaining the residence time T of each residence point.
相对于现有技术而言,本发明的有益效果是:Compared with the prior art, the beneficial effects of the present invention are:
(1)本发明的以光学系统的实际应用需求为导向直接评估多反光学系统的波像差而非面形偏差。采用光线追踪方式将多反光学系统中各镜面的面形偏差和位姿偏差均归结到了一个镜面上进行评估和补偿,具有更高效率的同时还能对装调引入的位姿偏差进行补偿,有效的提高了多反光学系统的光学性能。(1) The present invention is guided by the actual application requirements of the optical system and directly evaluates the wave aberration of the multi-reflector optical system instead of the surface deviation. The surface deviation and posture deviation of each mirror surface in the multi-reflector optical system are attributed to one mirror surface for evaluation and compensation by ray tracing, which has higher efficiency and can also compensate for the posture deviation introduced by the adjustment, effectively improving the optical performance of the multi-reflector optical system.
(2)多反光学系统的波前像差测量采用原位测量方式,直接在抛光装置内进行测量,避免了离线测量-加工循环过程的繁琐操作,提升了效率。(2) The wavefront aberration measurement of the multi-reflection optical system adopts an in-situ measurement method and is measured directly in the polishing device, avoiding the tedious operation of the offline measurement-processing cycle and improving efficiency.
应当理解,发明内容部分中所描述的内容并非旨在限定本发明的实施例的关键或重要特征,亦非用于限制本发明的范围。本发明的其它特征将通过以下的描述变得容易理解。It should be understood that the contents described in the summary of the invention are not intended to limit the key or important features of the embodiments of the present invention, nor are they intended to limit the scope of the present invention. Other features of the present invention will become easily understood through the following description.
附图说明BRIEF DESCRIPTION OF THE DRAWINGS
通过阅读参照以下附图所作的对非限制性实施例所作的详细描述,本发明的其它特征、目的和优点将会变得更明显:Other features, objects and advantages of the present invention will become more apparent from the detailed description of non-limiting embodiments made with reference to the following drawings:
图1为多反光学系统补偿抛光路径规划的流程图;FIG1 is a flow chart of the compensation polishing path planning of a multi-reflection optical system;
图2为迭代优化过程的流程图;FIG2 is a flow chart of an iterative optimization process;
图3为三反光学系统的光线追踪原理图;FIG3 is a schematic diagram of the ray tracing principle of a three-mirror optical system;
图4为三反光学系统波前像差测量的结构示意图;FIG4 is a schematic diagram of the structure of wavefront aberration measurement of a three-mirror optical system;
图5为三反光学系统补偿抛光前后的对比图。FIG5 is a comparison diagram of the three-mirror optical system before and after compensatory polishing.
具体实施方式DETAILED DESCRIPTION
下面结合附图和实施例对本发明作进一步的详细说明。可以理解的是,此处所描述的具体实施例仅仅用于解释相关发明,而非对该发明的限定。另外还需要说明的是,为了便于描述,附图中仅示出了与发明相关的部分。The present invention will be further described in detail below in conjunction with the accompanying drawings and embodiments. It is to be understood that the specific embodiments described herein are only used to explain the relevant invention, rather than to limit the invention. It should also be noted that, for ease of description, only the parts related to the invention are shown in the accompanying drawings.
需要说明的是,在不冲突的情况下,本发明中的实施例及实施例中的特征可以相互组合。下面将参考附图并结合实施例来详细说明本发明。It should be noted that, in the absence of conflict, the embodiments of the present invention and the features in the embodiments can be combined with each other. The present invention will be described in detail below with reference to the accompanying drawings and in combination with the embodiments.
请参考图1~图2,本发明的实施例提供了一种多反光学系统的光学性能测量及补偿抛光方法,包括如下步骤:Referring to FIG. 1 and FIG. 2 , an embodiment of the present invention provides an optical performance measurement and compensatory polishing method for a multi-reflection optical system, comprising the following steps:
1)确定待修面,首先根据多反光学系统的参数设计相应的光线追踪模型,物方入射光线的方向向量依次与光线追踪模型的各个反射表面求交点,然后根据反射定律计算出射光线,再计算光线追踪模型的出射波前像差Wi;1) Determine the surface to be repaired. First, design a corresponding ray tracing model according to the parameters of the multi-reflection optical system. The direction vector of the incident light from the object side intersects with each reflection surface of the ray tracing model in turn. Then, calculate the outgoing light according to the law of reflection, and then calculate the outgoing wavefront aberration W i of the ray tracing model.
然后分别对光线追踪模型的各反射表面添加相同大小的面形偏差或位姿偏差,得到使出射波前像差Wi变化最大的反射表面,将其定义为待修面,获取待修面的理想面型参数Mi;Then, the same size of surface shape deviation or position deviation is added to each reflective surface of the ray tracing model to obtain the reflective surface that causes the maximum change in the outgoing wavefront aberration Wi , which is defined as the surface to be repaired, and the ideal surface shape parameter Mi of the surface to be repaired is obtained;
2)波前像差测量,将待抛光的多反光学系统和原位测量装置安装到抛光装置中,原位测量装置对准多反光学系统;抛光装置对多反光学系统的各反射表面进行抛光后,将多反光学系统的各反射表面擦拭干净,通过原位测量装置对多反光学系统进行出射波前测量,计算当前出射波前像差Wr;2) Wavefront aberration measurement: the multi-reflection optical system to be polished and the in-situ measurement device are installed in the polishing device, and the in-situ measurement device is aligned with the multi-reflection optical system; after the polishing device polishes each reflection surface of the multi-reflection optical system, each reflection surface of the multi-reflection optical system is wiped clean, and the in-situ measurement device is used to measure the outgoing wavefront of the multi-reflection optical system, and the current outgoing wavefront aberration W r is calculated;
3)待修面面形解算,将Wr代入光线追踪模型,即将光线追踪模型中无像差的平行入射光设置为带有Wr的平行光,以多起点全局最优算法求解待修面的优化面型参数Mr,优化面型参数Mr为使出射波前像差最接近0的面型参数,进而得到去除函数H;3) Calculate the surface shape of the surface to be repaired. Substitute W r into the ray tracing model, that is, set the parallel incident light without aberration in the ray tracing model to be the parallel light with W r , and use the multi-starting point global optimal algorithm to solve the optimized surface shape parameter Mr of the surface to be repaired. The optimized surface shape parameter Mr is the surface shape parameter that makes the outgoing wavefront aberration closest to 0, and then obtain the removal function H;
H=λ(Mr-Mi);H = λ(M r -M i );
Mr=arcmin(||f(Wr,Mr)-Wi||);M r = arcmin(||f(W r ,M r )-W i ||);
其中,λ为缩放比例系数;f为Mr作用下所述多反光学系统对于输入波前的整形函数;Wherein, λ is the scaling factor; f is the shaping function of the multi-reflection optical system for the input wavefront under the action of Mr ;
4)补偿抛光路径规划,根据抛光装置的工艺参数进行驻留点布置并拟合得到驻留函数R,结合去除函数H采用迭代优化过程计算各驻留点处的驻留时间T,生成一系列含驻留点坐标和驻留时间的补偿抛光路径;4) Compensation polishing path planning: the dwell points are arranged according to the process parameters of the polishing device and the dwell function R is obtained by fitting. The dwell time T at each dwell point is calculated by an iterative optimization process in combination with the removal function H, and a series of compensation polishing paths containing the coordinates of the dwell points and the dwell time are generated;
迭代优化过程为:The iterative optimization process is:
根据待修面生成一系列合适间隔的驻留点,结合驻留函数R计算初始驻留时间T0:Generate a series of dwell points with appropriate intervals according to the surface to be repaired, and calculate the initial dwell time T 0 in combination with the dwell function R:
T0=H/R;T 0 =H/R;
初始残余误差E0为:The initial residual error E0 is:
E0=H-T0*R;E 0 = HT 0 * R;
对残余误差进一步逼近,第i次迭代求残余时间ti为:To further approximate the residual error, the residual time ti of the i-th iteration is:
ti=Ei-1/R;t i =E i-1 /R;
经过此次迭代后的新的驻留时间Ti和残余误差Ei为:The new dwell time Ti and residual error Ei after this iteration are:
Ti=Ti-1+λti; Ti = Ti -1 + λt i ;
Ei=H-(Ti+λti)*R;E i =H-(T i +λt i )*R;
通过迭代优化过程一步步精确求解T的值,直到残余误差的RMS小于预设的阈值为止,从而得到各驻留点的驻留时间T;The value of T is accurately solved step by step through the iterative optimization process until the RMS of the residual error is less than the preset threshold, thereby obtaining the dwell time T of each dwell point;
5)补偿抛光,根据补偿抛光路径对多反光学系统的对应待修面的反射面进行抛光,然后重复步骤2)-5),直到步骤2)中的当前出射波前像差Wr满足应用需求,完成多反光学系统的补偿抛光。5) Compensation polishing: polish the corresponding reflective surface to be repaired of the multi-reflection optical system according to the compensation polishing path, and then repeat steps 2)-5) until the current output wavefront aberration W r in step 2) meets the application requirements, and the compensation polishing of the multi-reflection optical system is completed.
实施例1Example 1
请参考图3~图5,以三反光学系统为例。将三反光学系统的三个离轴自由曲面的面形参数和位姿参数代入光线追踪程序中,构建光线追踪模型。Please refer to Figures 3 to 5, taking a three-mirror optical system as an example. Substitute the surface shape parameters and posture parameters of the three off-axis free-form surfaces of the three-mirror optical system into the ray tracing program to construct a ray tracing model.
如图3所示,由于该三反光学系统是物方无焦、像方汇聚的光路,所以在光线追踪模型中添加沿光轴的平行入射光并计算此时的出射波前像差Wi,此波相差为三反光学系统的理想出射波前相差。As shown in FIG3 , since the three-mirror optical system is an afocal optical path on the object side and converging optical path on the image side, parallel incident light along the optical axis is added to the ray tracing model and the outgoing wavefront aberration W i is calculated at this time. This wavefront aberration is the ideal outgoing wavefront aberration of the three-mirror optical system.
分别给一镜、二镜、三镜单独施加正弦形式的面形误差和位姿误差。面形误差的设置方式为:幅值不大于面形矢高的0.1%,空间频率不大于镜面口径的1/5;位姿误差的设置方式为:姿态偏差为绕X轴、Y轴和Z轴的旋转角度,均不大于1°,位置偏差为沿X轴、Y轴和Z轴的偏移量,均不大于0.01mm。Sinusoidal surface shape error and posture error are applied to the first, second and third mirrors respectively. The surface shape error is set as follows: the amplitude is not greater than 0.1% of the surface shape vector height, and the spatial frequency is not greater than 1/5 of the mirror aperture; the posture error is set as follows: the posture deviation is the rotation angle around the X-axis, Y-axis and Z-axis, which is not greater than 1°, and the position deviation is the offset along the X-axis, Y-axis and Z-axis, which is not greater than 0.01mm.
对于上述情况仿真并计算像面的出射波前像差,其中二镜的面形误差和位姿误差对像差的影响均超过了一镜和三镜,因此对于这个三反光学系统,二镜是我们所认定的待修面。For the above situation, the outgoing wavefront aberration of the image plane is simulated and calculated. The surface error and posture error of the second mirror have more influence on the aberration than the first and third mirrors. Therefore, for this three-mirror optical system, the second mirror is the surface to be corrected.
将三反光学系统和原位测量装置安装到抛光装置中并测量波前,评估出射波前像差Wr。系统结构示意如图4所示,整个系统是在一套机械臂抛光装置中搭建的,机械臂搭载气囊抛光头沿侧向对三反光学系统补偿抛光,三反光学系统放置在抛光池中。原位测量装置对准三反光学系统的出窗,平面镜或屏幕对准三反光学系统的入窗,当原位测量装置是基于夏克-哈特曼等原理的传感器时采用平面镜反射,当原位测量装置是基于逆哈特曼等原理的传感器时采用屏幕显示图案。The three-mirror optical system and the in-situ measurement device are installed in the polishing device and the wavefront is measured to evaluate the outgoing wavefront aberration W r . The schematic diagram of the system structure is shown in FIG4 . The entire system is built in a set of mechanical arm polishing devices. The mechanical arm is equipped with an airbag polishing head to perform compensation polishing on the three-mirror optical system in the lateral direction. The three-mirror optical system is placed in the polishing pool. The in-situ measurement device is aligned with the exit window of the three-mirror optical system, and the plane mirror or screen is aligned with the entrance window of the three-mirror optical system. When the in-situ measurement device is a sensor based on the Shack-Hartmann principle, a plane mirror reflection is used. When the in-situ measurement device is a sensor based on the inverse Hartmann principle, a screen display pattern is used.
将测量得到的出射波前像差Wr代入光线追踪模型求得待修面的面形参数Mr。即将光线追踪模型中无像差的平行入射光设置为带有出射波前像差Wr的平行光,以多起点全局最优算法进行求解,得到使光线追踪模型的出射像差最接近0的待修面面型参数Mr,所构建的优化函数为:Substitute the measured outgoing wavefront aberration W r into the ray tracing model to obtain the surface shape parameter Mr of the surface to be repaired. That is, the parallel incident light without aberration in the ray tracing model is set as the parallel light with the outgoing wavefront aberration W r , and the multi-starting point global optimal algorithm is used to solve the surface shape parameter Mr of the surface to be repaired that makes the outgoing aberration of the ray tracing model closest to 0. The constructed optimization function is:
Mr=arcmin(||f(Wr,Mr)-Wi||);M r = arcmin(||f(W r ,M r )-W i ||);
其中,f代表Mr作用下三反光学系统对于输入波前的整形函数。Where f represents the shaping function of the input wavefront of the three-mirror optical system under the action of Mr.
所生成的去除函数H如下:The generated removal function H is as follows:
H=λ(Mr-Mi);H = λ(M r -M i );
根据所需去除函数H迭代计算驻留时间分布。为了防止补偿过度,补偿加工时往往仅对残余误差进行一定比例的补偿,而非全部补偿,通过反复多次补偿迭代地逼近最优解,设置放缩比例系数λ=0.5。The dwell time distribution is iteratively calculated according to the required removal function H. In order to prevent over-compensation, only a certain proportion of the residual error is often compensated during compensation processing, rather than all compensation. The optimal solution is approached through repeated compensation iterations, and the scaling factor λ is set to 0.5.
根据待修面生成一系列合适间隔的驻留点,结合驻留函数R计算初始驻留时间T0:Generate a series of dwell points with appropriate intervals according to the surface to be repaired, and calculate the initial dwell time T0 in combination with the dwell function R:
T0=H/R;T 0 =H/R;
初始残余误差E0为:The initial residual error E0 is:
E0=H-T0*R;E 0 = HT 0 * R;
对残余误差进一步逼近,第i次迭代求残余时间ti为:To further approximate the residual error, the residual time ti of the i-th iteration is:
ti=Ei-1/R;t i =E i-1 /R;
经过这一次迭代后的新的驻留时间Ti和残余误差Ei为:After this iteration, the new dwell time Ti and residual error Ei are:
Ti=Ti-1+λti; Ti = Ti -1 + λt i ;
Ei=H-(Ti+λti)*R;E i =H-(T i +λt i )*R;
通过上述迭代过程一步步精确求解T的值,直到残余误差的RMS小于要求的阈值为止。此时各驻留点处的驻留时间分布已知,补偿抛光路径也相应地形成。Through the above iterative process, the value of T is accurately solved step by step until the RMS of the residual error is less than the required threshold. At this time, the dwell time distribution at each dwell point is known, and the compensation polishing path is formed accordingly.
根据补偿抛光路径进行补偿抛光,工艺参数与所使用的驻留函数相对应。抛光完毕后重复循环三反光学系统的波前测量至根据补偿抛光路径进行补偿抛光,直到测量三反光学系统时波前像差满足要求为止。Compensation polishing is performed according to the compensation polishing path, and the process parameters correspond to the dwell function used. After polishing is completed, the wavefront measurement of the three-mirror optical system is repeatedly cycled until compensation polishing is performed according to the compensation polishing path until the wavefront aberration meets the requirements when measuring the three-mirror optical system.
最终出射波前像差指导补偿抛光的效果如图5所示,补偿抛光前成像较模糊且波像差较大呈明显的环状误差,但经过补偿抛光后成像质量和波像差均有显著提升。The effect of the final output wavefront aberration-guided compensatory polishing is shown in Figure 5. Before compensatory polishing, the image is blurred and the wavefront aberration is large, showing an obvious annular error. However, after compensatory polishing, the image quality and wavefront aberration are significantly improved.
在本说明书的描述中,术语“一个实施例”、“一些实施例”等的描述意指结合该实施例或示例描述的具体特征、结构、材料或特点包含于本申请的至少一个实施例或示例中。在本说明书中,对上述术语的示意性表述不一定指的是相同的实施例或实例。而且,描述的具体特征、结构、材料或特点可以在任何的一个或多个实施例或示例中以合适的方式结合。In the description of this specification, the description of the terms "one embodiment", "some embodiments", etc. means that the specific features, structures, materials or characteristics described in conjunction with the embodiment or example are included in at least one embodiment or example of the present application. In this specification, the schematic representation of the above terms does not necessarily refer to the same embodiment or example. Moreover, the specific features, structures, materials or characteristics described can be combined in any one or more embodiments or examples in a suitable manner.
以上仅为本申请的优选实施例而已,并不用于限制本申请,对于本领域的技术人员来说,本申请可以有各种更改和变化。凡在本申请的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本申请的保护范围之内。The above are only preferred embodiments of the present application and are not intended to limit the present application. For those skilled in the art, the present application may have various modifications and variations. Any modification, equivalent replacement, improvement, etc. made within the spirit and principle of the present application shall be included in the protection scope of the present application.
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