CN107219626A - The freeform optics system optimization method of faying face shape and visual field optimisation strategy - Google Patents
The freeform optics system optimization method of faying face shape and visual field optimisation strategy Download PDFInfo
- Publication number
- CN107219626A CN107219626A CN201710528468.1A CN201710528468A CN107219626A CN 107219626 A CN107219626 A CN 107219626A CN 201710528468 A CN201710528468 A CN 201710528468A CN 107219626 A CN107219626 A CN 107219626A
- Authority
- CN
- China
- Prior art keywords
- field
- optimization
- view
- visual field
- zernike
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000005457 optimization Methods 0.000 title claims abstract description 171
- 238000000034 method Methods 0.000 title claims abstract description 54
- 230000000007 visual effect Effects 0.000 title claims description 17
- 230000003287 optical effect Effects 0.000 claims abstract description 56
- 238000011156 evaluation Methods 0.000 claims abstract description 6
- 238000012545 processing Methods 0.000 claims description 8
- 230000004075 alteration Effects 0.000 abstract description 27
- 230000008569 process Effects 0.000 abstract description 8
- 238000013461 design Methods 0.000 description 22
- 230000006870 function Effects 0.000 description 7
- 238000010586 diagram Methods 0.000 description 4
- 238000004088 simulation Methods 0.000 description 4
- 238000012512 characterization method Methods 0.000 description 3
- 238000012937 correction Methods 0.000 description 2
- 238000003384 imaging method Methods 0.000 description 2
- 238000012546 transfer Methods 0.000 description 2
- 238000004458 analytical method Methods 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000010354 integration Effects 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 230000008685 targeting Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/0012—Optical design, e.g. procedures, algorithms, optimisation routines
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B17/00—Systems with reflecting surfaces, with or without refracting elements
- G02B17/02—Catoptric systems, e.g. image erecting and reversing system
- G02B17/06—Catoptric systems, e.g. image erecting and reversing system using mirrors only, i.e. having only one curved mirror
- G02B17/0647—Catoptric systems, e.g. image erecting and reversing system using mirrors only, i.e. having only one curved mirror using more than three curved mirrors
- G02B17/0663—Catoptric systems, e.g. image erecting and reversing system using mirrors only, i.e. having only one curved mirror using more than three curved mirrors off-axis or unobscured systems in which not all of the mirrors share a common axis of rotational symmetry, e.g. at least one of the mirrors is warped, tilted or decentered with respect to the other elements
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/0025—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 for optical correction, e.g. distorsion, aberration
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B27/00—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
- G02B27/0081—Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00 with means for altering, e.g. enlarging, the entrance or exit pupil
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Lenses (AREA)
Abstract
本发明公开了一种结合面形和视场优化策略的自由曲面光学系统优化方法。该方法以表征光学系统波像差的Zernike标准多项式各项系数为评价依据,采用面形优化与视场优化相结合的逐步逼近策略开展优化过程,步骤如下:首先选取初始小视场,根据建立的XY多项式和多项式关系模型,每一步优化有针对性的找出系统像差最大项,选取自由曲面面形中相应XY多项式项作为新增变量对像差进行优化平衡,同时,根据系统各个视场的波像差rms值同步调整各视场的权重;在小视场范围内优化获取满足性能指标的结构后,逐步拓展视场,重复上述优化步骤,直至获取全视场范围内的光学系统结构参数。本发明具有视场大,优化速度快,有像差针对性和指导性的优点。
The invention discloses a method for optimizing a free-form surface optical system combined with surface shape and field of view optimization strategies. In this method, the coefficients of the Zernike standard polynomial that characterize the wave aberration of the optical system are used as the evaluation basis, and the optimization process is carried out by a stepwise approximation strategy combining surface shape optimization and field of view optimization. The steps are as follows: firstly, select the initial small field of view, XY polynomial and polynomial relationship model, each step of optimization is targeted to find out the largest item of system aberration, select the corresponding XY polynomial item in the free-form surface as a new variable to optimize and balance the aberration, and at the same time, according to each field of view of the system Synchronously adjust the weights of each field of view based on the rms value of the wave aberration; after optimizing and obtaining a structure that meets the performance index within a small field of view, gradually expand the field of view and repeat the above optimization steps until the structural parameters of the optical system within the entire field of view are obtained . The invention has the advantages of large field of view, fast optimization speed, pertinence and guidance of aberrations.
Description
技术领域technical field
本发明属于光学设计领域,具体涉及一种结合面形和视场优化策略的自由曲面光学系统优化方法。The invention belongs to the field of optical design, and in particular relates to a free-form surface optical system optimization method combined with surface shape and field of view optimization strategies.
背景技术Background technique
自由曲面离轴反射式光学系统设计方法广泛用于设计含有自由曲面的离轴反射式光学系统。近年来,自由曲面离轴反射式光学系统设计方法已经取得了很大的进步。为了实现具有大口径和大视场的光学系统,一些自由曲面光学系统设计方法被提出,比如朱钧等,在《Design method of freeform off-axis reflective imaging systems with adirect construction process》一文中提出的自由曲面离轴反射式成像系统直接设计方法,以及孟庆宇等在《Off-axis three-mirror freeform telescope with a largelinear field of view based on an integration mirror》一文中提出的利用自由曲面各项与像差的校正关系,利用XY多项式校正系统像差,这些方法均可以实现大视场大口径的离轴反射式光学系统设计。自由曲面离轴反射式光学系统设计方法是一个通过优化变量得到满足要求的系统的方法,常军等在《用于空间的三反射镜光学系统设计》一文中,将离轴三反光学系统设计方法成功应用于空间相机的设计加工。The free-form surface off-axis reflective optical system design method is widely used to design off-axis reflective optical systems with free-form surfaces. In recent years, freeform off-axis reflective optical system design methods have made great progress. In order to realize an optical system with a large aperture and a large field of view, some freeform surface optical system design methods have been proposed, such as Zhu Jun et al., in "Design method of freeform off-axis reflective imaging systems with adirect construction process". The direct design method of curved surface off-axis reflective imaging system, and the correction of aberrations and aberrations proposed by Meng Qingyu in the article "Off-axis three-mirror freeform telescope with a large linear field of view based on an integration mirror" relationship, using XY polynomials to correct system aberrations, these methods can realize the design of off-axis reflective optical systems with large field of view and large aperture. The free-form surface off-axis reflective optical system design method is a method to obtain a system that meets the requirements by optimizing variables. In the article "Design of Three-mirror Optical System for Space", Chang Jun et al. The method has been successfully applied to the design and processing of space cameras.
自由曲面离轴反射式光学系统设计方法是通过求解同轴反射式系统的初始结构,然后在同轴初始结构的基础上,对光学系统进行离轴化处理。得到离轴化处理后的光学系统的自由曲面采用多项式表征,然后对自由曲面增加优化变量对系统进行优化,最终得到满足技术指标的离轴反射式光学系统。由于自由曲面存在描述方法不够完善,可供借鉴的实例较少,像质平衡难度大以及边界条件控制复杂等问题,自由曲面光学系统的设计优化难度较大。自由曲面离轴系统的视场的采样数多,光线追迹数量较多,耗时长,光学系统平衡像差复杂,优化难度也随之变大。The free-form surface off-axis reflective optical system design method is to solve the initial structure of the coaxial reflective system, and then perform off-axis processing on the optical system on the basis of the coaxial initial structure. The free-form surface of the optical system obtained after off-axis processing is characterized by polynomials, and then optimization variables are added to the free-form surface to optimize the system, and finally an off-axis reflective optical system that meets the technical specifications is obtained. Due to the imperfect description methods of free-form surfaces, few examples for reference, difficulty in image quality balance, and complex control of boundary conditions, it is difficult to design and optimize free-form surface optical systems. The sampling number of the field of view of the free-form surface off-axis system is large, the number of ray tracing is large, and it takes a long time. The balance of aberrations in the optical system is complicated, and the difficulty of optimization also becomes greater.
为了更好的表征自由曲面,研究人员提出了Zernike多项式、XY多项式、高斯径向基函数以及非均匀有理B样条等方法对自由曲面面形进行表征。这些方法可以得到正确的表征形式,但是需要大量的计算。为了同时降低优化难度和提高优化效率,张新等在《基于矢量像差的自由曲面光学系统像差特性研究》一文中,提出了基于矢量像差的自由曲面设计方法。通过矢量像差分析,可以分析光学系统的像差特性。该方法主要是分析像差特性,但是在优化过程中,对像差的校正缺乏针对性。In order to better characterize free-form surfaces, researchers have proposed methods such as Zernike polynomials, XY polynomials, Gaussian radial basis functions, and non-uniform rational B-splines to characterize free-form surfaces. These methods can get the correct representation, but require a lot of computation. In order to reduce the optimization difficulty and improve the optimization efficiency at the same time, Zhang Xin et al. proposed a free-form surface design method based on vector aberration in the article "Aberration Characteristics of Free-form Surface Optical System Based on Vector Aberration". Through vector aberration analysis, the aberration characteristics of the optical system can be analyzed. This method mainly analyzes the aberration characteristics, but in the optimization process, the aberration correction is not targeted.
发明内容Contents of the invention
本发明的目的在于提供一种结合面形和视场优化策略的自由曲面光学系统优化方法,有针对性的校正含有自由曲面的离轴反射式光学系统像差,提高光学系统设计优化的效率。The purpose of the present invention is to provide a free-form surface optical system optimization method that combines the surface shape and field of view optimization strategy, which can correct the aberration of the off-axis reflective optical system containing the free-form surface in a targeted manner, and improve the efficiency of optical system design optimization.
实现本发明目的的技术解决方案为:一种结合面形和视场优化策略的自由曲面光学系统优化方法,方法步骤如下:The technical solution to realize the object of the present invention is: a method for optimizing a free-form surface optical system combining surface shape and field of view optimization strategy, the method steps are as follows:
步骤1、建立离轴三反初始结构:Step 1. Establish the initial structure of off-axis three counters:
参考离轴三反光学系统的实例,选取一个同轴三反光学系统初始结构;Referring to the example of the off-axis three-mirror optical system, select an initial structure of the coaxial three-mirror optical system;
步骤2、对离轴三反初始结构进行结构限制:Step 2. Structural constraints on the initial structure of the off-axis three-inverter:
在同轴反射式光学系统基础上进行离轴化处理,利用编写好的对应光学系统的限制光线遮挡的宏语言,在评价函数中加以调用,控制系统的结构,得到离轴系统初始结构和初始视场;On the basis of the coaxial reflective optical system, the off-axis processing is carried out, and the macro language corresponding to the optical system that limits light occlusion is used to call it in the evaluation function to control the structure of the system, and the initial structure and initial structure of the off-axis system are obtained. field of view;
步骤3、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行面形优化和视场优化;Step 3. Combining the optimization variables added by the surface shape optimization and the field of view weight of the field of view optimization, the system is optimized for surface shape and field of view;
步骤4、判断优化结果是否符合技术指标要求,若不满足当前视场要求,则转到步骤3对系统继续进行面形和视场优化;若不满足要求视场范围要求,则对系统进行视场拓展,然后转到步骤3结合视场和面形对系统进行优化;若符合当前视场指标要求并且视场范围符合指标要求,则结束优化。Step 4. Determine whether the optimization result meets the requirements of the technical indicators. If it does not meet the requirements of the current field of view, go to step 3 to continue to optimize the surface shape and field of view of the system; Expand the field, and then go to step 3 to optimize the system in combination with the field of view and surface shape; if the current field of view index requirements are met and the field of view range meets the index requirements, the optimization will end.
进一步地,步骤3所述面形优化的方法步骤如下:Further, the method steps of surface shape optimization described in step 3 are as follows:
1)导出分项表征的Zernike标准多项式系数Cij之后,计算全部视场各项Zernike系数平方和其中4≤j≤37;1) After deriving the Zernike standard polynomial coefficient C ij of the sub-item representation, calculate the sum of the squares of the Zernike coefficients for all fields of view where 4≤j≤37;
2)找出Zernike系数平方和最大项,记作Pm;2) Find the maximum term of the sum of squares of Zernike coefficients, denoted as P m ;
3)找到最大项Pm对应的XY多项式的自由项xmyn;3) Find the free term x m y n of the XY polynomial corresponding to the maximum term P m ;
4)判断最大项Pm对应的XY多项式的自由项xmyn中m是否为偶数,并且未曾作为优化变量,若满足这两个条件,则转到步骤6),若不满足,则转到步骤5);4) Determine whether m in the free term x m y n of the XY polynomial corresponding to the largest term P m is an even number, and has not been used as an optimization variable. If these two conditions are met, then go to step 6), if not, go to to step 5);
5)除去该Zernike项Pm,找出剩余项中系数平方和最大项,记作Pm;5) Remove the Zernike term P m , find out the maximum term of the square sum of coefficients in the remaining items, and denote it as P m ;
6)将xmyn设置为优化变量。6) Set x m y n as optimization variable.
进一步地,步骤3所述视场优化的方法步骤如下:Further, the method steps of field of view optimization described in step 3 are as follows:
1)对系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,计算得到单个视场的各项Zernike标准多项式系数平方和 1) Optimizing the field of view of the system, deriving the Zernike standard polynomial coefficient C ij of the sub-item representation, and calculating the sum of the squares of the Zernike standard polynomial coefficients of a single field of view
2)计算得到各个视场RMS值平均值 2) Calculate the average value of the RMS value of each field of view
3)计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。3) Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
本发明与现有技术相比,其显著优点在于:Compared with the prior art, the present invention has significant advantages in that:
(1)视场大:与其他自由曲面离轴反射式光学系统设计方法相比,该方法可以在优化过程中拓展视场,因此可以获得较大的视场范围;(1) Large field of view: Compared with other free-form surface off-axis reflective optical system design methods, this method can expand the field of view during the optimization process, so a larger field of view can be obtained;
(2)优化速度快:该方法结合面形优化和视场优化这两个方面对系统进行优化,能大大提高优化速度,提高优化效率;(2) Fast optimization speed: This method combines surface shape optimization and field of view optimization to optimize the system, which can greatly increase the optimization speed and improve the optimization efficiency;
(3)像差针对性:该方法结合Zernike多项式和XY多项式之间的关系,针对具体像差项进行校正,优化过程中具有像差针对性;(3) Aberration targeting: This method combines the relationship between Zernike polynomials and XY polynomials to correct specific aberration items, and the optimization process is aberration-specific;
(4)指导性:由于其他自由曲面离轴反射式光学系统设计方法都未公开具体的操作步骤,本文公开了具体的操作步骤,对光学系统设计具有指导性。(4) Guidance: Since other free-form surface off-axis reflective optical system design methods do not disclose specific operation steps, this paper discloses specific operation steps, which are instructive for optical system design.
附图说明Description of drawings
图1为本发明结构限制示意图。Fig. 1 is a schematic diagram of the structural limitations of the present invention.
图2为本发明的视场拓展的示意图。Fig. 2 is a schematic diagram of the field of view expansion of the present invention.
图3为本发明的实施例1仿真结果的是系统结构图。FIG. 3 is a system structure diagram showing the simulation results of Embodiment 1 of the present invention.
图4为本发明的实施例1仿真结果系统优化过程中的调制传递函数曲线图。FIG. 4 is a graph of the modulation transfer function during the system optimization process of the simulation results of Embodiment 1 of the present invention.
图5为本发明结合面形优化和视场优化策略的自由曲面离轴反射式光学系统设计方法流程图。FIG. 5 is a flow chart of the design method of the free-form surface off-axis reflective optical system combining surface shape optimization and field of view optimization strategies according to the present invention.
具体实施方式detailed description
下面结合附图对本发明作进一步详细描述。The present invention will be described in further detail below in conjunction with the accompanying drawings.
结合图1~5,本发明结合面形和视场优化策略的自由曲面光学系统优化方法,方法步骤如下:With reference to Figures 1 to 5, the present invention combines the surface shape and field of view optimization strategy for the free-form surface optical system optimization method, the method steps are as follows:
步骤1、建立离轴三反初始结构:Step 1. Establish the initial structure of off-axis three counters:
参考离轴三反光学系统的实例,选取一个同轴三反光学系统初始结构;Referring to the example of the off-axis three-mirror optical system, select an initial structure of the coaxial three-mirror optical system;
步骤2、结合图1,对离轴三反初始结构进行结构限制:Step 2. Combining with Figure 1, carry out structural restrictions on the initial structure of the off-axis three counters:
在同轴反射式光学系统基础上进行离轴化处理,利用编写好的对应光学系统的限制光线遮挡的宏语言,在评价函数中加以调用,控制系统的结构,得到离轴系统初始结构和初始视场;On the basis of the coaxial reflective optical system, the off-axis processing is carried out, and the macro language corresponding to the optical system that limits light occlusion is used to call it in the evaluation function to control the structure of the system, and the initial structure and initial structure of the off-axis system are obtained. field of view;
步骤3、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行面形优化和视场优化;Step 3. Combining the optimization variables added by the surface shape optimization and the field of view weight of the field of view optimization, the system is optimized for surface shape and field of view;
步骤4、判断优化结果是否符合技术指标要求,若不满足当前视场要求,则转到步骤3对系统继续进行面形和视场优化;若不满足要求视场范围要求,则对系统进行视场拓展,如图2所示,然后转到步骤3结合视场和面形对系统进行优化;若符合当前视场指标要求并且视场范围符合指标要求,则结束优化。Step 4. Determine whether the optimization result meets the requirements of the technical indicators. If it does not meet the requirements of the current field of view, go to step 3 to continue to optimize the surface shape and field of view of the system; Field expansion, as shown in Figure 2, and then go to step 3 to optimize the system in combination with the field of view and surface shape; if the current field of view index requirements are met and the field of view range meets the index requirements, then the optimization ends.
进一步地,步骤3所述面形优化的方法步骤如下:Further, the method steps of surface shape optimization described in step 3 are as follows:
1)导出分项表征的Zernike标准多项式系数Cij之后,计算全部视场各项Zernike系数平方和其中4≤j≤37;1) After deriving the Zernike standard polynomial coefficient C ij of the sub-item representation, calculate the sum of the squares of the Zernike coefficients for all fields of view where 4≤j≤37;
2)找出Zernike系数平方和最大项,记作Pm;2) Find the maximum term of the sum of squares of Zernike coefficients, denoted as P m ;
3)找到最大项Pm对应的XY多项式的自由项xmyn;3) Find the free term x m y n of the XY polynomial corresponding to the maximum term P m ;
4)判断最大项Pm对应的XY多项式的自由项xmyn中m是否为偶数,并且未曾作为优化变量,若满足这两个条件,则转到步骤6),若不满足,则转到步骤5);4) Determine whether m in the free term x m y n of the XY polynomial corresponding to the largest term P m is an even number, and has not been used as an optimization variable. If these two conditions are met, then go to step 6), if not, go to to step 5);
5)除去该Zernike项Pm,找出剩余项中系数平方和最大项,记作Pm;5) Remove the Zernike term P m , find out the maximum term of the square sum of coefficients in the remaining items, and denote it as P m ;
6)将xmyn设置为优化变量。6) Set x m y n as optimization variable.
进一步地,步骤3所述视场优化的方法步骤如下:Further, the method steps of field of view optimization described in step 3 are as follows:
1)对系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,计算得到单个视场的各项Zernike标准多项式系数平方和 1) Optimizing the field of view of the system, deriving the Zernike standard polynomial coefficient C ij of the sub-item representation, and calculating the sum of the squares of the Zernike standard polynomial coefficients of a single field of view
2)计算得到各个视场RMS值平均值 2) Calculate the average value of the RMS value of each field of view
3)计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。3) Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
图3为本发明的实施例1仿真结果的是系统结构图。图4为本发明的实施例1仿真结果系统优化过程中的调制传递函数曲线图。FIG. 3 is a system structure diagram showing the simulation results of Embodiment 1 of the present invention. FIG. 4 is a graph of the modulation transfer function during the system optimization process of the simulation results of Embodiment 1 of the present invention.
结合图5,一种结合面形优化和视场优化策略的自由曲面离轴反射式光学系统设计方法,方法步骤如下:Referring to Figure 5, a method for designing a free-form off-axis reflective optical system that combines surface shape optimization and field of view optimization strategies, the steps of the method are as follows:
步骤1、建立离轴三反初始结构:Step 1. Establish the initial structure of off-axis three counters:
参考离轴三反光学系统的实例,在同轴三反光学系统的基础上进行离轴化处理得到初始结构,系统焦距为1200mm,F数12,波长采用632.8nm的氦氖激光,其中主镜为偶次非球面,次镜为球面镜,三镜是采用XY多项式表征的自由曲面。Referring to the example of the off-axis three-mirror optical system, the initial structure is obtained by off-axis processing on the basis of the coaxial three-mirror optical system. It is an even-order aspheric surface, the secondary mirror is a spherical mirror, and the third mirror is a free-form surface characterized by XY polynomials.
步骤2、对离轴三反初始结构进行结构限制:Step 2. Structural constraints on the initial structure of the off-axis three-inverter:
利用编写好的对应光学系统的限制光线遮挡的宏语言,在评价函数中加以调用,控制系统的结构,得到初始结构和初始视场。Using the macro language that is written to limit light occlusion corresponding to the optical system, call it in the evaluation function, control the structure of the system, and obtain the initial structure and initial field of view.
步骤3、在初始视场的结构下,导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和按照图5流程图面形优化策略找出Zernike系数平方和最大项;找到最大项对应的XY多项式的自由项;对应的XY多项式的自由项中m是偶数,并且未曾作为优化变量,满足这两个条件,将自由项设置为优化变量。Step 3. Under the structure of the initial field of view, derive the Zernike standard polynomial coefficient C ij of the sub-item representation, and calculate the sum of the squares of Zernike coefficients for all fields of view Find the maximum term of the sum of the squares of Zernike coefficients according to the flow chart in Figure 5; find the free term of the XY polynomial corresponding to the maximum term; m in the free term of the corresponding XY polynomial is an even number, and has not been used as an optimization variable, satisfying these two condition, set the free term as the optimization variable.
步骤4、对当前系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 4. Optimize the field of view of the current system, derive the Zernike standard polynomial coefficient C ij of sub-item representation, and calculate the square sum of each Zernike standard polynomial coefficient of a single field of view according to the field of view optimization strategy in the flow chart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤5、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,优化得到的结果如图4(a)所示,符合当前技术指标的要求;Step 5. Combine the optimization variables added by the surface shape optimization and the field of view weight of the field of view optimization to optimize the system. The result of the optimization is shown in Figure 4(a), which meets the requirements of the current technical indicators;
步骤6、此时系统的视场范围不满足指标要求,需要对系统进行视场拓展;Step 6. At this time, the field of view of the system does not meet the requirements of the index, and the field of view of the system needs to be expanded;
步骤7、对系统进行视场拓展;Step 7, expand the field of view of the system;
步骤8、对拓展视场后的系统导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和按照图5流程图面形优化策略找出Zernike系数平方和最大项;找到最大项对应的XY多项式的自由项;对应的XY多项式的自由项中m是偶数,并且未曾作为优化变量,满足这两个条件,将XY多项式自由项设置为优化变量;Step 8. Deriving the Zernike standard polynomial coefficients C ij of sub-item representations for the system after the field of view is expanded, and calculating the sum of the squares of Zernike coefficients for all fields of view Find the maximum term of the sum of the squares of Zernike coefficients according to the flow chart in Figure 5; find the free term of the XY polynomial corresponding to the maximum term; m in the free term of the corresponding XY polynomial is an even number, and has not been used as an optimization variable, satisfying these two A condition, the XY polynomial free term is set as the optimization variable;
步骤9、对拓展视场后的系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 9. Optimize the field of view of the system after the field of view is expanded, derive the Zernike standard polynomial coefficient C ij of the sub-item representation, and calculate the square sum of the Zernike standard polynomial coefficients of a single field of view according to the field of view optimization strategy in the flow chart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤10、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,优化得到的结果如图4(b)所示,符合当前技术指标的要求Step 10. Combine the optimization variables added by the surface shape optimization and the field of view weight of the field of view optimization to optimize the system. The result of the optimization is shown in Figure 4(b), which meets the requirements of the current technical indicators
步骤11、此时系统的视场范围不满足指标要求,需要对系统进行视场拓展;Step 11. At this time, the field of view of the system does not meet the requirements of the index, and the field of view of the system needs to be expanded;
步骤12、对系统进行视场拓展;Step 12, expanding the field of view of the system;
步骤13、对拓展视场后的系统导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和按照图5流程图面形优化策略找出Zernike系数平方和最大项;找到最大项对应的XY多项式的自由项;对应的XY多项式的自由项中m是偶数,并且未曾作为优化变量,满足这两个条件,将XY多项式自由项设置为优化变量;Step 13. Deriving the Zernike standard polynomial coefficient C ij of the sub-item representation for the system after the field of view is expanded, and calculating the sum of the squares of Zernike coefficients for all fields of view Find the maximum term of the sum of the squares of Zernike coefficients according to the flow chart in Figure 5; find the free term of the XY polynomial corresponding to the maximum term; m in the free term of the corresponding XY polynomial is an even number, and has not been used as an optimization variable, satisfying these two A condition, the XY polynomial free term is set as the optimization variable;
步骤14、对拓展视场后的系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 14: Optimizing the field of view of the system after expanding the field of view, deriving Zernike standard polynomial coefficients C ij represented by sub-items, and calculating the sum of the squares of Zernike standard polynomial coefficients of a single field of view according to the field of view optimization strategy in the flow chart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤15、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,优化得到的结果如图4(c)所示,不符合当前技术指标的要求,需要对系统结合面形和视场优化策略对系统进一步优化;Step 15. Combine the optimization variables added by the surface shape optimization and the field of view weight of the field of view optimization to optimize the system. The result of the optimization is shown in Figure 4(c), which does not meet the requirements of the current technical indicators and needs to be combined with the system The surface shape and field of view optimization strategy further optimizes the system;
步骤16、对拓展视场后的系统导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和按照图5流程图面形优化策略找出Zernike系数平方和最大项;找到最大项对应的XY多项式的自由项;对应的XY多项式的自由项中m是偶数,并且未曾作为优化变量,满足这两个条件,将XY多项式自由项设置为优化变量;Step 16. Deriving the Zernike standard polynomial coefficient C ij of the sub-item representation for the system after the field of view is expanded, and calculating the sum of the squares of Zernike coefficients for all fields of view Find the maximum term of the sum of the squares of Zernike coefficients according to the flow chart in Figure 5; find the free term of the XY polynomial corresponding to the maximum term; m in the free term of the corresponding XY polynomial is an even number, and has not been used as an optimization variable, satisfying these two A condition, the XY polynomial free term is set as the optimization variable;
步骤17、对拓展视场后的系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 17: Optimizing the field of view of the system after the field of view is expanded, deriving Zernike standard polynomial coefficients C ij represented by sub-items, and calculating the sum of the squares of Zernike standard polynomial coefficients of a single field of view according to the field of view optimization strategy in the flowchart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤18、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,优化得到的结果如图4(d)所示,不符合当前技术指标的要求,需要对系统结合面形和视场优化策略对系统进一步优化;Step 18. Combine the optimization variables added by the surface shape optimization and the field of view weight of the field of view optimization to optimize the system. The result of the optimization is shown in Figure 4(d), which does not meet the requirements of the current technical indicators and needs to be combined with the system The surface shape and field of view optimization strategy further optimizes the system;
步骤19、对拓展视场后的系统导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和按照图5流程图面形优化策略找出Zernike系数平方和最大项;找到最大项对应的XY多项式的自由项;对应的XY多项式的自由项中m是偶数,并且未曾作为优化变量,满足这两个条件,将XY多项式自由项设置为优化变量;Step 19: Deriving Zernike standard polynomial coefficients C ij for sub-item representations of the expanded field of view system, and calculating the sum of the squares of Zernike coefficients for all fields of view Find the maximum term of the sum of the squares of Zernike coefficients according to the flow chart in Figure 5; find the free term of the XY polynomial corresponding to the maximum term; m in the free term of the corresponding XY polynomial is an even number, and has not been used as an optimization variable, satisfying these two A condition, the XY polynomial free term is set as the optimization variable;
步骤20、对拓展视场后的系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 20: Optimizing the field of view of the system after expanding the field of view, deriving the Zernike standard polynomial coefficients C ij represented by sub-items, and calculating the sum of the squares of the Zernike standard polynomial coefficients of a single field of view according to the field of view optimization strategy in the flowchart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤21、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,优化得到的结果如图4(e)所示,符合当前技术指标的要求;Step 21, optimize the system by combining the optimization variable added by the surface shape optimization and the field of view weight of the field of view optimization, and the result of the optimization is shown in Figure 4(e), which meets the requirements of the current technical indicators;
步骤22、此时系统的视场范围满足指标要求,结束优化。Step 22. At this time, the field of view of the system meets the index requirements, and the optimization ends.
实施例1Example 1
一种结合面形优化和视场优化策略的自由曲面离轴反射式光学系统设计方法,方法步骤如下:A free-form surface off-axis reflective optical system design method combining surface shape optimization and field of view optimization strategies, the method steps are as follows:
步骤1、建立离轴三反初始结构:Step 1. Establish the initial structure of off-axis three counters:
参考离轴三反光学系统的实例,在同轴三反光学系统的基础上进行离轴化处理得到初始结构,系统焦距为1200mm,F数12,波长采用632.8nm的氦氖激光,其中主镜为偶次非球面,次镜为球面镜,三镜是采用XY多项式表征的自由曲面。Referring to the example of the off-axis three-mirror optical system, the initial structure is obtained by off-axis processing on the basis of the coaxial three-mirror optical system. It is an even-order aspheric surface, the secondary mirror is a spherical mirror, and the third mirror is a free-form surface characterized by XY polynomials.
步骤2、对离轴三反初始结构进行结构限制:Step 2. Structural constraints on the initial structure of the off-axis three-inverter:
利用编写好的对应光学系统的限制光线遮挡的宏语言,在评价函数中加以调用,控制系统的结构,得到初始结构和初始视场0°×3°。Using the written macro language corresponding to the optical system to limit light occlusion, call it in the evaluation function, control the structure of the system, and obtain the initial structure and initial field of view 0°×3°.
步骤3、在初始视场的结构下,导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和按照图5流程图视场优化策略找出Zernike系数平方和最大项,此时Pm=P4;找到最大项P4对应的XY多项式的自由项为x2和y2项;P4对应的XY多项式的自由项x2和y2项中m是偶数,并且未曾作为优化变量,满足这两个条件,将x2和y2项设置为优化变量。Step 3. Under the structure of the initial field of view, derive the Zernike standard polynomial coefficient C ij of the sub-item representation, and calculate the sum of the squares of Zernike coefficients for all fields of view According to the field of view optimization strategy in the flow chart of Figure 5, find out the maximum term of the square sum of Zernike coefficients, at this time P m =P 4 ; find the free term of the XY polynomial corresponding to the maximum term P 4 as x 2 and y 2 items; P 4 corresponds to In the free term x2 and y2 of the XY polynomial, m is an even number and has not been used as an optimization variable. If these two conditions are met, the x2 and y2 items are set as optimization variables.
步骤4、对系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 4. Optimizing the field of view of the system, deriving the Zernike standard polynomial coefficient C ij of sub-item representation, and calculating the square sum of each Zernike standard polynomial coefficient of a single field of view according to the field of view optimization strategy in the flow chart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤5、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,优化得到的结果如图4(a)所示符合当前技术指标的要求;Step 5. Combine the optimization variables added by the surface shape optimization and the field of view weight of the field of view optimization to optimize the system, and the results obtained from the optimization meet the requirements of the current technical indicators as shown in Figure 4(a);
步骤6、判断此时系统的视场大小是否满足指标要求,此时视场不符合要求,需要对系统进行视场拓展;Step 6. Determine whether the field of view of the system meets the index requirements at this time. At this time, the field of view does not meet the requirements, and the field of view of the system needs to be expanded;
步骤7、对系统进行视场拓展;Step 7, expand the field of view of the system;
步骤8、在拓展视场的结构下,导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和按照图5流程图面形优化策略找出Zernike系数平方和最大项,此时Pm=P6;找到最大项P6对应的XY多项式的自由项为x2和y2项;P6项对应的XY多项式的自由项x2和y2项中m是偶数,然而已经作为优化变量,因此需要舍弃P6项,按照图5流程图面形优化的步骤,继续导出全部视场各项Zernike系数平方和找出Zernike系数平方和最大项,此时Pm=P4,与P6项类似,对应的XY多项式的自由项x2和y2项中m是偶数,然而已经作为优化变量,因此需要舍弃P4项,继续导出全部视场各项Zernike系数平方和找出Zernike系数平方和最大项,此时Pm=P5,对应的XY多项式的自由项xy项中m是奇数,不满足成为优化变量的条件,舍弃P5项;因此需要继续导出全部视场各项Zernike系数平方和找出Zernike系数平方和最大项,此时Pm=P7,对应P7的XY多项式的自由项x2y、y和y3项中m是偶数,而且未曾作为优化变量,因此,将x2y、y和y3项作为优化变量;;Step 8. Under the structure of expanding the field of view, derive the Zernike standard polynomial coefficient C ij of sub-item representation, and calculate the square sum of Zernike coefficients of all fields of view Find out the maximum term of the sum of the squares of Zernike coefficients according to the flowchart in Figure 5, at this time P m =P 6 ; find the free term of the XY polynomial corresponding to the maximum term P 6 to be x 2 and y 2 items; P 6 items correspond to Among the free terms x 2 and y 2 of the XY polynomial, m is an even number, but it has been used as an optimization variable, so it is necessary to discard the P 6 term, and continue to derive the Zernike coefficients of all fields of view according to the steps of graphic optimization in the flow chart of Figure 5 sum of square Find the maximum term of the square sum of Zernike coefficients. At this time, P m = P 4 , which is similar to the P 6 term. In the free term x 2 and y 2 of the corresponding XY polynomial, m is an even number, but it has already been used as an optimization variable, so it needs to be discarded P 4 items, continue to export the sum of the squares of Zernike coefficients in all fields of view Find the maximum term of the square sum of Zernike coefficients, at this time P m =P 5 , m in the free term xy term of the corresponding XY polynomial is an odd number, which does not meet the conditions for becoming an optimization variable, and the P 5 term is discarded; therefore, it is necessary to continue to derive all visual Sum of Squares of Zernike Coefficients in Field Find the maximum term of the sum of squares of Zernike coefficients, at this time P m =P 7 , the free term x 2 y, y and y of the XY polynomial corresponding to P 7 , m is an even number, and has not been used as an optimization variable. Therefore, x 2 y, y and y 3 items as optimization variables;
步骤9、对系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,计算得到单个视场的各项Zernike标准多项式系数平方和按照图5流程图视场优化策略计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 9. Optimizing the field of view of the system, deriving the Zernike standard polynomial coefficient C ij of sub-item representation, and calculating the sum of the squares of each Zernike standard polynomial coefficient of a single field of view According to the flow chart in Figure 5, the field of view optimization strategy is calculated to obtain the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤10、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,优化得到的结果如图4(b)所示符合当前技术指标的要求;Step 10, optimize the system by combining the optimization variable added by the surface shape optimization and the field of view weight of the field of view optimization, and the result of the optimization is shown in Figure 4(b) and meets the requirements of the current technical indicators;
步骤11、判断此时系统的视场大小是否满足指标要求,此时视场不符合要求,需要对系统进行视场拓展;Step 11. Determine whether the field of view of the system meets the index requirements at this time, and the field of view does not meet the requirements at this time, and the field of view of the system needs to be expanded;
步骤12、对系统进行视场拓展;Step 12, expanding the field of view of the system;
步骤13、导出此时光学系统的系统Zernike表征的波像差系数,按照图5流程图面形优化策略计算各视场单项像差系数平方和情况。导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和根据图5流程图中的面形优化策略,P4、P6、P5、P8、P7、P9对应的XY多项式的项不满足成为优化变量的两个条件,需要舍弃这六项,按照图5流程图视场优化策略找出Zernike系数平方和最大项,此时Pm=P11;找到最大项P11对应的XY多项式的自由项为x4、x2y2和y4项;P11对应的XY多项式的自由项x4、x2y2和y4项中m是偶数,并且未曾作为优化变量,满足这两个条件,将x4、x2y2和y4项这三项设置为优化变量。Step 13, deriving the wave aberration coefficients characterized by the system Zernike of the optical system at this time, and calculating the sum of the squares of the individual aberration coefficients of each field of view according to the graphic optimization strategy of the flowchart in Fig. 5 . Derive the Zernike standard polynomial coefficient C ij of sub-item characterization, and calculate the sum of the squares of Zernike coefficients for all fields of view According to the surface shape optimization strategy in the flow chart in Figure 5, the items of the XY polynomials corresponding to P 4 , P 6 , P 5 , P 8 , P 7 , and P 9 do not meet the two conditions for becoming optimization variables, and these six items need to be discarded , according to the field of view optimization strategy in the flow chart of Figure 5, find out the maximum term of the square sum of Zernike coefficients, at this time P m =P 11 ; find the free terms of the XY polynomial corresponding to the maximum term P 11 to be x 4 , x 2 y 2 and y 4 item; the free term x 4 , x 2 y 2 and y 4 of the XY polynomial corresponding to P 11 is an even number, and has not been used as an optimization variable. If these two conditions are met, x 4 , x 2 y 2 and y 4 These three items are set as optimization variables.
步骤14、对系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 14: Optimizing the field of view of the system, deriving Zernike standard polynomial coefficients C ij represented by sub-items, and calculating the sum of the squares of Zernike standard polynomial coefficients of a single field of view according to the field of view optimization strategy in the flowchart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤16、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,此时优化得到的结果如图4(c)所示不符合当前技术指标的要求,因此需要继续对系统进行面形和视场优化;Step 16. Combine the optimization variables added by surface shape optimization and the field of view weight of field of view optimization to optimize the system. At this time, the result obtained from the optimization does not meet the requirements of the current technical indicators as shown in Figure 4(c), so it is necessary to continue Optimize the surface shape and field of view of the system;
步骤17、导出此时光学系统的系统Zernike表征的波像差系数,按照图5流程图面形优化策略计算各视场单项像差系数平方和情况。导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和根据图5流程图中的面形优化策略,P4至P16项对应的XY多项式的项不满足成为优化变量的两个条件,需要舍弃这些项,按照图5流程图视场优化策略找出Zernike系数平方和最大项,此时Pm=P17;找到最大项P17对应的XY多项式的自由项为x4y、x2y3和y5项;P17对应的XY多项式的自由项x4y、x2y3和y5项中m是偶数,并且未曾作为优化变量,满足这两个条件,将x4y、x2y3和y5项这三项设置为优化变量。Step 17, deriving the wave aberration coefficients characterized by the system Zernike of the optical system at this time, and calculating the sum of the squares of the individual aberration coefficients of each field of view according to the graphic optimization strategy of the flowchart in Fig. 5 . Derive the Zernike standard polynomial coefficient C ij of sub-item characterization, and calculate the sum of the squares of Zernike coefficients for all fields of view According to the surface shape optimization strategy in the flow chart in Figure 5, the items of the XY polynomials corresponding to items P 4 to P 16 do not meet the two conditions for becoming optimization variables, and these items need to be discarded, and find out according to the field of view optimization strategy in the flow chart in Figure 5 Zernike coefficient square sum maximum term, at this time P m =P 17 ; find the free term of the XY polynomial corresponding to the maximum term P 17 to be x 4 y, x 2 y 3 and y 5 items; the free term of the XY polynomial corresponding to P 17 m in x 4 y, x 2 y 3 and y 5 items is an even number, and has not been used as an optimization variable. If these two conditions are met, the three items of x 4 y, x 2 y 3 and y 5 are set as optimization variables.
步骤18、对系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 18: Optimizing the field of view of the system, deriving Zernike standard polynomial coefficients C ij represented by sub-items, and calculating the sum of the squares of Zernike standard polynomial coefficients of a single field of view according to the field of view optimization strategy in the flowchart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤19、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,此时优化得到的结果如图4(d)所示不符合当前技术指标的要求,因此需要继续对系统进行面形和视场优化;Step 19: Combine the optimization variables added by the surface shape optimization and the field of view weight of the field of view optimization to optimize the system. At this time, the result obtained by the optimization does not meet the requirements of the current technical indicators as shown in Figure 4(d), so it is necessary to continue Optimize the surface shape and field of view of the system;
步骤20、导出此时光学系统的系统Zernike表征的波像差系数,按照图5流程图面形优化策略计算各视场单项像差系数平方和情况。导出分项表征的Zernike标准多项式系数Cij,计算全部视场各项Zernike系数平方和根据图5流程图中的面形优化策略,P4至P21项对应的XY多项式的项不满足成为优化变量的两个条件,需要舍弃,按照图5流程图视场优化策略找出Zernike系数平方和最大项,此时Pm=P22;找到最大项P22对应的XY多项式的自由项为x6、x2y4、x4y2和y6项;P22对应的XY多项式的自由项x6、x2y4、x4y2和y6项中m是偶数,并且未曾作为优化变量,满足这两个条件,将x6、x2y4、x4y2和y6项这四项设置为优化变量。Step 20, deriving the wave aberration coefficient characterized by the system Zernike of the optical system at this time, and calculating the sum of the squares of the individual aberration coefficients of each field of view according to the graphic optimization strategy of the flowchart in FIG. 5 . Derive the Zernike standard polynomial coefficient C ij of sub-item characterization, and calculate the sum of the squares of Zernike coefficients for all fields of view According to the surface shape optimization strategy in the flow chart in Figure 5, the XY polynomial items corresponding to items P 4 to P 21 do not meet the two conditions for becoming optimization variables and need to be discarded. Find the Zernike coefficient according to the field of view optimization strategy in the flow chart in Figure 5 The square sum of the maximum term, at this time P m =P 22 ; the free term of the XY polynomial corresponding to the maximum term P 22 is found to be x 6 , x 2 y 4 , x 4 y 2 and y 6 items; the corresponding XY polynomial of P 22 m in the free items x 6 , x 2 y 4 , x 4 y 2 and y 6 items is an even number, and has not been used as an optimization variable. If these two conditions are met, x 6 , x 2 y 4 , x 4 y 2 and y 6 items These four items are set as optimization variables.
步骤21、对系统进行视场优化,导出分项表征的Zernike标准多项式系数Cij,按照图5流程图视场优化策略计算得到单个视场的各项Zernike标准多项式系数平方和计算得到各个视场RMS值平均值计算单个视场的各项Zernike标准多项式系数平方和Qi除以平方和平均值A,得到Wi=Qi/A,将Wi作为每个视场的优化权重。Step 21: Optimizing the field of view of the system, deriving Zernike standard polynomial coefficients C ij represented by sub-items, and calculating the sum of the squares of Zernike standard polynomial coefficients of a single field of view according to the field of view optimization strategy in the flowchart in Figure 5 Calculate the average value of the RMS value of each field of view Calculate the square sum Q i of each Zernike standard polynomial coefficient of a single field of view and divide it by the average value A of the square sum to obtain W i =Q i /A , and take Wi as the optimization weight of each field of view.
步骤22、结合面形优化增加的优化变量和视场优化的视场权重,对系统进行优化,优化得到的结果如图4(e)所示,符合当前技术指标的要求;Step 22, optimize the system by combining the optimization variable added by the surface shape optimization and the field of view weight of the field of view optimization, and the result of the optimization is shown in Figure 4(e), which meets the requirements of the current technical indicators;
步骤23、判断此时系统的视场范围符合指标要求,结束优化。Step 23, judging that the field of view of the system meets the index requirements at this time, and ending the optimization.
本发明与其他含有自由曲面的离轴反射式光学系统相比,能够有针对性的校正光学系统中的像差,因此,优化具有针对性,优化速度提高,优化效率加大。同时在优化过程中逐步拓展视场,能够获得较大的视场范围。本发明公开了具体的设计方法的步骤,对于含有自由曲面的离轴反射式光学系统设计具有指导意义。Compared with other off-axis reflective optical systems containing free-form surfaces, the present invention can correct the aberration in the optical system in a targeted manner. Therefore, the optimization is targeted, the optimization speed is improved, and the optimization efficiency is increased. At the same time, the field of view is gradually expanded during the optimization process, and a larger field of view can be obtained. The invention discloses the steps of a specific design method, and has guiding significance for the design of off-axis reflective optical systems containing free-form surfaces.
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710528468.1A CN107219626B (en) | 2017-07-01 | 2017-07-01 | Optimization method of free-form surface optical system combining surface shape and field of view optimization strategy |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710528468.1A CN107219626B (en) | 2017-07-01 | 2017-07-01 | Optimization method of free-form surface optical system combining surface shape and field of view optimization strategy |
Publications (2)
Publication Number | Publication Date |
---|---|
CN107219626A true CN107219626A (en) | 2017-09-29 |
CN107219626B CN107219626B (en) | 2019-10-18 |
Family
ID=59951634
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201710528468.1A Active CN107219626B (en) | 2017-07-01 | 2017-07-01 | Optimization method of free-form surface optical system combining surface shape and field of view optimization strategy |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN107219626B (en) |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN110579277A (en) * | 2019-09-19 | 2019-12-17 | 中国科学院长春光学精密机械与物理研究所 | Optical system design method and optical system of large-field free-form surface spectrometer |
CN112130318A (en) * | 2020-09-24 | 2020-12-25 | 北京理工大学 | Optical free-form surface characterization method based on Gaussian radial basis function |
CN112305737A (en) * | 2019-08-01 | 2021-02-02 | 清华大学 | Design method of free-form surface reflective infrared imaging system |
CN113126289A (en) * | 2021-04-06 | 2021-07-16 | 北京理工大学 | Imaging system design method based on Gaussian radial basis function curved surface |
CN113238375A (en) * | 2021-04-20 | 2021-08-10 | 北京理工大学 | Method for generating initial structure of free-form surface imaging system based on deep learning |
CN114547855A (en) * | 2022-01-17 | 2022-05-27 | 北京理工大学 | Multi-objective automatic optimization method for optical imaging system |
CN118502113A (en) * | 2024-07-18 | 2024-08-16 | 中国科学院长春光学精密机械与物理研究所 | NURBS surface profile optimization method based on evaluation function |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105988214A (en) * | 2015-02-05 | 2016-10-05 | 清华大学 | Designing method of free-form surface off-axis imaging system with real exit pupil |
CN106199938A (en) * | 2016-09-18 | 2016-12-07 | 中国科学院长春光学精密机械与物理研究所 | Off-axis three reflecting optical systems in a kind of big visual field |
-
2017
- 2017-07-01 CN CN201710528468.1A patent/CN107219626B/en active Active
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105988214A (en) * | 2015-02-05 | 2016-10-05 | 清华大学 | Designing method of free-form surface off-axis imaging system with real exit pupil |
CN106199938A (en) * | 2016-09-18 | 2016-12-07 | 中国科学院长春光学精密机械与物理研究所 | Off-axis three reflecting optical systems in a kind of big visual field |
Non-Patent Citations (2)
Title |
---|
孟庆宇 等: "大线视场自由曲面离轴三反光学系统设计", 《红外与激光工程》 * |
巩盾等: "利用Zernik系数对离轴三反射系统进行计算机辅助装调", 《光学精密工程》 * |
Cited By (14)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN112305737B (en) * | 2019-08-01 | 2022-03-18 | 清华大学 | Design method of free-form surface reflective infrared imaging system |
CN112305737A (en) * | 2019-08-01 | 2021-02-02 | 清华大学 | Design method of free-form surface reflective infrared imaging system |
CN110579277A (en) * | 2019-09-19 | 2019-12-17 | 中国科学院长春光学精密机械与物理研究所 | Optical system design method and optical system of large-field free-form surface spectrometer |
CN110579277B (en) * | 2019-09-19 | 2021-02-12 | 中国科学院长春光学精密机械与物理研究所 | Optical system design method and optical system of large-field free-form surface spectrometer |
CN112130318B (en) * | 2020-09-24 | 2021-10-26 | 北京理工大学 | Optical free-form surface characterization method based on Gaussian radial basis function |
CN112130318A (en) * | 2020-09-24 | 2020-12-25 | 北京理工大学 | Optical free-form surface characterization method based on Gaussian radial basis function |
CN113126289A (en) * | 2021-04-06 | 2021-07-16 | 北京理工大学 | Imaging system design method based on Gaussian radial basis function curved surface |
CN113126289B (en) * | 2021-04-06 | 2022-02-11 | 北京理工大学 | A Design Method of Imaging System Based on Gaussian Radial Basis Function Surface |
CN113238375A (en) * | 2021-04-20 | 2021-08-10 | 北京理工大学 | Method for generating initial structure of free-form surface imaging system based on deep learning |
CN113238375B (en) * | 2021-04-20 | 2022-04-08 | 北京理工大学 | An initial structure generation method for free-form imaging system based on deep learning |
CN114547855A (en) * | 2022-01-17 | 2022-05-27 | 北京理工大学 | Multi-objective automatic optimization method for optical imaging system |
CN114547855B (en) * | 2022-01-17 | 2024-05-24 | 北京理工大学 | Multi-objective automatic optimization method for optical imaging system |
CN118502113A (en) * | 2024-07-18 | 2024-08-16 | 中国科学院长春光学精密机械与物理研究所 | NURBS surface profile optimization method based on evaluation function |
CN118502113B (en) * | 2024-07-18 | 2024-10-29 | 中国科学院长春光学精密机械与物理研究所 | NURBS surface profile optimization method based on evaluation function |
Also Published As
Publication number | Publication date |
---|---|
CN107219626B (en) | 2019-10-18 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN107219626A (en) | The freeform optics system optimization method of faying face shape and visual field optimisation strategy | |
CN105988213B (en) | The design method of free form surface off-axis optical system | |
CN104570340B (en) | The method for designing of free form surface imaging system | |
CN108152948B (en) | Design method of off-axis aspheric optical system | |
US8310481B2 (en) | Computer aided design method for enhancement of local refinement through T-splines | |
CN108227184B (en) | Design Method of Freeform Surface Imaging Optical System | |
CN104898275B (en) | The method for designing of off-axis three reflecting optical system of free form surface | |
CN109739019B (en) | Optimal design method of coaxial free-form optical system based on vector aberration theory | |
CN109387938B (en) | An Analysis Method for Tolerance Distribution of Free-form Surface of Optical System | |
JP2002139666A (en) | Method and device for optimizing optical system, and recording medium recording program for optimizing optical system | |
CN111487766B (en) | Design method of free-form surface off-axis three-mirror imaging system | |
CN105988212A (en) | Design method of three dimensional free-form curved surface | |
TW201935060A (en) | A method for making freeform surface off-axial imaging system | |
CN110727092A (en) | Off-axis reflection type two-mirror beam expanding system based on free-form surface | |
CN113126289B (en) | A Design Method of Imaging System Based on Gaussian Radial Basis Function Surface | |
CN108152939B (en) | Off-axis aspheric three-mirror optical system | |
TWI775093B (en) | Method for designing freeform imaging system | |
TWI748237B (en) | A method for making freeform surface reflective infrared imaging system | |
CN117406429A (en) | Sensitivity reduction design method of free-form optical system | |
Deng et al. | Three-mirror free-form off-axis antenna design of beam shaping on a circular substrate | |
CN115079391B (en) | Off-axis reflection system and design method of small F number multi-reflection off-axis system | |
CN116560075A (en) | Method for Determining Optical System Parameters | |
CN117930499A (en) | Optimization method of free-form surface prism and free-form surface prism | |
CN118151371A (en) | Automatic design method of long-focus lightweight free-form surface off-axis multi-reflection system | |
CN116859585A (en) | Off-axis reflective optical system initial structure design method |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |