CN114624877A - A Design Method of Large Field of View Diffractive Lenses Working in Infrared Bands - Google Patents

A Design Method of Large Field of View Diffractive Lenses Working in Infrared Bands Download PDF

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CN114624877A
CN114624877A CN202210257098.3A CN202210257098A CN114624877A CN 114624877 A CN114624877 A CN 114624877A CN 202210257098 A CN202210257098 A CN 202210257098A CN 114624877 A CN114624877 A CN 114624877A
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diffractive lens
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郑伊迪
雷柏平
何一苇
范斌
杨虎
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Abstract

The invention discloses a design method of a large-field-of-view diffraction lens working in an infrared band, which is different from the prior method that approximate microstructure height is obtained by a phase inversion or optimization method, but the microstructure is directly calculated, and a self-defined surface type which can be loaded by optical design software is provided, and the self-defined surface type can obtain a sudden change structure which is not contained in the prior optical design software and is similar to a Fresnel lens. The obtained microstructure can be further processed by using a ray tracing method, for example, defocusing is calculated, and data such as PSF (particle swarm optimization) can be further subjected to image analysis, processing and other operations. The invention can directly calculate and simulate the height of the microstructure through the wavelength and the material refractive index required in the optical design, and is suitable for both visible light and infrared bands.

Description

一种工作在红外波段的大视场衍射透镜的设计方法A Design Method of Large Field of View Diffractive Lenses Working in Infrared Bands

技术领域technical field

本发明涉及光学透镜技术领域,特别涉及一种工作在红外波段的大视场衍射透镜的设计方法。The invention relates to the technical field of optical lenses, in particular to a design method of a diffractive lens with a large field of view working in an infrared band.

背景技术Background technique

随着现代光学技术的发展,人们对于光学系统分辨率的要求越来越高,而根据分辨率公式

Figure BDA0003549081960000011
这里λ为光学系统的工作波长,D为光学系统的口径。由该公式可知,想要分辨率增加,这里的分辨率θ需要减小,这就需要光学系统的口径D不断增大,而口径的增大带来了加工所需精度高、光学系统较复杂以及光学系统重量大等问题。这导致光学系统的轻量化成像受到了限制,特别是对于便携式设备,比如手机相机,以及需要运载火箭进行托运的空间望远镜等应用提出了巨大的挑战。此外,高精度的光学系统带来的是对于透镜的高精度加工技术以及非常严格的公差分配的需要,非常不利于光学系统的量产。With the development of modern optical technology, people have higher and higher requirements for the resolution of optical systems, and according to the resolution formula
Figure BDA0003549081960000011
Here λ is the working wavelength of the optical system, and D is the aperture of the optical system. It can be seen from this formula that if the resolution is to be increased, the resolution θ here needs to be reduced, which requires the aperture D of the optical system to continuously increase, and the increase of the aperture brings about high processing precision and complex optical system. And the problem of the heavy weight of the optical system. This results in the limitation of lightweight imaging of optical systems, especially for applications such as portable devices, such as mobile phone cameras, and space telescopes that require a launch vehicle to be checked-in. In addition, the high-precision optical system brings the need for high-precision processing technology of the lens and very strict tolerance allocation, which is very unfavorable for the mass production of the optical system.

随着半导体微纳加工以及光学的发展,研究人员开始使用衍射光学系统作为替代传统折/反射式光学系统的解决方案。而衍射透镜具有强烈的负色散,于是为了消除衍射透镜的色散,设计了一大批比如折/衍光学系统,双/多层衍射元件以及Schupmann消色差光学结构等一系列可以消色差的光学结构。但是这些结构大多是将视场严格限制在很小的范围内,并且仍需要后方光学系统进行像差的校正。例如双/多层衍射元件所需的高精度对准也使这种结构依然停留在仿真过程。这些结构限制了衍射透镜在大视场光学系统中的应用。With the development of semiconductor micro-nano processing and optics, researchers began to use diffractive optical systems as a solution to replace traditional catadioptric/reflective optical systems. The diffractive lens has a strong negative dispersion, so in order to eliminate the dispersion of the diffractive lens, a series of achromatic optical structures, such as refractive/diffractive optical systems, double/multi-layer diffractive elements and Schupmann achromatic optical structures, are designed. However, most of these structures strictly limit the field of view to a small range, and still require the rear optical system for aberration correction. For example, the high precision alignment required for dual/multi-layer diffractive elements also keeps this structure still in the simulation process. These structures limit the application of diffractive lenses in large-field optical systems.

发明内容SUMMARY OF THE INVENTION

本发明提供了一种衍射透镜的设计方法,以解决当今衍射光学系统为了达到消色差的目的,导致光学系统视场受限制以及光学系统比较臃肿的问题。The present invention provides a method for designing a diffractive lens, so as to solve the problems that the current diffractive optical system achieves the purpose of achromatic, which causes the limited field of view of the optical system and the bloated optical system.

为了解决上述问题,本发明提供了如下技术方案:In order to solve the above problems, the present invention provides the following technical solutions:

一种工作在红外波段的大视场衍射透镜的设计方法,所述衍射透镜由具有不同微结构的环带组成,微结构求解步骤包括:A method for designing a diffractive lens with a large field of view working in an infrared band, the diffractive lens is composed of annular zones with different microstructures, and the microstructure solving steps include:

步骤S1,确定工作的目标波段,确定在该波段进行光学设计时使用的光学材料;Step S1, determine the target wavelength band of the work, and determine the optical material used in the optical design of the wavelength band;

步骤S2,确定所需衍射透镜的口径,焦距数据;Step S2, determine the aperture and focal length data of the required diffractive lens;

步骤S3,根据工作波长及所需材料的折射率,求解微结构高度;具体根据相位压缩公式,求出每个微结构的高度,表达式为:Step S3, according to the working wavelength and the refractive index of the required material, calculate the height of the microstructure; specifically, according to the phase compression formula, calculate the height of each microstructure, and the expression is:

Figure BDA0003549081960000021
Figure BDA0003549081960000021

其中,Hdoe为微结构高度,p为微结构高度的参数,λ0为衍射透镜的工作波长,n为所需材料的折射率;Among them, H doe is the height of the microstructure, p is the parameter of the height of the microstructure, λ 0 is the working wavelength of the diffractive lens, and n is the refractive index of the required material;

步骤S4,根据微结构高度,确定每个环带的最大半径,计算得出该环带的曲率半径数据,表达式为:Step S4, according to the height of the microstructure, determine the maximum radius of each annular zone, and calculate the radius of curvature data of the annular zone, and the expression is:

Figure BDA0003549081960000022
Figure BDA0003549081960000022

其中,Hdoe为微结构高度,Rmax为每个环带的最大半径,c为所求点的曲率半径,k为所求点的conic系数;Among them, H doe is the height of the microstructure, R max is the maximum radius of each annulus, c is the radius of curvature of the desired point, and k is the conic coefficient of the desired point;

步骤S5,根据衍射透镜的口径、焦距、微结构高度、曲率半径,求出衍射透镜微结构数据。In step S5, the microstructure data of the diffractive lens is obtained according to the aperture, focal length, microstructure height, and curvature radius of the diffractive lens.

进一步地,微结构高度随着p的增加而增加,这里的p是大于1的正整数,p值在200左右时效果较好。Further, the microstructure height increases with the increase of p, where p is a positive integer greater than 1, and the effect is better when the p value is around 200.

进一步地,得到每个环带的数据后,使用光学设计软件加载自定义表面,输入数据进行优化。Further, after obtaining the data for each annulus, use the optical design software to load the custom surface and input the data for optimization.

进一步地,光学设计软件通过加载自定义面型来得到具有突变结构的表面面型,进行优化求解表面面型坐标流程包括:Further, the optical design software obtains the surface shape with abrupt structure by loading the custom surface shape, and the optimization and solution of the surface shape coordinate process includes:

步骤S11,确定微结构的前一个面,在该面的的数据,确定在该面的结束点相对于入射面圆心的偏移量,形成衍射透镜前一个面的微结构;Step S11, determine the front surface of the microstructure, the data on this surface, determine the offset of the end point of the surface relative to the center of the incident surface, and form the microstructure of the front surface of the diffractive lens;

步骤S12,确定第Z个区域起始点的径向坐标,确定相对于前一个面结束点处的偏移量;Step S12, determine the radial coordinates of the starting point of the Zth area, and determine the offset relative to the end point of the previous surface;

步骤S13,与前一个面在S12规定点处偏移量相加,得到该区域结束点的总偏移量;Step S13, adding the offset of the previous surface at the specified point in S12 to obtain the total offset of the end point of the area;

步骤S14,确定给定点处的径向坐标,确定给定点所在的区域,计算给定点处的总偏移量;其中,给定点为非结束点;Step S14, determine the radial coordinates at the given point, determine the area where the given point is located, and calculate the total offset at the given point; wherein, the given point is a non-end point;

步骤S15,根据上述数据,画出衍射透镜剖面图。Step S15, according to the above data, draw a cross-sectional view of the diffractive lens.

进一步地,使用优化后所得的衍射透镜坐标数据进行加工。Further, processing is performed using the diffractive lens coordinate data obtained after optimization.

本发明提供的技术方案带来的有益效果:The beneficial effects brought by the technical scheme provided by the present invention:

1.本发明设计原理简单、效率高。1. The design principle of the present invention is simple and the efficiency is high.

2.解决了目前光学设计软件无法得到类似菲涅尔透镜的突变结构的问题。2. Solve the problem that the current optical design software cannot obtain the abrupt structure similar to the Fresnel lens.

3.具有一定的技术性,难以被模仿。3. It is technical and difficult to imitate.

附图说明Description of drawings

为了更清楚地说明本发明实施例中的技术方案,下面将对实施例描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to illustrate the technical solutions in the embodiments of the present invention more clearly, the following briefly introduces the accompanying drawings used in the description of the embodiments. Obviously, the accompanying drawings in the following description are only some embodiments of the present invention. For those of ordinary skill in the art, other drawings can also be obtained from these drawings without creative effort.

图1为本发明提供的工作在红外波段的大视场衍射透镜的设计方案流程图;Fig. 1 is the flow chart of the design scheme of the large field of view diffractive lens working in the infrared band provided by the present invention;

图2为本发明提供的自定义表面计算流程图;Fig. 2 is the custom surface calculation flow chart provided by the present invention;

图3为光学设计软件优化所得的系统点列图;Fig. 3 is the system dot diagram obtained by optical design software optimization;

图4为衍射透镜剖面示意图;4 is a schematic cross-sectional view of a diffractive lens;

图5为加工所得的衍射透镜实物图。Fig. 5 is the actual picture of the diffractive lens obtained by processing.

具体实施方式Detailed ways

以下结合附图和具体实例对本发明作进一步描述。The present invention will be further described below with reference to the accompanying drawings and specific examples.

本实例提供了一种工作在红外波段的大视场衍射透镜的设计方法,其中,所述大视场衍射透镜由根据非球面公式计算得到的具有高度差以及突变结构的微结构构成。本方法通过与光学设计软件相结合,设计了一种原理简单,加工方便,性能优异的大视场衍射透镜,具体的,如图1所示,该方法包括以下步骤:This example provides a method for designing a large field of view diffractive lens working in the infrared band, wherein the large field of view diffractive lens is composed of microstructures with height difference and abrupt structure calculated according to the aspheric surface formula. By combining this method with optical design software, a large field of view diffractive lens with simple principle, convenient processing and excellent performance is designed. Specifically, as shown in Figure 1, the method includes the following steps:

S1,确定工作的目标波段,确定在该波段进行光学设计时使用的光学材料;其中,所述光学材料为在所述目标工作波段内具有易加工性能的材料;具体的,本实施是针对入射波段在红外波段范围9-11μm处,以9μm为中心波长进行设计,采用的光学材料为锗(折射率为4)。S1, determine the working target wavelength band, and determine the optical material used in the optical design in this wavelength band; wherein, the optical material is a material with easy processing performance within the target working wavelength band; specifically, this implementation is for incident The wavelength band is in the infrared band range of 9-11 μm, and the center wavelength is 9 μm. The optical material used is germanium (refractive index is 4).

S2,确定所需衍射透镜的口径,焦距等数据;其中,所述衍射透镜直径为50mm,焦距为74.878mm,F数为4.5,视场角为21°。S2, determine the required diameter of the diffractive lens, focal length and other data; wherein, the diffractive lens has a diameter of 50mm, a focal length of 74.878mm, an F-number of 4.5, and a field of view angle of 21°.

S3,根据工作波长及所需材料的折射率,求解微结构高度;其中,选择p为20,对微结构高度进行计算,表达式为:S3, calculate the height of the microstructure according to the working wavelength and the refractive index of the required material; among them, select p to be 20, and calculate the height of the microstructure, and the expression is:

Figure BDA0003549081960000031
Figure BDA0003549081960000031

其中,Hdoe为微结构高度,Rmax为每个环带的最大半径,c为所求点的曲率半径,k为所求点的conic系数。Among them, H doe is the height of the microstructure, R max is the maximum radius of each annulus, c is the radius of curvature of the desired point, and k is the conic coefficient of the desired point.

S4,根据微结构高度,确定曲率半径等数据;表达式为:S4, according to the height of the microstructure, determine the radius of curvature and other data; the expression is:

Figure BDA0003549081960000041
Figure BDA0003549081960000041

其中,Hdoe为微结构高度,Rmax为每个环带的最大半径,c为所求点的曲率半径,k为所求点的conic系数。Among them, H doe is the height of the microstructure, R max is the maximum radius of each annulus, c is the radius of curvature of the desired point, and k is the conic coefficient of the desired point.

S5,根据上述数据,求出衍射透镜微结构数据。S5, based on the above data, obtain the microstructure data of the diffractive lens.

得到每个环带的数据后,使用光学设计软件加载自定义表面,输入数据进行优化。具体的,在本次施例中,所述每个环带的最大半径分别为(单位为mm):2.5,5,7.5,10,12,13.75,15.3,16.7,18,19.22,20.37,21.45,22.48,23.47,24.42,25.5,所述每个环带的conic系数均为0,所述每个环带的曲率半径分别为(单位为mm):229.214,229.381,229.650,229.894,230.106,230.276,230.431,230.590,230.740,230.917,231.092,231.226,231.414,231.602,231.839,231.975。Once the data for each annulus is obtained, use the optical design software to load the custom surface and enter the data for optimization. Specifically, in this embodiment, the maximum radius of each annular band is (in mm): 2.5, 5, 7.5, 10, 12, 13.75, 15.3, 16.7, 18, 19.22, 20.37, 21.45 , 22.48, 23.47, 24.42, 25.5, the conic coefficient of each annulus is 0, and the curvature radius of each annulus is (in mm): 229.214, 229.381, 229.650, 229.894, 230.106, 230.276 , 230.431, 230.590, 230.740, 230.917, 231.092, 231.226, 231.414, 231.602, 231.839, 231.975.

本实例使用光学设计软件对上述衍射透镜进行优化,光学设计软件所加载的自定义表面DLL流程图如图2所示,模拟得到了包括垂直入射条件下,大角度入射条件下的红外范围内的光斑分布。图3为各个角度的入射光经过光学系统后的系统点列图,点列图显示了不同角度入射下,光斑分布均位于艾里斑内,属于衍射受限系统,显示了该衍射透镜在工作波段内具有优异的大视场功能。In this example, the optical design software is used to optimize the above-mentioned diffractive lens. The flow chart of the custom surface DLL loaded by the optical design software is shown in Figure 2. The simulation results include the vertical incidence and the large-angle incidence in the infrared range. spot distribution. Figure 3 is the system spot diagram of the incident light at various angles after passing through the optical system. The spot diagram shows that under different angles of incidence, the light spot distribution is located in the Airy disk, which belongs to the diffraction limited system, which shows that the diffractive lens is working It has an excellent large field of view function within the band.

根据最终所得数据,画出了衍射透镜的剖面图,如图4所示。Based on the final data obtained, a cross-sectional view of the diffractive lens was drawn, as shown in Figure 4.

图5所示为最终加工得到的衍射透镜,使用金刚石车削技术进行加工,具有加工方便,误差较小的特点。Figure 5 shows the final processed diffractive lens, which is processed by diamond turning technology, which has the characteristics of convenient processing and small error.

综上,本发明根据聚焦所需的衍射透镜的波长以及光学材料,选定参数p,即可确定衍射透镜的微结构高度,通过合理设置各个环带的最大径向坐标,即可得到每个坐标的具体参数。所用微结构均为二次曲面,不存在复杂构型,且本衍射透镜对误差容忍度好,可以实现单片大视场透镜成像功能。To sum up, the present invention selects the parameter p according to the wavelength and optical material of the diffractive lens required for focusing, and the microstructure height of the diffractive lens can be determined. The specific parameters of the coordinates. The microstructures used are all quadric surfaces, there is no complex configuration, and the diffractive lens has good tolerance to errors, and can realize the imaging function of a single-piece large-field lens.

此外,需要说明的是,在本文中,术语“包括”、“包含”或者其任何其他变体意在涵盖非排他性的包含,从而使得包括一系列要素的过程、方法、物品或者终端设备不仅包括那些要素,而且还包括没有明确列出的其他要素,或者是还包括为这种过程、方法、物品或者终端设备所固有的要素。在没有更多限制的情况下,由语句“包括一个……”限定的要素,并不排除在包括所述要素的过程、方法、物品或者终端设备中还存在另外的相同要素。Furthermore, it should be noted that, herein, the terms "comprising", "comprising" or any other variation thereof are intended to encompass non-exclusive inclusion, such that a process, method, article or terminal device comprising a series of elements not only includes Those elements, but also other elements not expressly listed or inherent to such process, method, article or terminal equipment. Without further limitation, an element defined by the phrase "comprises a..." does not preclude the presence of additional identical elements in the process, method, article, or terminal device that includes the element.

最后需要说明的是,以上所述是本发明优选实施方式,应当指出,尽管已描述了本发明优选实施例,但对于本技术领域的技术人员来说,一旦得知了本发明的基本创造性概念,在不脱离本发明所述原理的前提下,还可以做出若干改进和润饰,这些改进和润饰也应视为本发明的保护范围。所以,所附权利要求意欲解释为包括优选实施例以及落入本发明实施例范围的所有变更和修改。Finally, it should be noted that the above are the preferred embodiments of the present invention. It should be pointed out that although the preferred embodiments of the present invention have been described, for those skilled in the art, once the basic inventive concept of the present invention is known , without departing from the principles of the present invention, several improvements and modifications can also be made, and these improvements and modifications should also be regarded as the protection scope of the present invention. Therefore, the appended claims are intended to be construed to include the preferred embodiments as well as all changes and modifications that fall within the scope of the embodiments of the present invention.

Claims (5)

1.一种工作在红外波段的大视场衍射透镜的设计方法,其特征在于,所述衍射透镜由具有不同微结构的环带组成,微结构求解步骤包括:1. a design method of a large field of view diffractive lens working in infrared waveband, is characterized in that, described diffractive lens is made up of the annular zone with different microstructures, and the microstructure solving step comprises: 步骤S1,确定工作的目标波段,确定在该波段进行光学设计时使用的光学材料;Step S1, determine the target wavelength band of the work, and determine the optical material used in the optical design of the wavelength band; 步骤S2,确定所需衍射透镜的口径,焦距数据;Step S2, determine the aperture and focal length data of the required diffractive lens; 步骤S3,根据工作波长及所需材料的折射率,求解微结构高度;具体根据相位压缩公式,求出每个微结构的高度,表达式为:Step S3, according to the working wavelength and the refractive index of the required material, calculate the height of the microstructure; specifically, according to the phase compression formula, calculate the height of each microstructure, and the expression is:
Figure FDA0003549081950000011
Figure FDA0003549081950000011
其中,Hdoe为微结构高度,p为微结构高度的参数,λ0为衍射透镜的工作波长,n为所需材料的折射率;Among them, H doe is the height of the microstructure, p is the parameter of the height of the microstructure, λ 0 is the working wavelength of the diffractive lens, and n is the refractive index of the required material; 步骤S4,根据微结构高度,确定每个环带的最大半径,计算得出该环带的曲率半径数据,表达式为:Step S4, according to the height of the microstructure, determine the maximum radius of each annular zone, and calculate the radius of curvature data of the annular zone, and the expression is:
Figure FDA0003549081950000012
Figure FDA0003549081950000012
其中,Hdoe为微结构高度,Rmax为每个环带的最大半径,c为所求点的曲率半径,k为所求点的conic系数;Among them, H doe is the height of the microstructure, R max is the maximum radius of each annulus, c is the radius of curvature of the desired point, and k is the conic coefficient of the desired point; 步骤S5,根据衍射透镜的口径、焦距、微结构高度、曲率半径,求出衍射透镜微结构数据。In step S5, the microstructure data of the diffractive lens is obtained according to the aperture, focal length, microstructure height, and curvature radius of the diffractive lens.
2.如权利要求1中所述的工作在红外波段的大视场衍射透镜的设计方法,其特征在于,微结构高度随着p的增加而增加,这里的p是大于1的正整数,p值在200左右时效果较好。2. The design method of a large field of view diffractive lens working in the infrared waveband as claimed in claim 1, wherein the height of the microstructure increases with the increase of p, where p is a positive integer greater than 1, and p Values around 200 work better. 3.如权利要求1中所述的工作在红外波段的大视场衍射透镜的设计方法,其特征在于,得到每个环带的数据后,使用光学设计软件加载自定义表面,输入数据进行优化。3. the design method of the large field of view diffractive lens working in the infrared waveband as claimed in claim 1, is characterized in that, after obtaining the data of each annular zone, use optical design software to load self-defined surface, input data to optimize . 4.如权利要求3中所述的工作在红外波段的大视场衍射透镜的设计方法,其特征在于,光学设计软件通过加载自定义面型来得到具有突变结构的表面面型,进行优化求解表面面型坐标流程包括:4. the design method of the large field of view diffractive lens working in the infrared band as claimed in claim 3, it is characterized in that, the optical design software obtains the surface profile with abrupt structure by loading the custom profile, and carries out the optimization solution The surface coordinate process includes: 步骤S11,确定微结构的前一个面的数据,确定在该面的结束点相对于入射面圆心的偏移量,形成衍射透镜前一个面的微结构;Step S11, determine the data of the previous surface of the microstructure, determine the offset of the end point of the surface relative to the center of the incident surface, and form the microstructure of the previous surface of the diffractive lens; 步骤S12,确定第Z个区域起始点的径向坐标,确定相对于前一个面结束点处的偏移量;Step S12, determine the radial coordinates of the starting point of the Zth area, and determine the offset relative to the end point of the previous surface; 步骤S13,与前一个面在S12规定点处偏移量相加,得到该区域结束点的总偏移量;Step S13, adding the offset of the previous surface at the specified point in S12 to obtain the total offset of the end point of the area; 步骤S14,确定给定点处的径向坐标,确定给定点所在的区域,计算给定点处的总偏移量;其中,给定点为非结束点;Step S14, determine the radial coordinates at the given point, determine the area where the given point is located, and calculate the total offset at the given point; wherein, the given point is a non-end point; 步骤S15,根据上述数据,画出衍射透镜剖面图。Step S15, according to the above data, draw a cross-sectional view of the diffractive lens. 5.如权利要求3中所述的工作在红外波段的大视场衍射透镜的设计方法,其特征在于,使用优化后所得的衍射透镜坐标数据进行加工。5 . The method for designing a diffractive lens with a large field of view working in the infrared waveband as claimed in claim 3 , wherein processing is performed using the optimized diffractive lens coordinate data. 6 .
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Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH10186231A (en) * 1996-10-24 1998-07-14 Asahi Optical Co Ltd How to design a diffractive lens
CN112394523A (en) * 2019-08-19 2021-02-23 上海鲲游光电科技有限公司 Dodging element, random rule manufacturing method and system thereof and electronic device
CN113281830A (en) * 2021-05-19 2021-08-20 烟台艾睿光电科技有限公司 Lens and optical lens

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH10186231A (en) * 1996-10-24 1998-07-14 Asahi Optical Co Ltd How to design a diffractive lens
CN112394523A (en) * 2019-08-19 2021-02-23 上海鲲游光电科技有限公司 Dodging element, random rule manufacturing method and system thereof and electronic device
CN113281830A (en) * 2021-05-19 2021-08-20 烟台艾睿光电科技有限公司 Lens and optical lens

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