CN103969787B - A kind of first assembling and positioning method of off-axis four anti-camera lenses - Google Patents
A kind of first assembling and positioning method of off-axis four anti-camera lenses Download PDFInfo
- Publication number
- CN103969787B CN103969787B CN201410219039.2A CN201410219039A CN103969787B CN 103969787 B CN103969787 B CN 103969787B CN 201410219039 A CN201410219039 A CN 201410219039A CN 103969787 B CN103969787 B CN 103969787B
- Authority
- CN
- China
- Prior art keywords
- reflector
- mirror
- interferometer
- axis
- compensator
- 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.)
- Active
Links
Landscapes
- Lenses (AREA)
- Telescopes (AREA)
Abstract
一种离轴四反镜头的初装定位方法,所述的离轴四反镜头包括主反射镜、次反射镜、第三反射镜、平面反射镜,其中主反射镜和第三反射镜为离轴非球面反射镜。利用零位补偿器对离轴反射镜光轴方向进行校准,四杆定位为各反射镜空间位置的调整提供基准,多台经纬仪组网实现、反射镜组件的初装定位。本发明结合光轴外引和四杆定位技术保证了离轴四反镜头初装达到一定的精度,为光学系统计算机辅助装调建立一个合理的起始点。
A method for initial installation and positioning of an off-axis four-mirror lens. The off-axis four-mirror lens includes a main reflector, a secondary reflector, a third reflector, and a plane reflector, wherein the main reflector and the third reflector are off-axis Axis Aspheric Mirrors. The zero position compensator is used to calibrate the optical axis direction of the off-axis mirror, the four-bar positioning provides a reference for the adjustment of the spatial position of each mirror, and the network of multiple theodolites realizes the initial assembly and positioning of the mirror components. The invention combines the optical axis external lead and the four-bar positioning technology to ensure that the initial assembly of the off-axis four-mirror lens reaches a certain accuracy, and establishes a reasonable starting point for the computer-aided assembly and adjustment of the optical system.
Description
技术领域technical field
本发明属于镜头装调与检测技术领域中,涉及一种离轴四反镜头的初装定位方法。The invention belongs to the technical field of lens assembly and detection, and relates to a method for initial assembly and positioning of an off-axis four-mirror lens.
背景技术Background technique
随着空间光学遥感器的广泛应用和飞速发展,大口径离轴光学系统因其具有无中心遮挡,能量利用率高,可以实现大视场和较高的地面分辨率等特点已得到广泛的应用。目前对离轴光学镜头的装调普遍采用计算机辅助装调技术,自准干涉法实时检测系统的波像差,计算机辅助装调软件分析干涉条纹,求解波面的多项式系数,给出各个光学元件的装调方向和量化值,指导修正各个元件相对位置误差达到最终设计要求。With the wide application and rapid development of space optical remote sensors, large-aperture off-axis optical systems have been widely used due to their characteristics of no central occlusion, high energy utilization, large field of view and high ground resolution. . At present, computer-aided adjustment technology is generally used for the adjustment of off-axis optical lenses. The self-collimating interferometry method detects the wave aberration of the system in real time. The computer-aided adjustment software analyzes the interference fringes, solves the polynomial coefficients of the wave surface, and gives the parameters of each optical element. Adjustment direction and quantitative value guide the correction of the relative position error of each component to meet the final design requirements.
针对传统的球面透射式光学系统和同轴全反射式非球面光学系统的装调可以利用较为成熟的定心装配工艺,专用的球心像定心仪可以准确的测量偏心量从而实现球面光学零件的定心,然后把多个光学零件严格地按照光轴的一致性进行装配。For the assembly and adjustment of traditional spherical transmissive optical system and coaxial total reflection aspheric optical system, relatively mature centering assembly technology can be used. Center, and then assemble multiple optical parts strictly according to the consistency of the optical axis.
由于离轴四反镜头零部件成型后本身就没有物理上的对称性,同时对系统的公差要求往往还更高,考虑到离轴反射镜作为母镜中的一部分,无法通过传统定心工艺准确确定反射镜的光轴;而同时离轴反射镜虚拟顶点给各镜空间位置调整带来困难,从而导致离轴四反镜头初装后存在较大的失调量,那么测试与计算机仿真计算结果的偏差将会很大,造成调整的效果无法收敛,导致计算机辅助装调失效。Since the off-axis four-mirror lens components have no physical symmetry after molding, and the tolerance requirements for the system are often higher, considering that the off-axis mirror is a part of the mother mirror, it cannot be accurately centered through the traditional centering process. Determine the optical axis of the mirror; at the same time, the virtual vertex of the off-axis mirror brings difficulties to the adjustment of the spatial position of each mirror, which leads to a large amount of misalignment after the initial installation of the off-axis four-mirror lens. The deviation will be very large, causing the effect of the adjustment to fail to converge, resulting in the failure of the computer-aided adjustment.
发明内容Contents of the invention
本发明解决的技术问题是:克服现有技术的不足,提供一种离轴四反镜头的初装定位方法,在离轴四反镜头初装阶段对光轴、离轴角、离轴量和镜间距有效控制,大大提高了光学系统初装定位精度,为下一步计算机辅助精密装调创造条件。The technical problem solved by the present invention is: to overcome the deficiencies of the prior art, to provide a kind of off-axis four-mirror lens initial installation positioning method, in the off-axis four-mirror lens initial installation stage, the optical axis, off-axis angle, off-axis amount and The effective control of the mirror distance greatly improves the positioning accuracy of the initial assembly of the optical system and creates conditions for the next step of computer-aided precision assembly.
本发明的技术解决方案:一种离轴四反镜头的初装定位方法,所述的离轴四反镜头包括主反射镜、次反射镜、第三反射镜、平面反射镜,其中主反射镜和第三反射镜为离轴非球面反射镜;步骤如下:The technical solution of the present invention: a method for initial installation and positioning of an off-axis four-mirror lens. The off-axis four-mirror lens includes a main reflector, a secondary reflector, a third reflector, and a plane reflector, wherein the main reflector and the third mirror are off-axis aspheric mirrors; the steps are as follows:
1)利用第一干涉仪、零位补偿器将主反射镜的光轴方向引出;设光束入射面为主反射镜正面,利用两台经纬仪交会对接测量获得主反射镜的光轴方向与主反射镜背面法线方向的夹角α;1) Use the first interferometer and zero compensator to lead out the direction of the optical axis of the main reflector; set the incident surface of the light beam to the front of the main reflector, and use two theodolites to measure and measure the optical axis of the main reflector and the direction of the main reflector The included angle α of the normal direction of the back of the mirror;
2)利用第一干涉仪、零位补偿器将第三反射镜的光轴方向引出;设光束入射面为第三反射镜正面,利用两台经纬仪交会对接测量获得第三反射镜的光轴方向与第三反射镜背面法线方向的夹角β;2) Utilize the first interferometer and the zero compensator to lead out the optical axis direction of the third reflector; set the incident surface of the light beam as the front of the third reflector, and obtain the optical axis direction of the third reflector by means of two theodolite rendezvous and docking measurements Angle β with the normal direction on the back of the third mirror;
3)由离轴四反镜头的光学设计数据计算并制作四根长杆,长杆材料选取低膨胀系数的石英玻璃,四根长杆的四个端头均制成球头型,四个球头位置分别代表入射视场中心位置、主反射镜的镜面中心位置、次反射镜的镜面中心位置和第三反射镜的镜面中心位置;3) Calculate and manufacture four long rods from the optical design data of the off-axis four-mirror lens. The material of the long rods is quartz glass with a low expansion coefficient. The four ends of the four long rods are all made into ball heads. The four balls The head positions respectively represent the center position of the incident field of view, the mirror center position of the primary reflector, the mirror center position of the secondary reflector and the mirror center position of the third reflector;
4)将四根长杆置于调整支架上,调整入射视场中心点和次反射镜中心点的高度,确定中心视场的弧矢面,次反射镜作为基准,依次调整主反射镜和第三反射镜,直至各反射镜镜面中心接触长杆球头;4) Place the four long rods on the adjustment bracket, adjust the height of the center point of the incident field of view and the center point of the secondary reflector, determine the sagittal plane of the central field of view, use the secondary reflector as a reference, and adjust the primary reflector and the third reflector in turn. reflector until the center of each reflector surface contacts the ball head of the long rod;
5)设光束入射面为主反射镜正面,架设两台经纬仪交会对接测量获得第二干涉仪标准平面镜和主反射镜背面法线方向的夹角α1,调整主反射镜使得α1与步骤1)中的α一致;5) Set the incident surface of the light beam on the front side of the main reflector, set up two theodolites to rendezvous and dock to measure the included angle α 1 between the standard plane mirror of the second interferometer and the normal direction on the back of the main reflector, and adjust the main reflector so that α 1 and step 1 ) in the same α;
6)设光束入射面为第三反射镜正面,架设两台经纬仪交会对接测量获得第二干涉仪标准平面镜和第三反射镜背面法线方向的夹角β1,调整第三反射镜使得β1与步骤2)中的β一致;6) Let the incident surface of the light beam be the front of the third reflector, set up two theodolites to meet and dock to measure the included angle β 1 between the standard plane mirror of the second interferometer and the normal direction on the back of the third reflector, and adjust the third reflector so that β 1 Consistent with β in step 2);
7)第二干涉仪发出的平行光经过离轴四反镜头的主反射镜、次反射镜、第三反射镜、平面反射镜后,汇聚到标准球面镜后返回并在第二干涉仪形成干涉条纹,完成离轴四反的初装定位。7) The parallel light emitted by the second interferometer passes through the main reflector, secondary reflector, third reflector, and plane reflector of the off-axis four-mirror lens, converges to the standard spherical mirror, returns and forms interference fringes in the second interferometer , to complete the initial installation and positioning of the off-axis four-anti.
步骤1)中光轴方向引出的具体方法为:将第一干涉仪、零位补偿器以及主反射镜从左至右依次放置,第一干涉仪出射的平面波经过零位补偿器变成非球面波,非球面波被主反射镜反射后按照原路返回,再经过零位补偿器后回到第一干涉仪,调整零位补偿器和主反射镜的位置,直至第一干涉仪测量得到的数值与主反射镜的面形参数值相等,固定零位补偿器和主反射镜的位置,此时主反射镜的光轴与第一干涉仪出射光方向平行。The specific method of drawing out the direction of the optical axis in step 1) is: place the first interferometer, the zero compensator and the main mirror in sequence from left to right, and the plane wave emitted by the first interferometer passes through the zero compensator and becomes an aspheric surface After the aspheric wave is reflected by the main reflector, it returns to the original path, and then returns to the first interferometer after passing through the zero compensator. Adjust the positions of the zero compensator and the main reflector until the first interferometer measures The value is equal to the surface shape parameter value of the main reflector, and the positions of the zero compensator and the main reflector are fixed. At this time, the optical axis of the main reflector is parallel to the outgoing light direction of the first interferometer.
步骤2)中光轴方向引出的具体方法为:将第一干涉仪、零位补偿器以及第三反射镜从左至右依次放置,第一干涉仪出射的平面波经过零位补偿器变成非球面波,非球面波被第三反射镜反射后按照原路返回,再经过零位补偿器后回到第一干涉仪,调整零位补偿器和第三反射镜的位置,直至第一干涉仪测量得到的数值与第三反射镜的面形参数值相等,固定零位补偿器和第三反射镜的位置,此时第三反射镜的光轴与第一干涉仪出射光方向平行。The specific method for extracting the direction of the optical axis in step 2) is: place the first interferometer, the zero compensator and the third reflector in sequence from left to right, and the plane wave emitted by the first interferometer passes through the zero compensator and becomes non- Spherical waves, aspheric waves are reflected by the third reflector and return to the original path, and then return to the first interferometer after passing through the zero compensator. Adjust the positions of the zero compensator and the third reflector until the first interferometer The measured value is equal to the surface shape parameter value of the third reflector, and the positions of the zero compensator and the third reflector are fixed. At this time, the optical axis of the third reflector is parallel to the outgoing light direction of the first interferometer.
本发明与现有技术相比的积极效果是:由于离轴四反镜头零部件成型后本身就没有物理上的对称性,虚拟顶点给各镜空间位置调整带来困难。因此,在离轴四反镜头光学系统进行计算机辅助装调前提出利用四杆定位和多台经纬仪组网方法来调整各反射镜在主体框中的空间位置,从而使得大口径离轴四反镜头的初装定位过程在理论指导下可视、定量、有序地完成,实现了对镜间距、光轴方向和离轴量的控制与精确调整,提高了离轴四反镜头中各反射镜空间位置摆放的定位精度,使得高精度干涉仪能够精确检测光学系统像质为计算机辅助装调算法建立一个合理的起始点,从而有效地提高了装调效率。同时,该方案也适应于所有离轴四反镜头的初装定位。Compared with the prior art, the positive effect of the present invention is that since the off-axis four-mirror lens parts have no physical symmetry after forming, the virtual vertex brings difficulties to the spatial position adjustment of each mirror. Therefore, before the computer-aided adjustment of the off-axis four-mirror lens optical system, it is proposed to use four-bar positioning and multiple theodolite networking methods to adjust the spatial position of each mirror in the main frame, so that the large-diameter off-axis four-mirror lens Under the guidance of theory, the positioning process of initial assembly is completed visually, quantitatively and orderly, which realizes the control and precise adjustment of the mirror distance, optical axis direction and off-axis amount, and improves the space of each mirror in the off-axis four-mirror lens. The positioning accuracy of the position placement enables the high-precision interferometer to accurately detect the image quality of the optical system and establish a reasonable starting point for the computer-aided adjustment algorithm, thereby effectively improving the adjustment efficiency. At the same time, this solution is also suitable for the initial installation and positioning of all off-axis four-mirror lenses.
附图说明Description of drawings
图1为离轴非球面零位补偿器光轴外引示意图;Figure 1 is a schematic diagram of the external introduction of the optical axis of the off-axis aspheric zero compensator;
图2为四杆定位和光轴调整示意图。Figure 2 is a schematic diagram of four-bar positioning and optical axis adjustment.
具体实施方式detailed description
本发明一种离轴四反镜头的初装定位方法,所述的离轴四反镜头包括主反射镜4、次反射镜5、第三反射镜6、平面反射镜7,其中主反射镜4和第三反射镜6为离轴非球面反射镜3;下面结合图1-图2对本发明的离轴四反镜头初装定位的具体实施方式作详细说明:The present invention is an initial installation and positioning method of an off-axis four-mirror lens. The off-axis four-mirror lens includes a main reflector 4, a secondary reflector 5, a third reflector 6, and a plane reflector 7, wherein the main reflector 4 And the 3rd reflector 6 is off-axis aspheric reflector 3; Below in conjunction with Fig. 1-Fig. 2, the specific embodiment of the off-axis four-mirror lens of the present invention is described in detail:
干涉仪1发出一束平面波经过零位补偿器2变成所需的非球面波,非球面波被离轴非球面反射镜反射后按照原路返回,经过零位补偿器回到干涉仪。如图1所示,补偿器与干涉仪的光路调节至严格平行(精度可控在10″以内),反复调节离轴非球面反射镜的方位直到测量得到的数值与离轴非球面反射镜的面形参数值相等,此时离轴非球面反射镜的主光轴与补偿器、干涉仪的光轴重合。两台经纬仪交会对接测试将离轴非球面反射镜光轴方向引到反射镜背面基准面。由于补偿器自身装配精度、检测光路调整误差和交会测量误差等引起光轴引出精度约为1′。Interferometer 1 emits a beam of plane waves and passes through zero compensator 2 to become the required aspheric wave. The aspheric wave is reflected by the off-axis aspheric mirror and then returns to the interferometer through the zero compensator. As shown in Figure 1, the optical paths of the compensator and the interferometer are adjusted to be strictly parallel (the accuracy can be controlled within 10″), and the orientation of the off-axis aspheric mirror is repeatedly adjusted until the measured value is consistent with that of the off-axis aspheric mirror. The surface shape parameter values are equal, at this time the main optical axis of the off-axis aspheric mirror coincides with the optical axis of the compensator and interferometer. Two theodolite rendezvous and docking tests lead the direction of the optical axis of the off-axis aspheric mirror to the back of the mirror Reference plane. Due to the assembly accuracy of the compensator itself, the adjustment error of the detection optical path and the error of intersection measurement, etc., the optical axis extraction accuracy is about 1′.
1)利用第一干涉仪1、零位补偿器2将主反射镜6的光轴方向引出;设光束入射面为主反射镜4正面,利用两台经纬仪交会对接测量获得主反射镜4的光轴方向与主反射镜4背面法线方向的夹角α,1) Utilize the first interferometer 1 and the zero compensator 2 to draw the optical axis direction of the main reflector 6; set the light beam incident surface on the front of the main reflector 4, and use two theodolites to measure and obtain the light of the main reflector 4 The included angle α between the axial direction and the normal direction of the back surface of the main reflector 4,
2)利用第一干涉仪1、零位补偿器2将第三反射镜6的光轴方向引出;设光束入射面为第三反射镜6正面,利用两台经纬仪(T1、T2)交会对接测量获得第三反射镜6的光轴方向与第三反射镜6背面法线方向的夹角β;2) Utilize the first interferometer 1 and the zero position compensator 2 to lead out the optical axis direction of the third reflector 6; set the incident surface of the light beam as the front of the third reflector 6, and use two theodolites (T1, T2) to meet and measure Obtain the angle β between the optical axis direction of the third reflector 6 and the normal direction on the back of the third reflector 6;
3)主体框放置于二维调整台10上,次反射镜5安装在主体框上作为基准,两台经纬仪交会测量第二干涉仪标准平面8与次反射镜5之间的夹角,通过旋转调整台10使得两者之间夹角为Φ,从而将光轴外引至标准平面反射镜8。3) The main body frame is placed on the two-dimensional adjustment table 10, the secondary reflector 5 is installed on the main frame as a reference, and the angle between the second interferometer standard plane 8 and the secondary reflector 5 is measured by the intersection of two theodolites, and the The adjustment table 10 makes the angle between the two is Φ, so that the optical axis is led out to the standard plane reflector 8 .
4)选取四根长杆的四个端点(A、B、C、D)分别代表入射视场、主反射镜4、次反射镜5和第三反射镜6的镜面中心位置。根据光学系统数据导入PRE结构设计软件,由各反射镜镜面中心位置计算得到四杆的理论长度和角度,材料为低膨胀系数的石英玻璃,两端制成球头。4) The four end points (A, B, C, D) of the four long rods are selected to represent the incident field of view, the mirror center positions of the primary reflector 4, the secondary reflector 5 and the third reflector 6, respectively. According to the optical system data imported into the PRE structure design software, the theoretical length and angle of the four rods are calculated from the center positions of the mirror surfaces of each mirror. The material is quartz glass with a low expansion coefficient, and the two ends are made of ball heads.
5)如图2所示,将四杆置于调整支架上,设第二干涉仪光束入射面为主反射镜6正面,激光器11发出一束激光经端点A和端点B,调整四杆使得AB连线与第二干涉仪标准平面镜法线方向平行,然后,调整入射视场中心点A和次反射镜5中心点C的高度一致,从而确定中心视场的弧矢面,依次调整主反射镜4、次反射镜5和第三反射镜6,直至接触位置B、C、D。5) As shown in Figure 2, place the four rods on the adjustment bracket, set the incident surface of the light beam of the second interferometer on the front of the main reflector 6, and the laser 11 emits a beam of laser light through endpoints A and B, and adjust the four rods so that AB The connecting line is parallel to the normal direction of the standard plane mirror of the second interferometer, and then, adjust the height of the center point A of the incident field of view and the center point C of the secondary reflector 5 to be consistent, thereby determining the sagittal plane of the central field of view, and adjusting the main reflector 4 in turn , the secondary mirror 5 and the third mirror 6, until the contact positions B, C, D.
6)架设三台经纬仪(T3、T4、T5)分别自准主反射镜背面、第三反射镜背面和干涉仪标准平面反射镜,调整主反射镜4和第三反射镜6倾斜和俯仰使得各镜光轴方向与系统光轴方向重合。设光束入射面为主反射镜4正面,架设两台经纬仪(T4、T5)交会对接测量获得第二干涉仪标准平面镜8和主反射镜4背面法线方向的夹角α1,调整主反射镜4使得α1与步骤1中的α一致;架设两台经纬仪(T3、T5)交会对接测量获得第二干涉仪标准平面镜8和第三反射镜6背面法线方向的夹角β1,调整第三反射镜6使得β1与步骤2)中的β一致;6) Set up three theodolites (T3, T4, T5) to self-align the back of the main mirror, the back of the third mirror and the standard plane mirror of the interferometer respectively, adjust the tilt and pitch of the main mirror 4 and the third mirror 6 so that each The mirror optical axis direction coincides with the system optical axis direction. Assume that the incident surface of the light beam is the front of the main reflector 4, set up two theodolites (T4, T5) to meet and dock to measure the included angle α 1 between the second interferometer standard plane mirror 8 and the normal direction on the back of the main reflector 4, and adjust the main reflector 4 Make α 1 consistent with α in step 1; set up two theodolites (T3, T5) for rendezvous and docking measurement to obtain the angle β 1 between the normal direction of the second interferometer standard plane mirror 8 and the back surface of the third mirror 6, adjust the first Three reflecting mirrors 6 make β 1 consistent with β in step 2);
7)采用自准干涉测量系统实时检测离轴四反镜头的波像差,如图2所示,第二干涉仪8发出平行光经过离轴四反镜头主反射镜4、次反射镜5、第三反射镜6和平面反射镜7,汇聚到标准球面镜9原路返回形成干涉条纹,高精度干涉仪测得初装定位后系统像差的均方根值(RMS值)为0.263λ(λ=632.8nm),然后经过四次计算机辅助装调各视场像质满足要求。实践证明该方案具有很高的定位精度使得调整收敛速度很快,有效地提高了装调效率,缩短了装调周期。7) The wave aberration of the off-axis four-mirror lens is detected in real time by using the self-aligning interferometry system. As shown in FIG. The third reflector 6 and the plane reflector 7 converge to the standard spherical mirror 9 and return to form interference fringes. The root mean square value (RMS value) of the system aberration measured by the high-precision interferometer after the initial installation and positioning is 0.263λ(λ =632.8nm), and then after four computer-aided adjustments, the image quality of each field of view meets the requirements. Practice has proved that this scheme has high positioning accuracy, which makes the adjustment convergence speed very fast, effectively improves the installation and adjustment efficiency, and shortens the installation and adjustment cycle.
本发明说明书中未作详细描述的内容属本领域技术人员的公知技术。The content that is not described in detail in the description of the present invention belongs to the well-known technology of those skilled in the art.
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201410219039.2A CN103969787B (en) | 2014-05-22 | 2014-05-22 | A kind of first assembling and positioning method of off-axis four anti-camera lenses |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201410219039.2A CN103969787B (en) | 2014-05-22 | 2014-05-22 | A kind of first assembling and positioning method of off-axis four anti-camera lenses |
Publications (2)
Publication Number | Publication Date |
---|---|
CN103969787A CN103969787A (en) | 2014-08-06 |
CN103969787B true CN103969787B (en) | 2016-08-17 |
Family
ID=51239495
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201410219039.2A Active CN103969787B (en) | 2014-05-22 | 2014-05-22 | A kind of first assembling and positioning method of off-axis four anti-camera lenses |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN103969787B (en) |
Families Citing this family (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105629431B (en) * | 2014-11-05 | 2018-07-27 | 北京航天计量测试技术研究所 | A kind of optical axis of Cassegrain's paraboloid primary mirror determines method |
CN104360492B (en) * | 2014-11-24 | 2017-01-18 | 中国航空工业集团公司洛阳电光设备研究所 | Adjusting method of off-axis four-reflector optical system |
CN104581150B (en) * | 2015-01-27 | 2017-01-11 | 北京空间机电研究所 | Positioning and error compensation method |
CN104655409B (en) * | 2015-02-13 | 2017-07-14 | 中国科学院长春光学精密机械与物理研究所 | Space optical remote sensor focus adjusting mechanism simulates in-orbit gravity release detection method |
CN104964648B (en) * | 2015-06-30 | 2017-07-28 | 中国科学院西安光学精密机械研究所 | Off-axis parabolic mirror key parameter calibration system and method |
CN105116515A (en) * | 2015-07-30 | 2015-12-02 | 北京理工大学 | Off-axis tri-reflector zooming optical system adjusting method |
CN105068259B (en) * | 2015-08-13 | 2017-08-25 | 中科院南京天文仪器有限公司 | Accurate method of adjustment for optics normal angle in two-dimensional scan device |
CN107132636B (en) * | 2017-06-29 | 2019-10-11 | 佛山科学技术学院 | A method and system for calibrating the installation and adjustment reference of the reflective surface of an aspheric primary mirror |
CN108828765B (en) * | 2018-06-04 | 2020-01-10 | 华中科技大学 | Kude optical path adjusting method based on double theodolites |
CN108956099A (en) * | 2018-07-21 | 2018-12-07 | 胡林亭 | The method of two transits measurement multiband system optical axis consistency |
CN109163663B (en) * | 2018-09-11 | 2020-09-11 | 苏州如期光电科技有限公司 | Manufacturing method of long-focus large-off-axis-amount off-axis paraboloid |
CN110554512B (en) * | 2019-08-16 | 2021-09-07 | 北京空间机电研究所 | High-precision secondary off-axis ellipsoid mirror optical axis extraction method and optical system |
CN111552054B (en) * | 2020-06-09 | 2021-12-28 | 河南平原光电有限公司 | Off-axis three-mirror optical system assembling and adjusting method |
CN112596259B (en) * | 2020-12-18 | 2022-08-12 | 北京空间机电研究所 | A high-precision off-axis aspheric mirror optical axis extraction method and system |
CN113031296B (en) * | 2021-03-24 | 2022-08-19 | 长春长光智欧科技有限公司 | Method for assembling and adjusting metal-based free-form surface three-reflection optical system capable of being assembled and adjusted quickly |
CN117168310B (en) * | 2023-11-02 | 2024-02-09 | 南京英田光学工程股份有限公司 | Eccentric measuring method for aspheric reflecting mirror |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE10359576A1 (en) * | 2003-12-18 | 2005-07-28 | Carl Zeiss Smt Ag | Method for producing an optical unit |
CN102073122B (en) * | 2010-12-24 | 2013-07-03 | 中国科学院长春光学精密机械与物理研究所 | Concentric assembly method for concentric optical element in off-axis concentric optical system |
CN102937738B (en) * | 2012-11-20 | 2014-10-15 | 中国科学院西安光学精密机械研究所 | System and method for accurately positioning optical axis of off-axis aspheric reflector |
-
2014
- 2014-05-22 CN CN201410219039.2A patent/CN103969787B/en active Active
Also Published As
Publication number | Publication date |
---|---|
CN103969787A (en) | 2014-08-06 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN103969787B (en) | A kind of first assembling and positioning method of off-axis four anti-camera lenses | |
CN103926058B (en) | The method using autocollimatic plane mirror measurement optical axis in Aspherical-surface testing | |
CN101858735B (en) | Large-caliber off-axis aspheric surface measuring and calibrating system | |
CN105157578B (en) | System and method for measuring off-axis quantity and off-axis angle of off-axis paraboloid main reflector | |
CN112596259B (en) | A high-precision off-axis aspheric mirror optical axis extraction method and system | |
CN103499330B (en) | A method for optically extracting vertex normals of large-aperture concave aspheric mirrors | |
CN102879182B (en) | Method for measuring off-axis aspheric surface eccentricity by laser tracker | |
CN110554512A (en) | High-precision secondary off-axis ellipsoidal reflector optical axis leading-out method and optical system thereof | |
CN103630073B (en) | The detection of wedge-shaped lens and bearing calibration | |
CN104075668A (en) | High-accuracy geographic sense measuring method in convex hyperboloid Hindle detection | |
CN105571514B (en) | The device and method of optical element is quickly adjusted in rotation translation absolute sense method | |
CN114185144B (en) | A Method for Mounting and Adjusting a Large-Aperture Optical System Based on a Small-Aperture Plane Mirror | |
CN107462402A (en) | A kind of detection scaling method of off-axis parabolic mirror geometric parameter | |
CN110082073B (en) | Device and method for adjusting inclination of plane mirror in transmission wavefront of subaperture splicing detection optical system | |
CN106871819B (en) | Aspherical vertex curvature radius error measurement method based on the optimal compensation position | |
CN106225712A (en) | A kind of off-axis three anti-aspheric optical systems benchmaring and processing method altogether | |
CN101339008A (en) | A device for detecting the K value coefficient of a large-diameter parabolic mirror | |
CN112097745A (en) | A method for improving the quality of line structured light in a vision measurement system | |
CN106705888B (en) | Calibration method of nonlinear relationship between CCD coordinate system and mirror coordinate system in interference detection | |
CN104048596B (en) | Compensator and the compensator control method coaxial with interferometer | |
CN204854637U (en) | System for measuring off-axis quantity and off-axis angle of off-axis paraboloid main reflector | |
CN106767471B (en) | Optical interval measuring system and method in aspheric surface detection light path | |
CN102589472A (en) | Method for highly precisely eliminating adjustment error in spherical surface shape interference detection | |
CN110567392B (en) | A method for measuring the surface shape of a convex free-form surface reflector | |
CN109099871B (en) | Interference detection alignment method based on circular target |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
C14 | Grant of patent or utility model | ||
GR01 | Patent grant |