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CN112684609B - A compact broadband polarization simultaneous imaging device and system with sub-aperture - Google Patents

A compact broadband polarization simultaneous imaging device and system with sub-aperture Download PDF

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CN112684609B
CN112684609B CN202110295384.4A CN202110295384A CN112684609B CN 112684609 B CN112684609 B CN 112684609B CN 202110295384 A CN202110295384 A CN 202110295384A CN 112684609 B CN112684609 B CN 112684609B
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CN112684609A (en
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任志广
李旭阳
王炜
袁灏
马子轩
褚楠清
姚睿
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XiAn Institute of Optics and Precision Mechanics of CAS
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Abstract

本发明涉及一种分孔径的紧凑型宽波段偏振同时成像装置及系统。本发明的目的是解决现有偏振成像系统存在低对比度或目标伪装等复杂背景下,难以实现对目标尤其是高速运动目标实时检测识别的技术问题。该装置的第一反射镜、第一透镜组、第二透镜组、第三反射镜和第四反射镜沿光轴依次设置;第二反射镜位于第一反射镜和第三反射镜之间,第二反射镜和第三反射镜的中央均开设有通光孔a;第一透镜组和第二透镜组设置于第二反射镜上的通光孔a处;第一反射镜与第二反射镜的反射面相对,第三反射镜与第四反射镜的反射面相对;望远物镜单元与缩焦准直物镜单元形成无焦系统;四个所述成像物镜单元的入瞳面均位于所述无焦系统的出瞳面上。

Figure 202110295384

The invention relates to a compact broadband polarization simultaneous imaging device and system with divided apertures. The purpose of the present invention is to solve the technical problem that it is difficult to realize real-time detection and recognition of targets, especially high-speed moving targets, under the complex background of low contrast or target camouflage in the existing polarization imaging system. The first reflecting mirror, the first lens group, the second lens group, the third reflecting mirror and the fourth reflecting mirror of the device are arranged in sequence along the optical axis; the second reflecting mirror is located between the first reflecting mirror and the third reflecting mirror, The center of the second reflecting mirror and the third reflecting mirror is provided with a light-passing hole a; the first lens group and the second lens group are arranged at the light-passing hole a on the second reflecting mirror; the first reflecting mirror and the second reflecting mirror The reflecting surfaces of the mirrors are opposite to each other, and the third reflecting mirror is opposite to the reflecting surface of the fourth reflecting mirror; the telescopic objective lens unit and the zooming and collimating objective lens unit form an afocal system; the entrance pupil surfaces of the four imaging objective lens units are all located in the on the exit pupil of the afocal system.

Figure 202110295384

Description

一种分孔径的紧凑型宽波段偏振同时成像装置及系统A compact broadband polarization simultaneous imaging device and system with sub-aperture

技术领域technical field

本发明涉及一种偏振同时成像装置及系统,具体涉及一种分孔径的紧凑型宽波段偏振同时成像装置及系统。The invention relates to a simultaneous polarization imaging device and system, in particular to a compact broadband polarization simultaneous imaging device and system with divided apertures.

背景技术Background technique

现有的目标检测成像方法主要有光度成像、光谱成像和偏振成像。The existing target detection imaging methods mainly include photometric imaging, spectral imaging and polarization imaging.

光度成像在面对目标光强与背景光强相似情况时,难以实现对目标的识别。随着新型特种(伪装和隐藏性)材料的研制以及在目标上的应用,目标的伪装和隐藏性能得到大幅度提升,光度成像逐渐难以胜任。而光谱成像容易被干扰,稳定性较差,光谱范围短,难以适应多样性目标等复杂应用环境。因此,在低对比度等复杂背景下,现有的光度成像和光谱成像方法难以实现对物体的精确检测识别,更难以精准识别复杂背景下伪装目标和潜在威胁。Photometric imaging is difficult to recognize the target when the target light intensity is similar to the background light intensity. With the development of new special (camouflage and concealment) materials and their application on targets, the camouflage and concealment performance of targets has been greatly improved, and photometric imaging has gradually become incompetent. However, spectral imaging is easily disturbed, has poor stability, and has a short spectral range, making it difficult to adapt to complex application environments such as diverse targets. Therefore, in complex backgrounds such as low contrast, the existing photometric imaging and spectral imaging methods are difficult to achieve accurate detection and recognition of objects, and it is even more difficult to accurately identify camouflaged targets and potential threats in complex backgrounds.

偏振成像是通过对目标反射自然光所产生的偏振光进行信息采集来实现偏振成像,对所采集信息进行技术处理,可以提高待检测目标图像的对比度信息,同时可以获取目标图像的外观特性、表面材料特性和表面粗糙度等多维信息。Polarization imaging realizes polarization imaging by collecting information on the polarized light generated by the reflected natural light of the target. The technical processing of the collected information can improve the contrast information of the target image to be detected, and at the same time, the appearance characteristics and surface materials of the target image can be obtained. Multidimensional information such as properties and surface roughness.

现有的偏振成像系统主要有时序型偏振成像系统、干涉型偏振成像系统和空域型偏振成像系统三种。其中,时序型偏振成像系统无法实时采集目标的偏振信息,且存在信息误差大的缺陷,故难以实现对运动目标尤其是高速运动目标偏振信息的实时采集。干涉型偏振成像系统不仅存在工作波长单一、多波段易串扰的问题,同时对于干涉条纹的解算也需要一定的时间,对计算机性能的要求较高,成像现场的环境一般难以满足干涉型偏振成像系统较为苛刻的使用要求。对于空域型偏振成像系统,由于采用分振幅的结构形式,在高分辨率和紧凑性需求方面存在互斥,导致系统存在体积庞大、分辨率低和装配难度大等问题。多种系统同时采集的结构形式则存在尺寸大、重量大、稳定性差以及成本高等缺点。Existing polarization imaging systems mainly include sequential polarization imaging systems, interference polarization imaging systems and spatial polarization imaging systems. Among them, the time series polarization imaging system cannot collect the polarization information of the target in real time, and has the defect of large information error, so it is difficult to realize the real-time collection of the polarization information of the moving target, especially the high-speed moving target. The interferometric polarization imaging system not only has the problem of single working wavelength and multi-band crosstalk, but also requires a certain amount of time to solve the interference fringes, which requires high computer performance. The environment of the imaging site is generally difficult to meet the interference polarization imaging The system is more demanding. For the spatial polarization imaging system, due to the use of the sub-amplitude structure, there are mutual exclusions in terms of high resolution and compactness, resulting in problems such as bulky volume, low resolution and difficult assembly. The structural form of simultaneous acquisition by multiple systems has the disadvantages of large size, heavy weight, poor stability and high cost.

公开号为CN111750997A的中国发明专利中公开了一种基于偏振分时光谱同步的光学成像探测装置,该装置的光学系统分为成像单元和分时变换偏振光谱单元,可通过分时变换偏振光谱单元特性,获取目标不同的偏振信息。这种光学系统存在空间分辨率低和系统轴向长度过长的缺点,当针对运动目标成像时,不能在同一时刻对目标的不同偏振性实时采集,无法满足复杂环境下高速运动目标的高分辨成像,并且存在较大的原理性误差和数据可靠性低等难以克服的缺点。The Chinese invention patent with publication number CN111750997A discloses an optical imaging detection device based on polarization time division spectral synchronization. The optical system of the device is divided into an imaging unit and a time division conversion polarization spectrum unit. feature to obtain different polarization information of the target. This optical system has the disadvantages of low spatial resolution and too long axial length of the system. When imaging a moving target, it cannot collect different polarization properties of the target at the same time in real time, and cannot meet the high resolution of high-speed moving targets in complex environments. imaging, and there are insurmountable shortcomings such as large principle errors and low data reliability.

综上,在低对比度或目标伪装等复杂背景下,现有偏振成像系统难以实现对目标尤其是高速运动目标的实时检测识别。To sum up, under complex backgrounds such as low contrast or target camouflage, it is difficult for existing polarization imaging systems to achieve real-time detection and recognition of targets, especially high-speed moving targets.

发明内容SUMMARY OF THE INVENTION

本发明的目的是解决现有偏振成像系统在低对比度或目标伪装等复杂背景下,难以实现对目标尤其是高速运动目标实时检测识别的技术问题,而提供一种分孔径的紧凑型宽波段偏振同时成像装置及系统。The purpose of the present invention is to solve the technical problem that the existing polarization imaging system is difficult to realize real-time detection and recognition of targets, especially high-speed moving targets under complex backgrounds such as low contrast or target camouflage, and to provide a compact broadband polarization with different apertures Simultaneous imaging device and system.

为解决上述技术问题,本发明提供的技术解决方案如下:For solving the above-mentioned technical problems, the technical solutions provided by the present invention are as follows:

本发明提供一种分孔径的紧凑型宽波段偏振同时成像装置,其特征在于:The present invention provides a compact broadband simultaneous imaging device with split aperture, which is characterized by:

包括用于收集目标信息的望远物镜单元、同于压缩和准直光路的缩焦准直物镜单元,以及四个用于偏正成像的成像物镜单元;Including a telescopic objective lens unit for collecting target information, a reduced focus collimating objective lens unit with the same compression and collimation optical paths, and four imaging objective lens units for polarized imaging;

所述望远物镜单元包括第一反射镜、第二反射镜和第一透镜组;The telescopic objective lens unit includes a first reflection mirror, a second reflection mirror and a first lens group;

所述缩焦准直物镜单元包括第三反射镜、第四反射镜和第二透镜组;The zooming and collimating objective lens unit includes a third reflecting mirror, a fourth reflecting mirror and a second lens group;

所述第一反射镜、第一透镜组、第二透镜组、第三反射镜和第四反射镜沿光轴依次设置;the first reflecting mirror, the first lens group, the second lens group, the third reflecting mirror and the fourth reflecting mirror are arranged in sequence along the optical axis;

所述第二反射镜沿光轴设置,位于第一反射镜和第三反射镜之间,第二反射镜和第三反射镜的中央均开设有通光孔a;第一透镜组和第二透镜组设置于第二反射镜上的通光孔a处,用于残余像差校正;The second reflecting mirror is arranged along the optical axis and is located between the first reflecting mirror and the third reflecting mirror, and the center of the second reflecting mirror and the third reflecting mirror is provided with a light-passing hole a; the first lens group and the second reflecting mirror The lens group is arranged at the light-passing hole a on the second reflector for residual aberration correction;

所述第一反射镜与第二反射镜的反射面相对,形成第一折返式结构,第三反射镜与第四反射镜的反射面相对,形成第二折返式结构,用于压缩轴向长度;The first reflecting mirror is opposite to the reflecting surface of the second reflecting mirror to form a first folding structure, and the third reflecting mirror is opposite to the reflecting surface of the fourth reflecting mirror to form a second folding structure for compressing the axial length ;

所述望远物镜单元与缩焦准直物镜单元形成无焦系统;四个所述成像物镜单元的入瞳面均位于所述无焦系统的出瞳面上,且以光轴为中心沿同一圆周均布,实现无焦系统与四个成像物镜单元的拼接。The telescopic objective lens unit and the zooming and collimating objective lens unit form an afocal system; the entrance pupil surfaces of the four imaging objective lens units are all located on the exit pupil surface of the afocal system, and are centered along the same optical axis. Evenly distributed around the circumference to realize the splicing of the afocal system and the four imaging objective lens units.

进一步地,所述成像物镜单元包括同轴依次设置的第五反射镜、第六反射镜、第三透镜组和偏振片;Further, the imaging objective lens unit includes a fifth reflector, a sixth reflector, a third lens group and a polarizer that are coaxially arranged in sequence;

所述第六反射镜的中央开设有通光孔c;The center of the sixth reflector is provided with a light-passing hole c;

所述第五反射镜与所述第六反射镜的反射面相对,形成第三折返式结构;The fifth reflecting mirror is opposite to the reflecting surface of the sixth reflecting mirror to form a third folding structure;

第三透镜组用于残余像差校正。The third lens group is used for residual aberration correction.

进一步地,所述无焦系统轴向长度的压缩比为

Figure DEST_PATH_IMAGE001
: Further, the compression ratio of the axial length of the afocal system is
Figure DEST_PATH_IMAGE001
:

Figure DEST_PATH_IMAGE002
Figure DEST_PATH_IMAGE002
;

其中,in,

Figure DEST_PATH_IMAGE003
为望远物镜单元的有效焦距;
Figure DEST_PATH_IMAGE003
is the effective focal length of the telescopic objective lens unit;

Figure DEST_PATH_IMAGE004
为缩焦准直物镜单元的有效焦距;
Figure DEST_PATH_IMAGE004
is the effective focal length of the zooming and collimating objective lens unit;

TTLA为第一反射镜的前表面至第四反射镜的后表面的轴向距离。 TTLA is the axial distance from the front surface of the first mirror to the rear surface of the fourth mirror.

进一步地,所述无焦系统的角放大倍率为

Figure DEST_PATH_IMAGE005
Figure DEST_PATH_IMAGE006
。 Further, the angular magnification of the afocal system is
Figure DEST_PATH_IMAGE005
,
Figure DEST_PATH_IMAGE006
.

进一步地,四个成像物镜单元与光轴的偏离距离均为d,偏离距离d与望远物镜单元、缩焦准直物镜单元和成像物镜单元的总焦距ƒ,满足以下关系式:Further, the deviation distances of the four imaging objective lens units from the optical axis are all d, and the deviation distance d and the total focal length ƒ of the telescopic objective lens unit, the zooming and collimating objective lens unit and the imaging objective lens unit satisfy the following relationship:

Figure DEST_PATH_IMAGE007
Figure DEST_PATH_IMAGE007
;

望远物镜单元、缩焦准直物镜单元和成像物镜单元的总焦距ƒ,与第一反射镜后表面至成像物镜单元偏振片后像面b的总体长度TTL,以及第三透镜组出射面至所述像面b的轴向距离BFL,三者满足以下关系式:The total focal length ƒ of the telescopic objective lens unit, the zooming and collimating objective lens unit, and the imaging objective lens unit, and the overall length TTL from the rear surface of the first reflecting mirror to the rear image surface b of the polarizing plate of the imaging objective lens unit, and the exit surface of the third lens group to The axial distance BFL of the image plane b satisfies the following relationship:

Figure DEST_PATH_IMAGE008
Figure DEST_PATH_IMAGE008
.

进一步地,所述第三反射镜的直径

Figure DEST_PATH_IMAGE009
与第六反射镜的直径
Figure DEST_PATH_IMAGE010
满足以下关系式:
Figure DEST_PATH_IMAGE011
。 Further, the diameter of the third mirror
Figure DEST_PATH_IMAGE009
with the diameter of the sixth mirror
Figure DEST_PATH_IMAGE010
Satisfy the following relation:
Figure DEST_PATH_IMAGE011
.

进一步地,所述第一透镜组和第二透镜组的总焦距

Figure DEST_PATH_IMAGE012
满足下式: Further, the total focal length of the first lens group and the second lens group
Figure DEST_PATH_IMAGE012
Satisfy the following formula:

Figure DEST_PATH_IMAGE013
Figure DEST_PATH_IMAGE013
.

进一步地,四个成像物镜单元的四个偏振片沿圆周方向依次为0°、60°和120°的偏振片,以及圆偏振偏振片。Further, the four polarizers of the four imaging objective lens units are sequentially 0°, 60° and 120° polarizers along the circumferential direction, and circular polarizers.

进一步地,所述第一反射、第三反射镜、第四反射镜、第五反射镜和第六反射镜均为双曲面镜;所述第二反射镜为抛物面镜。Further, the first reflection mirror, the third reflection mirror, the fourth reflection mirror, the fifth reflection mirror and the sixth reflection mirror are all hyperbolic mirrors; the second reflection mirror is a parabolic mirror.

本发明还提供一种分孔径的紧凑型宽波段偏振同时成像系统,其特征在于:基于上述的分孔径的紧凑型宽波段偏振同时成像装置,还包括计算机和与之连接的四个探测器,四个探测器位于四个所述像面b处,用于得到四组仅含单一偏振态信息的偏振图像,计算机用于对四组偏振图像进行处理和计算,得到目标的斯托克斯矩阵信息。The present invention also provides a compact broadband polarization simultaneous imaging system with sub-aperture, which is characterized in that: based on the above-mentioned compact broadband polarization simultaneous imaging device with sub-aperture, it also includes a computer and four detectors connected to it, The four detectors are located at the four image planes b, and are used to obtain four sets of polarization images containing only a single polarization state information. The computer is used to process and calculate the four sets of polarization images to obtain the Stokes matrix of the target. information.

本发明相比现有技术具有的有益效果如下:Compared with the prior art, the present invention has the following beneficial effects:

1、本发明提供的一种分孔径的紧凑型宽波段偏振同时成像装置及系统,通过采用折返式结构形式组成无焦系统的光学方案,压缩了系统的轴向长度,提升了系统的紧凑性,实现了对前置无焦系统轴向长度大于10倍的压缩比,极大地降低了系统的体积、长度和重量。1. The present invention provides a compact wide-band polarization simultaneous imaging device and system with different apertures. By adopting the optical scheme of forming an afocal system in the form of a fold-back structure, the axial length of the system is compressed and the compactness of the system is improved. , to achieve a compression ratio greater than 10 times the axial length of the front afocal system, which greatly reduces the volume, length and weight of the system.

2、本发明提供的一种分孔径的紧凑型宽波段偏振同时成像装置及系统,系统采用宽谱段进行成像,可应对复杂环境中不同目标的特征响应谱段,因此可适应于复杂环境中并提供较高的可靠性以及灵敏性。2. The present invention provides a compact wide-band polarization simultaneous imaging device and system with different apertures. The system adopts wide-spectrum imaging and can cope with the characteristic response spectrum of different targets in complex environments, so it can be adapted to complex environments. And provide high reliability and sensitivity.

3、本发明提供的一种分孔径的紧凑型宽波段偏振同时成像装置及系统,无焦系统与四个折返式成像物镜单元拼接组成偏振成像装置,四个成像物镜单元实现分孔径成像,该结构具备实时性好、装置结构紧凑,装置内能量密度高等优点,相比于传统的分时型偏振成像系统,该系统可对运动目标进行实时性信息采集,实现对目标的实时响应。3. The present invention provides a compact wide-band polarization simultaneous imaging device and system with different apertures. The afocal system and four fold-back imaging objective lens units are spliced together to form a polarized imaging device, and the four imaging objective lens units realize split-aperture imaging. The structure has the advantages of good real-time performance, compact device structure, and high energy density in the device. Compared with the traditional time-sharing polarization imaging system, the system can collect real-time information on moving targets and realize real-time response to the target.

4、本发明提供的一种分孔径的紧凑型宽波段偏振同时成像装置及系统,可通过对采集信息处理得到传统手段无法测得的目标表面材料特性和表面粗糙度等多维信息,通过三维重建技术,可以获得含有目标表面材料等信息的三维模型。4. The present invention provides a compact wide-band polarization simultaneous imaging device and system with different apertures, which can obtain multi-dimensional information such as target surface material characteristics and surface roughness that cannot be measured by traditional means by processing the collected information, and then reconstruct the data through three-dimensional reconstruction. technology, a 3D model containing information such as the target surface material can be obtained.

5、本发明提供的一种分孔径的紧凑型宽波段偏振同时成像装置及系统,由于采用了引入前置放大望远镜(望远物镜单元)结构形式的优势,在可以降低尺寸、设计、装配难度外,还有一个重要优点就是通过前置组提高总光通量,使后组光路中单位截面的光通量密度更大,利于弥补因偏振片带来的能量损失,增加图像信噪比、可以用更短的积分时间工作,避免因能量不足延长积分时间造成的像移导致成像质量劣化。5. A compact wide-band polarization simultaneous imaging device and system with different apertures provided by the present invention can reduce the difficulty of size, design and assembly due to the advantages of introducing a pre-amplifying telescope (telephoto objective lens unit) structure. In addition, another important advantage is that the total luminous flux is increased through the front group, so that the luminous flux density per unit section in the optical path of the rear group is larger, which is beneficial to make up for the energy loss caused by the polarizer, increase the image signal-to-noise ratio, and can be used for a shorter time. The integration time can be used to avoid image shift caused by insufficient energy and prolong the integration time, which will lead to the deterioration of image quality.

附图说明Description of drawings

图1为本发明分孔径的紧凑型宽波段偏振同时成像装置的结构示意图;Fig. 1 is the structure schematic diagram of the compact broadband polarization simultaneous imaging device of sub-aperture of the present invention;

图2为本发明分孔径的紧凑型宽波段偏振同时成像装置第一透镜组和第二透镜组的结构示意图;2 is a schematic structural diagram of the first lens group and the second lens group of the compact broadband polarization simultaneous imaging device of the present invention;

图3为本发明分孔径的紧凑型宽波段偏振同时成像装置单一偏振光通道上成像物镜单元的结构示意图;3 is a schematic structural diagram of an imaging objective lens unit on a single polarized light channel of a compact broadband polarization simultaneous imaging device with sub-aperture of the present invention;

图4至6为实施例中表1的25个透镜面的箭头指示图,其中第9面是虚拟表面(实际中不存在的面,所以图中未显示);4 to 6 are arrow indication diagrams of the 25 lens surfaces in Table 1 in the embodiment, wherein the ninth surface is a virtual surface (a surface that does not exist in reality, so it is not shown in the figure);

图7为仿真所得本发明0°偏振光通道在波长为450nm~850nm光谱范围内工作时的MTF(调制传递函数)曲线,表示子午方向上的成像质量;Fig. 7 is the MTF (modulation transfer function) curve when the 0° polarized light channel of the present invention obtained by simulation works in the spectral range of 450nm to 850nm, indicating the imaging quality in the meridional direction;

图8为仿真所得本发明60°偏振光通道在波长450nm~850nm光谱范围内工作时的MTF(调制传递函数)曲线,表示弧矢方向上的成像质量。8 is the MTF (modulation transfer function) curve obtained by simulation when the 60° polarized light channel of the present invention operates in the spectral range of wavelength 450nm~850nm, indicating the imaging quality in the sagittal direction.

附图标记说明:Description of reference numbers:

101-第一反射镜、102-第二反射镜、103-第一透镜组;101-first reflector, 102-second reflector, 103-first lens group;

201-第三反射镜、202-第四反射镜、203-第二透镜组;201-third mirror, 202-fourth mirror, 203-second lens group;

301-第五反射镜、302-第六反射镜、303-第三透镜组、304-偏振片。301-fifth reflector, 302-sixth reflector, 303-third lens group, 304-polarizer.

具体实施方式Detailed ways

下面结合附图和实施例对本发明作进一步地说明。The present invention will be further described below with reference to the accompanying drawings and embodiments.

参见图1、图2,本发明提供一种分孔径的紧凑型宽波段偏振同时成像装置,可在低对比度或目标伪装等复杂背景下,实现对目标尤其是高速运动目标实时地检测识别。该装置由三部分组成,包括用于收集目标信息的望远物镜单元、同于压缩和准直光路的缩焦准直物镜单元,以及四个用于偏正成像(将含有目标不同偏振态信息的光线汇聚在像面b上)的成像物镜单元;前两个单元形成无焦系统;所述望远物镜单元包括第一反射镜101、第二反射镜102和第一透镜组103;所述缩焦准直物镜单元包括第三反射镜201、第四反射镜202和第二透镜组203;所述第一反射镜101、第一透镜组103、第二透镜组203、第三反射镜201和第四反射镜202沿光轴依次设置;所述第二反射镜102沿光轴设置,位于第一反射镜101和第三反射镜201之间,第二反射镜102和第三反射镜201的中央均开设有通光孔a;第一透镜组103和第二透镜组203组合作为校正透镜组合设置于第二反射镜102上的通光孔a处,用于残余像差校正;所述第一反射镜101与第二反射镜102的反射面相对,形成第一折返式结构,第三反射镜201与第四反射镜202的反射面相对,形成第二折返式结构,用于压缩轴向长度。Referring to FIG. 1 and FIG. 2 , the present invention provides a compact broadband polarization simultaneous imaging device with different apertures, which can realize real-time detection and recognition of targets, especially high-speed moving targets, under complex backgrounds such as low contrast or target camouflage. The device consists of three parts, including a telescopic objective lens unit for collecting target information, a reduced focus collimating objective lens unit with the same compression and collimation optical paths, and four for polarized imaging (which will contain information about different polarization states of the target). The first two units form an afocal system; the telescopic objective lens unit includes a first reflecting mirror 101, a second reflecting mirror 102 and a first lens group 103; the The focusing and collimating objective lens unit includes a third reflecting mirror 201 , a fourth reflecting mirror 202 and a second lens group 203 ; the first reflecting mirror 101 , the first lens group 103 , the second lens group 203 , and the third reflecting mirror 201 and the fourth reflecting mirror 202 are arranged in sequence along the optical axis; the second reflecting mirror 102 is arranged along the optical axis, between the first reflecting mirror 101 and the third reflecting mirror 201, the second reflecting mirror 102 and the third reflecting mirror 201 A light-passing hole a is opened in the center of the lens; the combination of the first lens group 103 and the second lens group 203 is set at the light-passing hole a on the second mirror 102 as a correction lens combination for residual aberration correction; the The reflecting surfaces of the first reflecting mirror 101 and the second reflecting mirror 102 are opposite to form a first fold-back structure, and the reflecting surfaces of the third reflecting mirror 201 and the fourth reflecting mirror 202 are opposite to form a second fold-back structure for compressing the shaft to length.

四个所述成像物镜单元的入瞳面均位于所述无焦系统的出瞳面上分割出瞳,且以光轴为中心沿同一圆周均布,即在无焦系统的出瞳处,以光轴为原点建立xy坐标系,将四个成像物镜单元整体绕光轴分别向±x、±y方向偏离d,实现无焦系统与四个成像物镜单元的拼接,无焦系统与四个折返式成像物镜单元拼接组成偏振成像装置,该结构具备实时性好、装置结构紧凑,装置内能量密度高等优点。The entrance pupil planes of the four imaging objective lens units are all located on the exit pupil plane of the afocal system to divide the exit pupils, and are evenly distributed along the same circumference with the optical axis as the center, that is, at the exit pupil of the afocal system, with The optical axis is the origin to establish an xy coordinate system, and the entire four imaging objective lens units are deviated by d in the ±x and ±y directions respectively around the optical axis, so as to realize the splicing of the afocal system and the four imaging objective lens units, and the afocal system and the four return The polarized imaging device is formed by splicing the single-type imaging objective lens units, and the structure has the advantages of good real-time performance, compact device structure, and high energy density in the device.

所述成像物镜单元包括同轴依次设置的第五反射镜301、第六反射302、第三透镜组303和偏振片304;所述第六反射镜302的中央开设有通光孔c;所述第五反射镜301与所述第六反射镜302的反射面相对,形成第三折返式结构,三组折返式结构可以显著压缩装置的轴向长度;第三透镜组303用于残余像差校正。当然,成像物镜单元可替换为透射式结构,但这样会造成系统总长度加长,重量增大。The imaging objective lens unit includes a fifth reflector 301, a sixth reflector 302, a third lens group 303 and a polarizer 304 that are coaxially arranged in sequence; the sixth reflector 302 is provided with a light through hole c in the center; The fifth reflecting mirror 301 is opposite to the reflecting surface of the sixth reflecting mirror 302, forming a third fold-back structure, and the three-group fold-back structure can significantly compress the axial length of the device; the third lens group 303 is used for residual aberration correction . Of course, the imaging objective lens unit can be replaced with a transmissive structure, but this will increase the overall length and weight of the system.

所述第一反射镜101、第三反射镜201、第四反射镜202、第五反射镜301和第六反射镜302均为双曲面镜;所述第二反射镜102为抛物面镜(双曲面镜中的一种)。The first reflecting mirror 101, the third reflecting mirror 201, the fourth reflecting mirror 202, the fifth reflecting mirror 301 and the sixth reflecting mirror 302 are all hyperbolic mirrors; the second reflecting mirror 102 is a parabolic mirror (hyperbolic mirror). one of the mirrors).

所述无焦系统轴向长度的压缩比为

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: The compression ratio of the axial length of the afocal system is
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:

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;

其中,in,

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为望远物镜单元的有效焦距;
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is the effective focal length of the telescopic objective lens unit;

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为缩焦准直物镜单元的有效焦距;
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is the effective focal length of the zooming and collimating objective lens unit;

TTLA为第一反射镜101的前表面至第四反射镜202的后表面的轴向距离,即无焦系统的总长。 TTLA is the axial distance from the front surface of the first reflector 101 to the back surface of the fourth reflector 202 , that is, the total length of the afocal system.

所述无焦系统的角放大倍率为

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,通过无焦系统的放大倍率压缩无 焦系统出瞳直径,提升无焦系统出瞳处以及出瞳后端成像物镜单元内的能量密度。 The angular magnification of the afocal system is
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,
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, through the magnification of the afocal system, the diameter of the exit pupil of the afocal system is compressed, and the energy density at the exit pupil of the afocal system and in the imaging objective lens unit behind the exit pupil is increased.

四个成像物镜单元与光轴的偏离距离均为d,偏离距离d与望远物镜单元、缩焦准直物镜单元和成像物镜单元的总焦距ƒ,满足以下关系式:The deviation distances of the four imaging objective lens units from the optical axis are all d, and the deviation distance d is related to the total focal length ƒ of the telescopic objective lens unit, the zooming and collimating objective lens unit and the imaging objective lens unit, which satisfies the following relationship:

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Figure DEST_PATH_IMAGE015
;

望远物镜单元、缩焦准直物镜单元和成像物镜单元的总焦距(即装置的总焦距)ƒ,与第一反射镜101后表面至成像物镜单元偏振片304后像面b的总体长度(即装置的总体长度)TTL,以及第三透镜组303出射面至所述像面b的轴向距离BFL,三者满足以下关系式:The total focal length of the telescopic objective lens unit, the zooming and collimating objective lens unit and the imaging objective lens unit (that is, the total focal length of the device) ƒ, and the total length from the rear surface of the first reflecting mirror 101 to the rear image surface b of the polarizing plate 304 of the imaging objective lens unit ( That is, the overall length of the device) TTL , and the axial distance BFL from the exit surface of the third lens group 303 to the image plane b, the three satisfy the following relationship:

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.

所述第三反射镜201的直径(即缩焦准直物镜单元的通光口径)

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与第六反射镜 302的直径(成像物镜单元的入瞳直径)
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满足以下关系式: The diameter of the third reflecting mirror 201 (that is, the clear aperture of the reduced-focus collimating objective lens unit)
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and the diameter of the sixth mirror 302 (the entrance pupil diameter of the imaging objective lens unit)
Figure 130364DEST_PATH_IMAGE010
Satisfy the following relation:

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Figure 773835DEST_PATH_IMAGE011
.

所述第一透镜组103和第二透镜组203的总焦距

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满足下式: The total focal length of the first lens group 103 and the second lens group 203
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Satisfy the following formula:

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.

图3中为单一偏振光通道的成像物镜单元的示意图,总系统共有四组通道;四组通道中各自状态的偏振片304,沿圆周依次为0°、60°、120°以及圆偏振偏振片。其中,0°偏振光通道位于+x方向;60°偏振光通道位于+y方向;120°偏振光通道位于-x方向。Figure 3 is a schematic diagram of an imaging objective lens unit with a single polarized light channel. The total system has four groups of channels; the polarizers 304 in their respective states in the four groups of channels are 0°, 60°, 120° and circularly polarized polarizers in sequence along the circumference. . Among them, the 0° polarized light channel is located in the +x direction; the 60° polarized light channel is located in the +y direction; the 120° polarized light channel is located in the -x direction.

本发明还提供一种分孔径的紧凑型宽波段偏振同时成像系统,基于上述的分孔径的紧凑型宽波段偏振同时成像装置,还包括计算机和与之连接的四个探测器,四个探测器位于四个所述像面b处,用于得到四组仅含单一偏振态信息的偏振图像,计算机用于对四组偏振图像进行处理和计算,得到目标的斯托克斯矩阵信息,通过其他技术处理得到目标其他维度的信息。The present invention also provides a compact broadband polarization simultaneous imaging system with divided apertures, based on the above-mentioned compact broadband polarization simultaneous imaging device with divided apertures, further comprising a computer and four detectors connected thereto, the four detectors Located at the four image planes b, it is used to obtain four sets of polarization images containing only a single polarization state information. The computer is used to process and calculate the four sets of polarization images to obtain the Stokes matrix information of the target. Technical processing obtains information on other dimensions of the target.

上述装置及系统中,三个单元均采用折返式结构,尤其是前两个单元采用折返式结构,极大地压缩了系统的轴向长度,压缩比大于10倍。In the above-mentioned device and system, all three units adopt a folded structure, especially the first two units adopt a folded structure, which greatly compresses the axial length of the system, and the compression ratio is greater than 10 times.

整个系统的工作过程如下:The working process of the whole system is as follows:

目标反射或者发出的光经第二反射镜102收集到系统内,经过第一反射镜101到达第一透镜组103中的一次像面b;再经第四反射镜202反射,通过第三反射镜201准直后射出;在出瞳处进入成像物镜单元,通过偏振片304后,在像面b处得到仅含有单一偏振态信息的偏振图像,通过对四组偏振图像的处理,计算得到目标的斯托克斯矩阵信息,通过其他技术处理得到目标其他维度的信息(可通过对采集信息处理得到传统手段无法测得的目标表面材料特性和表面粗糙度等多维信息,通过三维重建技术,可以获得含有目标表面材料等信息的三维模型)。The light reflected or emitted by the target is collected into the system by the second mirror 102, and reaches the primary image plane b in the first lens group 103 through the first mirror 101; 201 is collimated and emitted; it enters the imaging objective lens unit at the exit pupil, and after passing through the polarizer 304, a polarized image containing only a single polarization state information is obtained at the image plane b. Stokes matrix information can be processed by other technologies to obtain information of other dimensions of the target (multi-dimensional information such as the material properties and surface roughness of the target surface that cannot be measured by traditional methods can be obtained by processing the collected information, and through 3D reconstruction technology, it can be obtained. 3D model with information such as target surface material).

实施例Example

技术指标如下:The technical indicators are as follows:

光学系统总长TTL:830mm;Optical system total length TTL : 830mm;

系统总焦距ƒ:2000mm;System total focal length ƒ: 2000mm;

无焦系统角放大倍率

Figure 900240DEST_PATH_IMAGE005
:6; Afocal system angular magnification
Figure 900240DEST_PATH_IMAGE005
:6;

光学系统光圈FNO:10;Optical system aperture FNO: 10;

光学系统视场角:0.42°;Field of view of optical system: 0.42°;

光学系统使用波段范围:450nm~850nm。Optical system using wavelength range: 450nm ~ 850nm.

分孔径的紧凑型宽波段偏振同时成像装置中各个镜片的结构参数:Structural parameters of each lens in a compact broadband polarization simultaneous imaging device with different apertures:

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Figure DEST_PATH_IMAGE017

表中,Mirror为反射镜,SILICA_SPECIAL为熔融石英。图4至图6为上表1的25个透镜面的箭头指示图,其中,第9面是虚拟表面(实际中不存在的面,所以图中未显示);In the table, Mirror is a mirror, and SILICA_SPECIAL is fused silica. Figures 4 to 6 are arrow indication diagrams of the 25 lens surfaces in Table 1 above, wherein the ninth surface is a virtual surface (a surface that does not exist in reality, so it is not shown in the figure);

图7为仿真所得0°偏振光通道在波长为450nm~850nm光谱范围内工作时的MTF(调制传递函数)曲线,表示子午方向上的成像质量,从图中可以看出在奈奎斯特频率为50 lp/mm处,0、0.5、0.707、0.866以及1视场的MTF值均在0.4以上且接近衍射极限(图中的虚线),达到了良好的成像质量。Figure 7 shows the MTF (modulation transfer function) curve of the simulated 0° polarized light channel operating in the spectral range of 450nm to 850nm, indicating the imaging quality in the meridian direction. It can be seen from the figure that the Nyquist frequency At 50 lp/mm, the MTF values of 0, 0.5, 0.707, 0.866 and 1 field of view are all above 0.4 and close to the diffraction limit (dashed line in the figure), achieving good imaging quality.

图8为仿真所得60°偏振光通道在波长450nm~850nm光谱范围内工作时的MTF(调制传递函数)曲线,表示弧矢方向上的成像质量,从图中可以看出在奈奎斯特频率50 lp/mm处,0、0.5、0.707、0.866以及1视场的MTF值均在0.4以上且接近衍射极限,达到了良好的成像质量。Figure 8 is the MTF (modulation transfer function) curve of the simulated 60° polarized light channel operating in the wavelength range of 450nm~850nm, which indicates the imaging quality in the sagittal direction. It can be seen from the figure that the Nyquist frequency At 50 lp/mm, the MTF values of 0, 0.5, 0.707, 0.866 and 1 field of view are all above 0.4 and close to the diffraction limit, achieving good imaging quality.

当然,各镜片的材料不局限于上表,使用中可根据具体需要,调整各镜片的材料。Of course, the material of each lens is not limited to the above table, and the material of each lens can be adjusted according to specific needs during use.

此外,当工作波段较宽时或者追求高透过率时,可将第一透镜组103和第二透镜组203成的校正透镜组合去掉。这样无焦系统的像质会劣化,但可通过在后面的成像物镜单元中增加校正透镜组对像差进行适度修正,或者在第一反射镜101、第二反射镜102、第三反射镜201和第四反射镜202中引入非球面或者自由曲面进行像差补偿修正,通过减少透镜数量的方式进而减少了折射面,这样系统的能量损失会有所改善。In addition, when the working wavelength band is wider or high transmittance is pursued, the correction lens combination of the first lens group 103 and the second lens group 203 can be removed. In this way, the image quality of the afocal system will be degraded, but the aberration can be appropriately corrected by adding a correction lens group in the imaging objective lens unit at the rear, or by adding the first reflecting mirror 101, the second reflecting mirror 102, and the third reflecting mirror 201 The aspheric surface or free-form surface is introduced into the fourth reflecting mirror 202 to perform aberration compensation correction, and the refractive surface is reduced by reducing the number of lenses, so that the energy loss of the system will be improved.

最后应说明的是:以上实施例仅用以说明本发明的技术方案,而非对其限制,对于本领域的普通专业技术人员来说,可以对前述各实施例所记载的具体技术方案进行修改,或者对其中部分技术特征进行等同替换,而这些修改或者替换,并不使相应技术方案的本质脱离本发明所保护技术方案的范围。Finally, it should be noted that the above embodiments are only used to illustrate the technical solutions of the present invention, but not to limit them. For those of ordinary skill in the art, the specific technical solutions recorded in the foregoing embodiments can be modified. , or equivalently replace some of the technical features, and these modifications or replacements do not make the essence of the corresponding technical solutions deviate from the scope of the technical solutions protected by the present invention.

Claims (10)

1. A kind of wide band polarization of compact that divides the aperture is formed the image device at the same time, characterized by:
the device comprises a telescope objective unit for collecting target information, a focusing collimator objective unit which is the same as a compression and collimation optical path, and four imaging objective units for polarization imaging;
the telescopic objective lens unit comprises a first reflector (101), a second reflector (102) and a first lens group (103);
the zooming collimating objective unit comprises a third reflector (201), a fourth reflector (202) and a second lens group (203);
the first reflector (101), the first lens group (103), the second lens group (203), the third reflector (201) and the fourth reflector (202) are sequentially arranged along an optical axis;
the second reflector (102) is arranged along the optical axis and is positioned between the first reflector (101) and the third reflector (201), and the centers of the second reflector (102) and the third reflector (201) are both provided with a light through hole a; the first lens group (103) and the second lens group (203) are arranged at a light-passing hole a on the second reflector (102) and used for residual aberration correction;
the first reflector (101) is opposite to the reflecting surface of the second reflector (102) to form a first folding structure, and the third reflector (201) is opposite to the reflecting surface of the fourth reflector (202) to form a second folding structure for compressing the axial length;
the telescope objective lens unit and the focus-reducing collimator objective lens unit form an afocal system; the entrance pupil surfaces of the four imaging objective lens units are all located on the exit pupil surface of the afocal system and are uniformly distributed along the same circumference by taking the optical axis as the center, so that the afocal system and the four imaging objective lens units are spliced.
2. The apertured compact wide-band simultaneous polarization imaging device according to claim 1, wherein:
the imaging objective unit comprises a fifth reflector (301), a sixth reflector (302), a third lens group (303) and a polaroid (304) which are coaxially and sequentially arranged;
the center of the sixth reflector (302) is provided with a light through hole c;
the reflecting surface of the fifth reflector (301) is opposite to the reflecting surface of the sixth reflector (302) to form a third folding structure;
the third lens group (303) is used for residual aberration correction.
3. The small aperture compact wide band simultaneous polarization imaging device of claim 1 or 2, wherein:
the compression ratio of the axial length of the coke-free system is
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Wherein,
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is the effective focal length of the telescopic objective lens unit;
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is the effective focal length of the convergent-collimation objective lens unit;
TTLAis the axial distance from the front surface of the first mirror (101) to the rear surface of the fourth mirror (202).
4. The apertured compact wide-band simultaneous polarization imaging device according to claim 3, wherein:
the angular magnification of the afocal system is
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5. The apertured compact wide-band simultaneous polarization imaging device according to claim 4, wherein:
the deviation distances between the four imaging objective lens units and the optical axis are d, and the deviation distances d are equal to the total focal length of the telescopic objective lens unit, the zooming collimation objective lens unit and the imaging objective lens unit
Figure 159573DEST_PATH_IMAGE007
The following relational expression is satisfied:
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total focal length of telescopic objective lens unit, focusing collimator objective lens unit and imaging objective lens unit
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And the total length from the rear surface of the first reflector (101) to the rear image surface b of the polarizer (304) of the imaging objective unitTTLAnd the axial distance from the exit surface of the third lens group (303) to the image surface bBFLThe three satisfy the following relational expression:
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6. the apertured compact wide-band simultaneous polarization imaging device according to claim 5, wherein:
diameter of the third reflector (201)
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And the diameter of the sixth reflector (302)
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The following relation is satisfied:
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7. the apertured compact wide-band simultaneous polarization imaging device according to claim 6, wherein:
a total focal length of the first lens group (103) and the second lens group (203)
Figure 321061DEST_PATH_IMAGE013
Satisfies the following formula:
Figure 596185DEST_PATH_IMAGE014
8. the apertured compact wide-band simultaneous polarization imaging device according to claim 7, wherein:
the four polarizers (304) of the four imaging objective units are 0 °, 60 ° and 120 ° polarizers in order in the circumferential direction, and a circularly polarizing polarizer.
9. The apertured compact wide-band simultaneous polarization imaging device according to claim 8, wherein:
the first reflector (101), the third reflector (201), the fourth reflector (202), the fifth reflector (301) and the sixth reflector (302) are hyperboloidal reflectors; the second mirror (102) is a parabolic mirror.
10. The utility model provides a wide band polarization simultaneous imaging system of compact of branch aperture which characterized in that: the aperture-dividing compact wide-band polarization simultaneous imaging device according to any one of claims 5 to 9, further comprising a computer and four detectors connected to the computer, wherein the four detectors are located at the four image planes b and are used for obtaining four groups of polarization images only containing single polarization state information, and the computer is used for processing and calculating the four groups of polarization images to obtain stokes matrix information of a target.
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Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6323946B1 (en) * 1998-04-08 2001-11-27 Kla-Tencor Corporation Spectroscopic measurement system using curved mirror
CN103140803A (en) * 2010-09-30 2013-06-05 卡尔蔡司Smt有限责任公司 Imaging optical system for microlithography
CN209674115U (en) * 2019-02-21 2019-11-22 中国电子科技集团公司第十一研究所 Reflective REAL TIME INFRARED THERMAL IMAGE polarizes double separate imaging optical systems
CN111750997A (en) * 2020-06-29 2020-10-09 中国科学院西安光学精密机械研究所 Optical Imaging Detection Device Based on Polarization Time Division Spectral Synchronization
CN111896480A (en) * 2020-08-12 2020-11-06 长春理工大学 An Off-axis Broadband Reflective Simultaneous Polarization Imaging System
CN112432707A (en) * 2020-09-30 2021-03-02 天津大学 Polarization aperture-division and multispectral imaging device for infrared band

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6323946B1 (en) * 1998-04-08 2001-11-27 Kla-Tencor Corporation Spectroscopic measurement system using curved mirror
CN103140803A (en) * 2010-09-30 2013-06-05 卡尔蔡司Smt有限责任公司 Imaging optical system for microlithography
CN209674115U (en) * 2019-02-21 2019-11-22 中国电子科技集团公司第十一研究所 Reflective REAL TIME INFRARED THERMAL IMAGE polarizes double separate imaging optical systems
CN111750997A (en) * 2020-06-29 2020-10-09 中国科学院西安光学精密机械研究所 Optical Imaging Detection Device Based on Polarization Time Division Spectral Synchronization
CN111896480A (en) * 2020-08-12 2020-11-06 长春理工大学 An Off-axis Broadband Reflective Simultaneous Polarization Imaging System
CN112432707A (en) * 2020-09-30 2021-03-02 天津大学 Polarization aperture-division and multispectral imaging device for infrared band

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