CN206038152U - Polarized interference spectral imaging system - Google Patents
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Abstract
本实用新型公开了一种偏振干涉光谱成像系统,包括沿光路方向依次布置的:用于接收目标物发出的光并对入射光进行准直的透镜组;微透镜阵列,包括以阵列形式排布的N个微透镜;用于将每一子图像光分成振动方向正交的平行分量和垂直分量,并形成每一分量的两束具有预设光程差的线偏振光的双折射分光系统;用于将每一分量的两束线偏振光形成的干涉光汇聚到光电探测器的成像透镜;光电探测器;用于将光电探测器获取的N个由平行分量形成的干涉图像以及N个由垂直分量形成的干涉图像进行处理得到带有偏振信息的光谱图的数据处理器。本实用新型偏振干涉光谱成像系统,具有结构简单稳定、光谱带通宽、光谱分辨率高等特点,并能够实现对动态目标的实时探测。
The utility model discloses a polarization interference spectrum imaging system, which comprises sequentially arranged along the direction of the optical path: a lens group for receiving light emitted by an object and collimating the incident light; a microlens array, including N microlenses; a birefringent beam splitting system for dividing each sub-image light into a parallel component and a vertical component perpendicular to the vibration direction, and forming two beams of linearly polarized light with a preset optical path difference for each component; The imaging lens used to converge the interference light formed by the two beams of linearly polarized light of each component to the photodetector; the photodetector; the N interference images formed by the parallel components and the N interference images obtained by A data processor that processes the interference image formed by the vertical component to obtain a spectrogram with polarization information. The polarization interference spectrum imaging system of the utility model has the characteristics of simple and stable structure, wide spectral bandpass, high spectral resolution, etc., and can realize real-time detection of dynamic targets.
Description
技术领域technical field
本实用新型涉及偏振光谱成像技术领域,特别是涉及一种偏振干涉光谱成像系统。The utility model relates to the technical field of polarization spectrum imaging, in particular to a polarization interference spectrum imaging system.
背景技术Background technique
偏振光谱成像技术融合了光谱成像技术和偏振技术的优点,可以同时获得目标的空间信息、光谱以及偏振信息,是光学遥感和空间探测中重要的技术手段。Polarization spectral imaging technology combines the advantages of spectral imaging technology and polarization technology. It can simultaneously obtain the spatial information, spectrum and polarization information of the target. It is an important technical means in optical remote sensing and space detection.
差分偏振光谱成像技术是由差分偏振成像技术发展而来。差分偏振成像技术仅获得目标正交偏振分量的偏振图像,用以去除背景,提高目标对比度,差分偏振光谱成像技术是将光谱成像技术与差分偏振成像技术相融合。目前,有基于光栅光谱仪的差分偏振光谱成像仪、基于声光调谐滤光片的差分偏振光谱成像仪,这类光谱成像仪存在信噪比低、光谱带通窄、机械结构容易抖动、分辨率低等缺点,并且只能探测静态目标;另外有基于偏振分光器件的差分偏振光谱成像仪,这类光谱成像仪虽然结构稳定、光谱带通宽,但采集图像时使用窗扫描,需要在时间段内采集目标的多次图像,根据多次采集的图像获得目标的偏振光谱测量结果,属于时空调制型,也无法对动态目标进行探测。Differential polarization spectroscopy imaging technology is developed from differential polarization imaging technology. The differential polarization imaging technology only obtains the polarization image of the orthogonal polarization component of the target to remove the background and improve the contrast of the target. The differential polarization spectral imaging technology is a combination of spectral imaging technology and differential polarization imaging technology. At present, there are differential polarization spectral imagers based on grating spectrometers and differential polarization spectral imagers based on acousto-optic tuning filters. Low-level disadvantages, and can only detect static targets; In addition, there are differential polarization spectral imagers based on polarization spectroscopic devices. Although this type of spectral imager has a stable structure and wide spectral bandpass, it uses window scanning when collecting images, and it needs to be scanned within a time period. Multiple images of the target are collected within the target, and the polarization spectrum measurement results of the target are obtained according to the images collected multiple times, which belongs to the space-time modulation type and cannot detect dynamic targets.
实用新型内容Utility model content
鉴于此,本实用新型提供一种偏振干涉光谱成像系统,具有结构简单稳定、光谱带通宽、光谱分辨率高等特点,并能够实现对动态目标的实时探测。In view of this, the utility model provides a polarization interference spectral imaging system, which has the characteristics of simple and stable structure, wide spectral bandpass and high spectral resolution, and can realize real-time detection of dynamic targets.
为实现上述目的,本实用新型提供如下技术方案:In order to achieve the above object, the utility model provides the following technical solutions:
一种偏振干涉光谱成像系统,包括沿光路方向依次布置的:A polarization interference spectrum imaging system, including sequentially arranged along the direction of the optical path:
用于接收目标物发出的光并对入射光进行准直的透镜组;A lens group for receiving the light emitted by the target and collimating the incident light;
用于产生目标物的N个子图像的微透镜阵列,所述微透镜阵列包括以阵列形式排布的N个微透镜,N为大于零的正整数;A microlens array for generating N sub-images of the target, the microlens array includes N microlenses arranged in an array, and N is a positive integer greater than zero;
用于将每一子图像光分成振动方向正交的平行分量和垂直分量,并形成每一分量的两束具有预设光程差的线偏振光的双折射分光系统;A birefringent beam splitting system for dividing each sub-image light into a parallel component and a vertical component perpendicular to the vibration direction, and forming two beams of linearly polarized light with a preset optical path difference for each component;
用于将每一分量的两束线偏振光形成的干涉光汇聚到光电探测器的成像透镜;An imaging lens for converging the interference light formed by two beams of linearly polarized light of each component to the photodetector;
所述光电探测器;said photodetector;
与所述光电探测器相连的、用于将所述光电探测器获取的N个由平行分量形成的干涉图像以及N个由垂直分量形成的干涉图像进行处理得到带有偏振信息的光谱图的数据处理器。connected to the photodetector, used to process the N interference images formed by the parallel components and the N interference images formed by the vertical components obtained by the photodetector to obtain the data of the spectral diagram with polarization information processor.
可选地,所述双折射分光系统包括:Optionally, the birefringence splitting system includes:
用于将每一子图像光分成振动方向正交的平行分量和垂直分量的双折射偏光镜;a birefringent polarizer for splitting each sub-image light into parallel and perpendicular components with orthogonal vibration directions;
用于将每一子图像光的每一分量分成振动方向正交的两束线偏振光的双折射棱镜对;a pair of birefringent prisms for splitting each component of each sub-image light into two linearly polarized beams whose directions of vibration are orthogonal;
用于将每一线偏振光的偏振方向转化的线偏振元件。A linear polarizing element for converting the polarization direction of each linearly polarized light.
可选地,所述双折射偏光镜包括相互贴合的具有第一光轴方向的第一偏光板和具有第二光轴方向的第二偏光板,第一光轴方向在xy平面的投影与第二光轴方向在xy平面的投影的夹角为90度;Optionally, the birefringent polarizer includes a first polarizing plate with a first optical axis direction and a second polarizing plate with a second optical axis direction that are attached to each other, and the projection of the first optical axis direction on the xy plane is the same as The included angle of the projection of the second optical axis direction on the xy plane is 90 degrees;
所述双折射棱镜对的光轴与x轴的夹角分别为0度和90度;The included angles between the optical axis and the x-axis of the pair of birefringent prisms are respectively 0 degrees and 90 degrees;
所述线偏振元件的偏振方向与所述双折射偏光镜的任意一个光轴方向平行;The polarization direction of the linear polarization element is parallel to any optical axis direction of the birefringent polarizer;
沿入射光传播的方向为z轴方向,垂直于z轴方向的竖直方向为y轴方向,垂直于z轴方向的水平方向为x轴方向,x轴、y轴、z轴三者符合右手螺旋定则。The direction along which the incident light propagates is the z-axis direction, the vertical direction perpendicular to the z-axis direction is the y-axis direction, and the horizontal direction perpendicular to the z-axis direction is the x-axis direction, and the x-axis, y-axis, and z-axis are right-handed Spiral rule.
可选地,所述光电探测器的光感应面位于所述成像透镜的焦平面上。Optionally, the photosensitive surface of the photodetector is located on the focal plane of the imaging lens.
可选地,所述透镜组为望远透镜组。Optionally, the lens group is a telephoto lens group.
可选地,所述光电探测器包括CCD探测器。Optionally, the photodetector includes a CCD detector.
可选地,所述数据处理器为计算机。Optionally, the data processor is a computer.
由上述技术方案可知,本实用新型所提供的偏振干涉光谱成像系统,包括沿光路方向依次布置的透镜组、微透镜阵列、双折射分光系统、成像透镜、光电探测器和数据处理器。目标物发出的光经透镜组转换为平行光,经过微透镜阵列形成N个携带相同信息的子图像;每一子图像光经过双折射分光系统,被分为振动方向正交的平行分量和垂直分量,并形成每一分量的两束具有预设光程差的线偏振光;每一子图像光的平行分量对应的两束线偏振光形成的干涉光经成像透镜汇聚到光电探测器,形成平行分量的干涉图像,每一子图像光的垂直分量对应的两束线偏振光形成的干涉光经成像透镜汇聚到光电探测器,形成垂直分量的干涉图像;数据处理器将N个平行分量的干涉图像以及N个垂直分量的干涉图像进行处理得到带有偏振信息的光谱图。It can be seen from the above technical solutions that the polarization interference spectrum imaging system provided by the utility model includes a lens group, a microlens array, a birefringent spectroscopic system, an imaging lens, a photodetector and a data processor arranged in sequence along the direction of the optical path. The light emitted by the target object is converted into parallel light by the lens group, and N sub-images carrying the same information are formed through the micro-lens array; each sub-image light is divided into parallel components orthogonal to the vibration direction and vertical components, and form two beams of linearly polarized light with a preset optical path difference for each component; the interference light formed by the two beams of linearly polarized light corresponding to the parallel component of each sub-image light is converged to the photodetector through the imaging lens to form The interference image of the parallel component, the interference light formed by the two beams of linearly polarized light corresponding to the vertical component of each sub-image light is converged to the photodetector through the imaging lens to form the interference image of the vertical component; the data processor combines the N parallel components The interference image and the interference image of N vertical components are processed to obtain a spectrogram with polarization information.
本实用新型偏振干涉光谱成像系统,同时获得N个平行分量的干涉图像和N个垂直分量的干涉图像,根据N个平行分量的干涉图像和N个垂直分量的干涉图像,处理获得目标物的带有偏振信息的光谱图。能够实现对动态目标的实时探测,并且所述偏振干涉光谱成像系统具有结构简单稳定、光谱带通宽、光谱分辨率高等特点。The polarization interference spectrum imaging system of the utility model obtains the interference images of N parallel components and the interference images of N vertical components at the same time, and processes and obtains the band of the target object according to the interference images of N parallel components and the interference images of N vertical components. A spectrogram with polarization information. Real-time detection of dynamic targets can be realized, and the polarization interference spectral imaging system has the characteristics of simple and stable structure, wide spectral bandpass, high spectral resolution and the like.
附图说明Description of drawings
为了更清楚地说明本实用新型实施例或现有技术中的技术方案,下面将对实施例或现有技术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实用新型的一些实施例,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 more clearly illustrate the technical solutions in the embodiments of the present invention or the prior art, the following will briefly introduce the accompanying drawings that need to be used in the description of the embodiments or the prior art. Obviously, the accompanying drawings in the following description These are only some embodiments of the utility model, and those skilled in the art can also obtain other drawings based on these drawings without creative work.
图1为本实用新型实施例提供的一种偏振干涉光谱成像系统的示意图;Fig. 1 is the schematic diagram of a kind of polarization interference spectrum imaging system provided by the embodiment of the utility model;
图2为本实用新型又一实施例提供的一种偏振干涉光谱成像系统的示意图;Fig. 2 is a schematic diagram of a polarization interference spectrum imaging system provided by another embodiment of the present invention;
图3为本实用新型实施例中双折射偏光镜的结构示意图;Fig. 3 is the structural representation of birefringent polarizer in the utility model embodiment;
图4为本实用新型实施例中双折射棱镜对的结构示意图。Fig. 4 is a schematic structural diagram of a pair of birefringent prisms in an embodiment of the present invention.
具体实施方式detailed description
为了使本技术领域的人员更好地理解本实用新型中的技术方案,下面将结合本实用新型实施例中的附图,对本实用新型实施例中的技术方案进行清楚、完整地描述,显然,所描述的实施例仅仅是本实用新型一部分实施例,而不是全部的实施例。基于本实用新型中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获得的所有其他实施例,都应当属于本实用新型保护的范围。In order to enable those skilled in the art to better understand the technical solution in the utility model, the technical solution in the utility model embodiment will be clearly and completely described below in conjunction with the accompanying drawings in the utility model embodiment. Obviously, The described embodiments are only some of the embodiments of the present utility model, but not all of them. Based on the embodiments of the present utility model, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts shall fall within the protection scope of the present utility model.
请参考图1,为实用新型本实施例提供的一种偏振干涉光谱成像系统的示意图,本实施例偏振干涉光谱成像系统包括沿光路方向依次布置的:Please refer to FIG. 1, which is a schematic diagram of a polarization interference spectrum imaging system provided in this embodiment of the utility model. The polarization interference spectrum imaging system of this embodiment includes sequentially arranged along the optical path direction:
用于接收目标物发出的光并对入射光进行准直的透镜组10;A lens group 10 for receiving the light emitted by the target object and collimating the incident light;
用于产生目标物的N个子图像的微透镜阵列11,所述微透镜阵列11包括以阵列形式排布的N个微透镜,N为大于零的正整数;A microlens array 11 for generating N sub-images of the target, said microlens array 11 comprising N microlenses arranged in an array, where N is a positive integer greater than zero;
用于将每一子图像光分成振动方向正交的平行分量和垂直分量,并形成每一分量的两束具有预设光程差的线偏振光的双折射分光系统12;A birefringent beam splitting system 12 for dividing each sub-image light into a parallel component and a vertical component perpendicular to the vibration direction, and forming two beams of linearly polarized light with a preset optical path difference for each component;
用于将每一分量的两束线偏振光形成的干涉光汇聚到光电探测器14的成像透镜13;An imaging lens 13 for converging the interference light formed by two beams of linearly polarized light of each component to the photodetector 14;
所述光电探测器14;The photodetector 14;
与所述光电探测器14相连的、用于将所述光电探测器14获取的N个由平行分量形成的干涉图像以及N个由垂直分量形成的干涉图像进行处理得到带有偏振信息的光谱图的数据处理器15。The one connected to the photodetector 14 is used to process the N interference images formed by the parallel components and the N interference images formed by the vertical components acquired by the photodetector 14 to obtain a spectral diagram with polarization information The data processor 15.
本实施例提供的偏振干涉光谱成像系统,包括沿光路方向依次布置的透镜组10、微透镜阵列11、双折射分光系统12、成像透镜13、光电探测器14和数据处理器15。目标物发出的光由透镜组进入成像系统,经透镜组转换为平行光,经过微透镜阵列形成N个携带相同信息的子图像;每一子图像光经过双折射分光系统,每一子图像光被分为振动方向正交的平行分量和垂直分量,并形成每一分量的两束具有预设光程差的线偏振光;每一子图像光的平行分量对应的两束线偏振光形成的干涉光经成像透镜汇聚到光电探测器,形成每一子图像平行分量的干涉图像,每一子图像光的垂直分量对应的两束线偏振光形成的干涉光经成像透镜汇聚到光电探测器,形成每一子图像垂直分量的干涉图像;数据处理器将N个平行分量的干涉图像以及N个垂直分量的干涉图像进行处理得到带有偏振信息的光谱图。The polarization interference spectroscopy imaging system provided in this embodiment includes a lens group 10 , a microlens array 11 , a birefringent spectroscopic system 12 , an imaging lens 13 , a photodetector 14 and a data processor 15 sequentially arranged along the optical path direction. The light emitted by the target enters the imaging system through the lens group, is converted into parallel light by the lens group, and forms N sub-images carrying the same information through the micro-lens array; It is divided into parallel components and vertical components that are orthogonal to the vibration direction, and forms two beams of linearly polarized light with a preset optical path difference for each component; the parallel component of each sub-image light is formed by two beams of linearly polarized light The interference light is converged to the photodetector through the imaging lens to form an interference image of the parallel component of each sub-image, and the interference light formed by two beams of linearly polarized light corresponding to the vertical component of each sub-image light is converged to the photodetector through the imaging lens. An interference image of the vertical component of each sub-image is formed; the data processor processes the interference image of N parallel components and the interference image of N vertical components to obtain a spectrogram with polarization information.
本实施例偏振干涉光谱成像系统,能同时获得N个平行分量的干涉图像和N个垂直分量的干涉图像,根据N个平行分量的干涉图像和N个垂直分量的干涉图像,处理获得目标物的带有偏振信息的光谱图。因此能够对动态目标进行成像,能够实现对动态目标的实时探测,且所述偏振干涉光谱成像系统具有结构简单稳定、光谱带通宽、光谱分辨率高等特点。The polarization interference spectrum imaging system of this embodiment can simultaneously obtain the interference images of N parallel components and the interference images of N vertical components, and process and obtain the image of the target object according to the interference images of N parallel components and the interference images of N vertical components. Spectrogram with polarization information. Therefore, the dynamic target can be imaged, and the real-time detection of the dynamic target can be realized, and the polarization interference spectral imaging system has the characteristics of simple and stable structure, wide spectral bandpass, high spectral resolution and the like.
下面对本实施例偏振干涉光谱成像系统进行详细说明。本实施例提供的偏振干涉光谱成像系统包括透镜组10、微透镜阵列11、双折射分光系统12、成像透镜13、光电探测器14和数据处理器15。本实施例中定义:沿入射光传播的方向为z轴方向,垂直于z轴方向的竖直方向为y轴方向,垂直于z轴方向的水平方向为x轴方向,x轴、y轴、z轴三者符合右手螺旋定则。The polarization interference spectroscopy imaging system of this embodiment will be described in detail below. The polarization interference spectroscopy imaging system provided in this embodiment includes a lens group 10 , a microlens array 11 , a birefringent spectroscopic system 12 , an imaging lens 13 , a photodetector 14 and a data processor 15 . In this embodiment, it is defined that the direction along which the incident light propagates is the z-axis direction, the vertical direction perpendicular to the z-axis direction is the y-axis direction, the horizontal direction perpendicular to the z-axis direction is the x-axis direction, and the x-axis, y-axis, The three on the z-axis conform to the right-hand spiral rule.
其中,透镜组10用于接收目标物发出的光并对入射光进行准直,使目标物发出的光经过透镜组转换为平行光。所述透镜组10可以是望远透镜组,该成像系统能够进行遥感探测。Wherein, the lens group 10 is used for receiving the light emitted by the target object and collimating the incident light, so that the light emitted by the target object is converted into parallel light through the lens group. The lens group 10 may be a telescopic lens group, and the imaging system is capable of remote sensing detection.
所述微透镜阵列11包括以阵列形式排布的N个微透镜,平行光经过微透镜阵列11后,形成目标物的N个携带相同信息的子图像。The microlens array 11 includes N microlenses arranged in an array. After the parallel light passes through the microlens array 11, N sub-images of the target object are formed, which carry the same information.
本实施例中,参考图2所示,所述双折射分光系统12包括:In this embodiment, as shown in FIG. 2 , the birefringence splitting system 12 includes:
用于将每一子图像光分成振动方向正交的平行分量和垂直分量的双折射偏光镜120;A birefringent polarizer 120 for dividing each sub-image light into a parallel component and a vertical component perpendicular to the vibration direction;
用于将每一子图像光的每一分量分成振动方向正交的两束线偏振光的双折射棱镜对121;A pair of birefringent prisms 121 for dividing each component of each sub-image light into two beams of linearly polarized light whose vibration directions are orthogonal;
用于将每一线偏振光的偏振方向转化的线偏振元件122。A linear polarization element 122 for converting the polarization direction of each linearly polarized light.
具体的,本实施例中所述双折射偏光镜120为萨瓦尔偏光镜,双折射偏光镜120包括相互贴合的具有第一光轴方向的第一偏光板和具有第二光轴方向的第二偏光板,第一光轴方向在xy平面的投影与第二光轴方向在xy平面的投影的夹角为90度,可参考图3所示,图3为本实施例中双折射偏光镜的结构示意图,图中箭头所指方向为光轴方向。每一子图像光经过所述双折射偏光镜被120分成振动方向正交的平行分量和垂直分量,平行分量指平行于x轴方向的分量,垂直分量指垂直于x轴方向的分量。Specifically, the birefringent polarizer 120 in this embodiment is a Savall polarizer, and the birefringent polarizer 120 includes a first polarizer with a first optical axis direction and a second polarizer with a second optical axis direction that are attached to each other. Two polarizers, the angle between the projection of the first optical axis direction on the xy plane and the projection of the second optical axis direction on the xy plane is 90 degrees, as shown in Figure 3, which is a birefringent polarizer in this embodiment Schematic diagram of the structure, the direction of the arrow in the figure is the direction of the optical axis. Each sub-image light passes through the birefringent polarizer and is divided by 120 into a parallel component and a vertical component perpendicular to the vibration direction. The parallel component refers to the component parallel to the x-axis direction, and the vertical component refers to the component perpendicular to the x-axis direction.
所述双折射棱镜对121为渥拉斯顿棱镜,所述双折射棱镜对121的光轴与x轴的夹角分别为0度和90度,可参考图4所示,图中箭头所指方向为棱镜的光轴方向。每一子图像光的平行分量经过双折射棱镜对121,被分成振动方向正交的两束线偏振光;每一子图像光的垂直分量经过双折射棱镜对121,被分成振动方向正交的两束线偏振光。The pair of birefringent prisms 121 is a Wollaston prism, and the angles between the optical axis and the x-axis of the pair of birefringent prisms 121 are respectively 0 degrees and 90 degrees, as shown in Fig. The direction is the direction of the optical axis of the prism. The parallel component of each sub-image light passes through the pair of birefringent prisms 121, and is divided into two beams of linearly polarized light whose vibration directions are orthogonal; Two beams of linearly polarized light.
每一分量光的两束线偏振光经过双折射棱镜对121产生的光程差,与该分量光在双折射棱镜对上的入射位置的y坐标值具有线性关系,光程差表达式为:Δ=2(ne-no)ytanθ,其中Δ表示光程差,ne表示棱镜中e光折射率、no表示棱镜中o光折射率,θ表示棱镜的楔角,y表示入射光入射位置的y坐标。因此,对于N个子图像光,入射到双折射棱镜的位置不同,相同分量的两束线偏振光的光程差不同,可产生N个具有不同光程差的平行分量的干涉图像和N个具有不同光程差的垂直分量的干涉图像。The optical path difference generated by the two linearly polarized lights of each component light passing through the birefringent prism pair 121 has a linear relationship with the y-coordinate value of the incident position of the component light on the birefringent prism pair, and the expression of the optical path difference is: Δ=2(n e -n o )ytanθ, where Δ represents the optical path difference, n e represents the refractive index of e light in the prism, n o represents the refractive index of o light in the prism, θ represents the wedge angle of the prism, and y represents the incident light The y coordinate of the incident location. Therefore, for N sub-image lights, the positions incident on the birefringent prism are different, and the optical path differences of the two linearly polarized lights of the same component are different, so N interference images with parallel components with different optical path differences and N interference images with different optical path differences can be produced. Interference images of the vertical components of different optical path differences.
所述线偏振元件122的偏振方向与所述双折射偏光镜120的任意一个光轴方向平行。The polarization direction of the linear polarization element 122 is parallel to any optical axis direction of the birefringent polarizer 120 .
每一子图像光的平行分量的两束线偏振光经过线偏振元件122,转化为与线偏振元件的偏振方向相同的线偏振光,两束线偏振光形成的干涉光经成像透镜汇聚到光电探测器光感应面,得到每一子图像的平行分量的干涉图像。每一子图像光的垂直分量的两束线偏振光经过线偏振元件,转化为偏振方向与线偏振元件相同偏振方向的线偏振光,两束线偏振光形成的干涉光经成像透镜汇聚到光电探测器光感应面,得到每一子图像的垂直分量的干涉图像。The two beams of linearly polarized light of the parallel component of each sub-image pass through the linear polarization element 122, and are converted into linearly polarized light with the same polarization direction as the linear polarization element, and the interference light formed by the two beams of linearly polarized light is converged to the photoelectric The photosensitive surface of the detector is used to obtain the interference image of the parallel component of each sub-image. The two beams of linearly polarized light of the vertical component of each sub-image pass through the linear polarization element and are converted into linearly polarized light with the same polarization direction as the linear polarization element. The interference light formed by the two beams of linearly polarized light is converged to the photoelectric The photosensitive surface of the detector is used to obtain the interference image of the vertical component of each sub-image.
本实施例中优选的,所述光电探测器14的光感应面位于所述成像透镜13的焦平面上。Preferably in this embodiment, the photosensitive surface of the photodetector 14 is located on the focal plane of the imaging lens 13 .
在光电探测器14的光感应面上,对于每一子图像,形成正交偏振分量的电场矢量的表达式分别如下:On the photosensitive surface of the photodetector 14, for each sub-image, the expressions of the electric field vectors forming the orthogonal polarization components are respectively as follows:
其中,Jwp1+Jwp2ei2πΔλ表示渥拉斯顿棱镜的琼斯矩阵,Jsp1和Jsp2表示萨瓦尔偏光镜的琼斯矩阵,JLA表示线偏振元件的琼斯矩阵,E||表示目标图像的电场矢量的平行分量,E⊥表示目标图像的电场矢量的垂直分量。Among them, J wp1 + J wp2 e i2πΔλ represents the Jones matrix of the Wollaston prism, J sp1 and J sp2 represent the Jones matrix of the Savall polarizer, J LA represents the Jones matrix of the linear polarization element, E || represents the target image The parallel component of the electric field vector, E ⊥ represents the vertical component of the electric field vector of the target image.
在光电探测器14的光感应面上接收的正交偏振分量的两幅干涉图像表达式分别为:The expressions of the two interference images of the orthogonal polarization components received on the photosensitive surface of the photodetector 14 are respectively:
对于N个子图像光,由于入射到双折射棱镜的位置不同,不同子图像之间的光程差是不相同,不同子图像的相同分量的两束线偏振光的光程差不同,即可产生N个具有不同光程差的平行分量的干涉图像和N个具有不同光程差的垂直分量的干涉图像。数据处理器根据得到的N个平行分量的干涉图像和N个垂直分量的干涉图像,对平行分量的干涉图序列和垂直分量的干涉图序列分别进行数据提取和重构,得到目标物的三维干涉图像,再利用傅里叶变换反演出两幅光谱图,即正交偏振分量光谱图,两光谱图像之差即为目标物的差分偏振光谱图像,两光谱图像之差与两光谱图像之和的比值即为目标物的线偏振度光谱图像。For N sub-image lights, due to the different positions incident on the birefringent prism, the optical path difference between different sub-images is different, and the optical path difference between two beams of linearly polarized light of the same component in different sub-images is different, which can produce Interference images of N parallel components with different optical path differences and N interference images of perpendicular components with different optical path differences. The data processor extracts and reconstructs the data of the interferogram sequence of the parallel component and the interferogram sequence of the vertical component respectively according to the interference image of N parallel components and the interference image of N vertical components, and obtains the three-dimensional interference of the target object image, and then use the Fourier transform to invert two spectral images, that is, the orthogonal polarization component spectral image, the difference between the two spectral images is the differential polarization spectral image of the target object, and the difference between the two spectral images and the sum of the two spectral images The ratio is the linear polarization spectrum image of the target object.
本实施例中,所述光电探测器可采用CCD探测器。所述数据处理器15为计算机。In this embodiment, the photodetector may be a CCD detector. The data processor 15 is a computer.
以上对本实用新型所提供的一种偏振干涉光谱成像系统进行了详细介绍。本文中应用了具体个例对本实用新型的原理及实施方式进行了阐述,以上实施例的说明只是用于帮助理解本实用新型的方法及其核心思想。应当指出,对于本技术领域的普通技术人员来说,在不脱离本实用新型原理的前提下,还可以对本实用新型进行若干改进和修饰,这些改进和修饰也落入本实用新型权利要求的保护范围内。A polarization interference spectrum imaging system provided by the utility model has been introduced in detail above. In this paper, specific examples are used to illustrate the principle and implementation of the present utility model, and the descriptions of the above embodiments are only used to help understand the method and core idea of the present utility model. It should be pointed out that for those of ordinary skill in the art, without departing from the principle of the utility model, some improvements and modifications can also be made to the utility model, and these improvements and modifications also fall into the protection of the claims of the utility model. within range.
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