CN115494024A - Optical path device and focusing method for terahertz continuous wave tomography - Google Patents
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Abstract
Description
技术领域technical field
本发明属于太赫兹成像技术领域,具体涉及一种用于太赫兹连续波层析成像的光路装置及聚焦方法。The invention belongs to the technical field of terahertz imaging, and in particular relates to an optical path device and a focusing method for terahertz continuous wave tomography.
背景技术Background technique
太赫兹段的工作频率为100GHz~10THz,对应波长为3mm~30μm。该频段高于微波、毫米波频段,低于红外、可见光频段;并且由于这个频段的电磁波位于宏观电子学至微观光子学过渡的区域,具有一些独有的特性。在成像领域中,相比于微波、毫米波成像,太赫兹成像分辨率远高于微波、毫米波频段;相比于红外、可见光成像,太赫兹波对于非极性物质穿透能力更强;相比于X射线,太赫兹成像对低介电常数材料成像对比度更高,并且其光子能量远低于X射线,因此不会对材料和生物体造成电离,因此更加安全。目前太赫兹成像主要应用于无损检测,生物医学等领域。The operating frequency of the terahertz segment is 100 GHz to 10 THz, and the corresponding wavelength is 3 mm to 30 μm. This frequency band is higher than the microwave and millimeter wave frequency bands, and lower than the infrared and visible light frequency bands; and because the electromagnetic waves in this frequency band are located in the transition region from macroelectronics to microphotonics, they have some unique characteristics. In the field of imaging, compared with microwave and millimeter-wave imaging, the resolution of terahertz imaging is much higher than that of microwave and millimeter-wave frequency bands; compared with infrared and visible light imaging, terahertz waves have a stronger ability to penetrate non-polar substances; Compared with X-rays, terahertz imaging has higher imaging contrast for materials with low dielectric constant, and its photon energy is much lower than that of X-rays, so it will not ionize materials and organisms, so it is safer. At present, terahertz imaging is mainly used in non-destructive testing, biomedicine and other fields.
目前在太赫兹三维成像技术中,比较成熟的技术是太赫兹计算机辅助层析成像(CT)。在太赫兹CT成像中,又分为连续波(CW)和脉冲(TDS)两种成像方式,其中,THz-CW成像系统因为具备系统简单、成本低、成像速度快等优势,得到了广泛应用。THz-CW成像结果的优劣很大程度决定与光路装置的设计,因此太赫兹连续波层析成像的光路装置就成为研究重点之一。为了满足成像分辨率的要求,需要将太赫兹连续波发生器所发射的波束聚焦到样品处,聚焦到样品处的波束为较细高斯波束,即样品处的束腰半径较小。然而到目前为止,大部分传统THz-CT-CW成像系统的光路装置是采用不少于4个反射镜或透镜,或两种的组合。例如,文献《太赫兹层析成像的理论与实验研究》的THz-CT-CW系统采用4个透镜,其光路装置结构示意图如图1所示:先将太赫兹连续波发生器所发射的波束进行准直,然后聚焦到样品处,波束透射样品后再进行准直,最后聚焦到太赫兹连续波接收装置;文献《Investigation on reconstruction methods applied to 3D terahertz computedtomography》所提出的THz-CT-CW系统采用2个抛物面反射镜和2个透镜,其光路装置结构示意图如图2所示:太赫兹连续波发生器所发射的波束经过抛物面反射镜反射后准直,然后通过透镜聚焦在样品上,透射样品后的波束再经过透镜进行准直,最后经过抛物面反射镜聚焦到太赫兹连续波接收装置。由此可以看出,现有技术中所提出的THz-CT-CW系统的光路装置采用的光路元件均不少于4个,此时,光路实现较为复杂,并且在调节透镜之间的位置时会面临很大困难。At present, in the terahertz three-dimensional imaging technology, the relatively mature technology is terahertz computer-aided tomography (CT). In terahertz CT imaging, it is divided into continuous wave (CW) and pulse (TDS) imaging methods. Among them, THz-CW imaging system has been widely used because of its simple system, low cost, and fast imaging speed. . The quality of THz-CW imaging results largely depends on the design of the optical path device, so the optical path device of THz continuous wave tomography has become one of the research focuses. In order to meet the requirements of imaging resolution, the beam emitted by the terahertz continuous wave generator needs to be focused on the sample, and the beam focused on the sample is a thinner Gaussian beam, that is, the beam waist radius at the sample is smaller. However, so far, the optical path devices of most traditional THz-CT-CW imaging systems use no less than 4 mirrors or lenses, or a combination of the two. For example, the THz-CT-CW system in the document "Theoretical and Experimental Research on Terahertz Tomography" uses four lenses, and the schematic diagram of the optical path device structure is shown in Figure 1: firstly, the beam emitted by the terahertz continuous wave generator Collimate, then focus on the sample, collimate the beam after it passes through the sample, and finally focus on the terahertz continuous wave receiving device; the THz-CT-CW system proposed in the document "Investigation on reconstruction methods applied to 3D terahertz computedtomography" Two parabolic reflectors and two lenses are used, and the structural diagram of the optical path device is shown in Figure 2: the beam emitted by the terahertz continuous wave generator is collimated after being reflected by the parabolic reflector, and then focused on the sample through the lens, transmitted The beam after the sample is collimated by the lens, and finally focused to the terahertz continuous wave receiving device by the parabolic mirror. It can be seen from this that the optical path device of the THz-CT-CW system proposed in the prior art uses no less than four optical path elements. At this time, the realization of the optical path is relatively complicated, and when adjusting the position between the lenses will face great difficulties.
因此,如何设计光路装置,使其能够用较少的光路元件就能实现THz-CT-CW系统所需要的光路性能,就成为研究重点。Therefore, how to design the optical path device so that it can achieve the optical path performance required by the THz-CT-CW system with fewer optical path components has become a research focus.
发明内容Contents of the invention
针对背景技术所存在的问题,本发明的目的在于提供一种用于太赫兹连续波层析成像的光路装置及聚焦方法。该光路装置仅采用两个离轴椭球面反射镜,就能实现将太赫兹连续波发生器所发射的发射波束直接聚焦到样品处,然后再将透射样品后的聚焦波束直接聚焦到太赫兹连续波接收装置;省去了准直过程所需要的两个透镜或反射面,实现对传统THz-CT-CW成像系统光路图的简化,降低调节透镜位置的难度。In view of the problems existing in the background technology, the purpose of the present invention is to provide an optical path device and a focusing method for terahertz continuous wave tomography. The optical path device only uses two off-axis ellipsoid mirrors, which can directly focus the emission beam emitted by the terahertz continuous wave generator to the sample, and then directly focus the focused beam transmitted through the sample to the terahertz continuous wave generator. Wave receiving device; two lenses or reflective surfaces required for the collimation process are omitted, the simplification of the optical path diagram of the traditional THz-CT-CW imaging system is realized, and the difficulty of adjusting the lens position is reduced.
为实现上述目的,本发明的技术方案如下:To achieve the above object, the technical scheme of the present invention is as follows:
一种用于太赫兹连续波层析成像的光路装置,包括三维平移台30、旋转台31和关于旋转台31竖直对称设置的左光路和右光路,对称轴为旋转台31的竖直中心线,其中,左光路包括太赫兹连续波发生器1、矩形波导2、喇叭天线3和第一离轴椭球面反射镜12,右光路包括第二离轴椭球面反射镜12和太赫兹连续波接收装置11;所述旋转台31固定设置于三维平移台30上,待测样品放置于旋转台31中心;An optical path device for terahertz continuous wave tomography, including a three-
太赫兹连续波发生器1用于生成发射波束5,发射波束5经矩形波导2和喇叭天线3后发射至第一离轴椭球面反射镜12的反射面19,反射后所得到的第一聚焦波束I(7)入射至待测样品表面,透过待测样品的第一聚焦波束I(7)经第二离轴椭球面反射镜12的反射面19反射,反射后所得到的第二聚焦波束II(10)被太赫兹连续波接收装置11接收;The terahertz
发射波束5和第二聚焦波束II(10)的最小束腰半径均为w1,第一聚焦波束I(7)的最小束腰半径w2,发射波束5的最小束腰半径所在平面到第一离轴椭球面反射镜12反射点6的距离为d1,第一聚焦波束I(7)的最小束腰半径所在平面到第一离轴椭球面反射镜12反射点6的距离为d2;第一离轴椭球面反射镜的椭球面长轴15与发射波束5的入射方向4之间的夹角,以及第二离轴椭球面反射镜的椭球面长轴15与第二聚焦波束II(10)的传播方向之间的夹角均为α;第一聚焦波束I(7)的传播方向与发射波束5的入射方向4之间的夹角,以及第一聚焦波束I(7)的传播方向与第二聚焦波束II(10)的传播方向之间的夹角均为β;所述喇叭天线3的相位中心位于第一离轴椭球面反射镜12所在椭圆25第一焦点22处,太赫兹连续波接收装置11的相位中心位于第二离轴椭球面反射镜12所在椭圆25第一焦点22处;所述第一聚焦波束I(7)的相位中心位于第一离轴椭球面反射镜12所在椭圆25第二焦点23处;两个离轴椭球面反射镜12的反射面19深度为d3,宽度为W,长度L,离轴椭球面反射镜12的椭圆25第一焦点22到该反射镜反射点6的距离为R1,第二焦点23到该反射镜反射点6的距离为R2。The minimum beam waist radius of the
进一步地,所述喇叭天线3的副瓣电平比主瓣电平小20dB以上。Further, the side lobe level of the
进一步地,所述喇叭天线3为圆锥双模喇叭天线或波纹喇叭天线,保证喇叭天线3所辐射的发射波束5为更高质量的高斯波束。Further, the
进一步地,所述离轴椭球面反射镜12采用铝合金加工制作,且反射面19应抛光,使得第一聚焦波束I(7)和第二聚焦波束II(10)均为高质量的高斯波束。Further, the off-
进一步地,所述离轴椭球面反射镜12的反射面19为旋转椭球面的一部分,选取旋转椭球面与离轴椭球面反射镜12面积较小的重叠部分作为所述离轴椭球面反射镜12的反射面19;其中,所述旋转椭球面为椭圆25绕椭球面长轴15旋转一周得到。Further, the
本发明还提供了所述离轴椭球面反射镜12的反射面19的聚焦方法,包括以下步骤:The present invention also provides a focusing method for the reflecting
S1.根据实际需要确定光路装置基本参数,所述光路装置基本参数包括:发射波束5的最小束腰半径w1(13),第一聚焦波束I(7)的最小束腰半径w2(16),第一聚焦波束I的最小束腰半径所在平面到第一离轴椭球面反射镜反射点6的距离d2,以及第一聚焦波束I(7)的传播方向与发射波束5的入射方向4之间的夹角β;S1. Determine the basic parameters of the optical path device according to actual needs, the basic parameters of the optical path device include: the minimum beam waist radius w1 (13) of the
S2.计算得到任一离轴椭球面反射镜12的反射面19的焦距f和距离d1(14),具体计算公式为:S2. calculate the focal length f and the distance d1 (14) of the
其中,λ0为太赫兹波的真空波长;Wherein, λ 0 is the vacuum wavelength of the terahertz wave;
S3.计算得到离轴椭球面反射镜12的椭圆25参数,具体计算公式为:S3. Calculate the
a=(R1+R2)/2a=(R 1 +R 2 )/2
其中i=1,2,a为椭圆25的半长轴,b为椭圆25的半短轴,c为椭圆25半焦距,α为第一离轴椭球面反射镜12的椭球面长轴15与发射波束5的入射方向4之间的夹角,或第二离轴椭球面反射镜12的椭球面长轴15与第二聚焦波束II(10)的传播方向之间的夹角;R1(20)为喇叭天线3的相位中心到第一离轴椭球面反射镜12反射点6的距离,或太赫兹连续波接收装置11的相位中心到第二离轴椭球面反射镜12反射点6的距离,R2(21)为第一聚焦波束I(7)的相位中心到第一离轴椭球面反射镜12反射点6的距离。Wherein i=1,2, a is the semi-major axis of the
进一步地,步骤S1中,为了保证所述喇叭天线3所辐射的发射波束5和聚焦在旋转台31中心处的第一聚焦波束I(7)具有较高的方向性,w1(13)和w2(16)均大于λ0;d2(17)需要选择合适值,以保证旋转台31和样品能够放在两个离轴椭球面反射镜12之间;w2(16)需要选择合适值,以保证待测样品任意高度截面的最大半径R0满足:Further, in step S1, in order to ensure that the
进一步地,步骤S3中,为了保证喇叭天线3所发射的发射波束5的大部分能量被离轴椭球面反射镜12的反射面19反射,离轴椭球面反射镜12的反射面19大小需要适当选取,其反射面19的覆盖角度θ(即反射面19遮盖喇叭天线的角度)(26)应满足,Further, in step S3, in order to ensure that most of the energy of the
其中A和B为常数。where A and B are constants.
进一步地,夹角α(18)的取值范围优选为35°~55°;夹角β的选取范围优选为70°~110°,使得离轴椭球面反射镜12的反射性能较佳。Further, the value range of the included angle α(18) is preferably 35°-55°; the selected range of the included angle β is preferably 70°-110°, so that the reflection performance of the off-
综上所述,由于采用了上述技术方案,本发明的有益效果是:In summary, owing to adopting above-mentioned technical scheme, the beneficial effect of the present invention is:
本发明提供的太赫兹连续波三维层析成像光路装置,实现了对喇叭天线所发射的发射波束直接聚焦到样品处,然后再将透射样品后的聚焦波束直接聚焦到太赫兹连续波接收装置;该装置省去了传统光路装置准直过程所需要的两个透镜或反射面,进而实现对传统THz-CT-CW成像系统光路图的简化,降低调节透镜位置的难度。The terahertz continuous wave three-dimensional tomographic optical path device provided by the present invention realizes direct focusing of the transmission beam emitted by the horn antenna to the sample, and then directly focuses the focused beam transmitted through the sample to the terahertz continuous wave receiving device; The device saves two lenses or reflective surfaces required in the collimation process of the traditional optical path device, thereby realizing the simplification of the optical path diagram of the traditional THz-CT-CW imaging system and reducing the difficulty of adjusting the lens position.
附图说明Description of drawings
图1是传统太赫兹连续波三维层析成像光路装置的示意图,包括4个透镜。Fig. 1 is a schematic diagram of a traditional terahertz continuous wave three-dimensional tomography optical path device, including four lenses.
图2是传统太赫兹连续波三维层析成像光路装置示意图,包括2个反射镜和2个透镜。Fig. 2 is a schematic diagram of a traditional terahertz continuous wave three-dimensional tomography optical path device, including 2 mirrors and 2 lenses.
图3是本发明用于太赫兹连续波层析成像的光路装置的示意图。Fig. 3 is a schematic diagram of an optical path device for terahertz continuous wave tomography of the present invention.
图4是本发明左光路装置的示意图。Fig. 4 is a schematic diagram of the left optical path device of the present invention.
图5是本发明右光路装置的示意图。Fig. 5 is a schematic diagram of the right optical path device of the present invention.
图6是本发明光路装置中的离轴椭球面反射镜对应的椭球面示意图。Fig. 6 is a schematic diagram of an ellipsoid corresponding to an off-axis ellipsoid reflector in the optical path device of the present invention.
图7是本发明光路装置中的离轴椭球面反射镜的示意图。Fig. 7 is a schematic diagram of an off-axis ellipsoidal reflector in the optical path device of the present invention.
图8是本发明光路装置中的离轴椭球面反射镜的正视图。Fig. 8 is a front view of the off-axis ellipsoid reflector in the optical path device of the present invention.
图9是本发明光路装置中的离轴椭球面反射镜的俯视图。Fig. 9 is a top view of the off-axis ellipsoid reflector in the optical path device of the present invention.
图10是本发明光路装置中的离轴椭球面反射镜的左视图。Fig. 10 is a left side view of the off-axis ellipsoid mirror in the optical path device of the present invention.
图11是本发明用于太赫兹连续波层析成像的光路装置的FEKO仿真结果图。Fig. 11 is a diagram of FEKO simulation results of the optical path device for terahertz continuous wave tomography of the present invention.
图12是基于本发明提供的光路装置的THz-CT-CW系统的成像目标和结果图。Fig. 12 is a diagram of the imaging target and results of the THz-CT-CW system based on the optical path device provided by the present invention.
图中,1为太赫兹连续波发生器,2为矩形波导,3为喇叭天线,4为入射方向,5为发射波束,6为反射点,7为聚焦波束I,8为反射方向I,9为反射方向II,10为聚焦波束II,11为太赫兹连续波接收装置,12为离轴椭球面反射镜,13为发射波束5或聚焦波束II(10)的最小束腰半径w1,14为w1(13)所在平面到反射点6的距离d1,15为椭球面长轴,16为聚焦波束I(7)的最小束腰半径w2,17为w2(16)所在平面到反射点6的距离d2,18为椭球面长轴15与入射方向4或反射方向II(9)之间的夹角α,19为离轴椭球面反射镜12的反射面,20为椭圆25的焦点22到反射点6的距离R1,21为椭圆25的焦点23到反射点6的距离R2,22和23为椭圆25的焦点,24为椭圆25的短轴,25为椭圆,26为反射面19的覆盖角度θ,27为离轴椭球面反射镜12的长度L,28为反射面19的深度d3,29为离轴椭球面反射镜12的宽度W,30为三维平移台,31为旋转台,32为聚焦透镜,33为抛物面反射镜,34为椭球面在反射点6处切平面。In the figure, 1 is the terahertz continuous wave generator, 2 is the rectangular waveguide, 3 is the horn antenna, 4 is the incident direction, 5 is the transmitting beam, 6 is the reflection point, 7 is the focused beam I, 8 is the reflection direction I, 9 is the reflection direction II, 10 is the focused beam II, 11 is the terahertz continuous wave receiving device, 12 is the off-axis ellipsoid mirror, 13 is the minimum beam waist radius w1 of the transmitted
具体实施方式detailed description
为使本发明的目的、技术方案和优点更加清楚,下面结合实施方式和附图,对本发明作进一步地详细描述。In order to make the purpose, technical solution and advantages of the present invention clearer, the present invention will be further described in detail below in conjunction with the implementation methods and accompanying drawings.
一种用于太赫兹连续波层析成像的光路装置,其结构示意图如图3所示,包括三维平移台30、旋转台31和关于旋转台31竖直对称设置的左光路和右光路,其中,左光路包括太赫兹连续波发生器1、矩形波导2、喇叭天线3和第一离轴椭球面反射镜12,右光路包括第二离轴椭球面反射镜12和太赫兹连续波接收装置11;所述旋转台31固定设置于三维平移台30上,待测样品放置于旋转台31中心;An optical path device for terahertz continuous wave tomography, its structural schematic diagram is shown in Figure 3, including a three-
太赫兹连续波发生器1用于生成发射波束5,发射波束5经矩形波导2和喇叭天线3后发射至第一离轴椭球面反射镜12的反射面19,反射后所得到的第一聚焦波束I(7)入射至待测样品表面,透过待测样品的第一聚焦波束I(7)经第二离轴椭球面反射镜12的反射面19反射,反射后所得到的第二聚焦波束II(10)被太赫兹连续波接收装置11接收;The terahertz
发射波束5和第二聚焦波束II(10)的最小束腰半径均为w1,第一聚焦波束I(7)的最小束腰半径w2,发射波束5的最小束腰半径所在平面到第一离轴椭球面反射镜反射点6的距离为d1,第一聚焦波束I(7)的最小束腰半径所在平面到第一离轴椭球面反射镜反射点6的距离为d2;第一离轴椭球面反射镜的椭球面长轴15与发射波束5的入射方向4之间的夹角,以及第二离轴椭球面反射镜的椭球面长轴15与第二聚焦波束II(10)的传播方向之间的夹角均为α;第一聚焦波束I(7)的传播方向与发射波束5的入射方向4之间的夹角,以及第一聚焦波束I(7)的传播方向与第二聚焦波束II(10)的传播方向之间的夹角均为β;所述喇叭天线3的相位中心位于第一离轴椭球面反射镜12所在椭圆的第一焦点22处,太赫兹连续波接收装置11的相位中心位于第二离轴椭球面反射镜12所在椭圆的第一焦点22处,所述第一聚焦波束I(7)的相位中心位于第一离轴椭球面反射镜12所在椭圆25第二焦点23处;所述旋转台31的中心位于第一反射方向I(8,即第一聚焦波束的传播方向)上,且离两个离轴椭球面反射镜12的反射点6的距离均为d2(17);两个离轴椭球面反射镜的反射面深度为d3,宽度为W,长度L,椭圆25第一焦点22到反射点6的距离为R1,椭圆25第二焦点23到反射点6的距离为R2。The minimum beam waist radius of the
图4和图5分别是本发明光路装置的左光路装置和右光路装置示意图。如图4和5所示,离轴椭球面反射镜12的椭球面长轴15与发射波束5的入射方向4以及反射方向II(9)呈夹角α(15);反射方向I(8)与入射方向4以及反射方向II(9)为β。图6是本发明光路装置中的离轴椭球面反射镜对应的椭球面示意图。如图6所示,喇叭天线3的相位中心位于第一离轴椭球面反射镜12的椭球面焦点22处,发射波束5的最小束腰半径w1所在平面到第一离轴椭球面反射镜反射点6的距离d1,和喇叭天线3的相位中心到第一离轴椭球面反射镜反射点6的距离R1并不相等;第一聚焦波束I(7)的最小束腰半径w2所在平面到第一离轴椭球面反射镜反射点6的距离d2,与第一离轴椭球面反射镜所在椭圆25的第二焦点23到反射点6的距离R2也并不相等。Fig. 4 and Fig. 5 are respectively schematic diagrams of the left optical path device and the right optical path device of the optical path device of the present invention. As shown in Figures 4 and 5, the
图7是本发明光路装置中的离轴椭球面反射镜的示意图,从图中可以看出,离轴椭球面反射镜12的反射面19与太赫兹连续波发生器1的覆盖范围。图中,喇叭天线辐射电磁波传播方向为轴x+,并且能量在x轴处最强,离x轴越远,能量越弱,为了保证天线辐射电磁波的大部分能量被反射面19反射,离轴椭球面反射镜12的反射面19的覆盖角度为θ。喇叭天线3和太赫兹连续波接收装置11相位中心分别位于两个离轴椭球面反射镜12的焦点22处,所述旋转台31的中心位于反射方向I(8)上,且离两个离轴椭球面反射镜12的反射点6的距离为d2(17)。7 is a schematic diagram of the off-axis ellipsoid reflector in the optical path device of the present invention. It can be seen from the figure that the
图8、图9和图10分别是本发明光路装置中的离轴椭球面反射镜的正视图、俯视图和左视图。所述离轴椭球面反射镜12的反射面19为旋转椭球面的一部分;反射面19通过以下方式得到:椭圆25绕椭球面长轴15旋转一周得到旋转椭球面,然后用平行于椭球面在反射点6处切平面34的平面对旋转椭球面切割后取面积较小的部分得到所述离轴椭球面反射镜12的反射面19。Fig. 8, Fig. 9 and Fig. 10 are respectively the front view, top view and left side view of the off-axis ellipsoid mirror in the optical path device of the present invention. The
实施例1Example 1
上述光路装置中离轴椭球面反射镜12的反射面19的聚焦方法,包括以下步骤:The focusing method of the
S1.根据实际需要确定光路装置基本参数,所述光路装置基本参数包括:发射波束5的最小束腰半径w1(13),聚焦在旋转台31中心处的第一聚焦波束I(7)的最小束腰半径w2(16),第一聚焦波束I的最小束腰半径所在平面到第一离轴椭球面反射镜反射点6的距离d2(17),以及第一聚焦波束I(7)的传播方向(反射方向I(8))与第二聚焦波束II(10)的传播方向(反射方向II(9))之间的夹角β;在本例中,太赫兹连续波发生器1的工作频率为110GHz,对应波长λ0=2.73mm,设置w1(13)=7mm,w2(16)=6mm,d2(17)=170mm,β=90°,成像目标最大半径为40mm;S1. Determine the basic parameters of the optical path device according to actual needs. The basic parameters of the optical path device include: the minimum beam waist radius w1 (13) of the
则样品任意高度截面(截面平行于xoy)的最大半径R0应为:Then the maximum radius R0 of the cross-section at any height of the sample (the cross-section is parallel to xoy ) should be:
该尺寸的样品在瑞利范围内,聚焦波束I(7)近似为平面波,满足CT成像基本条件;The sample of this size is within the Rayleigh range, and the focused beam I(7) is approximately a plane wave, which satisfies the basic conditions of CT imaging;
S2.根据以下公式,求出反射面19焦距f和w1(13)到反射点6的距离d1(14):S2. According to the following formula, find the distance d1(14) from the focal length f and w1(13) of the
在本实施例中f=97.47,d1=196.19mm;In the present embodiment f=97.47, d1=196.19mm;
S3.确定椭圆25参数:喇叭天线3或太赫兹连续波接收装置11的相位中心位于椭圆25的焦点22处,聚焦波束I(7)的相位中心位于椭圆25的焦点23处;因此,椭圆25的焦点22与反射点6的距离R1(20),椭圆25的焦点23与反射点6的距离R2(21),椭圆25的半长轴a,半短轴b,半焦距c以及椭球面长轴15与入射方向4或反射方向II(9)之间的夹角α可以由关系式表示出:S3. Determine the parameters of the ellipse 25: the phase center of the
a=(R1+R2)/2(5)a=(R 1 +R 2 )/2(5)
其中i=1,2;where i=1,2;
可得R1=212.43mm,R2=180.12mm,α=40.3°,a=196.27mm,b=138.31mm,c=139.26mm。It can be obtained that R1=212.43mm, R2=180.12mm, α=40.3°, a=196.27mm, b=138.31mm, c=139.26mm.
于是,椭球面可由椭圆25沿椭球面长轴15旋转一周得到。确定椭球面参数后,截取椭球面与离轴椭球面反射镜重叠较小的面积部分作为为离轴椭球面反射镜12的反射面19。如图7、8、9和10,在本实施例中,为了保证喇叭天线3所发射的发射波束5的大部分能量被离轴椭球面反射镜12的反射面19反射,取离轴椭球面反射镜12的长度L(27)=210mm,离轴椭球面反射镜12的宽度W(29)=130mm,反射面19的深度d3(28)=17mm;则反射面19的覆盖角度θ(26)≈16.4°,取A=2, Thus, the ellipsoid can be obtained by rotating the
此时,at this time,
因此反射面19的覆盖角度θ(26)满足要求。Therefore, the coverage angle θ(26) of the
将上述光路装置应用于THz-CT-CW成像系统中,其光路FEKO仿真结果如图11所示,可以看出,图3所展示的光路成功实现,并且采用的光学元件也少于图1和图2所采用的光学元件。采用传统的THz-CT-CW成像方式对待测样品进行成像,图12(a)为待测样品示意图,图12(b)采用滤波反投影算法对采集到的某个截面数据进行重建后的结果图,可以看出,基本本发明光路装置,可以实现THz-CT-CW成像系统对杯子边缘和螺钉的轮廓能够重建。Applying the above-mentioned optical path device to the THz-CT-CW imaging system, the FEKO simulation result of the optical path is shown in Figure 11. It can be seen that the optical path shown in Figure 3 is successfully realized, and the number of optical elements used is less than that in Figure 1 and Figure 2 Optical components used. The sample to be tested is imaged using the traditional THz-CT-CW imaging method. Figure 12(a) is a schematic diagram of the sample to be tested, and Figure 12(b) is the result of reconstructing the collected cross-sectional data using the filtered back projection algorithm From the figure, it can be seen that based on the optical path device of the present invention, the THz-CT-CW imaging system can reconstruct the contours of the edge of the cup and the screw.
以上所述,仅为本发明的具体实施方式,本说明书中所公开的任一特征,除非特别叙述,均可被其他等效或具有类似目的的替代特征加以替换;所公开的所有特征、或所有方法或过程中的步骤,除了互相排斥的特征和/或步骤以外,均可以任何方式组合。The above is only a specific embodiment of the present invention. Any feature disclosed in this specification, unless specifically stated, can be replaced by other equivalent or alternative features with similar purposes; all the disclosed features, or All method or process steps may be combined in any way, except for mutually exclusive features and/or steps.
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Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1128063A (en) * | 1993-07-30 | 1996-07-31 | 考金特光学技术公司 | Condensing and collecting optical system using an ellipsoidal reflector |
| CN103308160A (en) * | 2013-06-24 | 2013-09-18 | 中国科学院长春光学精密机械与物理研究所 | Large-relative-aperture wide-view-field miniaturized imaging spectrometer optical system |
| CN109696713A (en) * | 2019-03-01 | 2019-04-30 | 南京大学 | Bifocus Terahertz active imaging system based on Nb5N6 detector |
| CN110411578A (en) * | 2019-08-29 | 2019-11-05 | 河南师范大学 | A low-temperature spectral emissivity measurement device based on an off-axis ellipsoid mirror |
| CN110554512A (en) * | 2019-08-16 | 2019-12-10 | 北京空间机电研究所 | High-precision secondary off-axis ellipsoidal reflector optical axis leading-out method and optical system thereof |
| CN114002160A (en) * | 2021-12-30 | 2022-02-01 | 北京理工大学 | A terahertz frequency modulated continuous wave nondestructive testing imaging system and method |
-
2022
- 2022-08-15 CN CN202210977547.1A patent/CN115494024B/en active Active
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN1128063A (en) * | 1993-07-30 | 1996-07-31 | 考金特光学技术公司 | Condensing and collecting optical system using an ellipsoidal reflector |
| CN103308160A (en) * | 2013-06-24 | 2013-09-18 | 中国科学院长春光学精密机械与物理研究所 | Large-relative-aperture wide-view-field miniaturized imaging spectrometer optical system |
| CN109696713A (en) * | 2019-03-01 | 2019-04-30 | 南京大学 | Bifocus Terahertz active imaging system based on Nb5N6 detector |
| CN110554512A (en) * | 2019-08-16 | 2019-12-10 | 北京空间机电研究所 | High-precision secondary off-axis ellipsoidal reflector optical axis leading-out method and optical system thereof |
| CN110411578A (en) * | 2019-08-29 | 2019-11-05 | 河南师范大学 | A low-temperature spectral emissivity measurement device based on an off-axis ellipsoid mirror |
| CN114002160A (en) * | 2021-12-30 | 2022-02-01 | 北京理工大学 | A terahertz frequency modulated continuous wave nondestructive testing imaging system and method |
Non-Patent Citations (3)
| Title |
|---|
| T. FENG: "Simplifying THz-CT-CW Imaging System Using Vector Network Analyzer and Two Ellipsoid Mirrors", 2022 2ND INTERNATIONAL CONFERENCE ON FRONTIERS OF ELECTRONICS, INFORMATION AND COMPUTATION TECHNOLOGIES (ICFEICT), 28 November 2022 (2022-11-28) * |
| 安红宇: "基于双路微波源的太赫兹连续波快速三维层析成像", 第十七届全国电波传播年会会议论文集, 17 August 2022 (2022-08-17) * |
| 胡伟: "太赫兹扫描光路系统的仿真与分析", 半导体光电, vol. 36, no. 3, 30 March 2015 (2015-03-30) * |
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