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CN103411559B - Based on the accurate confocal microstructure measuring method of angular spectrum scanning of matrix lamp - Google Patents

Based on the accurate confocal microstructure measuring method of angular spectrum scanning of matrix lamp Download PDF

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CN103411559B
CN103411559B CN201310355083.1A CN201310355083A CN103411559B CN 103411559 B CN103411559 B CN 103411559B CN 201310355083 A CN201310355083 A CN 201310355083A CN 103411559 B CN103411559 B CN 103411559B
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angular spectrum
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microstructure
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CN103411559A (en
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刘俭
谭久彬
王宇航
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Harbin Institute of Technology Shenzhen
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Abstract

基于阵列照明的角谱扫描准共焦微结构测量装置与方法属于超精密三维微细结构表面形貌测量领域;该装置设计有角谱扫描照明光路,从LED阵列发出的光束依次经过成像透镜、分光棱镜、显微物镜后,平行照射到被测微结构样品表面,LED阵列中的不同LED对应不同的角谱照明;该方法首先获得所有像素在不同角谱扫描照明下的层析图像,然后利用共焦三维测量原理,判断每个像素的轴向坐标,最后拟合出被测微结构样品的三维形貌;这种设计使被测微结构样品的每一部分都能找到对应的最佳照明角度,避免被测微结构样品自身表面轮廓的高低起伏导致的某些区域无法照明或者发生复杂反射,提高探测信号强度,降低背景噪声,进而提高测量精度。

The angular spectrum scanning quasi-confocal microstructure measurement device and method based on array illumination belong to the field of ultra-precise three-dimensional microstructure surface topography measurement; After the prism and the microscope objective lens, it is irradiated in parallel to the surface of the microstructure sample to be tested, and different LEDs in the LED array correspond to different angular spectrum illuminations; this method first obtains tomographic images of all pixels under different angular spectrum scanning illuminations, and then uses Confocal three-dimensional measurement principle, judging the axial coordinates of each pixel, and finally fitting the three-dimensional shape of the microstructure sample to be tested; this design enables each part of the microstructure sample to be tested to find the corresponding optimal illumination angle , to avoid some areas that cannot be illuminated or complex reflections caused by the ups and downs of the surface profile of the microstructure sample to be measured, improve the detection signal strength, reduce background noise, and improve measurement accuracy.

Description

基于阵列照明的角谱扫描准共焦微结构测量方法Quasi-confocal Microstructure Measurement Method Based on Array Illumination

技术领域 technical field

基于阵列照明的角谱扫描准共焦微结构测量装置与方法属于超精密三维微细结构表面形貌测量领域。 The invention relates to an angular spectrum scanning quasi-confocal microstructure measurement device and method based on array illumination, belonging to the field of ultra-precise three-dimensional microstructure surface topography measurement.

背景技术 Background technique

微结构的加工应用主要体现在微电子技术、微系统技术和微光学技术三个方面,如计算机芯片、生物芯片和微透镜阵列等典型应用。上述技术其共同特征是具有三维结构、功能结构尺寸在微米、亚微米或纳米量级,这种结构的微纳米化不仅仅带来能源与原材料的节省,更推动了现代科技的进步,直接带动了相关产业的发展。随着微加工技术的飞速发展,能够对该类样品进行快速无损三维检测的仪器将拥有巨大的应用前景。 The processing and application of microstructures are mainly reflected in three aspects: microelectronics technology, microsystem technology and micro-optical technology, such as typical applications such as computer chips, biochips and microlens arrays. The common feature of the above-mentioned technologies is that they have a three-dimensional structure, and the size of the functional structure is on the order of micron, submicron or nanometer. development of related industries. With the rapid development of micromachining technology, instruments capable of rapid and non-destructive three-dimensional detection of such samples will have great application prospects.

美国专利US3013467,第一次公开了一种共焦成像技术,该发明通过引入点光源、点照明和点探测三点光学共轭的共焦成像技术,获得了对样品轮廓的轴向探测能力,配合水平方向载物台的移动进而实现三维测量。中国专利CN1395127A,公开了一种共焦显微测量系统。该发明利用共焦技术,通过在共焦光路中引入干涉光路,获得高灵敏度的干涉测量信号,实现对样品轴向的高精度测量。美国专利US6282020B1,公开了一种基于扫描振镜的共焦显微系统。该发明利用共焦原理,通过引入振镜扫描技术,获得了汇聚照明光斑在样品表面高速移动的能力,实现了快速共焦探测,提高了测量速度。但是上述三种方法都是将平行光束通过显微物镜汇聚到样品表面进行照明,当进行三维样品测量时,由于样品自身表面轮廓的高低起伏,对汇聚照明光束进行遮挡,会导致某些区域无法照明或者发生复杂反射,进而造成探测信号强度的衰减和背景噪声的增强,使得测量精度降低,甚至无法测量。 U.S. Patent US3013467 discloses a confocal imaging technology for the first time. This invention obtains the axial detection ability of the sample contour by introducing the confocal imaging technology of the three-point optical conjugation of point light source, point illumination and point detection. Cooperate with the movement of the stage in the horizontal direction to realize three-dimensional measurement. Chinese patent CN1395127A discloses a confocal microscopic measurement system. The invention utilizes confocal technology and introduces an interference optical path into the confocal optical path to obtain a highly sensitive interferometric signal and realize high-precision measurement of the axial direction of the sample. US Patent US6282020B1 discloses a confocal microscope system based on a scanning galvanometer. The invention utilizes the confocal principle and introduces the galvanometer scanning technology to obtain the ability of converging the illumination spot to move at high speed on the sample surface, realize fast confocal detection, and improve the measurement speed. However, the above three methods converge parallel light beams to the surface of the sample for illumination through a microscope objective lens. When measuring a three-dimensional sample, due to the ups and downs of the surface profile of the sample itself, the converged illumination beam is blocked, which will cause some areas to be unavailable. Illumination or complex reflections will cause the attenuation of the detection signal strength and the enhancement of background noise, which will reduce the measurement accuracy or even make it impossible to measure.

发明内容 Contents of the invention

为了解决上述问题,本发明公开了一种基于阵列照明的角谱扫描准共焦微结构测量装置与方法,使被测微结构样品的每一部分都能找到对应的最佳照明角度,避免被测微结构样品自身表面轮廓的高低起伏导致的某些区域无法照明或者发生复杂反射,提高探测信号强度,降低背景噪声,进而提高测量精度。 In order to solve the above problems, the present invention discloses a quasi-confocal microstructure measurement device and method based on array illumination, so that each part of the microstructure sample to be measured can find the corresponding optimal illumination angle, avoiding the Some areas cannot be illuminated or undergo complex reflections due to the ups and downs of the surface profile of the microstructure sample itself, which improves the detection signal strength, reduces background noise, and improves measurement accuracy.

本发明的目的是这样实现的: The purpose of the present invention is achieved like this:

基于阵列照明的角谱扫描准共焦微结构测量装置,包括角谱扫描照明光路和准共焦测量光路; An angular spectrum scanning quasi-confocal microstructure measurement device based on array illumination, including an angular spectrum scanning illumination optical path and a quasi-confocal measurement optical path;

所述的角谱扫描照明光路包括:LED阵列、成像透镜、分光棱镜、第一光阑和显微物镜;从LED阵列发出的光束依次经过成像透镜、分光棱镜、显微物镜后,平行照射到随载物台轴向移动的被测微结构样品表面; The described angular spectrum scanning illumination optical path comprises: LED array, imaging lens, dichroic prism, first aperture and microscopic objective lens; After the light beam sent from LED array passes through imaging lens, dichroic prism and microscopic objective lens in turn, it is irradiated in parallel to The surface of the microstructure sample to be measured moves axially with the stage;

所述的准共焦测量光路包括:载物台、显微物镜、第一光阑、分光棱镜、管镜、第二光阑、扫描透镜、二维扫描振镜、聚焦透镜、针孔和探测器;随载物台轴向移动的被测微结构样品表面反射的光束依次经过显微物镜、第一光阑、分光棱镜、管镜、第二光阑、扫描透镜、二维扫描振镜、聚焦透镜,成像到针孔位置,并由探测器成像;所述的二维扫描振镜在其所在平面或与其平行平面内,以相互垂直的两个方向为转轴,进行二维转动; The quasi-confocal measurement optical path includes: stage, microscope objective lens, first aperture, dichroic prism, tube mirror, second aperture, scanning lens, two-dimensional scanning galvanometer, focusing lens, pinhole and detection The light beam reflected by the surface of the microstructure sample that moves axially with the stage passes through the microscope objective lens, the first aperture, the beam splitting prism, the tube lens, the second aperture, the scanning lens, the two-dimensional scanning galvanometer, The focusing lens is imaged to the position of the pinhole and imaged by the detector; the two-dimensional scanning galvanometer performs two-dimensional rotation on the plane where it is located or in a plane parallel to it, with two directions perpendicular to each other as rotation axes;

所述的角谱扫描照明光路和准共焦测量光路共用分光棱镜、第一光阑和显微物镜; The angular spectrum scanning illumination light path and the quasi-confocal measurement light path share a dichroic prism, a first diaphragm and a microscope objective lens;

所述的LED阵列位于成像透镜的物平面,成像透镜的像平面与显微物镜的后焦平面重合于第一光阑所在平面;管镜的前焦平面与扫描透镜的后焦平面重合于第二光阑所在平面;针孔位于聚焦透镜的前焦平面,与探测器紧贴。 The LED array is located on the object plane of the imaging lens, and the image plane of the imaging lens coincides with the rear focal plane of the microscope objective lens on the plane where the first diaphragm is located; the front focal plane of the tube mirror coincides with the rear focal plane of the scanning lens on the second The plane where the second diaphragm is located; the pinhole is located at the front focal plane of the focusing lens, and is close to the detector.

上述基于阵列照明的角谱扫描准共焦微结构测量装置,所述的LED阵列为水平竖直方向排布或与水平方向成45°和135°两个方向排布。 In the aforementioned angular spectrum scanning quasi-confocal microstructure measurement device based on array illumination, the LED arrays are arranged in horizontal and vertical directions or in two directions at 45° and 135° to the horizontal direction.

所述的LED阵列为等间距排布或不等间距排布。 The LED arrays are arranged at equal intervals or at unequal intervals.

上述基于阵列照明的角谱扫描准共焦微结构测量装置,在二维扫描振镜背离光束传播的方向,设置有十字轴或球笼式万向节。 The above-mentioned angle-spectrum scanning quasi-confocal microstructure measurement device based on array illumination is provided with a cross axis or a spherical cage type universal joint in the direction that the two-dimensional scanning galvanometer deviates from the beam propagation direction.

基于阵列照明的角谱扫描准共焦微结构测量方法,包括以下步骤: The angular spectrum scanning quasi-confocal microstructure measurement method based on array illumination comprises the following steps:

步骤a、将被测微结构样品的厚度分为N层; Step a, dividing the thickness of the tested microstructure sample into N layers;

步骤b、设定二维扫描振镜共有P个空间位置; Step b, setting a total of P spatial positions for the two-dimensional scanning galvanometer;

所述的步骤a、步骤b的顺序可调换; The order of described step a, step b can be exchanged;

步骤c、根据LED阵列中的LED数量M,被测微结构样品的厚度分层N,二维扫描振镜的空间位置P,形成M×N张角谱照明图像,每张角谱照明图像像素个数为P; Step c. According to the number M of LEDs in the LED array, the thickness layer N of the microstructure sample to be tested, and the spatial position P of the two-dimensional scanning galvanometer, M×N angular spectrum illumination images are formed, and each angular spectrum illumination image pixel The number is P;

步骤d、定义相同角谱下的不同层之间的角谱照明图像为层析图像,对比相同空间位置在M个角谱照明下的层析图像之间的轴向包络曲线,挑选出最接近sinc函数四次方的包络曲线,根据共焦三维测量原理,判断P个空间位置点的轴向坐标; Step d, define the angular spectrum illumination images between different layers under the same angular spectrum as tomographic images, compare the axial envelope curves between the tomographic images at the same spatial position under M angular spectrum illuminations, and select the best The envelope curve close to the fourth power of the sinc function, according to the principle of confocal three-dimensional measurement, judge the axial coordinates of P spatial position points;

步骤e、根据P个空间位置点及其轴向坐标,拟合出被测微结构样品的三维形貌。 Step e, fitting the three-dimensional shape of the microstructure sample to be tested according to the P spatial position points and their axial coordinates.

上述基于阵列照明的角谱扫描准共焦微结构测量方法,所述的步骤c具体为: In the method for measuring the quasi-confocal microstructure based on array illumination, the described step c is specifically:

步骤c1:通过载物台调整被测微结构样品,使N层中的每一层依次置于显微物镜的前焦平面; Step c1: adjusting the microstructure sample to be tested through the stage, so that each layer in the N layers is placed in the front focal plane of the microscope objective lens in turn;

步骤c2:通过依次点亮LED阵列中的M个LED形成对被测微结构样品的M个角谱照明; Step c2: M LEDs in the LED array are sequentially turned on to form M angular spectrum illuminations for the microstructure sample to be tested;

步骤c3:通过调整二维扫描振镜的P个空间位置,实现探测器对照明图像的采集; Step c3: by adjusting the P spatial positions of the two-dimensional scanning galvanometer, the acquisition of the illumination image by the detector is realized;

所述步骤c1、步骤c2、步骤c3形成三重循环,从外到内的循环顺序依次为以下顺序中的一个: The step c1, step c2, and step c3 form a triple cycle, and the cycle sequence from outside to inside is one of the following sequences:

步骤c1、步骤c2、步骤c3; Step c1, step c2, step c3;

步骤c1、步骤c3、步骤c2; Step c1, step c3, step c2;

步骤c2、步骤c1、步骤c3; Step c2, step c1, step c3;

步骤c2、步骤c3、步骤c1; Step c2, step c3, step c1;

步骤c3、步骤c1、步骤c2; Step c3, step c1, step c2;

步骤c3、步骤c2、步骤c1; Step c3, step c2, step c1;

最终形成M×N张角谱照明图像,每张角谱照明图像像素个数为P。 Finally, M×N angular spectrum illumination images are formed, and the number of pixels in each angular spectrum illumination image is P.

由于本发明设计有照明光路,使照明光束平行入射到被测微结构样品表面,并且通过点亮LED阵列中的不同LED来改变照明光束的照射角度,并利用共焦三维测量原理,拟合出被测微结构样品的三维形貌;这种设计使被测微结构样品的每一部分都能找到对应的最佳照明角度,避免被测微结构样品自身表面轮廓的高低起伏导致的某些区域无法照明或者发生复杂反射,提高探测信号强度,降低背景噪声,进而提高测量精度。 Since the present invention is designed with an illumination optical path, the illumination beam is incident on the surface of the microstructure sample in parallel, and the illumination angle of the illumination beam is changed by lighting different LEDs in the LED array, and the confocal three-dimensional measurement principle is used to fit the The three-dimensional shape of the microstructure sample to be tested; this design enables each part of the microstructure sample to be tested to find the corresponding optimal lighting angle, avoiding the undulation of the surface profile of the microstructure sample itself. Illumination or complex reflections can increase the detection signal strength and reduce background noise, thereby improving measurement accuracy.

附图说明 Description of drawings

图1是本发明基于阵列照明的角谱扫描准共焦微结构测量装置结构示意图。 Fig. 1 is a schematic diagram of the structure of the angular spectrum scanning quasi-confocal microstructure measurement device based on the array illumination of the present invention.

图2是本发明基于阵列照明的角谱扫描准共焦微结构测量装置角谱扫描照明光路图。 Fig. 2 is a diagram of the angular spectrum scanning illumination light path of the angular spectrum scanning quasi-confocal microstructure measurement device based on the array illumination of the present invention.

图3是本发明基于阵列照明的角谱扫描准共焦微结构测量装置准共焦测量光路图。 Fig. 3 is a diagram of the quasi-confocal measurement light path of the angular spectrum scanning quasi-confocal microstructure measurement device based on the array illumination of the present invention.

图4是本发明基于阵列照明的角谱扫描准共焦微结构测量方法流程图。 Fig. 4 is a flow chart of the method for measuring quasi-confocal microstructures based on array illumination in the present invention.

图中:1LED阵列、2成像透镜、3分光棱镜、4第一光阑、5显微物镜、6载物台、7管镜、8第二光阑、9扫描透镜、10二维扫描振镜、11聚焦透镜、12针孔、13探测器。 In the figure: 1LED array, 2 imaging lens, 3 dichroic prism, 4 first aperture, 5 microscope objective lens, 6 stage, 7 tube mirror, 8 second aperture, 9 scanning lens, 10 two-dimensional scanning galvanometer , 11 focusing lenses, 12 pinholes, 13 detectors.

具体实施方式 Detailed ways

下面结合附图对本发明具体实施方式作进一步详细描述。 The specific embodiments of the present invention will be further described in detail below in conjunction with the accompanying drawings.

所谓角谱扫描照明,是以平行光束照明被测微结构样品表面并且通过扫描机构或其它技术手段实现连续改变或离散改变平行光的入射角度,该种照明方式在频域中的描述即为角谱扫描照明。 The so-called angular spectrum scanning illumination is to illuminate the surface of the microstructure sample to be measured with a parallel beam and realize continuous or discrete change of the incident angle of the parallel light through a scanning mechanism or other technical means. The description of this illumination method in the frequency domain is the angle Spectrum scanning illumination.

共焦测量方法是:利用点照明、点物和点探测三点光学共轭的方法实现光轴方向的测量能力,进而完成三维测量。本专利中提到的准共焦测量方法是:利用角谱扫描照明代替点照明,同时保留点物和点探测两点光学共轭的方法。该方法既保留了共焦测量的三维测量能力,同时引入角谱扫描照明,提高探测信号强度,降低背景噪声,进而提高测量精度。 The confocal measurement method is to use the three-point optical conjugate method of point illumination, point object and point detection to realize the measurement ability of the optical axis direction, and then complete the three-dimensional measurement. The quasi-confocal measurement method mentioned in this patent is: use angular spectrum scanning illumination instead of point illumination, while retaining the optical conjugate of point object and point detection. This method not only retains the three-dimensional measurement capability of confocal measurement, but also introduces angular spectrum scanning illumination to improve the detection signal strength, reduce background noise, and improve measurement accuracy.

具体实施例一: Specific embodiment one:

本实施例的基于阵列照明的角谱扫描准共焦微结构测量装置结构示意图如图1所示,角谱扫描照明光路图如图2所示,准共焦测量光路图如图3所示。 Figure 1 shows the structural diagram of the angular spectrum scanning quasi-confocal microstructure measurement device based on array illumination in this embodiment, Figure 2 shows the angular spectrum scanning illumination light path, and Figure 3 shows the quasi-confocal measurement light path.

该测量装置包括角谱扫描照明光路和准共焦测量光路; The measurement device includes an angular spectrum scanning illumination optical path and a quasi-confocal measurement optical path;

所述的角谱扫描照明光路包括:LED阵列1、成像透镜2、分光棱镜3、第一光阑4和显微物镜5;从LED阵列1发出的光束依次经过成像透镜2、分光棱镜3、显微物镜5后,平行照射到随载物台6轴向移动的被测微结构样品表面; The described angular spectrum scanning illumination light path includes: LED array 1, imaging lens 2, dichroic prism 3, first aperture 4 and microscopic objective lens 5; Behind the microscope objective lens 5, parallel irradiation is carried out to the surface of the microstructure sample to be measured which moves axially with the stage 6;

所述的准共焦测量光路包括:载物台6、显微物镜5、第一光阑4、分光棱镜3、管镜7、第二光阑8、扫描透镜9、二维扫描振镜10、聚焦透镜11、针孔12和探测器13;随载物台6轴向移动的被测微结构样品表面反射的光束依次经过显微物镜5、第一光阑4、分光棱镜3、管镜7、第二光阑8、扫描透镜9、二维扫描振镜10、聚焦透镜11,成像到针孔12位置,并由探测器13成像;所述的二维扫描振镜10在其所在平面或与其平行平面内,以相互垂直的两个方向为转轴,进行二维转动; The quasi-confocal measurement optical path includes: a stage 6, a microscope objective lens 5, a first aperture 4, a dichroic prism 3, a tube lens 7, a second aperture 8, a scanning lens 9, and a two-dimensional scanning galvanometer 10 , focusing lens 11, pinhole 12 and detector 13; The light beam reflected by the surface of the measured microstructure sample that moves axially with the stage 6 passes through the microscopic objective lens 5, the first diaphragm 4, the beam splitting prism 3, the tube mirror in sequence 7. The second diaphragm 8, the scanning lens 9, the two-dimensional scanning vibrating mirror 10, and the focusing lens 11 are imaged to the position of the pinhole 12 and imaged by the detector 13; Or in a plane parallel to it, take the two directions perpendicular to each other as the rotation axis to perform two-dimensional rotation;

所述的角谱扫描照明光路和准共焦测量光路共用分光棱镜3、第一光阑4和显微物镜5; The angular spectrum scanning illumination light path and the quasi-confocal measurement light path share the dichroic prism 3, the first diaphragm 4 and the microscope objective lens 5;

所述的LED阵列1为水平竖直方向等间距排布,且位于成像透镜2的物平面,图1中的LED阵列1的上方绘制了LED阵列1的左视图;成像透镜2的像平面与显微物镜5的后焦平面重合于第一光阑4所在平面;管镜7的前焦平面与扫描透镜9的后焦平面重合于第二光阑8所在平面;针孔12位于聚焦透镜11的前焦平面,与探测器13紧贴。 The LED array 1 is arranged at equal intervals in the horizontal and vertical directions, and is positioned at the object plane of the imaging lens 2, and the left view of the LED array 1 is drawn above the LED array 1 in Fig. 1; the image plane of the imaging lens 2 and The rear focal plane of the microscope objective lens 5 coincides with the plane where the first diaphragm 4 is located; the front focal plane of the tube mirror 7 and the rear focal plane of the scanning lens 9 coincide with the plane where the second diaphragm 8 is located; the pinhole 12 is located at the plane of the focusing lens 11 The front focal plane is close to the detector 13.

上述基于阵列照明的角谱扫描准共焦微结构测量装置,在二维扫描振镜10背离光束传播的方向,设置有电动十字轴,实现对二维扫描振镜10空间位置的控制。 The above-mentioned angular spectrum scanning quasi-confocal microstructure measurement device based on array illumination is provided with a motorized cross axis in the direction that the two-dimensional scanning galvanometer 10 deviates from the beam propagation direction, so as to realize the control of the spatial position of the two-dimensional scanning galvanometer 10 .

本实施例的基于阵列照明的角谱扫描准共焦微结构测量方法流程图如图4所示,该方法包括以下步骤: The flow chart of the method for measuring the quasi-confocal microstructure based on array illumination and angular spectrum scanning in this embodiment is shown in Figure 4. The method includes the following steps:

步骤a、将被测微结构样品的厚度分为N层; Step a, dividing the thickness of the tested microstructure sample into N layers;

步骤b、设定二维扫描振镜10共有P个空间位置; Step b, setting the two-dimensional scanning galvanometer 10 to have a total of P spatial positions;

步骤c、根据LED阵列1中的LED数量M,被测微结构样品的厚度分层N,二维扫描振镜10的空间位置P,形成M×N张角谱照明图像,每张角谱照明图像像素个数为P; Step c, according to the number M of LEDs in the LED array 1, the thickness layer N of the microstructure sample to be tested, and the spatial position P of the two-dimensional scanning galvanometer 10, M×N angular spectrum illumination images are formed, and each angular spectrum illumination The number of image pixels is P;

步骤d、定义相同角谱下的不同层之间的角谱照明图像为层析图像,对比相同空间位置在M个角谱照明下的层析图像之间的轴向包络曲线,挑选出最接近sinc函数四次方的包络曲线,根据共焦三维测量原理,判断该空间位置点的轴向坐标; Step d, define the angular spectrum illumination images between different layers under the same angular spectrum as tomographic images, compare the axial envelope curves between the tomographic images at the same spatial position under M angular spectrum illuminations, and select the best The envelope curve close to the fourth power of the sinc function, according to the principle of confocal three-dimensional measurement, judge the axial coordinates of the spatial position point;

步骤e、根据P个空间位置点及其轴向坐标,拟合出被测微结构样品的三维形貌。 Step e, fitting the three-dimensional shape of the microstructure sample to be tested according to the P spatial position points and their axial coordinates.

其中步骤c具体为: Wherein step c is specifically:

步骤c1:通过载物台6调整被测微结构样品,使N层中的每一层依次置于显微物镜5的前焦平面; Step c1: adjust the microstructure sample to be measured through the stage 6, so that each layer in the N layers is placed in the front focal plane of the microscope objective lens 5 in sequence;

步骤c2:通过依次点亮LED阵列1中的M个LED形成对被测微结构样品的M个角谱照明; Step c2: M LEDs in the LED array 1 are sequentially turned on to form M angular spectrum illuminations for the microstructure sample to be tested;

步骤c3:通过调整二维扫描振镜10的P个空间位置,实现探测器13对照明图像的采集; Step c3: by adjusting the P spatial positions of the two-dimensional scanning galvanometer 10, the acquisition of the illumination image by the detector 13 is realized;

所述步骤c1、步骤c2、步骤c3形成三重循环,从外到内的循环顺序依次为:步骤c1、步骤c3、步骤c2。 The step c1, step c2, and step c3 form a triple cycle, and the order of the cycle from outside to inside is: step c1, step c3, and step c2.

具体实施例二: Specific embodiment two:

本实施例与具体实施例一不同在于,所述的基于阵列照明的角谱扫描准共焦微结构测量装置中,LED阵列1为水平竖直方向不等间距排布,其有益效果在于可以在该方向对某个照明角谱范围内更精确调整。 The difference between this embodiment and the specific embodiment 1 is that in the described angular spectrum scanning quasi-confocal microstructure measurement device based on array illumination, the LED array 1 is arranged at unequal intervals in the horizontal and vertical directions, and its beneficial effect is that it can be The direction is adjusted more precisely within a certain range of illumination angle spectrum.

具体实施例三: Specific embodiment three:

本实施例与具体实施例一不同在于,所述的基于阵列照明的角谱扫描准共焦微结构测量装置中,LED阵列1为与水平方向成45°和135°两个方向等间距排布,其有益效果在于可以在该方向对角谱均匀调整。 The difference between this embodiment and the specific embodiment 1 is that in the described angular spectrum scanning quasi-confocal microstructure measurement device based on array illumination, the LED arrays 1 are arranged at equal intervals in two directions of 45° and 135° from the horizontal direction. , the beneficial effect is that the diagonal spectrum can be uniformly adjusted in this direction.

具体实施例四: Specific embodiment four:

本实施例与具体实施例一不同在于,所述的基于阵列照明的角谱扫描准共焦微结构测量装置中,LED阵列1为与水平方向成45°和135°两个方向不等间距排布,其有益效果在于可以在该方向对某个照明角谱范围内更精确调整。 The difference between this embodiment and the specific embodiment 1 is that in the array illumination-based angular spectrum scanning quasi-confocal microstructure measurement device, the LED array 1 is arranged at unequal distances in two directions of 45° and 135° from the horizontal direction. The beneficial effect is that the direction can be adjusted more precisely within a certain range of illumination angle spectrum.

具体实施例五: Specific embodiment five:

本实施例与具体实施例一不同在于,所述的基于阵列照明的角谱扫描准共焦微结构测量方法中,步骤c优选三重循环的顺序为步骤c3、步骤c1、步骤c2;使执行速度最快的步骤c2放置在最内层,执行速度最慢的步骤c3放置在最外层,可以减小角谱照明图像的用时,提高被测微结构样品的三维形貌重构效率。 The difference between this embodiment and the specific embodiment 1 is that in the array illumination-based angle-spectrum scanning quasi-confocal microstructure measurement method, step c is preferably in the order of three cycles of step c3, step c1, and step c2; the execution speed The fastest step c2 is placed in the innermost layer, and the slowest step c3 is placed in the outermost layer, which can reduce the time spent on the angular spectrum illumination image and improve the three-dimensional shape reconstruction efficiency of the microstructure sample under test.

Claims (2)

1., based on the accurate confocal microstructure measuring method of angular spectrum scanning of matrix lamp, the device used comprises angular spectrum scanning illumination path and accurate confocal measurement light path;
Described angular spectrum scanning illumination path comprises: LED array (1), imaging len (2), Amici prism (3), the first diaphragm (4) and microcobjective (5); The light beam sent from LED array (1) is successively after imaging len (2), Amici prism (3), microcobjective (5), and parallel radiation is to the tested microstructure sample surface moved axially with objective table (6);
Described accurate confocal measurement light path comprises: objective table (6), microcobjective (5), the first diaphragm (4), Amici prism (3), Guan Jing (7), the second diaphragm (8), scanning lens (9), two-dimensional scanning mirrors (10), condenser lens (11), pin hole (12) and detector (13); The light beam of the tested microstructure sample surface reflection moved axially with objective table (6) is successively through microcobjective (5), the first diaphragm (4), Amici prism (3), Guan Jing (7), the second diaphragm (8), scanning lens (9), two-dimensional scanning mirrors (10), condenser lens (11), be imaged onto pin hole (12) position, and by detector (13) imaging; Described two-dimensional scanning mirrors (10), in its place plane or plane in parallel, with orthogonal both direction for rotating shaft, carries out two-dimensional rotary;
Described angular spectrum scanning illumination path and accurate confocal measurement light path share Amici prism (3), the first diaphragm (4) and microcobjective (5);
Described LED array (1) is positioned at the object plane of imaging len (2), and the picture plane of imaging len (2) and the back focal plane of microcobjective (5) coincide with the first diaphragm (4) place plane; The front focal plane of Guan Jing (7) and the back focal plane of scanning lens (9) coincide with the second diaphragm (8) place plane; Pin hole (12) is positioned at the front focal plane of condenser lens (11), is close to detector (13);
Described LED array (1) is for horizontal vertical direction arrangement or from the horizontal by 45 ° and 135 ° of both direction arrangements;
Described LED array (1) is equidistantly arrangement or unequal-interval arrangement;
Deviate from the direction of beam propagation at two-dimensional scanning mirrors (10), be provided with joint spider or rzeppa joint;
It is characterized in that: said method comprising the steps of:
Step a, the thickness of tested microstructure sample is divided into N layer;
Step b, total P the locus of setting two-dimensional scanning mirrors (10);
The order interchangeable of described step a, step b;
Step c, according to the LED quantity M in LED array (1), the thickness layering N of tested microstructure sample, the locus P of two-dimensional scanning mirrors (10), form M × N subtended angle spectrum illumination image, and every subtended angle spectrum illumination image number of pixels is P;
Steps d, the angular spectrum illumination image defining under identical angular spectrum between different layers are tomographic map, axial envelope curve between the tomographic map of contrast same spatial location under M angular spectrum illumination, pick out closest to the quadruplicate enveloping curve of sinc function, according to confocal three-dimensional measurement principle, judge the axial coordinate of P locus point;
Step e, according to P locus point and axial coordinate thereof, simulate the three-dimensional appearance of tested microstructure sample.
2. the accurate confocal microstructure measuring method of the scanning of the angular spectrum based on matrix lamp according to claim 1, is characterized in that: described step c is specially:
Step c1: adjust tested microstructure sample by objective table (6), makes the every one deck in N layer be placed in the front focal plane of microcobjective (5) successively;
Step c2: form M the angular spectrum illumination to tested microstructure sample by M the LED lighted successively in LED array (1);
Step c3: by P locus of adjustment two-dimensional scanning mirrors (10), realize detector (13) to the collection of illumination image;
Described step c1, step c2, step c3 form three and recirculate, and circular order is from outside to inside followed successively by one in following order:
Step c1, step c2, step c3;
Step c1, step c3, step c2;
Step c2, step c1, step c3;
Step c2, step c3, step c1;
Step c3, step c1, step c2;
Step c3, step c2, step c1;
Final formation M × N subtended angle spectrum illumination image, every subtended angle spectrum illumination image number of pixels is P.
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