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WO2004081493A1 - Method of measuring accurate parallelism - Google Patents

Method of measuring accurate parallelism Download PDF

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Publication number
WO2004081493A1
WO2004081493A1 PCT/CN2003/000245 CN0300245W WO2004081493A1 WO 2004081493 A1 WO2004081493 A1 WO 2004081493A1 CN 0300245 W CN0300245 W CN 0300245W WO 2004081493 A1 WO2004081493 A1 WO 2004081493A1
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WIPO (PCT)
Prior art keywords
measured object
reference plane
measured
plane
rotation
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PCT/CN2003/000245
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French (fr)
Chinese (zh)
Inventor
Zaili Dong
Jun Wang
Yingming Hao
Feng Zhu
Jinjun Ou
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Shenyang Institute of Automation of CAS
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Shenyang Institute of Automation of CAS
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Priority to AU2003236107A priority Critical patent/AU2003236107A1/en
Publication of WO2004081493A1 publication Critical patent/WO2004081493A1/en
Anticipated expiration legal-status Critical
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B11/00Measuring arrangements characterised by the use of optical techniques
    • G01B11/26Measuring arrangements characterised by the use of optical techniques for measuring angles or tapers; for testing the alignment of axes

Definitions

  • the invention relates to measurement technology, and in particular to a precise parallelism measurement method. Background technique
  • Precision parallelism measurement is a key technology for precision (sub-micron) inspection and attitude adjustment operations in the large-scale integrated circuit (IC) manufacturing industry.
  • IC integrated circuit
  • Traditional methods use precision distance sensors (such as capacitive, optical ranging, and electromagnetic methods) to measure the distance from the measured plane (such as a wafer, defined as M) to a reference plane (such as a template mounting plane, defined as W).
  • M the measured plane
  • W a template mounting plane
  • the object of the present invention is to provide a precise parallelism measurement method that can accurately reflect the parallel relationship between the measured object and the reference plane and adjust the accuracy ⁇ , that is, a method for measuring the relative parallelism between the flat surface of the measured object and the reference plane.
  • the specific technical solution of the present invention is: Let M be the measured object, W be the reference plane, Z be the rotation axis, and mount the measured object M on a platform having a rotation axis Z, which can be rotated around the rotation axis Z Rotate, the axis of rotation Z is perpendicular to the reference plane W; Equipped with a beam of light and a camera as a measuring device, the camera lens is aimed at the side of the object M to be imaged by the reflected light that can be received and projected on the side of the object M ; Let the horizontal axis u and the vertical axis V be the image coordinate system after imaging, and the origin point is at the center of the imaged image, where the intersection point between the upper or lower plane of the measured object M and its side through the vertical axis V is on the side of the measured object M; Detection point A of the image; When the measured object M rotates about the rotation axis Z, through continuous image acquisition, the image position measurement value of the
  • the detection position of the detection point A is a discrete quantity that changes approximately continuously; when the measured object M and the reference plane W are not When parallel, the position detection value of the detection point A will show an offset change curve during the rotation period.
  • the curve measured during the rotation period is approximately parallel and straight, the two planes, namely the measured object M plane and the reference plane W, are approximately parallel;
  • the offset change curve quantitatively reflects the angular position of the non-parallel amplitude and the maximum deviation amplitude of the measured object M plane and the reference plane W, and the vertical axis of the offset change curve indicates that the measured object M has a rotation angle of ⁇
  • the X represents the maximum inclination
  • the horizontal axis represents the rotation angle ⁇ , where Y is the angle ⁇ rotated relative to the starting position of rotation at the maximum inclination X
  • the reference plane may be located above the measured object M Or below.
  • the present invention can detect the non-parallelism of the measured object (such as a wafer) relative to the reference system as a whole, so it has a more obvious technical advantage than the existing technology, that is, : Can accurately reflect the parallel relationship between the measured object and the reference plane, at the same time easy to operate, and also has achievability.
  • the present invention is an optical measurement method, which is not only free of electromagnetic pollution (such as electromagnetic interference), but also has high adjustment accuracy.
  • the measurement accuracy depends on the image resolution and can reach more than 0.1 micron.
  • the present invention is based on the optical imaging position measurement method, and realizes the parallelism detection between two planes, that is, the measured plane and the reference plane on the sub-micron level, so as to achieve ultra-precision positioning detection during IC processing and improve IC.
  • the integrated circuit processing level and integration further improve the existing IC processing technology. Attached picture
  • Figure 1 shows the measurement principle and measurement structure.
  • Fig. 2 is a reflection image of the side of the wafer which enables the camera to receive the illumination light source.
  • Fig. 3 is a graph showing the change in the displacement of the position detection value of the imaging detection point A on the side of the measured plane M in the rotation period.
  • M be the measured object
  • W be the reference plane
  • Z be the rotation axis.
  • the measured object M is mounted on a platform with a rotation axis Z and can be rotated about the rotation axis Z.
  • the rotation axis Z and The reference plane W is vertical; it is equipped with a beam of illumination light source and a camera (a CCD camera is used in this embodiment) as a measuring device, so that the camera lens is aligned with the side of the object M to be measured.
  • Reflective imaging that is, the imaging of the reflected light projected on the side of the measured object on the camera; set the horizontal axis 11 and the vertical axis V as the image coordinate system after imaging, and the origin is at the center of the image after imaging, where the measured object M is below versus The intersection point A whose side passes through the vertical axis v is the detection point of the side image of the measured object M; when the measured object M rotates around the rotation axis Z, continuous image acquisition is used to describe the image position measurement value of the detection point A
  • the parallel state of the plane of the measured object M with respect to the reference plane W so as to determine the non-parallelism and the adjusted position of the measured object M with respect to the reference plane W;
  • the detection position of the detection point A is a discrete quantity that changes approximately continuously; when the measured object M is not parallel to the reference plane W , The position detection value of the detection point A will show an offset change curve during the rotation period.
  • the curve measured in a rotation period is approximately parallel straight lines, the two planes are the measured object M plane and the reference.
  • the plane W is approximately parallel;
  • the offset change curve quantitatively reflects the angular position of the non-parallel amplitude and the maximum deviation amplitude of the plane of the measured object M and the reference plane W, and the vertical axis of the offset change curve represents the measured position of the measured object M when the rotation angle is ⁇ .
  • the inclination amplitude where X represents the maximum inclination amplitude; the horizontal axis represents the rotation angle 6, and Y represents the angle ⁇ that has been rotated relative to the starting position of rotation at the maximum inclination amplitude X.
  • the specific operation of the parallelism measuring method is as follows: the measured object M is rotated around the rotation axis Z axis, and the CCD is used to continuously acquire images, and the image position of the imaging detection point A on the side of the measured object M is detected as a continuous image;
  • the detection position of the detection point A is a discrete quantity that changes approximately continuously;
  • the measured object M is not parallel to the reference plane W, The position detection value of the detection point A will show an offset change curve during the rotation period, see FIG. 3 (FIG.
  • the vertical axis indicates that the measured object is at The inclination amplitude when the rotation angle is ⁇ represents the required adjustment amount;
  • X is the maximum inclination amplitude of the measured plane M relative to the reference plane W;
  • the horizontal axis is the rotation angle ⁇ , which represents the position to be adjusted in the measured plane M;
  • Y is the rotation angle ⁇ at the detection point A).
  • the measured object M is a wafer, and it is mounted on a rotating shaft.
  • the rotation axis Z is perpendicular to a given reference plane W.
  • a mask is installed on the reference plane W.
  • the reference plane W is parallel to the template, if the measured object M and the reference plane W can be measured, The flatness and the attitude between the two can be adjusted as required.
  • the detection accuracy depends on the position resolution of the measurement system.
  • Measurement imaging mechanism Let M be the measured object, W be the reference plane, and Z be the rotation perpendicular to the reference plane W Rotation axis, the measured object M can rotate around the rotation axis Z axis.
  • W be the reference plane
  • Z be the rotation perpendicular to the reference plane W
  • the measured object M can rotate around the rotation axis Z axis.
  • A (the intersection point of the lower plane of the measured object M and its side passing the V axis) is the detection point defined on the side of the measured object M
  • u and V are image coordinate systems
  • 5 is the side of the measured plane M Imaging in the reflection domain, 6 for background domain imaging.
  • the core idea of the present invention is to describe the parallel state of the plane of the measured object M with respect to the reference plane W by measuring the image position measurement value of the detection point A, including the inclination width and the maximum inclination distance from the starting position.
  • the rotation angle determines the non-parallelism of M and W and the adjustment position.
  • the resolution of the CCD is 1000, and the magnification of the lens is 50.
  • the rotation angle ⁇ is determined.
  • the detection accuracy of the non-parallelism of the present invention depends on the image resolution.
  • the image resolution is less than micron (sub-micron)
  • the non-parallel state reflected by the measurement curve of the detection point A can be achieved.
  • Sub-micron level Since the field of view of the CCD can be designed to include only the area near the detection point A, the magnification of the lens can also be sufficiently large, so the image resolution can be sufficiently high, and theoretically the limit of the combination of the lens and the CCD resolution can be reached. In this way, when the resolution of the CCD imaging system is sufficiently high, precise measurement of the non-parallelism of the measured object M and the reference plane W can be achieved.
  • a linear high-resolution CCD camera can be used, and the magnification of the lens can be taken as required. After image processing, it can meet the measurement accuracy of 0.1 micron or more. Noise signal will appear on the measurement curve of the position of detection point A due to noise (caused by the unevenness of the boundary between the wafer surface and the side) at the measured edge. Therefore, technical processing such as smoothing filtering (conventional technology) needs to be added to correctly obtain The accurate position measurement curve of the detection point A, so as to accurately give non-parallel parameters for mechanism adjustment.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Length Measuring Devices By Optical Means (AREA)
  • Testing Or Measuring Of Semiconductors Or The Like (AREA)

Abstract

The present invention relates to a measuring technique and especially relates to a method of accurately measuring the parallelism. The method is used to measure the relative parallelism which a flat surface of measured object M opposite to a reference plane W. Firstly, the measured object M is installed on a platform having rotating axis Z. The rotating axis Z is perpendicular to with the reference plane W; A measuring apparatus comprise a optical source 1 and a camera 2 so that the lens 3 of the camera 2 aligns the side surface of said measured object to imaged a reflecting beam from which projected to the side surface of said measured object M; A lateral coordinate axis u and a longitudinal coordinate axis u are a image's coordinate system of formed image. An origin of the coordinate system is defined at the center of the formed image. The measured point is the point that the higher or lower surface of said measured object intersect with its side face of throgh the longitudinal coordinate axis v; When said measured object M rotated around the rotating axis, the parallel state of the surface of said measured object M was depict relatively that of the reference plane by detecting the position of image of measured point on the successive survey, so that determined non parallelism and adjusted position of said measured object M relative to the reference plane W. The invention can depict the parallel relationship between said measured object M with reference plane W and having high adjusting precision.

Description

一种精密平行度测量方法 技术领域  TECHNICAL FIELD

本发明涉及测量技术, 具体地说是一种精密平行度测量方法。 背景技术  The invention relates to measurement technology, and in particular to a precise parallelism measurement method. Background technique

精密平行度测量是用于大规模集成电路 (IC)制造业精密 (亚微米级)检测与姿 态调整作业的关键技术。 典型 IC加工中存在的模板(mask)与晶片(wafer)平行定 位工艺, 在定位完成之后, 对晶片进行曝光加工。传统方法采用精密距离传感器(如 采用电容法、 光学测距法、 电磁法等结构)只能测量被测平面 (如晶片, 定义为 M) 距离参考平面 (如模板安装平面, 定义为 W) 的有限几个位置的相对距离量, 当晶 片表面平整度无法髙于要求测量的精度时,这些测量点的测量数据就无法在更高技术 要求水平上正确反映 M与 W之间的平行关系, 从而限制了 IC加工的精度。 发明内容  Precision parallelism measurement is a key technology for precision (sub-micron) inspection and attitude adjustment operations in the large-scale integrated circuit (IC) manufacturing industry. In a typical IC process, a mask and a wafer are positioned in parallel. After the positioning is completed, the wafer is exposed. Traditional methods use precision distance sensors (such as capacitive, optical ranging, and electromagnetic methods) to measure the distance from the measured plane (such as a wafer, defined as M) to a reference plane (such as a template mounting plane, defined as W). The relative distance of a few positions is limited. When the flatness of the wafer surface cannot meet the required measurement accuracy, the measurement data of these measurement points cannot accurately reflect the parallel relationship between M and W at a higher technical level. Limits the accuracy of IC processing. Summary of the Invention

本发明的目的是提供一种能正确反映被测物体与参考平面之间的平行关系、调节 精度髙的精密平行度测量的方法,即测量被测物体平整表面与参考平面的相对平行度 方法。  The object of the present invention is to provide a precise parallelism measurement method that can accurately reflect the parallel relationship between the measured object and the reference plane and adjust the accuracy 髙, that is, a method for measuring the relative parallelism between the flat surface of the measured object and the reference plane.

为了实现上述目的, 本发明的具体技术方案是: 设 M为被测物体, W为参考平 面, Z为旋转轴, 将被测物体 M安装在具有旋转轴 Z的平台上, 可绕旋转轴 Z旋转, 旋转轴 Z与参考平面 W垂直; 配有一束照明光源和摄像机作为测量装置, 让摄像机 镜头对准被测物体 M的侧面, 凭借可以接收的、投射在被测物体 M侧面的反射光成 像; 设橫轴 u与纵轴 V为成像后的图像坐标系, 原点在成像后的图像中心,其中被测 物体 M上或下平面与其侧面过纵轴 V的交汇点为在被测物体 M侧面图像的检测点 A; 当被测物体 M绕旋转轴 Z旋转时、 通过连续图象采集, 利用检测点 A的图像位置测 量值描述被测物体 M的平面相对参考平面 W的平行状态, 从而确定被测物体 M相 对参考平面 W的不平行度和调整位置;  In order to achieve the above object, the specific technical solution of the present invention is: Let M be the measured object, W be the reference plane, Z be the rotation axis, and mount the measured object M on a platform having a rotation axis Z, which can be rotated around the rotation axis Z Rotate, the axis of rotation Z is perpendicular to the reference plane W; Equipped with a beam of light and a camera as a measuring device, the camera lens is aimed at the side of the object M to be imaged by the reflected light that can be received and projected on the side of the object M ; Let the horizontal axis u and the vertical axis V be the image coordinate system after imaging, and the origin point is at the center of the imaged image, where the intersection point between the upper or lower plane of the measured object M and its side through the vertical axis V is on the side of the measured object M; Detection point A of the image; When the measured object M rotates about the rotation axis Z, through continuous image acquisition, the image position measurement value of the detection point A is used to describe the parallel state of the plane of the measured object M with respect to the reference plane W, thereby determining Non-parallelism and adjusted position of the measured object M relative to the reference plane W;

当所述光源与摄像机位置不变时,当釆样速率远大于被测物体 M的旋转速度时, 检测点 A的检测位置为近似连续变化的离散量; 当被测物体 M与参考平面 W不平 行时, 检测点 A点的位置检测值在旋转周期内会呈现偏移量变化曲线, 当在一个旋 转周期内测得的这个曲线近似平行直线时, 则两个平面即被测物体 M平面和参考平 面 W近似平行; When the positions of the light source and the camera remain unchanged, when the sampling rate is much greater than the rotation speed of the measured object M, the detection position of the detection point A is a discrete quantity that changes approximately continuously; when the measured object M and the reference plane W are not When parallel, the position detection value of the detection point A will show an offset change curve during the rotation period. When the curve measured during the rotation period is approximately parallel and straight, the two planes, namely the measured object M plane and the reference plane W, are approximately parallel;

所述偏移量变化曲线定量反映了被测物体 M平面与参考平面 W的不平行幅度和 最大偏离幅度的角度位置, 偏移量变化曲线的纵轴表示被测物体 M在旋转角为 Θ时 的倾斜幅度, 其中 X表示最大倾斜幅度; 横轴表示旋转角 Θ , 其中 Y为最大倾斜幅 度 X时相对旋转起始位置所旋转过的角度 Θ; 所述参考平面可以位于被测物体 M的 上方或下方。  The offset change curve quantitatively reflects the angular position of the non-parallel amplitude and the maximum deviation amplitude of the measured object M plane and the reference plane W, and the vertical axis of the offset change curve indicates that the measured object M has a rotation angle of Θ Where the X represents the maximum inclination; the horizontal axis represents the rotation angle Θ, where Y is the angle Θ rotated relative to the starting position of rotation at the maximum inclination X; the reference plane may be located above the measured object M Or below.

本发明具有如下优点:  The invention has the following advantages:

1. 基于其原理及其合理设计, 本发明可从整体上检测了被测物体 (如晶片)相 对于参考系的不平行度, 因而与现有技术相比, 具有更明显的技术优势, 即: 能正确 反映被测物体与参考平面之间的平行关系, 同时易操作, 也具有可实现性。  1. Based on its principle and reasonable design, the present invention can detect the non-parallelism of the measured object (such as a wafer) relative to the reference system as a whole, so it has a more obvious technical advantage than the existing technology, that is, : Can accurately reflect the parallel relationship between the measured object and the reference plane, at the same time easy to operate, and also has achievability.

2. 本发明为光学测量方式, 不仅无电磁污染(如电磁干扰), 而且调节精度高, 测量精度取决于图象分辨率, 可达 0.1微米以上。  2. The present invention is an optical measurement method, which is not only free of electromagnetic pollution (such as electromagnetic interference), but also has high adjustment accuracy. The measurement accuracy depends on the image resolution and can reach more than 0.1 micron.

3. 本发明基于光学成象位置测量方法, 在亚微米级上实现两个平面即被测平面 与参考平面之间的平行度检测, 从而可实现 IC加工过程中的超精密定位检测, 提高 IC集成电路的加工水平和集成度, 进一步实现对现有 IC加工工艺的改进。 附图说  3. The present invention is based on the optical imaging position measurement method, and realizes the parallelism detection between two planes, that is, the measured plane and the reference plane on the sub-micron level, so as to achieve ultra-precision positioning detection during IC processing and improve IC. The integrated circuit processing level and integration further improve the existing IC processing technology. Attached picture

图 1为测量原理与测量结构示意图。  Figure 1 shows the measurement principle and measurement structure.

图 2为使摄像机可以接收照明光源投射在晶片侧面的反射成像。  Fig. 2 is a reflection image of the side of the wafer which enables the camera to receive the illumination light source.

图 3为被测平面 M侧面的成像检测点 A的位置检测值在旋转周期内的偏移量变 化曲线。 具体实施方式  Fig. 3 is a graph showing the change in the displacement of the position detection value of the imaging detection point A on the side of the measured plane M in the rotation period. detailed description

设 M为被测物体, W为参考平面, 位于参考平面 W的下方, Z为旋转轴, 将被 测物体 M安装在具有旋转轴 Z的平台上, 可绕旋转轴 Z旋转, 旋转轴 Z与参考平面 W垂直; 配有一束照明光源和摄像机(本实施例采用 CCD摄像机)作为测量装置, 让摄像机镜头对准被测物体 M的侧面, 凭借可以接收的、投射在被测物体 M侧面的 光源反射成像,即在摄像机上产生投射在被测物体侧面的反射光成像;设横轴 11与纵 轴 V为成像后的图像坐标系, 原点在成像后的图像中心, 其中被测物体 M下平面与 其侧面过纵轴 v的交汇点 A为在被测物体 M侧面图像的检测点;当被测物体 M绕旋 转轴 Z旋转时、 通过连续图象采集, 利用检测点 A的图像位置测量值描述被测物体 M的平面相对参考平面 W的平行状态, 从而确定被测物体 M相对参考平面 W的不 平行度和调整位置; Let M be the measured object, W be the reference plane, be located below the reference plane W, and Z be the rotation axis. The measured object M is mounted on a platform with a rotation axis Z and can be rotated about the rotation axis Z. The rotation axis Z and The reference plane W is vertical; it is equipped with a beam of illumination light source and a camera (a CCD camera is used in this embodiment) as a measuring device, so that the camera lens is aligned with the side of the object M to be measured. Reflective imaging, that is, the imaging of the reflected light projected on the side of the measured object on the camera; set the horizontal axis 11 and the vertical axis V as the image coordinate system after imaging, and the origin is at the center of the image after imaging, where the measured object M is below versus The intersection point A whose side passes through the vertical axis v is the detection point of the side image of the measured object M; when the measured object M rotates around the rotation axis Z, continuous image acquisition is used to describe the image position measurement value of the detection point A The parallel state of the plane of the measured object M with respect to the reference plane W, so as to determine the non-parallelism and the adjusted position of the measured object M with respect to the reference plane W;

当所述光源与摄像机位置不变时, 当采样速率远大于被测物体 M的旋转速度时, 检测点 A的检测位置为近似连续变化的离散量; 当被测物体 M与参考平面 W不平 行时, 检测点 A点的位置检测值在旋转周期内会呈现偏移量变化曲线, 当在一个旋 转周期内测得的这个曲线近似平行直线时, 则两个平面即被测物体 M平面和参考平 面 W近似平行;  When the position of the light source and the camera is unchanged, when the sampling rate is much greater than the rotation speed of the measured object M, the detection position of the detection point A is a discrete quantity that changes approximately continuously; when the measured object M is not parallel to the reference plane W , The position detection value of the detection point A will show an offset change curve during the rotation period. When the curve measured in a rotation period is approximately parallel straight lines, the two planes are the measured object M plane and the reference. The plane W is approximately parallel;

所述偏移量变化曲线定量反映了被测物体 M平面与参考平面 W的不平行幅度和 最大偏离幅度的角度位置, 偏移变化曲线的纵轴表示被测物体 M在旋转角为 Θ时的 倾斜幅度, 其中 X表示最大倾斜幅度; 横轴表示旋转角 6, 其中 Y表示最大倾斜幅 度 X时相对旋转起始位置所旋转过的角度 Θ 。  The offset change curve quantitatively reflects the angular position of the non-parallel amplitude and the maximum deviation amplitude of the plane of the measured object M and the reference plane W, and the vertical axis of the offset change curve represents the measured position of the measured object M when the rotation angle is Θ. The inclination amplitude, where X represents the maximum inclination amplitude; the horizontal axis represents the rotation angle 6, and Y represents the angle Θ that has been rotated relative to the starting position of rotation at the maximum inclination amplitude X.

平行度测量方法具体操作为:令被测物体 M绕旋转轴 Z轴转动,并且采用 CCD 连续采集图象, 则捡测出被测物体 M侧面的成像检测点 A的图象位置为连续图像; 当光源与 CCD位置不变时, 当采样速率远大于被测物体 M的旋转速度时,检测点 A 的检测位置为近似连续变化的离散量; 当被测物体 M与参考平面 W不平行时,检测 点 A点的位置检测值在旋转周期内会呈现偏移量变化曲线,参见图 3 (图 3反映了被 测平面 M相对于参考平面 W的倾斜曲线;所述纵轴表示被测物体在旋转角为 Θ时的 倾斜幅度, 代表所需调节量; 其中 X为被测平面 M相对于参考平面 W的最大倾斜幅 度; 横轴为旋转角度 Θ , 代表被测平面 M所需调节的位置; 其中 Y为检测点 A处的 旋转角度 Θ ), 当在一个旋转周期内测得的这个曲线近似平行直线时, 则两个平面即 被测物体 M平面和参考平面 W近似平行。  The specific operation of the parallelism measuring method is as follows: the measured object M is rotated around the rotation axis Z axis, and the CCD is used to continuously acquire images, and the image position of the imaging detection point A on the side of the measured object M is detected as a continuous image; When the position of the light source and the CCD is constant, when the sampling rate is much greater than the rotation speed of the measured object M, the detection position of the detection point A is a discrete quantity that changes approximately continuously; when the measured object M is not parallel to the reference plane W, The position detection value of the detection point A will show an offset change curve during the rotation period, see FIG. 3 (FIG. 3 reflects the tilt curve of the measured plane M relative to the reference plane W; the vertical axis indicates that the measured object is at The inclination amplitude when the rotation angle is Θ represents the required adjustment amount; where X is the maximum inclination amplitude of the measured plane M relative to the reference plane W; the horizontal axis is the rotation angle Θ, which represents the position to be adjusted in the measured plane M; Where Y is the rotation angle Θ at the detection point A). When the curve measured in a rotation period is approximately parallel straight line, the two planes are the measured object M plane and the reference plane W Approximately parallel.

测量原理: 如图 1所示(其中: 1为光源, 2为 CCD摄像机 3为摄像机镜头, 4 为反射域), 设被测物体 M为圆盘形晶片(wafer), 安装在具有一个旋转轴 Z的平台 上, 该旋转轴 Z与给定的参考平面 W垂直; 模板 (mask)安装在参考平面 W上, 假设参考平面 W与模板平行, 如果能够测量被测物体 M与参考平面 W的之间平整 度并可以按要求调整两者之间的姿态,则通过这种测量与调整,就可以实现模板与晶 片的平行度测量与调整, 其检测精度取决于测量系统的位置分辨率。  Measuring principle: As shown in Figure 1 (where: 1 is the light source, 2 is the CCD camera, 3 is the camera lens, and 4 is the reflection field), the measured object M is a wafer, and it is mounted on a rotating shaft. On the platform of Z, the rotation axis Z is perpendicular to a given reference plane W. A mask is installed on the reference plane W. Assuming that the reference plane W is parallel to the template, if the measured object M and the reference plane W can be measured, The flatness and the attitude between the two can be adjusted as required. Through this measurement and adjustment, the parallelism measurement and adjustment of the template and the wafer can be achieved. The detection accuracy depends on the position resolution of the measurement system.

测量成像机理: 设 M为被测物体, W为参考平面, Z为与参考平面 W垂直的旋 转轴, 被测物体 M可绕旋转轴 Z轴旋转。 当使用 CCD摄像机与一束照明光源按图 1 中的配置时, 使 CCD可以接收照明光投射在晶片侧面的反射成像如图 2所示。 其中 A (本实施例为被测物体 M下平面与其侧面过 V轴的交汇点) 为定义在被测物体 M 侧面图像的检测点, u与 V为图像坐标系; 5为被测平面 M侧面的反射域成像, 6为 背景域成像。 Measurement imaging mechanism: Let M be the measured object, W be the reference plane, and Z be the rotation perpendicular to the reference plane W Rotation axis, the measured object M can rotate around the rotation axis Z axis. When a CCD camera and a lighting source are used in the configuration shown in FIG. 1, the reflection imaging that enables the CCD to receive illumination light and project it on the side of the wafer is shown in FIG. 2. Among them, A (the intersection point of the lower plane of the measured object M and its side passing the V axis) is the detection point defined on the side of the measured object M, u and V are image coordinate systems; 5 is the side of the measured plane M Imaging in the reflection domain, 6 for background domain imaging.

平行度测量机理: 本发明的核心思想是通过测量检测点 A的图像位置测量值进 而描述被测物体 M的平面相对参考平面 W的平行状态,包括倾斜幅度、最大倾斜幅 度相距起始位置所在的旋转角, 从而确定了 M相对 W的不平行度和调整位置。  Parallelism measurement mechanism: The core idea of the present invention is to describe the parallel state of the plane of the measured object M with respect to the reference plane W by measuring the image position measurement value of the detection point A, including the inclination width and the maximum inclination distance from the starting position. The rotation angle determines the non-parallelism of M and W and the adjustment position.

本实施例设 CCD分辩率为 1000,镜头放大倍数为 50,则测量系统分辩率为 1000 X 50=5 X 104, 设视场为 5mm (即: 图象包含的景物的实际高度范围), 则测量精度 为 5mm/ (5 X 104) =l X l(T4 min =0.1 μηι。实验时取 X值为调节幅度,调节其值至(趋 于) 0, 调节位置由 Υ所示的旋转角 Θ确定。 In this embodiment, the resolution of the CCD is 1000, and the magnification of the lens is 50. The resolution of the measurement system is 1000 X 50 = 5 X 10 4 , and the field of view is 5 mm (that is, the actual height range of the scene included in the image). Then the measurement accuracy is 5mm / (5 X 10 4 ) = l X l (T 4 min = 0.1 μηι. During the experiment, take the X value as the adjustment range, adjust its value to (toward) 0, and the adjustment position is shown by Υ The rotation angle Θ is determined.

平行度的精度分析:本发明不平行度检测精度取决于图象分辨率, 当图象分辨率 髙到小于微米 (亚微米) 时, 检测点 Α的测量曲线所反映的不平行状态就可以达到 亚微米级。 由于 CCD的视场可以设计为仅包含检测点 A附近的区域, 镜头的放大倍 数也可以足够大, 因此图像分辨率可以足够高, 理论上可以达到镜头与 CCD分辨率 组合的极限。 这样, 当 CCD成像系统的分辨率足够高时, 就可以实现对被测物体 M 与参考平面 W的不平行度精密测量。根据科研经验,可以釆用线阵高分辨率 CCD摄 像机, 并按要求取镜头的放大倍数, 经图象处理, 可以满足测量大于、 等于 0.1微米 的测量精度。由于被测边缘存在噪声(由晶片表面与侧面交界边缘的不平整度引起), 会在检测点 A的位置测量曲线上出现噪声信号, 因此需要加入平滑滤波等技术处理 (常规技术) 以正确得到检测点 A的准确位置测量曲线, 以便精确给出不平行参数, 用于机构调节。  Analysis of the accuracy of parallelism: The detection accuracy of the non-parallelism of the present invention depends on the image resolution. When the image resolution is less than micron (sub-micron), the non-parallel state reflected by the measurement curve of the detection point A can be achieved. Sub-micron level. Since the field of view of the CCD can be designed to include only the area near the detection point A, the magnification of the lens can also be sufficiently large, so the image resolution can be sufficiently high, and theoretically the limit of the combination of the lens and the CCD resolution can be reached. In this way, when the resolution of the CCD imaging system is sufficiently high, precise measurement of the non-parallelism of the measured object M and the reference plane W can be achieved. According to scientific research experience, a linear high-resolution CCD camera can be used, and the magnification of the lens can be taken as required. After image processing, it can meet the measurement accuracy of 0.1 micron or more. Noise signal will appear on the measurement curve of the position of detection point A due to noise (caused by the unevenness of the boundary between the wafer surface and the side) at the measured edge. Therefore, technical processing such as smoothing filtering (conventional technology) needs to be added to correctly obtain The accurate position measurement curve of the detection point A, so as to accurately give non-parallel parameters for mechanism adjustment.

Claims

刺 要 求 书 Thorn request 1. 一种精密平行度测量方法, 其特征在于: 将被测物体 M可绕旋转轴 Z旋转, 安装在具有旋转轴 Z的平台上, 所述旋转轴 Z与参考平面 W垂直; 配有光源和摄像 机作为测量装置, 让摄像机镜头对准被测物体 M的侧面, 凭借可以接收的、 投射在 被测物体 M侧面的光源反射成像; 设横轴 u与纵轴 V为成像后的图像坐标系, 原点 在成像后的图像中心, 其中被测物体 M上或下平面与其侧面过纵轴 V的交汇点为在 被测物体 M侧面图像的检测点 A; 当被测物体 M绕旋转轴 Z旋转时、通过连续图象 采集, 利用检测点 A的图像位置测量值描述被测物体 M的平面相对参考平面 W的 平行状态, 从而确定被测物体 M相对参考平面 W的不平行度和调整位置。 1. A precise parallelism measuring method, characterized in that: the measured object M can be rotated around a rotation axis Z, and is mounted on a platform having a rotation axis Z, the rotation axis Z is perpendicular to the reference plane W; equipped with a light source The camera and the camera are used as measuring devices, and the camera lens is aligned at the side of the object M to be imaged by the light source reflection that can be received and projected at the side of the object M. Let the horizontal axis u and the vertical axis V be the image coordinate system after imaging The origin is at the center of the imaged image, where the intersection of the upper or lower plane of the measured object M and its side through the longitudinal axis V is the detection point A on the side image of the measured object M; when the measured object M rotates around the rotation axis Z The parallel state of the plane of the measured object M with respect to the reference plane W is described by continuous image acquisition, using the image position measurement value of the detection point A, so as to determine the non-parallelism of the measured object M with respect to the reference plane W and the adjusted position. 2. 按照权利要求 1所述精密平行度测量方法, 其特征在于: 当所述光源与摄像 机位置不变时, 当釆样速率远大于被测物体 M的旋转速度时, 检测点 A的检测位置 为近似连续变化的离散量; 当被测物体 M与参考平面 W不平行时, 检测点 A点的 位置检测值在旋转周期内会呈现偏移量变化曲线,当在一个旋转周期内测得的这个曲 线近似平行直线时, 则两个平面即被测物体 M平面和参考平面 W近似平行。  2. The precise parallelism measuring method according to claim 1, characterized in that: when the position of the light source and the camera is unchanged, when the sampling rate is much greater than the rotation speed of the measured object M, the detection position of the detection point A Is a discrete quantity that changes approximately continuously; when the measured object M is not parallel to the reference plane W, the position detection value of the detection point A will show an offset change curve in the rotation period, and when measured in a rotation period When this curve is approximately parallel and straight, the two planes, namely the measured object M plane and the reference plane W are approximately parallel. 3. 按照权利要求 2所述精密平行度测量方法, 其特征在于: 所述偏移量变化曲 线定量反映了被测物体 M平面与参考平面 W的不平行幅度和最大偏离幅度的角度位 置,其纵轴表示被测物体 M在旋转角为 Θ时的倾斜幅度,其中 X表示最大倾斜幅度; 横轴为旋转角度 Θ , 其中 Y表示最大倾斜幅度 X时相对旋转起始位置所旋转过的角 度 Θ。  3. The method for measuring precision parallelism according to claim 2, characterized in that: said offset variation curve quantitatively reflects the angular position of the non-parallel amplitude and the maximum deviation amplitude of the measured object M plane and the reference plane W, which The vertical axis represents the inclination of the measured object M when the rotation angle is Θ, where X represents the maximum inclination; the horizontal axis is the rotation angle Θ, where Y represents the angle θ that has been rotated relative to the starting position of rotation at the maximum inclination X. . 4. 按照权利要求 1所述精密平行度测量方法, 其特征在于: 所述参考平面可以 位于被测物体 M的上方或下方。  4. The method for measuring precision parallelism according to claim 1, wherein the reference plane is located above or below the measured object M.
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