CN104897076A - Three dimensional shape measurement method for micro nanoscale - Google Patents
Three dimensional shape measurement method for micro nanoscale Download PDFInfo
- Publication number
- CN104897076A CN104897076A CN201410086820.7A CN201410086820A CN104897076A CN 104897076 A CN104897076 A CN 104897076A CN 201410086820 A CN201410086820 A CN 201410086820A CN 104897076 A CN104897076 A CN 104897076A
- Authority
- CN
- China
- Prior art keywords
- measurement
- optical path
- sample
- dimensional shape
- frequency
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Landscapes
- Length Measuring Devices By Optical Means (AREA)
Abstract
Description
技术领域technical field
本发明涉及一种采用飞秒激光频率梳测量表面三维形貌特征的方法,该方法主要用于半导体集成电路、MEMS器件等微纳尺度表面三维形貌特征的测量。The invention relates to a method for measuring surface three-dimensional topographic features by using a femtosecond laser frequency comb. The method is mainly used for measuring the three-dimensional topographic features of micro-nano scale surfaces such as semiconductor integrated circuits and MEMS devices.
背景技术Background technique
随着半导体集成电路制造技术、微纳米超精密加工技术的进一步发展,大尺寸、纳米级大规模集成电路和微型化、精密化微机电系统的出现,对相关测量方法和测量仪器的检测能力与检测精度提出了新的要求和挑战。With the further development of semiconductor integrated circuit manufacturing technology and micro-nano ultra-precision processing technology, the emergence of large-scale, nano-scale large-scale integrated circuits and miniaturized and precise micro-electromechanical systems, the detection capabilities of related measurement methods and measuring instruments Detection accuracy poses new requirements and challenges.
目前现有的微纳尺度表面三维形貌特征测量方法有诸多的限制,如单次测量的横向视场较小,纵向测量的扫场、快描速度较慢,测量精度与机械扫描装置相关等,已不能满足对微纳尺度表面三维形貌特征进行大视速测量的要求。At present, the existing methods for measuring the three-dimensional topography characteristics of micro-nano scale surfaces have many limitations, such as the small horizontal field of view for a single measurement, the slow speed of scanning field and fast scanning for longitudinal measurement, and the measurement accuracy is related to the mechanical scanning device, etc. , can no longer meet the requirements of large visual velocity measurement of the three-dimensional surface features of micro-nano scale.
飞秒激光频率梳在精密光谱学、光频计量和绝对测距等方面有着独特的时间和光谱特性,飞秒激光脉冲的低时间相干、高空间相干的特性方法是一种新型的测量方法,具有测量视场大、测量速度快等优点,在半导体集成电路制造、MEMS器件加工和其他微纳制造在大尺寸表面三维形貌特征测量中具有前所未有的优势,基于飞秒激光频率梳的表面三维形貌特征测量等领域具有重要应用价值。Femtosecond laser frequency comb has unique time and spectral characteristics in precision spectroscopy, optical frequency metrology and absolute distance measurement. The characteristic method of femtosecond laser pulse with low temporal coherence and high spatial coherence is a new type of measurement method. It has the advantages of large measurement field of view and fast measurement speed. It has unprecedented advantages in the measurement of three-dimensional topography of large-scale surfaces in semiconductor integrated circuit manufacturing, MEMS device processing and other micro-nano manufacturing. The surface three-dimensional surface measurement based on femtosecond laser frequency comb It has important application value in fields such as shape feature measurement.
发明内容Contents of the invention
本发明采用飞秒激光频率梳作为光源,利用其低时间相干、高空间相干的特性实现大尺寸的微纳测量,而且频率梳的重复频率可以调节,通过重复频率的变化完成对样品表面的扫描测量。本发明采用测量光路是非平衡非对称光路,由光纤光路、倍频系统和扩束光路组成,以实现跨尺度微纳测量。测量得到的干涉图样由高速CCD探测,进行处理和分析后可以得到样品表面三维形貌特征参量,并通过三维模型重建可以还原样品表面三维形貌。The invention adopts femtosecond laser frequency comb as the light source, utilizes its characteristics of low temporal coherence and high spatial coherence to realize large-scale micro-nano measurement, and the repetition frequency of the frequency comb can be adjusted, and the scanning of the sample surface can be completed by changing the repetition frequency Measurement. In the present invention, the measurement optical path is an unbalanced and asymmetric optical path, which is composed of an optical fiber optical path, a frequency doubling system and a beam expanding optical path, so as to realize cross-scale micro-nano measurement. The measured interference pattern is detected by a high-speed CCD. After processing and analysis, the characteristic parameters of the three-dimensional topography of the sample surface can be obtained, and the three-dimensional topography of the sample surface can be restored through three-dimensional model reconstruction.
与传统测量方法相比,本发明采用飞秒激光频率梳作为光源,扩大了测量视场;采用电扫描方法进行扫描,提高了扫描速度,同时避免了机械扫描对测量精度的影响;可以实现跨尺度微纳测量。Compared with the traditional measurement method, the present invention uses a femtosecond laser frequency comb as the light source, which expands the measurement field of view; uses the electronic scanning method to scan, improves the scanning speed, and avoids the influence of mechanical scanning on the measurement accuracy; Scale micro-nano measurement.
附图说明Description of drawings
为了更清楚、准确地说明本发明实施例中的技术方案,下面将对实施例或者现有技术描述中所需要使用的附图做简单地介绍,显而易见,下面描述中的附图仅仅是本发明的实施例,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,还可以根据提供的附图获得其他的附图。In order to more clearly and accurately illustrate the technical solutions in the embodiments of the present invention, the following will briefly introduce the drawings that need to be used in the embodiments or the description of the prior art. Obviously, the drawings in the following description are only the present invention. For the embodiment of the present invention, those of ordinary skill in the art can also obtain other drawings according to the provided drawings on the premise of not paying creative efforts.
图1为飞秒激光频率梳三维面型测量方法组成框图Figure 1 is a block diagram of the femtosecond laser frequency comb three-dimensional surface shape measurement method
图2为飞秒激光频率梳三维面型测量系统结构示意图Figure 2 is a schematic diagram of the structure of the femtosecond laser frequency comb three-dimensional surface measurement system
图3为飞秒激光频率梳三维面型测量方法流程图Figure 3 is a flow chart of the femtosecond laser frequency comb three-dimensional surface measurement method
其中,21:光纤耦合器;22,23:单模光纤;24:色散补偿光纤;25,33,34:透镜;26:分色镜;27:倍频晶体;31:平面镜;32:分光棱镜;35:被测样品;41:高速CCD相机Among them, 21: fiber coupler; 22, 23: single-mode fiber; 24: dispersion compensation fiber; 25, 33, 34: lens; 26: dichroic mirror; 27: frequency doubling crystal; 31: plane mirror; 32: beam splitting prism ;35: Tested sample; 41: High-speed CCD camera
具体实施方式Detailed ways
下面将结合本发明实施例中的附图,对本发明实施例中的技术方案件进行准确、完整地描述,显然,所描述的实施例仅仅是本发明一部分实施例,并不是全部的实施例。基于此,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,都属于本发明的保护范围。The technical solutions in the embodiments of the present invention will be accurately and completely described below in conjunction with the accompanying drawings in the embodiments of the present invention. Obviously, the described embodiments are only some, not all, embodiments of the present invention. Based on this, all other embodiments obtained by persons of ordinary skill in the art without making creative efforts belong to the protection scope of the present invention.
本发明涉及的飞秒激光频率梳测量表面三维形貌特征的方法包括:重复频率可调的飞秒激光频率梳系统1,光纤光路和倍频系统组成的光路系统2,迈克尔逊干涉光路和扩束光路构成的测量系统3和高速CCD相机组成的信号接收系统4,如图1所示。本发明涉及的飞秒激光频率梳三维面型测量系统如图2所示,飞秒激光频率梳产生的飞秒脉冲通过光纤耦合器21分成两束光进入由参考光路和测量光路组成的光纤光路。其中参考光路由一段长单模光纤23组成,同时结合使用色散补偿光纤24以补偿由于长距离传输引起的色散。测量光路由一段短单模光纤22组成。同时参考光路与测量光路之间设计有较大的光程差。由光纤光路出射后的飞秒脉冲经平面镜25、分色镜26入射到倍频晶体27进行倍频,且只有倍频后的飞秒脉冲可以通过分色镜26反射进入测量系统。测量系统是由平面镜31、分光棱镜32、透镜33和34、被测样品35构成的迈克尔逊干涉光路组成的,其中透镜33和34组成扩束光路以更好探测样品表面。通过调整飞秒激光频率梳的重复频率完成对被测样品的扫描,在高速CCD相机41上得到相应的干涉图样。The femtosecond laser frequency comb method of the present invention for measuring surface three-dimensional topography features includes: femtosecond laser frequency comb system 1 with adjustable repetition rate, optical path system 2 composed of optical fiber optical path and frequency doubling system, Michelson interference optical path and expansion The measurement system 3 composed of the optical beam path and the signal receiving system 4 composed of the high-speed CCD camera are shown in Fig. 1 . The femtosecond laser frequency comb three-dimensional surface measurement system involved in the present invention is shown in Figure 2. The femtosecond pulse generated by the femtosecond laser frequency comb is divided into two beams of light by the fiber coupler 21 and enters the optical fiber optical path composed of the reference optical path and the measurement optical path. . The reference optical path is composed of a long single-mode optical fiber 23, and at the same time, the dispersion compensation optical fiber 24 is used in combination to compensate the dispersion caused by long-distance transmission. The measurement optical path consists of a short single-mode optical fiber 22 . At the same time, a large optical path difference is designed between the reference optical path and the measurement optical path. The femtosecond pulse emitted from the optical fiber path enters the frequency doubling crystal 27 through the plane mirror 25 and the dichroic mirror 26 for frequency doubling, and only the frequency multiplied femtosecond pulse can be reflected by the dichroic mirror 26 and enter the measurement system. The measurement system is composed of a Michelson interference optical path composed of a plane mirror 31, a dichroic prism 32, lenses 33 and 34, and a measured sample 35, wherein the lenses 33 and 34 form a beam expanding optical path to better detect the surface of the sample. By adjusting the repetition frequency of the femtosecond laser frequency comb, the scanning of the sample to be tested is completed, and the corresponding interference pattern is obtained on the high-speed CCD camera 41 .
本发明测量方法流程如图3所示,首先根据实际样品确定重复频率调整步长,然后从初始重复频率开始,每一步进调整后的重频完成一次对样品表面的测量并在CCD上得到一帧相应的图像,如此周而复始直至对被测样品表面的扫描完成。扫描完成后通过对CCD上所得干涉图样的分析处理,可以得到样品表面三维形貌特征参量,并通过三维模型重建可以还原样品表面三维形貌。The flow chart of the measurement method of the present invention is shown in Figure 3. First, the repetition frequency adjustment step is determined according to the actual sample, and then starting from the initial repetition frequency, the repetition frequency after each step is adjusted to complete a measurement of the sample surface and obtained on the CCD. One frame of corresponding images, repeating this cycle until the scanning of the surface of the tested sample is completed. After scanning, through the analysis and processing of the interference pattern obtained on the CCD, the characteristic parameters of the three-dimensional topography of the sample surface can be obtained, and the three-dimensional topography of the sample surface can be restored through three-dimensional model reconstruction.
对所公开的实施例的上述说明,使本领域专业技术人员能够实现或者使用本发明,对这些实施例的多种修改对本领域的专利技术人员来说将是显而易见的。本文中所定义的一般原理可以在不脱离本发明的精神或者范围的情况下,在其它实施例中实现。因此,本发明将不会被限制于本文所示的这些实施例,而是要符合本文所公开的原理和新颖性特点相一致的最宽的范围。The foregoing description of the disclosed embodiments enables those skilled in the art to make or use the invention, and various modifications to these embodiments will be apparent to those skilled in the art. The general principles defined herein may be implemented in other embodiments without departing from the spirit or scope of the invention. Therefore, the present invention will not be limited to the embodiments shown herein, but is to be accorded the widest scope consistent with the principles and novel features disclosed herein.
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201410086820.7A CN104897076A (en) | 2014-03-07 | 2014-03-07 | Three dimensional shape measurement method for micro nanoscale |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201410086820.7A CN104897076A (en) | 2014-03-07 | 2014-03-07 | Three dimensional shape measurement method for micro nanoscale |
Publications (1)
Publication Number | Publication Date |
---|---|
CN104897076A true CN104897076A (en) | 2015-09-09 |
Family
ID=54029890
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201410086820.7A Pending CN104897076A (en) | 2014-03-07 | 2014-03-07 | Three dimensional shape measurement method for micro nanoscale |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN104897076A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105444785A (en) * | 2015-12-25 | 2016-03-30 | 中国科学院光电研究院 | Optical distance compensation device and method of scanning plane laser |
CN107063125A (en) * | 2017-06-15 | 2017-08-18 | 清华大学 | A kind of length scanning three dimensional shape measurement system of frequency comb reference |
CN108844493A (en) * | 2018-07-04 | 2018-11-20 | 天津大学 | The double light comb topography measurement devices of Electro-optical Modulation and its method of calibration |
CN111504190A (en) * | 2020-04-30 | 2020-08-07 | 天津大学 | Three-dimensional coordinate measuring device for correcting nonlinearity of frequency modulated continuous wave by Kerr optical comb |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008151640A (en) * | 2006-12-18 | 2008-07-03 | Nikon Corp | Measurement device |
CN102494615A (en) * | 2011-11-15 | 2012-06-13 | 清华大学 | Step distance measuring device based on femtosecond optical-frequency comb and measuring method thereof |
CN102967274A (en) * | 2012-11-14 | 2013-03-13 | 广东汉唐量子光电科技有限公司 | A method for measuring the surface topography of an object |
-
2014
- 2014-03-07 CN CN201410086820.7A patent/CN104897076A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2008151640A (en) * | 2006-12-18 | 2008-07-03 | Nikon Corp | Measurement device |
CN102494615A (en) * | 2011-11-15 | 2012-06-13 | 清华大学 | Step distance measuring device based on femtosecond optical-frequency comb and measuring method thereof |
CN102967274A (en) * | 2012-11-14 | 2013-03-13 | 广东汉唐量子光电科技有限公司 | A method for measuring the surface topography of an object |
Non-Patent Citations (1)
Title |
---|
JOO W D 等: "Femtosecond laser pulses for fast 3-D surface profilometry of microelectronic step-structures", 《OPTICS EXPRESS》 * |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105444785A (en) * | 2015-12-25 | 2016-03-30 | 中国科学院光电研究院 | Optical distance compensation device and method of scanning plane laser |
CN107063125A (en) * | 2017-06-15 | 2017-08-18 | 清华大学 | A kind of length scanning three dimensional shape measurement system of frequency comb reference |
CN107063125B (en) * | 2017-06-15 | 2019-08-02 | 清华大学 | A kind of length scanning three dimensional shape measurement system of frequency comb reference |
CN108844493A (en) * | 2018-07-04 | 2018-11-20 | 天津大学 | The double light comb topography measurement devices of Electro-optical Modulation and its method of calibration |
CN111504190A (en) * | 2020-04-30 | 2020-08-07 | 天津大学 | Three-dimensional coordinate measuring device for correcting nonlinearity of frequency modulated continuous wave by Kerr optical comb |
CN111504190B (en) * | 2020-04-30 | 2021-05-25 | 天津大学 | 3D Coordinate Measuring Device Using Kerr Comb to Correct FM CW Nonlinearity |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN103727891B (en) | Synchronize three-dimensional speckle interferometer measuration system and measuring method | |
CN109341574B (en) | Micro-nano structure three-dimensional morphology high-speed detection method based on structured light | |
CN107036534B (en) | Method and system for measuring displacement of vibrating target based on laser speckle | |
CN105865370B (en) | A white light scanning interferometry method and system | |
CN104808254B (en) | High-precision absolute gravimeter optics frequency multiplier type laser interference system and application | |
CN104897076A (en) | Three dimensional shape measurement method for micro nanoscale | |
CN107144217A (en) | Fiber optic interferometric confocal system for optical element crudy on-line checking | |
CN102183486A (en) | Gas refractive index measurer and measuring method thereof based on optical frequency comb | |
CN106197310A (en) | Modulation degree-based wide-spectrum micro-nano structure three-dimensional morphology detection method | |
CN106289726B (en) | A kind of photon band-gap optical fiber backscattering distributed measurement method and device | |
Fang et al. | Measurement of micro-V-groove dihedral using white light interferometry | |
CN104634282B (en) | Phase error compensation device in the measurement of optical probe interferometric phase | |
CN112729135A (en) | Area array frequency sweep distance measuring/thickness measuring device and method with active optical anti-shake function | |
CN103900639A (en) | High-speed multi-scale vibration and deformation detecting device and method | |
CN104792269B (en) | A kind of calculation method of the fiber end face height value insensitive to linear phase-shift error | |
CN108507981B (en) | Silicon-based waveguide back reflection sensing device based on OFDR (optical frequency domain reflectometry) and measuring method thereof | |
US7859683B2 (en) | Fast three-dimensional shape measuring apparatus and method | |
CN205482840U (en) | Dualbeam component roughness measuring device based on mach -Zehnder | |
JP2014102192A (en) | White color interference device, measuring method of position and displacement of the same | |
CN205785104U (en) | A kind of white light scanning interferometer measuration system | |
CN204902763U (en) | Acousto -optic modulation moves looks interferometer | |
CN204854621U (en) | Lightning modulation moves looks interferometer | |
CN204630653U (en) | Based on the vibration at high speed measuring system of wide spectrum light source principle of interference | |
CN204807037U (en) | Modulation of lightning intelligence moves looks interferometer | |
CN204902762U (en) | Reaction type acousto -optic modulation moves interferes system mutually |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
WD01 | Invention patent application deemed withdrawn after publication | ||
WD01 | Invention patent application deemed withdrawn after publication |
Application publication date: 20150909 |