CN106546368A - A kind of method for characterizing film residual stress - Google Patents
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- 238000010897 surface acoustic wave method Methods 0.000 description 4
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- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
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- G01L5/00—Apparatus for, or methods of, measuring force, work, mechanical power, or torque, specially adapted for specific purposes
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Abstract
本发明涉及一种表征薄膜残余应力的方法,包括:采用薄膜/衬底结构的样片,控制激光器发射出一定频率和能量的短脉冲激光束,在样片表面汇聚成线性激光束,样片表面产生超声表面波;压电传感器探测,并采集离散时域电压信号;得到实验频散曲线;建模并得到无残余应力状态下的薄膜/基底模型理论频散曲线;将实验频散曲线与理论频散曲线进行比较,定性确定样片薄膜残余应力的大小排列。本发明可以快速、无损检测薄膜残余应力。
The invention relates to a method for characterizing the residual stress of a film, comprising: using a film/substrate structure sample, controlling a laser to emit a short pulse laser beam with a certain frequency and energy, converging into a linear laser beam on the surface of the sample, and generating ultrasonic waves on the surface of the sample Surface waves; detection by piezoelectric sensors, and acquisition of discrete time-domain voltage signals; obtaining experimental dispersion curves; modeling and obtaining theoretical dispersion curves of film/substrate models in the state of no residual stress; comparing experimental dispersion curves with theoretical dispersion The curves are compared to qualitatively determine the magnitude and arrangement of the residual stress of the sample film. The invention can quickly and non-destructively detect the residual stress of the film.
Description
技术领域technical field
本发明属于薄膜特性表征领域,是一种超声表面波技术无损检测薄膜残余应力的方法。The invention belongs to the field of thin film characteristic characterization, and relates to a method for non-destructive detection of thin film residual stress by ultrasonic surface wave technology.
背景技术Background technique
薄膜中的残余应力在力的外部效应来看分为压应力和拉应力,当压应力过大的时候,就会使薄膜发生屈曲,这样使薄膜的附着力减弱,使薄膜与衬底脱离;当拉应力过大的时候,会使薄膜产生褶皱,甚至出现破裂。若在集成电路制造过程中,不能及时察觉薄膜中残余应力过大的情况,继续进行下一步的工作,则势必会严重影响集成电路的性能。因此,薄膜中残余应力的检测具有重要意义。超声表面波方法测量薄膜机械特性参数依据的原理是:超声表面波在薄膜/基底的分层结构中传播时是色散的,表面波波速除了与频率有关,还与薄膜的厚度、密度、弹性常数、残余应力以及基底材料的密度、弹性常数有关。将分别由理论模型和实验信号处理获得的色散曲线进行逼近匹配就可以测出薄膜样片的参数。本发明基于此提供一种无损表征样片薄膜残余应力的方法,即:基于声弹性理论,建立一种初级的理论计算模型,研究不同残余应力作用下的频散曲线变化规律,通过与激光激发声表面波检测薄膜特性的实验得出的频散曲线进行拟合,从而定性表征薄膜残余应力的大小。The residual stress in the film is divided into compressive stress and tensile stress in terms of the external effect of force. When the compressive stress is too large, the film will buckle, which will weaken the adhesion of the film and separate the film from the substrate; When the tensile stress is too large, the film will wrinkle or even crack. If the excessive residual stress in the thin film cannot be detected in time during the manufacturing process of the integrated circuit and the next step of work is continued, the performance of the integrated circuit will inevitably be seriously affected. Therefore, the detection of residual stress in thin films is of great significance. The principle of ultrasonic surface wave method to measure the mechanical parameters of thin film is that ultrasonic surface wave is dispersed when propagating in the layered structure of film/substrate, and the surface wave velocity is not only related to frequency, but also related to the thickness, density and elastic constant of the film. , residual stress and the density and elastic constant of the base material. By approximating and matching the dispersion curves obtained from the theoretical model and experimental signal processing, the parameters of the film sample can be measured. Based on this, the present invention provides a method for non-destructively characterizing the residual stress of a sample film, that is: based on the theory of acoustoelasticity, a primary theoretical calculation model is established to study the variation law of the dispersion curve under different residual stresses, and through the excitation of the laser with the acoustic The dispersion curve obtained from the experiment of measuring the properties of the film by the surface wave is fitted to qualitatively characterize the magnitude of the residual stress of the film.
发明内容Contents of the invention
本发明的目的是提供一种快速、无损检测薄膜残余应力的方法,有效的对low-k薄膜残余应力进行表征。技术方案如下:The purpose of the present invention is to provide a method for quickly and non-destructively detecting the residual stress of a thin film, and effectively characterize the residual stress of a low-k thin film. The technical solution is as follows:
一种表征薄膜残余应力的方法,包括下列步骤:A method for characterizing film residual stress, comprising the steps of:
1)采用薄膜/衬底结构的样片,控制激光器发射出一定频率和能量的短脉冲激光束,经过光学调整系统最终在样片表面汇聚成线性激光束,样片表面产生超声表面波;1) Using a sample with a film/substrate structure, the laser is controlled to emit a short pulse laser beam of a certain frequency and energy, which is finally converged into a linear laser beam on the surface of the sample through an optical adjustment system, and ultrasonic surface waves are generated on the surface of the sample;
2)表面波在样片表面传播一定距离后被压电传感器探测,再经过信号调理和数据采集后获得离散时域电压信号;2) The surface wave is detected by the piezoelectric sensor after propagating a certain distance on the surface of the sample, and then the discrete time-domain voltage signal is obtained after signal conditioning and data acquisition;
3)对采集到的离散时域电压信号进行包括傅立叶变换在内的数学处理,得到实验频散曲线;3) Perform mathematical processing including Fourier transform on the collected discrete time-domain voltage signal to obtain the experimental dispersion curve;
4)将样片的薄膜和衬底的密度、杨氏模量、泊松比、厚度在内其他参数代入MATLAB理论模型中,4) Substituting other parameters such as the density, Young's modulus, Poisson's ratio, and thickness of the sample film and substrate into the MATLAB theoretical model,
5)在理论模型中用应力t来表征残余应力的大小,令t=0,运行程序则得到无残余应力状态下的薄膜/基底模型理论频散曲线;5) In the theoretical model, the stress t is used to represent the size of the residual stress, and t=0, and the program is run to obtain the theoretical dispersion curve of the film/substrate model under the state of no residual stress;
6)将实验频散曲线与应力t=0时的理论频散曲线进行比较,规定t<0时表现为压应力,t>0时表现为拉应力,由此判断其残余应力类型,然后通过改变应力t的值来找出与实验频散曲线最相近的理论曲线应力t的值,重复试验测得一组样片的应力t值,进行排序,从而定性确定样片薄膜残余应力的大小排列。6) Comparing the experimental dispersion curve with the theoretical dispersion curve when the stress t=0, it is stipulated that when t<0, it is expressed as compressive stress, and when t>0, it is expressed as tensile stress, so as to judge the type of residual stress, and then pass Change the value of stress t to find the value of theoretical curve stress t that is closest to the experimental dispersion curve, repeat the test to measure the stress t value of a group of samples, and sort them, so as to qualitatively determine the size and arrangement of the residual stress of the sample film.
附图说明Description of drawings
图1为本发明采用的激光激发声表面波检测薄膜残余应力系统示意图。FIG. 1 is a schematic diagram of a laser-excited surface acoustic wave detection system for film residual stress adopted in the present invention.
图2表面波沿Si[100]方向传播时,不同压应力对色散曲线的影响。Fig. 2 The effect of different compressive stresses on the dispersion curve when the surface wave propagates along the Si[100] direction.
图3表面波沿Si[100]方向传播时,不同拉应力对色散曲线的影响。Fig. 3 The effect of different tensile stresses on the dispersion curve when the surface wave propagates along the Si[100] direction.
图4表面波沿Si[110]方向传播时,不同压应力对色散曲线的影响。Fig. 4 The effect of different compressive stresses on the dispersion curve when the surface wave propagates along the Si[110] direction.
图5表面波沿Si[110]方向传播时,不同拉应力对色散曲线的影响。Fig. 5 The effect of different tensile stresses on the dispersion curve when the surface wave propagates along the Si[110] direction.
具体实施方式detailed description
利用激光激发声表面波实验系统测得声表面波在样片表面传播的试验曲线,激光激发声表面波检测薄膜残余应力系统示意图如图1所示,其中采用MNL 801S型氮分子激光器,波长为337.1nm,平均脉冲能量为400uJ。压电传感器由聚偏氟乙烯薄膜(PVDF)和自制楔形探头组成。放大器为高倍宽频电压放大器MITEQ AU-1338型,数字示波器采用TektronicsTDS3000B型,带宽为300MHz,最高采样次速率为2.5GS/s。实验所用样片为薄膜/衬底结构,为使得结果更加准确,需保证所测量的样片属于同一批,具有高度相似的杨氏模量,密度和泊松比,在测量过程应保证同一组数据相同的晶向进行测量。具体测量过程如下:The experimental curve of surface acoustic wave propagation on the sample surface was measured by the laser-excited surface acoustic wave experimental system. The schematic diagram of the laser-excited surface acoustic wave detection film residual stress system is shown in Figure 1, in which the MNL 801S nitrogen molecular laser is used with a wavelength of 337.1 nm, the average pulse energy is 400uJ. The piezoelectric sensor consists of a polyvinylidene fluoride film (PVDF) and a self-made wedge probe. The amplifier is MITEQ AU-1338 type high frequency broadband voltage amplifier, the digital oscilloscope adopts Tektronics TDS3000B type, the bandwidth is 300MHz, and the highest sampling rate is 2.5GS/s. The sample used in the experiment is a film/substrate structure. In order to make the results more accurate, it is necessary to ensure that the measured samples belong to the same batch and have highly similar Young's modulus, density and Poisson's ratio. During the measurement process, the same set of data should be guaranteed to be the same crystallographic measurements. The specific measurement process is as follows:
(1)通过计算机控制激光器发射出一定频率和能量的短脉冲激光束。经过光学调整系统最终在样片表面汇聚成线性激光束,由于热弹效应,样片表面将会产生超声表面波;(1) The computer controls the laser to emit a short pulse laser beam with a certain frequency and energy. After the optical adjustment system finally converges into a linear laser beam on the surface of the sample, due to the thermoelastic effect, ultrasonic surface waves will be generated on the surface of the sample;
(2)表面波在样片表面传播一定距离后被压电传感器探测,经过放大器放大后采样存储在数字示波器中。(2) The surface wave is detected by the piezoelectric sensor after propagating for a certain distance on the surface of the sample, and is sampled and stored in the digital oscilloscope after being amplified by the amplifier.
(3)对采集到的离散时域电压信号进行包括傅立叶变换在内的一系列数学处理,从而得到实验频散曲线。(3) Perform a series of mathematical processing including Fourier transform on the collected discrete time-domain voltage signal to obtain the experimental dispersion curve.
将样片其他参数代入MATLAB理论模型中,薄膜及基底的相关参数设定见表1。在理论模型中用应力t来表征残余应力的大小。令t=0,运行程序则得到无残余应力状态下的薄膜/基底模型理论频散曲线。The other parameters of the sample were substituted into the MATLAB theoretical model, and the relevant parameter settings of the film and the substrate are shown in Table 1. In the theoretical model, the stress t is used to characterize the magnitude of the residual stress. Let t=0, run the program to get the theoretical dispersion curve of the film/substrate model in the state of no residual stress.
将实验频散曲线与应力t=0时的理论频散曲线进行比较,规定t<0时表现为压应力,t>0时表现为拉应力,由此判断其残余应力类型。当表面波沿不同晶向传播时分析如下:Comparing the experimental dispersion curve with the theoretical dispersion curve at stress t=0, it is stipulated that when t<0, it is expressed as compressive stress, and when t>0, it is expressed as tensile stress, so the type of residual stress can be judged. When the surface wave propagates along different crystal directions, the analysis is as follows:
(1)设定表面波沿Si表面[100]方向传播,当t为压应力时,频率-速度色散曲线如图2所示,在固定频率下,随着压应力的增大而减小;当t为拉应力时,频率-速度色散曲线如图3所示,在固定频率下,随着拉应力的增大而增大。且在[100]方向传播时,相差200MPa的曲线变化相对较小;(1) It is assumed that the surface wave propagates along the [100] direction of the Si surface. When t is the compressive stress, the frequency-velocity dispersion curve is shown in Figure 2. At a fixed frequency, it decreases with the increase of the compressive stress; When t is the tensile stress, the frequency-velocity dispersion curve is shown in Figure 3. At a fixed frequency, it increases with the increase of the tensile stress. And when propagating in the [100] direction, the change of the curve with a difference of 200MPa is relatively small;
(2)设定表面波沿Si表面[110]方向传播,当t为压应力时,频率-速度色散曲线如图4所示,在固定频率下,随着压应力的增大而减小;当t为拉应力时,频率-速度色散曲线如图5所示,在固定频率下,随着拉应力的增大而增大。且在[110]方向传播时,相差200MPa的曲线变化相对较大。(2) It is assumed that the surface wave propagates along the [110] direction of the Si surface. When t is the compressive stress, the frequency-velocity dispersion curve is shown in Figure 4. At a fixed frequency, it decreases with the increase of the compressive stress; When t is the tensile stress, the frequency-velocity dispersion curve is shown in Figure 5. At a fixed frequency, it increases with the increase of the tensile stress. And when propagating in the [110] direction, the curve with a difference of 200MPa changes relatively greatly.
根据以上规律即可对样片薄膜残余应力的大小进行排序。通过改变应力t的值来找出与实验频散曲线最相近的理论曲线,从而确定被测样片所对应的t值。重复试验测得一组样片的应力t值,进行排序,从而定性确定样片薄膜残余应力的大小排列。According to the above rules, the residual stress of the sample film can be sorted. By changing the value of stress t to find the theoretical curve closest to the experimental dispersion curve, so as to determine the value of t corresponding to the tested sample. Repeat the test to measure the stress t values of a group of samples and sort them, so as to qualitatively determine the size and arrangement of the residual stress of the sample films.
表1薄膜/衬底结构的参数设定Table 1 Parameter setting of film/substrate structure
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Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108168747A (en) * | 2018-02-11 | 2018-06-15 | 浙江大学 | A kind of workpiece surface residual stress measurement devices and methods therefor based on laser-ultrasound |
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Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5546811A (en) * | 1995-01-24 | 1996-08-20 | Massachusetts Instittue Of Technology | Optical measurements of stress in thin film materials |
CN101876647A (en) * | 2010-07-05 | 2010-11-03 | 天津大学 | Ultrasonic surface wave two-way detection method of Young's modulus and Poisson's constant |
CN102520066A (en) * | 2011-11-24 | 2012-06-27 | 天津大学 | Method for measuring Young modulus of inlaid thin film |
CN203688116U (en) * | 2013-12-18 | 2014-07-02 | 深圳职业技术学院 | Thin film stress tester |
CN105300578A (en) * | 2015-11-20 | 2016-02-03 | 西南交通大学 | Ultrasonic-wave stress detection device capable of adjusting acoustic beam angle and test area |
CN205449361U (en) * | 2015-12-23 | 2016-08-10 | 北京航天益森风洞工程技术有限公司 | Residual stress test equipment |
-
2016
- 2016-10-21 CN CN201610919414.3A patent/CN106546368A/en active Pending
Patent Citations (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5546811A (en) * | 1995-01-24 | 1996-08-20 | Massachusetts Instittue Of Technology | Optical measurements of stress in thin film materials |
CN101876647A (en) * | 2010-07-05 | 2010-11-03 | 天津大学 | Ultrasonic surface wave two-way detection method of Young's modulus and Poisson's constant |
CN102520066A (en) * | 2011-11-24 | 2012-06-27 | 天津大学 | Method for measuring Young modulus of inlaid thin film |
CN203688116U (en) * | 2013-12-18 | 2014-07-02 | 深圳职业技术学院 | Thin film stress tester |
CN105300578A (en) * | 2015-11-20 | 2016-02-03 | 西南交通大学 | Ultrasonic-wave stress detection device capable of adjusting acoustic beam angle and test area |
CN205449361U (en) * | 2015-12-23 | 2016-08-10 | 北京航天益森风洞工程技术有限公司 | Residual stress test equipment |
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CN108168747A (en) * | 2018-02-11 | 2018-06-15 | 浙江大学 | A kind of workpiece surface residual stress measurement devices and methods therefor based on laser-ultrasound |
CN108426545A (en) * | 2018-03-22 | 2018-08-21 | 天津大学 | A method of using ultrasonic surface wave non-destructive testing film thickness |
CN108871640A (en) * | 2018-06-13 | 2018-11-23 | 西安交通大学 | Residual stress nondestructive detection system and method based on transient grating Laser thermo-elastic generated surface acoustic waves |
CN108871640B (en) * | 2018-06-13 | 2020-03-31 | 西安交通大学 | Residual stress non-destructive testing system and method based on transient grating laser ultrasonic surface wave |
CN108827514A (en) * | 2018-07-19 | 2018-11-16 | 天津大学 | A kind of method of laser nondestructive characterisation (NDC) silica membrane residual stress |
CN109521090A (en) * | 2018-10-18 | 2019-03-26 | 天津大学 | A kind of optimization method of laser nondestructive characterisation (NDC) film Young's modulus |
CN112880895A (en) * | 2019-11-29 | 2021-06-01 | 哈尔滨工业大学 | Nonlinear ultrasonic wave-based large-scale high-speed rotation equipment blade residual stress measurement method |
CN112880895B (en) * | 2019-11-29 | 2022-09-20 | 哈尔滨工业大学 | Nonlinear ultrasonic wave-based large-scale high-speed rotation equipment blade residual stress measurement method |
CN111931405A (en) * | 2020-07-31 | 2020-11-13 | 天津大学 | Parameter optimization method of laser-excited surface acoustic wave measurement system |
CN113543548A (en) * | 2021-07-14 | 2021-10-22 | 深圳普泰电气有限公司 | Ultrahigh current monitoring and processing system |
CN113543548B (en) * | 2021-07-14 | 2022-09-09 | 深圳普泰电气有限公司 | Ultrahigh current monitoring and processing system |
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