CN1632518A - Measurement Method of Atomic Force Microscope Based on Angle Measurement - Google Patents
Measurement Method of Atomic Force Microscope Based on Angle Measurement Download PDFInfo
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Abstract
Description
技术领域Technical field
本发明涉及一种基于角度测量的原子力显微镜测量方法,属于原子力显微镜(AFM)的探针/悬臂梁信号的检测方法。The invention relates to an atomic force microscope measurement method based on angle measurement, which belongs to a detection method of a probe/cantilever beam signal of an atomic force microscope (AFM).
背景技术 Background technique
当悬臂梁的端部受力时,其端部会产生两种变形,一种是挠度,另一种是转角。原子力显微镜利用微悬臂梁尖端的探针,当探针接近或接触被测物体表面时,探针与样品之间会发生力的相互作用,该作用力会使微悬臂梁产生弯曲变化,因此,微悬臂梁弯曲量的变化可以通过两种方式进行检测,即测量原子力显微镜的微悬臂梁的挠度变化,或者测量原子力显微镜的微悬臂梁的尖端转角变化。When the end of the cantilever beam is stressed, two deformations will occur at the end, one is deflection and the other is rotation angle. The atomic force microscope uses the probe at the tip of the micro-cantilever beam. When the probe approaches or touches the surface of the object to be measured, there will be a force interaction between the probe and the sample, and the force will cause the micro-cantilever beam to bend. Therefore, The change of the bending amount of the micro-cantilever can be detected in two ways, that is, measuring the change of the deflection of the micro-cantilever of the atomic force microscope, or measuring the change of the tip rotation angle of the micro-cantilever of the atomic force microscope.
目前以原子力显微镜为代表的通过检测微悬臂梁的弯曲变化得到被测物体表面信息的这一类仪器,均采用测量微悬臂梁的受力后的挠度变化,如美国Veeco公司的多功能原子力显微镜,日本精工的原子力显微镜等,当激光打到微悬臂梁上时,由于微悬臂梁挠度的变化,引起反射光的偏摆,使光电探测器上光点位置发生变化,通过检测光点位置的变化量,从而得到微悬臂梁的挠度变化量,进而得到测力变化量和物体表面轮廓。这种方法虽然结构上简单适于商业生产,但在此类显微镜的恒力模式下扫描过程中,由于探针固定端位置的改变,从而引入测量原理误差,要获得高精度的测量结果,必须进行误差修正或严格的校正。At present, the type of instruments represented by atomic force microscopes that obtain the surface information of the measured object by detecting the bending change of the micro-cantilever beam all use the measurement of the deflection change of the micro-cantilever beam after being stressed, such as the multifunctional atomic force microscope of the American Veeco company. , Japan's Seiko's atomic force microscope, etc., when the laser hits the micro-cantilever beam, due to the change in the deflection of the micro-cantilever beam, the deflection of the reflected light is caused, and the position of the light spot on the photodetector changes. By detecting the position of the light spot The amount of change, so as to obtain the amount of deflection change of the micro-cantilever beam, and then obtain the amount of change in force measurement and the surface profile of the object. Although this method is simple in structure and suitable for commercial production, in the scanning process of this type of microscope under the constant force mode, due to the change of the position of the fixed end of the probe, the error of the measurement principle is introduced. To obtain high-precision measurement results, it is necessary to Make error corrections or strict corrections.
发明内容Contents of Invention
本发明的目的在于提供一种基于角度测量的原子力显微镜测量方法,该方法可以克服现有原子力显微镜探针挠度测量方法引入的原理性误差及其后续修正问题,又能减小现有方法对于被测样品形状、体积、重量等的限制,扩大原子力显微镜的适用范围。The object of the present invention is to provide a measurement method of atomic force microscope based on angle measurement, which can overcome the principle error and subsequent correction problems introduced by the existing method of measuring the probe deflection of atomic force microscope, and can reduce the impact of the existing method on the Measure the limitations of the sample shape, volume, weight, etc., and expand the scope of application of the atomic force microscope.
本发明的目的是这样实现的:基于角度测量的AFM测量方法,实现该方法采用角度测量型原子力显微镜测量装置,原子力显微镜的悬臂梁位移测量装置采用光学差动式角度传感器,所述的角度测量传感器包括准直光源、会聚透镜、1/4波片、偏光分光镜、分光镜、两个临界角棱镜、两个光电二极管。该方法的特征在于将入射光汇聚后垂直入射到原子力显微镜的探针表面,其反射光的偏转角度经角度测量传感器检测,被反射的激光携带悬臂梁的转角变化信息进入该角度测量装置;角度测量装置采用光学差动式测量方法,该方法在初始测力设定值时,角度测量装置输出信号为零,当扫描过程中测力发生变化时,悬臂梁的弯曲角度发生变化,该变化量被角度测量装置检测并转换成与角度变化值成比例的电信号;该电信号经放大后再经信号分析处理,得到由于测力变化而引起的悬臂梁的角度变化,进而得到探针的测力变化/物体表面形貌轮廓。The object of the present invention is achieved like this: based on the AFM measurement method of angle measurement, the method adopts an angle measurement type atomic force microscope measurement device, and the cantilever beam displacement measurement device of the atomic force microscope adopts an optical differential angle sensor, and the angle measurement The sensor includes a collimated light source, a converging lens, a 1/4 wave plate, a polarizing beam splitter, a beam splitter, two critical angle prisms, and two photodiodes. The method is characterized in that after the incident light is converged, it is vertically incident on the probe surface of the atomic force microscope, and the deflection angle of the reflected light is detected by the angle measurement sensor, and the reflected laser carries the angle change information of the cantilever beam into the angle measurement device; The measurement device adopts the optical differential measurement method. In this method, the output signal of the angle measurement device is zero when the initial force measurement is set. When the force measurement changes during the scanning process, the bending angle of the cantilever beam changes. It is detected by the angle measuring device and converted into an electrical signal proportional to the angle change value; the electrical signal is amplified and then analyzed and processed to obtain the angle change of the cantilever beam caused by the change of the force measurement, and then obtain the measured value of the probe. Force variation/object surface topography profile.
本发明的优点在于平面内扫描(XY)驱动装置与纵向(Z)跟踪驱动装置分离,样品台与XY扫描驱动装置结合在一起,样品台只进行平面内扫描;探针经探针夹持架与Z向跟踪驱动器相结合,实现Z向与XY向运动的分离,从而减小了被测样品形状、体积、重量等的限制,扩大原子力显微镜的适用范围,同时由于测量的是微悬臂梁尖端的角度变化,在恒力模式下探针固定端的位置改变不会影响转角的测量,因此该方法既可克服由于采用挠度测量方法引入的原理性误差及其后续修正问题。The advantage of the present invention is that the in-plane scanning (XY) driving device is separated from the longitudinal (Z) tracking driving device, the sample stage is combined with the XY scanning driving device, and the sample stage only performs in-plane scanning; the probe passes through the probe holder Combined with the Z-direction tracking driver, the separation of Z-direction and XY-direction motion is realized, thereby reducing the limitation of the shape, volume, weight, etc. of the sample to be measured, and expanding the scope of application of the atomic force microscope. In the constant force mode, the position change of the fixed end of the probe will not affect the measurement of the rotation angle. Therefore, this method can overcome the principle error introduced by the deflection measurement method and its subsequent correction problems.
附图说明Description of drawings
图1为实现本发明方法的装置结构示意图。Fig. 1 is a schematic diagram of the device structure for realizing the method of the present invention.
图2为基于角度测量的AFM测量方法原理图Figure 2 is a schematic diagram of the AFM measurement method based on angle measurement
图中:1、8为临界角棱镜,2为集成了1/4波片的分光镜,3为集成了1/4波片5的偏光分光镜,4为集成了会聚透镜的半导体激光器,6为Z向跟踪用压电陶瓷驱动器PZT,它集成了AFM探针夹持器和AFM探针,7、9为光电接收器。In the figure: 1 and 8 are critical angle prisms, 2 is a beam splitter integrated with a 1/4 wave plate, 3 is a polarizing beam splitter integrated with a 1/4 wave plate 5, 4 is a semiconductor laser integrated with a converging lens, 6 PZT is the piezoelectric ceramic driver for Z-direction tracking, which integrates the AFM probe holder and AFM probe, and 7 and 9 are photoelectric receivers.
具体实施方式 Detailed ways
基于角度测量的AFM测量方法,采用光学差动式角度测量装置,检测原子力显微镜微悬臂梁的转角变化量,其过程是:半导体激光器4发出的光首先经透镜汇聚,经偏光分光镜3后,原光束被分为S偏光和P偏光,其中S偏光被反射后经1/4波片5后成为圆偏光,入射到原子力显微镜的探针6反射面上,从AFM探针表面被反射回来的圆偏光,该圆偏光携带悬臂梁的转角变化信息,通过1/4波片后成为P偏光,再经分光镜2后分成能量相等的两束互相正交的光,其偏振状态保持不变,分别入射到两个沿直角方向安置的棱镜1和8内,出射光光强分别被光电接受器9和7检测;在初始测力设定值时,可以认为角度测量装置输出信号为“零”;当扫描过程中测力发生变化时,悬臂梁的弯曲角度发生变化,反射光即相对于角度测量装置的入射光,其入射角度也产生相应的变化,该变化量为微悬臂梁角度变化量的一倍,使被测量得到放大。The AFM measurement method based on angle measurement uses an optical differential angle measurement device to detect the change in the rotation angle of the micro-cantilever beam of the atomic force microscope. The process is as follows: the light emitted by the semiconductor laser 4 first converges through the lens, and after passing through the polarizing beam splitter 3, The original beam is divided into S-polarized light and P-polarized light. After the S-polarized light is reflected, it passes through the 1/4 wave plate 5 and becomes circularly polarized light. It is incident on the reflective surface of the probe 6 of the atomic force microscope and is reflected back from the surface of the AFM probe. Circularly polarized light, the circularly polarized light carries the change information of the cantilever beam’s rotation angle, becomes P polarized light after passing through the 1/4 wave plate, and then splits into two mutually orthogonal beams of equal energy after passing through the beam splitter 2, and its polarization state remains unchanged. Respectively incident into two
由于采用差动测量方法,来自悬臂梁的反射光被半透半反镜2分成两束光后,分别入射进两个棱镜,即图1中的(1)、(2)两部分,当反射光的角度有偏摆时,两个棱镜的入射光的入射角分别增大/减小Δθ,反射率变化量也分别增大或减小,出射光的光强被光电二极管检测并转化为光电流,两路光电流信号经过电流-电压变换以及加法、减法和除法运算后,得到线性化处理后的角度变化量,即该变化量被角度测量装置检测并转换成与角度变化值成比例的电信号。该电信号经放大后再经信号分析处理,得到由于测力变化而引起的悬臂梁的角度变化,由于AFM探针/悬臂梁尖端的角度与挠度存在确定的比例关系,根据此关系得到物体表面高低变化量,进而得到探针的测力变化/物体表面形貌轮廓。Due to the differential measurement method, the reflected light from the cantilever beam is divided into two beams by the half-mirror 2, and then enters into two prisms respectively, that is, the two parts (1) and (2) in Fig. 1. When the reflection When the angle of light is deflected, the incident angles of the incident light of the two prisms increase/decrease Δθ respectively, and the reflectivity changes also increase or decrease respectively. The light intensity of the outgoing light is detected by the photodiode and converted into light Current, the two-way photocurrent signal undergoes current-voltage conversion and addition, subtraction and division operations to obtain the angle change after linearization, that is, the change is detected by the angle measuring device and converted into a value proportional to the angle change. electric signal. The electrical signal is amplified and then analyzed and processed to obtain the angle change of the cantilever beam caused by the change of force measurement. Since there is a certain proportional relationship between the angle of the tip of the AFM probe/cantilever beam and the deflection, the surface of the object can be obtained according to this relationship. High and low changes, and then obtain the force measurement changes of the probe/surface topography of the object.
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Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
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| CN102338620A (en) * | 2011-10-13 | 2012-02-01 | 镇江耐丝新型材料有限公司 | Device and method for measuring rotation angle and wave height of metal wire |
| CN105408721A (en) * | 2013-06-27 | 2016-03-16 | 科磊股份有限公司 | Polarization Measurement of Metrology Target and Corresponding Target Design |
| CN107064564A (en) * | 2016-01-26 | 2017-08-18 | 三星电子株式会社 | Cantilever device, inspection device, method of analyzing surface, and method of forming micro pattern |
| CN107807269A (en) * | 2017-11-26 | 2018-03-16 | 吉林大学 | A kind of photoelectrical current detection means and its detection method for a variety of cables |
| CN110869772A (en) * | 2017-04-07 | 2020-03-06 | 英菲尼特斯马有限公司 | Scanning probe system for controlling inclination angle of probe tip |
| WO2020206826A1 (en) * | 2019-04-09 | 2020-10-15 | 天津大学 | Ultra-thin atomic force microscope head |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| JPH06258068A (en) * | 1993-03-04 | 1994-09-16 | Canon Inc | Interatomic force microscope |
| JP2967965B2 (en) * | 1993-06-18 | 1999-10-25 | 株式会社日立製作所 | Scanner for scanning probe microscope and scanning probe microscope provided with the same |
| CN1076474C (en) * | 1993-12-27 | 2001-12-19 | 松下电气产业株式会社 | Device and method for evaluating crystallization |
| JPH0961442A (en) * | 1995-08-23 | 1997-03-07 | Mitsubishi Electric Corp | Atomic force microscope and its measuring head |
| CN100387968C (en) * | 1999-06-05 | 2008-05-14 | 株式会社大宇电子 | Atomic force microscope and method for driving the same |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| CN102338620A (en) * | 2011-10-13 | 2012-02-01 | 镇江耐丝新型材料有限公司 | Device and method for measuring rotation angle and wave height of metal wire |
| CN105408721A (en) * | 2013-06-27 | 2016-03-16 | 科磊股份有限公司 | Polarization Measurement of Metrology Target and Corresponding Target Design |
| US10458777B2 (en) | 2013-06-27 | 2019-10-29 | Kla-Tencor Corporation | Polarization measurements of metrology targets and corresponding target designs |
| CN105408721B (en) * | 2013-06-27 | 2020-01-10 | 科磊股份有限公司 | Polarization measurement of metrology targets and corresponding target design |
| US11060845B2 (en) | 2013-06-27 | 2021-07-13 | Kla Corporation | Polarization measurements of metrology targets and corresponding target designs |
| CN107064564A (en) * | 2016-01-26 | 2017-08-18 | 三星电子株式会社 | Cantilever device, inspection device, method of analyzing surface, and method of forming micro pattern |
| CN107064564B (en) * | 2016-01-26 | 2022-02-11 | 三星电子株式会社 | Cantilever device, inspection device, method of analyzing surface, and micropatterning method |
| CN110869772A (en) * | 2017-04-07 | 2020-03-06 | 英菲尼特斯马有限公司 | Scanning probe system for controlling inclination angle of probe tip |
| CN110869772B (en) * | 2017-04-07 | 2022-06-07 | 英菲尼特斯马有限公司 | Scanning probe system for controlling inclination angle of probe tip |
| CN107807269A (en) * | 2017-11-26 | 2018-03-16 | 吉林大学 | A kind of photoelectrical current detection means and its detection method for a variety of cables |
| CN107807269B (en) * | 2017-11-26 | 2023-12-15 | 吉林大学 | A photoelectric current detection device for various cables and its detection method |
| WO2020206826A1 (en) * | 2019-04-09 | 2020-10-15 | 天津大学 | Ultra-thin atomic force microscope head |
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