CN106855389A - The AFM system mechanical drift compensation method of view-based access control model sensing - Google Patents
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Abstract
Description
技术领域 technical field
本发明属于精密测量领域,具体涉及一种基于视觉传感的AFM系统机械漂移补偿方法。 The invention belongs to the field of precision measurement, and in particular relates to a method for compensating mechanical drift of an AFM system based on vision sensing.
背景技术 Background technique
AFM(Atomic Force Microscope,原子力显微镜)通过检测探针与样品表面原子间作用力进行形貌探测及微纳制造加工,现广泛应用于半导体、纳米功能材料、生物、化工等纳米相关学科的研究领域中。AFM长时间工作过程中,环境温度变化、机械震动、电磁干扰等因素导致系统存在严重的漂移,引起待测物体形貌图像畸变失真以及位置测量误差。 AFM (Atomic Force Microscope, Atomic Force Microscope) conducts morphology detection and micro-nano manufacturing and processing by detecting the force between the probe and the surface atoms of the sample. It is now widely used in the research fields of semiconductors, nano-functional materials, biology, and chemical engineering. middle. During the long-term working process of AFM, environmental temperature changes, mechanical vibration, electromagnetic interference and other factors lead to serious drift of the system, causing distortion of the image of the object to be measured and position measurement errors.
目前对AFM系统漂移研究研究方向可以分成两个大类:其一是在硬件设计上抑制漂移,其二是从算法上对漂移进行校正。硬件设计上有附加传感器,优化扫描平台和建立双悬臂模型。附加传感器是在原子力系统添加辅助传感器,可用于测量垂直漂移或干扰,优化扫描平台通过提高扫描平台刚度,减小耦合从而减小测量过程中漂移,建立双悬臂模型引入参考探针作为位置参考,以上漂移补偿方法受到AFM系统组成结构的限制。软件算法补偿漂移方面,对于XY方向漂移,使用连续的AFM图像序列进行离线校正,实时跟踪的特征或结构的位置,通过原子跟踪结合前馈控制进行漂移补偿。对于垂直方向的漂移,研究者提出了通过控制环境温度,以减少AFM系统热漂移。以上针对AFM系统漂移的补偿方案均对系统漂移进行了改善,硬件改造的方法成本高且受AFM系统结构限制、软件算法离线校正的等方法不具有实时性,限制了其推广应用。 At present, the research direction of AFM system drift can be divided into two categories: one is to suppress drift in hardware design, and the other is to correct drift from an algorithm. There are additional sensors in the hardware design, optimizing the scanning platform and establishing a double cantilever model. The additional sensor is an auxiliary sensor added to the atomic force system, which can be used to measure vertical drift or interference. The optimization of the scanning platform increases the stiffness of the scanning platform and reduces the coupling to reduce the drift during the measurement process. The dual cantilever model is established and the reference probe is used as a position reference. The above drift compensation methods are limited by the composition structure of the AFM system. In terms of software algorithm compensation drift, for XY direction drift, continuous AFM image sequences are used for offline correction, and the position of features or structures tracked in real time is compensated by atomic tracking combined with feedforward control. For the drift in the vertical direction, the researchers proposed to reduce the thermal drift of the AFM system by controlling the ambient temperature. The above compensation schemes for AFM system drift all improve the system drift. The method of hardware transformation is costly and limited by the structure of the AFM system, and the offline correction of software algorithms is not real-time, which limits its popularization and application.
发明内容 Contents of the invention
本发明的技术解决问题是:克服现有AFM系统漂移补偿方法的不足,提出一种新的AFM系统漂移补偿方法,在非接触模式和不改造硬件的条件下,对AFM系统漂移进行实时高精度补偿。 The technical solution problem of the present invention is: to overcome the deficiencies of the existing AFM system drift compensation method, propose a new AFM system drift compensation method, under the condition of non-contact mode and no modification of hardware, real-time high-precision for AFM system drift compensate.
本发明的技术解决方案为:提供了一种基于视觉传感的AFM系统机械漂移补偿方法,其特征在于,所述视觉传感部分包括一个AFM悬臂末端微球和一个样品表面微球,通过视觉传感技术对AFM悬臂末端微球和样品表面微球之间距离的测量,计算AFM系统的漂移量,包括以下步骤: The technical solution of the present invention is to provide a method for compensating mechanical drift of an AFM system based on visual sensing, wherein the visual sensing part includes a microsphere at the end of an AFM cantilever and a microsphere on the surface of a sample. Sensing technology measures the distance between the microspheres at the end of the AFM cantilever and the microspheres on the sample surface, and calculates the drift of the AFM system, including the following steps:
步骤一、基于视觉传感技术计算AFM悬臂末端微球和样品表面微球位置; Step 1. Calculate the position of the microsphere at the end of the AFM cantilever and the microsphere on the sample surface based on the visual sensing technology;
步骤二、根据悬臂末端微球和样品表面微球位置计算两者之间距离变化量,从而得到AFM系统漂移量; Step 2. According to the position of the microsphere at the end of the cantilever and the position of the microsphere on the sample surface, the distance change between the two is calculated, so as to obtain the drift of the AFM system;
步骤三、根据步骤二计算的漂移量,调节AFM悬臂末端微球所在扫描平台的驱动电压,使AFM悬臂末端微球与样品表面微球之间距离在阈值范围内。 Step 3. According to the drift calculated in step 2, adjust the driving voltage of the scanning platform where the microsphere at the end of the AFM cantilever is located, so that the distance between the microsphere at the end of the AFM cantilever and the microsphere on the sample surface is within the threshold range.
进一步,所述步骤一之前,设定AFM悬臂末端微球与样品表面微球之间距离阈值。 Further, before the first step, a distance threshold between the microspheres at the end of the AFM cantilever and the microspheres on the sample surface is set.
所述步骤二中,计算悬臂末端微球和样品表面微球位置之间距离变化量的是对悬臂末端微球和样品表面微球位置变化量作差,具体为, In the second step, the calculation of the distance change between the microsphere at the end of the cantilever and the microsphere on the sample surface is to make a difference between the position change of the microsphere at the end of the cantilever and the microsphere on the sample surface, specifically,
ddrift=d′-d=dcant,drift-dsubs,drift d drift =d′-d=d cant, drift -d subs, drift
其中,d为AFM系统中AFM悬臂末端微球和样品表面微球之间初始距离,d′为AFM悬臂末端微球和样品表面微球之间漂移之后的距离,dcant,drift为AFM悬臂末端微球漂移量,dsubs,drift为样品表面微球漂移量。 Among them, d is the initial distance between the microsphere at the end of the AFM cantilever and the microsphere on the sample surface in the AFM system, d' is the distance after the drift between the microsphere at the end of the AFM cantilever and the microsphere on the sample surface, d cant,drift is the end of the AFM cantilever Microsphere drift, d subs, drift is the microsphere drift on the sample surface.
所述的AFM悬臂末端微球漂移量dcant,drift,其特征在于,dcant,drift由测量AFM悬臂末端微球位置变化的变化量的得到。 The drift d cant,drift of the microsphere at the end of the AFM cantilever is characterized in that d cant,drift is obtained by measuring the change in the position of the microsphere at the end of the AFM cantilever.
所述的样品表面微球漂移量dsubs,drift,其特征在于,dsubs,drift是样品表面微球位置变化量。 The sample surface microsphere drift d subs,drift is characterized in that, d subs,drift is the amount of position change of the sample surface microsphere.
所述步骤三中,通过PID闭环控制,根据漂移量调节AFM悬臂压电平台驱动电压,从而控制AFM悬臂末端微球位置,使悬臂末端微球与样品表面微球之间距离在阈值范围内。 In the third step, the driving voltage of the AFM cantilever piezoelectric platform is adjusted according to the drift amount through PID closed-loop control, thereby controlling the position of the microsphere at the end of the AFM cantilever, so that the distance between the microsphere at the end of the cantilever and the microsphere on the sample surface is within a threshold value.
所述的通过视觉传感技术对AFM悬臂末端微球和样品表面微球之间距离的测量,包括以下步骤: The measurement of the distance between the microspheres at the end of the AFM cantilever and the microspheres on the sample surface by the visual sensing technology comprises the following steps:
步骤一、采集一系列已知位置处的微球图像,将每处位置的微球图像提取特征转换为径向矢量,建立关于微球位置信息的微球图像标定模型; Step 1. Collect a series of microsphere images at known positions, convert the extracted features of the microsphere images at each position into radial vectors, and establish a microsphere image calibration model for the position information of the microspheres;
步骤二、采集标定位置范围内的微球图像与步骤一中标定模型比较,得到微球位置。 Step 2: collecting microsphere images within the range of the calibration position and comparing with the calibration model in step 1 to obtain the position of the microsphere.
进一步,所述的步骤一中微球图像提取特征,其特征在于,根据图像中灰度值强度重心确定微球中心位置,将图像视为以中心位置为圆心的一系列圆环,计算每个圆环上灰度值的平均值,一系列圆环上的灰度值平均值按序组合为一个径向矢量。 Further, the microsphere image extraction feature in the step 1 is characterized in that the center position of the microsphere is determined according to the gray value intensity center of gravity in the image, the image is regarded as a series of rings with the center position as the center, and each The average value of the gray value on the ring, the average value of the gray value on a series of rings is combined into a radial vector in sequence.
所述的步骤二,其特征在于,将采集的微球图像转换为径向矢量,与关于位置信息的标定模型比较,根据非线性最小二乘法定位微球位置。 The second step is characterized in that the collected microsphere image is converted into a radial vector, compared with the calibration model of position information, and the position of the microsphere is located according to the non-linear least square method.
本发明基于视觉传感的AFM系统机械漂移补偿方法,通过基于视觉传感技术测量悬臂末端微球与样品表面微球位置测量AFM系统漂移,在不修改原始AFM系统基础上直接测量AFM悬臂和样品表面之间漂移,可以在扫描过程中实时地解决漂移问题,这种方法可以有效的适应长时间扫描中的漂移校正,具有能适应普通的样品、自动、实时校正等优点。 The mechanical drift compensation method of the AFM system based on visual sensing in the present invention measures the drift of the AFM system by measuring the position of the microsphere at the end of the cantilever and the microsphere on the sample surface based on the visual sensing technology, and directly measures the AFM cantilever and the sample without modifying the original AFM system. Drift between surfaces can solve the drift problem in real time during the scanning process. This method can effectively adapt to drift correction in long-term scanning, and has the advantages of being able to adapt to ordinary samples, automatic, and real-time correction.
附图说明 Description of drawings
图1为AFM悬臂末端微球与样品表面微球示意图。 Figure 1 is a schematic diagram of the microspheres at the end of the AFM cantilever and the microspheres on the sample surface.
图1中,(1)为样品基底玻片,(2)为样品表面微球,(3)为AFM悬臂末端微球,(4)为微悬臂,(5)为压电驱动器,(6)为悬臂支撑片,虚线为漂移后的示意位置。 In Fig. 1, (1) is the sample substrate glass slide, (2) is the microsphere on the sample surface, (3) is the microsphere at the end of the AFM cantilever, (4) is the microcantilever, (5) is the piezoelectric driver, (6) is the cantilever supporting piece, and the dotted line is the schematic position after drifting.
图2为基于视觉传感定位的AFM系统机械漂移补偿流程图。 Fig. 2 is a flow chart of AFM system mechanical drift compensation based on visual sensing positioning.
图3为微球定位过程流程图。图4为根据微球位置进行漂移补偿流程图。 Figure 3 is a flow chart of the microsphere positioning process. Fig. 4 is a flow chart of drift compensation according to the position of the microsphere.
具体实施方式 detailed description
为了使本发明的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本发明进行进一步详细说明。此处所描述的具体实施例仅用以解释本发明,并不用于限定本发明。 In order to make the object, technical solution and advantages of the present invention clearer, the present invention will be further described in detail below in conjunction with the accompanying drawings and embodiments. The specific embodiments described here are only used to explain the present invention, not to limit the present invention.
本发明方法在不改造AFM系统硬件的条件下,采用视觉传感技术,以非接触方式实 时地测量和补偿AFM系统漂移。基于视觉传感的AFM系统机械漂移补偿方法,其特征在于,所述视觉传感部分包括一个AFM悬臂末端微球和一个样品表面微球,微球是直径为10μm-50μm的微球,通过视觉传感技术对AFM悬臂末端微球和样品表面微球之间距离的测量,计算AFM系统的漂移量。 The method of the invention adopts the visual sensing technology to measure and compensate the drift of the AFM system in real time in a non-contact manner without modifying the hardware of the AFM system. The mechanical drift compensation method of the AFM system based on visual sensing is characterized in that the visual sensing part includes a microsphere at the end of the AFM cantilever and a microsphere on the surface of the sample, and the microsphere is a microsphere with a diameter of 10 μm-50 μm. Sensing technology measures the distance between the microspheres at the end of the AFM cantilever and the microspheres on the sample surface, and calculates the drift of the AFM system.
所述的基于视觉传感的AFM系统机械漂移补偿方法具体包括以下步骤: The described AFM system mechanical drift compensation method based on visual sensing specifically includes the following steps:
步骤一、基于视觉传感技术计算AFM悬臂末端微球和样品表面微球位置; Step 1. Calculate the position of the microsphere at the end of the AFM cantilever and the microsphere on the sample surface based on the visual sensing technology;
步骤二、根据悬臂末端微球和样品表面微球位置计算两者之间距离变化量,从而得到AFM系统漂移量; Step 2. According to the position of the microsphere at the end of the cantilever and the position of the microsphere on the sample surface, the distance change between the two is calculated, so as to obtain the drift of the AFM system;
步骤三、根据步骤二计算的漂移量,调节AFM悬臂末端微球所在扫描平台的驱动电压,使AFM悬臂末端微球与样品表面微球之间距离在阈值范围内。 Step 3. According to the drift calculated in step 2, adjust the driving voltage of the scanning platform where the microsphere at the end of the AFM cantilever is located, so that the distance between the microsphere at the end of the AFM cantilever and the microsphere on the sample surface is within the threshold range.
进一步,所述步骤一之前,设定AFM悬臂末端微球与样品表面微球之间距离阈值。 Further, before the first step, a distance threshold between the microspheres at the end of the AFM cantilever and the microspheres on the sample surface is set.
所述步骤一中,通过视觉传感技术对AFM悬臂末端微球和样品表面微球之间距离的测量,包括以下步骤: In said step one, the measurement of the distance between the microspheres at the end of the AFM cantilever and the microspheres on the sample surface by visual sensing technology includes the following steps:
步骤一、采集一系列已知位置处的微球图像,将每处位置的微球图像提取特征转换为径向矢量,建立关于微球位置信息的微球图像标定模型; Step 1. Collect a series of microsphere images at known positions, convert the extracted features of the microsphere images at each position into radial vectors, and establish a microsphere image calibration model for the position information of the microspheres;
步骤二、采集标定位置范围内的微球图像与步骤一中标定模型比较,得到微球位置。 Step 2: collecting microsphere images within the range of the calibration position and comparing with the calibration model in step 1 to obtain the position of the microsphere.
所述的微球图像提取特征,其特征在于,根据图像中灰度值强度重心确定微球中心位置,将图像视为以中心位置为圆心的一系列圆环,计算每个圆环上灰度值的平均值,一系列圆环上的灰度值平均值按序组合为一个径向矢量。 The microsphere image extraction feature is characterized in that the central position of the microsphere is determined according to the gray value intensity center of gravity in the image, the image is regarded as a series of rings with the center position as the center, and the gray level on each ring is calculated. The average value of the value, the average value of the gray value on a series of rings is combined into a radial vector in sequence.
所述的采集标定位置范围内的微球图像与标定模型比较,其特征在于,将采集的微球图像转换为径向矢量,与关于位置信息的标定模型比较,根据非线性最小二乘法定位微球位置。 The microsphere image within the scope of the collected calibration position is compared with the calibration model, which is characterized in that the collected microsphere image is converted into a radial vector, compared with the calibration model about the position information, and the microsphere is positioned according to the non-linear least squares method. ball position.
所述步骤二中,计算悬臂末端微球和样品表面微球位置之间距离变化量的是对悬臂末端微球和样品表面微球位置变化量作差,具体为,ddrift=d′-d=dcant,drift-dsubs,drift In the second step, the calculation of the distance change between the microsphere at the end of the cantilever and the microsphere on the sample surface is to make a difference between the position change of the microsphere at the end of the cantilever and the microsphere on the sample surface, specifically, d drift = d'-d =d cant, drift -d subs, drift
其中,d为AFM系统中AFM悬臂末端微球和样品表面微球之间初始距离,d′为AFM悬臂末端微球和样品表面微球之间漂移之后的距离,dcant,drift为AFM悬臂末端微球漂移量,dsubs,drift为样品表面微球漂移量。 Among them, d is the initial distance between the microsphere at the end of the AFM cantilever and the microsphere on the sample surface in the AFM system, d' is the distance after the drift between the microsphere at the end of the AFM cantilever and the microsphere on the sample surface, d cant,drift is the end of the AFM cantilever Microsphere drift, d subs, drift is the microsphere drift on the sample surface.
在常规的AFM系统形貌探测中,由AFM悬臂末端微球探测到的样品形变量理论为,δideal=dpiezo,drive-ddef In the conventional AFM system shape detection, the theory of the sample deformation detected by the microsphere at the end of the AFM cantilever is, δ ideal = d piezo, drive -d def
其中,dpiezo,drive为压电驱动器驱动AFM悬臂末端微球位移,ddef为由于样品与探针间相互作用力引起的位移。 Among them, d piezo, drive is the displacement of the microsphere at the end of the AFM cantilever driven by the piezoelectric driver, and d def is the displacement caused by the interaction force between the sample and the probe.
由于AFM系统漂移的影响,实际的样品形变量为, Due to the influence of AFM system drift, the actual sample deformation is,
δreal=dpiezo,drive+dcant,drift-dsubs,drift-ddef δ real =d piezo,drive +d cant,drift -d subs,drift -d def
其中,样品表面漂移可以根据样品表面微球位置dbead2测量得到,悬臂漂移dcant,drift可以通过AFM悬臂末端微球位置dbead1测量得到,具体为, Among them, the sample surface drift can be obtained by measuring the position of the microsphere on the sample surface d bead2 , and the cantilever drift d cant,drift can be obtained by measuring the position of the microsphere at the end of the AFM cantilever d bead1 , specifically,
dbead1=dpiezo,drive+dcant,drift-ddef d bead1 = d piezo,drive +d cant,drift -d def
dcant,drift=dbead1-dpiezo,drive+ddef d cant, drift = d bead1 -d piezo, drive +d def
所述的压电驱动器驱动AFM悬臂末端微球位移dpiezo,drive,以及由于样品与探针间相互作用力引起的位移ddef可以直接从AFM系统中测量。 The piezoelectric driver drives the displacement d piezo,drive of the microsphere at the end of the AFM cantilever, and the displacement d def caused by the interaction force between the sample and the probe can be directly measured from the AFM system.
所述步骤三中,根据测量的微球位置实时地补偿漂移量。通过PID闭环控制,根据漂移量调节AFM悬臂压电平台驱动电压,从而控制AFM悬臂末端微球位置,使悬臂末端微球与样品表面微球之间距离在阈值范围内。 In the third step, the drift amount is compensated in real time according to the measured position of the microsphere. Through the PID closed-loop control, the driving voltage of the piezoelectric platform of the AFM cantilever is adjusted according to the drift, so as to control the position of the microsphere at the end of the AFM cantilever, so that the distance between the microsphere at the end of the cantilever and the microsphere on the sample surface is within the threshold range.
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