CN112964647B - Method and device for detecting ultrathin metal film by using spectroscopic ellipsometer - Google Patents
Method and device for detecting ultrathin metal film by using spectroscopic ellipsometer Download PDFInfo
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Abstract
Description
技术领域technical field
本发明涉及光学测量技术领域,具体涉及一种利用光谱椭偏仪检测超薄金属膜的方法和装置。另外,还涉及一种利用光谱椭偏仪的超薄金属膜的光学表征方法及装置。The invention relates to the technical field of optical measurement, in particular to a method and a device for detecting an ultra-thin metal film by using a spectroscopic ellipsometer. In addition, it also relates to an optical characterization method and device of an ultra-thin metal film using a spectroscopic ellipsometer.
背景技术Background technique
光谱椭偏仪是一种利用光的偏振特性获取待测样品信息的通用光学测量仪器。其基本原理是通过起偏器将特殊的椭圆偏振光投射到待测样品表面,通过测量待测样品的反射光(或透射光),以获得偏振光在反射(或透射)前后的偏振态变化(包括振幅比和相位差),从而提取出待测样品的相关物理(如光学参数、薄膜厚度等)信息。椭偏测量技术由于其属于无损检测且具有高灵敏度、高精度、可用于超薄膜及其制备过程中的实时监测等特点,具有其他测厚仪器所无法比拟的优势,已成为薄膜厚度和光学常数精确测量的重要手段之一,在薄膜研究领域具有不可替代的地位。通过光谱椭偏仪进行椭偏测量,能够获得材料的折射率、消光系数和复介电函数等光学性质,还可以进一步计算得到包括材料反射率、吸收率、透射率、光学带隙在内的相关光学参数。同时,椭偏技术还可用于获取材料组分、界面层性质和粗糙度等综合信息。然而,利用常规椭偏方法测量材料参数/性质还存在诸多局限,比如包括:在测量超厚(或超薄)金属膜时,由于超厚(或超薄)金属膜严重衰减(几乎不改变)椭偏信号使得常规方法难以准确测定超厚(或超薄)金属膜的光学参数和物理厚度等;常规椭偏测量方法所基于的椭偏方程是一组超越方程,无法得到解析解,必须首先建立物理模型再通过反演的方法确定模型中的参数,即所谓的trial and error方法,因此,在拟合过程中由于未知量的增加和限制条件的不足导致薄膜厚度和光学常数经常出现不唯一性;通常薄膜存在三种生长模式,即岛状生长,层状生长和岛-层混合生长,对于纳米尺度金属膜,薄膜形态受衬底表面、结构及形貌的影响较大,往往出现与常规薄膜或体材完全不同的形态或/和性质,利用椭偏仪分析这类薄膜(如表面粗糙,存在大量界面及孔洞等缺陷的薄膜)常需要谨慎选择合适的色散方程,约束方程的不足以及色散方程选择的复杂性使常规椭偏测量在弱信号条件下难以精确测定光学参量和物理参数等。Spectroscopic ellipsometer is a general-purpose optical measuring instrument that uses the polarization characteristics of light to obtain information about the sample to be measured. The basic principle is to project special elliptically polarized light onto the surface of the sample to be measured through a polarizer, and measure the reflected light (or transmitted light) of the sample to obtain the polarization state change of the polarized light before and after reflection (or transmission) (including amplitude ratio and phase difference), so as to extract the relevant physical (such as optical parameters, film thickness, etc.) information of the sample to be tested. Ellipsometry technology has the characteristics of non-destructive testing, high sensitivity, high precision, and can be used for real-time monitoring of ultra-thin films and their preparation process. It is one of the important means of accurate measurement and has an irreplaceable position in the field of thin film research. The ellipsometry of the spectroscopic ellipsometer can obtain the optical properties such as the refractive index, extinction coefficient and complex dielectric function of the material, and can also be further calculated to obtain the reflectivity, absorption rate, transmittance, and optical bandgap of the material. related optical parameters. At the same time, ellipsometry can also be used to obtain comprehensive information such as material composition, interface layer properties and roughness. However, there are still many limitations in using the conventional ellipsometry method to measure material parameters/properties, such as: when measuring ultra-thick (or ultra-thin) metal films, due to the serious attenuation (almost no change) of ultra-thick (or ultra-thin) metal films The ellipsometric signal makes it difficult for conventional methods to accurately measure the optical parameters and physical thickness of ultra-thick (or ultra-thin) metal films. Establish a physical model and then determine the parameters in the model by inversion method, which is the so-called trial and error method. Therefore, due to the increase of unknown quantities and the lack of limiting conditions in the fitting process, the film thickness and optical constants often appear to be non-unique. Generally, there are three growth modes in thin films, namely island growth, layer growth and island-layer mixed growth. Conventional films or bulk materials have completely different shapes and/or properties. Using ellipsometry to analyze such films (such as films with rough surfaces and a large number of defects such as interfaces and holes) often requires careful selection of appropriate dispersion equations. The lack of constraint equations And the complexity of the selection of the dispersion equation makes it difficult for conventional ellipsometry to accurately measure optical and physical parameters under weak signal conditions.
近年来,随着各种器件的微型化及集成度的提高,纳米厚度金属膜在半导体芯片和各种器件制造中愈加重要。纳米厚度金属薄膜由于其不同于其相应体材的独特性质,在微电子、集成光学、太阳能电池、生物医学、化学及航天技术等领域应用愈加广泛,并且表现出特定的新型功能而不可或缺。目前,检测纳米厚度薄膜的手段包括原子力显微镜、扫描电子显微镜、透射电子显微镜、扫描隧道显微镜、分光光度计以及各种膜厚仪等,这些手段或许能够实现亚纳米分辨率的检测,但由于其对器件的破坏性、操作复杂、检测效率低,而无法应用于实际生产线中。因此,无法满足快速发展的先进工艺控制及优化的检测要求。为了更好地解决纳米薄膜的厚度无法被快速、无损、高效地精确测量问题,尤其是针对常规椭偏测量无法精确测定超薄金属膜(比如厚度在10nm以下)的问题,目前人们已经提出了一些改进措施,包括发展了一些技术和方法,如多角度测量、干涉增强、介电函数参数化建模、将椭偏参数和透射率测量以及椭偏参数和反射率测量相结合等。比如:利用椭偏参量和反射率协同分析方法实现了厚度为2.86 -12.6nm的金属Cu纳米膜厚度的测定;利用上述方法测得的厚度值为3.9nm,而采用AFM技术测得厚度为2.86nm,两者产生的厚度偏差高达36.4%(|椭偏测量厚度-AFM测量厚度|/AFM测量厚度×100)。因此,目前使用的方法测量的厚度偏差较大。In recent years, with the miniaturization and integration of various devices, nanometer-thick metal films have become more and more important in the manufacture of semiconductor chips and various devices. Nano-thick metal thin films are widely used in microelectronics, integrated optics, solar cells, biomedicine, chemistry and aerospace technology due to their unique properties different from their corresponding materials, and they are indispensable for exhibiting specific new functions . At present, the methods for detecting thin films with nanometer thickness include atomic force microscope, scanning electron microscope, transmission electron microscope, scanning tunneling microscope, spectrophotometer and various film thickness meters, etc. These methods may be able to achieve sub-nanometer resolution detection, but due to their It is destructive to devices, complicated to operate, and low in detection efficiency, so it cannot be applied in actual production lines. Therefore, it cannot meet the rapidly developing advanced process control and optimized detection requirements. In order to better solve the problem that the thickness of nanometer films cannot be accurately measured quickly, non-destructively and efficiently, especially for the problem that conventional ellipsometry cannot accurately measure ultra-thin metal films (such as thickness below 10nm), people have proposed Some improvement measures include the development of some technologies and methods, such as multi-angle measurement, interference enhancement, dielectric function parametric modeling, and the combination of ellipsometric parameters and transmittance measurements, ellipsometric parameters and reflectivity measurements, etc. For example: using the method of synergy analysis of ellipsometric parameters and reflectivity to realize the determination of the thickness of metal Cu nano-film with a thickness of 2.86-12.6nm; the thickness measured by the above method is 3.9nm, while the thickness measured by AFM technology is 2.86nm nm, the thickness deviation between the two is as high as 36.4% (|Thickness measured by ellipsometry-Thickness measured by AFM|/Thickness measured by AFM×100). Therefore, the thickness measured by the currently used method has a large deviation.
由此可见,发展精确测量厚度为10nm以下超薄金属膜的新方法不仅对于科学研究十分重要,而且对于工业生产具有重要的实际意义和价值。It can be seen that the development of a new method for accurately measuring ultra-thin metal films with a thickness below 10nm is not only very important for scientific research, but also has important practical significance and value for industrial production.
发明内容Contents of the invention
为此,本发明提供一种利用光谱椭偏仪检测超薄金属膜的方法及装置,以解决现有技术中存在的测量方法测量数据偏差较大,灵敏度较差,导致无法满足实际使用需求的问题。To this end, the present invention provides a method and device for detecting ultra-thin metal films using a spectroscopic ellipsometer to solve the problem of large deviations in measurement data and poor sensitivity in the existing measurement methods in the prior art, resulting in failure to meet actual use requirements. question.
本发明提供一种利用光谱椭偏仪检测超薄金属膜的方法,包括:构建硅衬底和自然氧化硅层组成的第一体系,利用光谱椭偏仪测量所述第一体系中硅衬底和自然氧化硅层的椭偏参量;根据所述椭偏参量,确定所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据;The invention provides a method for detecting an ultra-thin metal film by using a spectroscopic ellipsometer, comprising: constructing a first system composed of a silicon substrate and a natural silicon oxide layer, and measuring the silicon substrate in the first system by using a spectroscopic ellipsometer and the ellipsometric parameters of the natural silicon oxide layer; according to the ellipsometric parameters, determine the optical constants corresponding to the silicon substrate and the optical constants and thickness data corresponding to the natural silicon oxide layer;
在所述第一体系上制备非吸收介质层,构建硅衬底、自然氧化硅层及非吸收介质层组成的第二体系,利用光谱椭偏仪测量所述第二体系中非吸收介质层的椭偏参量;根据所述非吸收介质层的椭偏参量、所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,确定所述非吸收介质层的光学常数和厚度数据;Prepare a non-absorbing medium layer on the first system, construct a second system consisting of a silicon substrate, a natural silicon oxide layer and a non-absorbing medium layer, and measure the non-absorbing medium layer in the second system by using a spectroscopic ellipsometer Ellipsometric parameter; determine the optical constant of the non-absorbing medium layer according to the ellipsometric parameter of the non-absorbing medium layer, the corresponding optical constant of the silicon substrate, and the corresponding optical constant and thickness data of the natural silicon oxide layer and thickness data;
在所述第二体系上制备金属膜层,构建硅衬底、自然氧化硅层、非吸收介质层及金属膜层组成的第三体系,利用光谱椭偏仪测量所述第三体系中金属膜层的椭偏参量;根据所述金属膜层的椭偏参量、所述硅衬底对应的光学常数、所述自然氧化硅层对应的光学常数和厚度数据以及所述非吸收介质层的光学常数和厚度数据,确定所述金属膜层的光学常数和厚度数据。Prepare a metal film layer on the second system, construct a third system composed of a silicon substrate, a natural silicon oxide layer, a non-absorbing medium layer and a metal film layer, and measure the metal film in the third system by using a spectroscopic ellipsometer Layer ellipsometric parameters; according to the ellipsometric parameters of the metal film layer, the corresponding optical constants of the silicon substrate, the corresponding optical constants and thickness data of the natural silicon oxide layer, and the optical constants of the non-absorbing medium layer and thickness data to determine the optical constant and thickness data of the metal film layer.
进一步的,所述在所述第一体系上制备非吸收介质层,具体包括:在所述自然氧化硅层上采用化学气相沉积、磁控溅射沉积以及电子束蒸发沉积中的任意一种或者两种方式制备非吸收介质层。Further, the preparation of the non-absorbing medium layer on the first system specifically includes: using any one of chemical vapor deposition, magnetron sputtering deposition and electron beam evaporation deposition on the natural silicon oxide layer or The non-absorbing medium layer was prepared in two ways.
进一步的,所述非吸收介质层为在椭偏仪测量光谱范围内对光是非吸收的介质材料,所述非吸收介质层包含SiO2膜、Si3N4膜以及 MgF2膜中任意一种;所述非吸收介质层的厚度数据为500nm~2um。Further, the non-absorbing medium layer is a medium material that is non-absorbing to light within the spectral range of the ellipsometer measurement, and the non - absorbing medium layer includes any one of SiO2 film, Si3N4 film and MgF2 film ; The thickness data of the non-absorbing medium layer is 500nm-2um.
进一步的,利用光谱椭偏仪测量椭偏参量的过程中,确定所述光谱椭偏仪的入射光的波长范围参数为190nm~2500nm以及所述入射光的入射角参数为45°~70°。Further, in the process of measuring the ellipsometric parameters by using the spectroscopic ellipsometer, it is determined that the wavelength range parameter of the incident light of the spectroscopic ellipsometer is 190nm-2500nm and the parameter of the incident angle of the incident light is 45°-70°.
进一步的,所述根据所述椭偏参量,确定所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,具体包括:Further, according to the ellipsometric parameters, determining the optical constants corresponding to the silicon substrate and the optical constants and thickness data corresponding to the natural silicon oxide layer, specifically includes:
构建所述第一体系对应的第一椭偏拟合模型,利用所述第一椭偏拟合模型对所述第一体系中硅衬底和自然氧化硅层的椭偏参量进行拟合,得到并记录所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据;Constructing a first ellipsometric fitting model corresponding to the first system, using the first ellipsometric fitting model to fit the ellipsometric parameters of the silicon substrate and the natural silicon oxide layer in the first system, to obtain and recording the optical constants corresponding to the silicon substrate and the optical constants and thickness data corresponding to the natural silicon oxide layer;
所述根据所述非吸收介质层的椭偏参量、所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,确定所述非吸收介质层的光学常数和厚度数据,具体包括:Determining the optical constant and thickness of the non-absorbing medium layer according to the ellipsometric parameters of the non-absorbing medium layer, the corresponding optical constant of the silicon substrate, and the corresponding optical constant and thickness data of the natural silicon oxide layer Data, specifically:
构建所述第二体系对应的第二椭偏拟合模型,利用所述第二椭偏拟合模型对所述第二体系中非吸收介质层的椭偏参量进行拟合,得到并记录所述非吸收介质层的光学常数和厚度数据;Construct a second ellipsometric fitting model corresponding to the second system, use the second ellipsometric fitting model to fit the ellipsometric parameters of the non-absorbing medium layer in the second system, obtain and record the Optical constants and thickness data of the non-absorbing dielectric layer;
所述根据所述金属膜层的椭偏参量、所述硅衬底对应的光学常数、所述自然氧化硅层对应的光学常数和厚度数据以及所述非吸收介质层的光学常数和厚度数据,确定所述金属膜层的光学常数和厚度数据,具体包括:According to the ellipsometric parameters of the metal film layer, the optical constants corresponding to the silicon substrate, the optical constants and thickness data corresponding to the natural silicon oxide layer, and the optical constants and thickness data of the non-absorbing medium layer, Determine the optical constants and thickness data of the metal film layer, specifically including:
构建所述第三体系对应的第三椭偏拟合模型,利用所述第三椭偏拟合模型对所述第三体系中金属膜层的椭偏参量进行拟合,得到所述金属膜层的光学常数和厚度数据。Constructing a third ellipsometric fitting model corresponding to the third system, using the third ellipsometric fitting model to fit the ellipsometric parameters of the metal film layer in the third system, to obtain the metal film layer Optical constants and thickness data for .
进一步的,所述金属膜层包括金、铂、钯、钛中的任意一种金属元素,所述金属膜层的厚度数据小于10nm。Further, the metal film layer includes any metal element among gold, platinum, palladium and titanium, and the thickness data of the metal film layer is less than 10 nm.
本发明提供一种利用光谱椭偏仪的超薄金属膜的光学表征方法,包括:The invention provides an optical characterization method of an ultra-thin metal film using a spectroscopic ellipsometer, comprising:
设定光谱椭偏仪的操作参数;Setting the operating parameters of the spectroscopic ellipsometer;
构建测量金属膜层的椭偏拟合模型;Build an ellipsometric fitting model for measuring the metal film layer;
利用所述光谱椭偏仪分别测量所述椭偏拟合模型的结构层所对应的椭偏参量;所述结构层包括硅衬底层、自然氧化硅层、非吸收介质层、过渡层、金属膜层、空气粗糙层以及空气层;Using the spectroscopic ellipsometer to measure the ellipsometric parameters corresponding to the structural layers of the ellipsometric fitting model; the structural layers include a silicon substrate layer, a natural silicon oxide layer, a non-absorbing medium layer, a transition layer, and a metal film layer, air roughness layer, and air layer;
其中,所述过渡层中的第二非吸收介层对应的椭偏参量与所述非吸收介质层对应的椭偏参量相同;Wherein, the ellipsometric parameter corresponding to the second non-absorbing medium layer in the transition layer is the same as the ellipsometric parameter corresponding to the non-absorbing medium layer;
将所述结构层对应的椭偏参量与所述椭偏拟合模型进行拟合,得到所述金属膜层的光学常数及厚度数据。Fitting the ellipsometric parameters corresponding to the structural layer with the ellipsometric fitting model to obtain the optical constant and thickness data of the metal film layer.
进一步的,所述操作参数包括:入射角参数、测量波长范围参数、测量波长的间隔参数以及参考表征波长参数中的至少一种;Further, the operating parameters include: at least one of an incident angle parameter, a measurement wavelength range parameter, a measurement wavelength interval parameter, and a reference characteristic wavelength parameter;
所述过渡层由第二非吸收介质层与第二金属膜层组成;The transition layer is composed of a second non-absorbing medium layer and a second metal film layer;
所述空气粗糙层由第三金属膜层与第二空气层组成。The rough air layer is composed of the third metal film layer and the second air layer.
本发明提供一种利用光谱椭偏仪检测超薄金属膜的装置,包括:The invention provides a device for detecting an ultra-thin metal film using a spectroscopic ellipsometer, comprising:
第一体系参数确定单元,用于构建硅衬底和自然氧化硅层组成的第一体系,利用光谱椭偏仪测量所述第一体系中硅衬底和自然氧化硅层的椭偏参量;根据所述椭偏参量,确定所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据;The first system parameter determination unit is used to construct a first system composed of a silicon substrate and a natural silicon oxide layer, and use a spectroscopic ellipsometer to measure the ellipsometric parameters of the silicon substrate and the natural silicon oxide layer in the first system; according to The ellipsometric parameters determine the optical constants corresponding to the silicon substrate and the optical constants and thickness data corresponding to the natural silicon oxide layer;
第二体系参数确定单元,用于在所述第一体系上制备非吸收介质层,构建硅衬底、自然氧化硅层及非吸收介质层组成的第二体系,利用光谱椭偏仪测量所述第二体系中非吸收介质层的椭偏参量;根据所述非吸收介质层的椭偏参量、所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,确定所述非吸收介质层的光学常数和厚度数据;The second system parameter determination unit is used to prepare a non-absorbing medium layer on the first system, construct a second system composed of a silicon substrate, a natural silicon oxide layer and a non-absorbing medium layer, and use a spectroscopic ellipsometer to measure the The ellipsometric parameter of the non-absorbing medium layer in the second system; determined according to the ellipsometric parameter of the non-absorbing medium layer, the corresponding optical constant of the silicon substrate, and the corresponding optical constant and thickness data of the natural silicon oxide layer Optical constants and thickness data of the non-absorbing medium layer;
第三体系参数确定单元,用于在所述第二体系上制备金属膜层,构建硅衬底、自然氧化硅层、非吸收介质层及金属膜层组成的第三体系,利用光谱椭偏仪测量所述第三体系中金属膜层的椭偏参量;根据所述金属膜层的椭偏参量、所述硅衬底对应的光学常数、所述自然氧化硅层对应的光学常数和厚度数据以及所述非吸收介质层的光学常数和厚度数据,确定所述金属膜层的光学常数和厚度数据。The third system parameter determination unit is used to prepare a metal film layer on the second system, construct a third system composed of a silicon substrate, a natural silicon oxide layer, a non-absorbing medium layer and a metal film layer, and use a spectroscopic ellipsometer Measuring the ellipsometric parameter of the metal film layer in the third system; according to the ellipsometric parameter of the metal film layer, the optical constant corresponding to the silicon substrate, the optical constant and thickness data corresponding to the natural silicon oxide layer, and The optical constant and thickness data of the non-absorbing medium layer determine the optical constant and thickness data of the metal film layer.
进一步的,所述第二体系参数确定单元,具体用于:在所述自然氧化硅层上采用化学气相沉积、磁控溅射沉积以及电子束蒸发沉积中的任意一种或者两种方式制备非吸收介质层。Further, the second system parameter determination unit is specifically used to: prepare non-metallic silicon dioxide on the natural silicon oxide layer by any one or two methods of chemical vapor deposition, magnetron sputtering deposition and electron beam evaporation deposition. absorbent layer.
进一步的,所述非吸收介质层为在椭偏仪测量光谱范围内对光是非吸收的介质材料,所述非吸收介质层包含SiO2膜、Si3N4膜以及 MgF2膜中任意一种;所述非吸收介质层的厚度数据为500nm~2um。Further, the non-absorbing medium layer is a medium material that is non-absorbing to light within the spectral range of the ellipsometer measurement, and the non - absorbing medium layer includes any one of SiO2 film, Si3N4 film and MgF2 film ; The thickness data of the non-absorbing medium layer is 500nm-2um.
进一步的,利用光谱椭偏仪测量椭偏参量的过程中,确定所述光谱椭偏仪的入射光的波长范围参数为190nm~2500nm以及所述入射光的入射角参数为45°~70°。Further, in the process of measuring the ellipsometric parameters by using the spectroscopic ellipsometer, it is determined that the wavelength range parameter of the incident light of the spectroscopic ellipsometer is 190nm-2500nm and the parameter of the incident angle of the incident light is 45°-70°.
进一步的,所述第一体系参数确定单元,具体用于:构建所述第一体系对应的第一椭偏拟合模型,利用所述第一椭偏拟合模型对所述第一体系中硅衬底和自然氧化硅层的椭偏参量进行拟合,得到并记录所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据;Further, the first system parameter determination unit is specifically configured to: construct a first ellipsometric fitting model corresponding to the first system, and use the first ellipsometric fitting model to Fitting the ellipsometric parameters of the substrate and the natural silicon oxide layer, obtaining and recording the optical constants corresponding to the silicon substrate and the optical constants and thickness data corresponding to the natural silicon oxide layer;
所述第二体系参数确定单元,具体用于:构建所述第二体系对应的第二椭偏拟合模型,利用所述第二椭偏拟合模型对所述第二体系中非吸收介质层的椭偏参量进行拟合,得到并记录所述非吸收介质层的光学常数和厚度数据;The second system parameter determination unit is specifically configured to: construct a second ellipsometric fitting model corresponding to the second system, and use the second ellipsometric fitting model to analyze the non-absorbing medium layer in the second system The ellipsometric parameters are fitted, and the optical constant and thickness data of the non-absorbing medium layer are obtained and recorded;
所述第三体系参数确定单元,具体用于:构建所述第三体系对应的第三椭偏拟合模型,利用所述第三椭偏拟合模型对所述第三体系中金属膜层的椭偏参量进行拟合,得到所述金属膜层的光学常数和厚度数据。The third system parameter determination unit is specifically configured to: construct a third ellipsometric fitting model corresponding to the third system, and use the third ellipsometric fitting model to analyze the metal film layer in the third system The ellipsometric parameters are fitted to obtain the optical constant and thickness data of the metal film layer.
进一步的,所述金属膜层包括金、铂、钯、钛中的任意一种金属元素,所述金属膜层的厚度数据小于10nm。Further, the metal film layer includes any metal element among gold, platinum, palladium and titanium, and the thickness data of the metal film layer is less than 10 nm.
本发明提供一种利用光谱椭偏仪的超薄金属膜的光学表征装置,包括:The invention provides an optical characterization device using a spectroscopic ellipsometer for an ultra-thin metal film, comprising:
操作参数设定单元,用于设定光谱椭偏仪的操作参数;An operating parameter setting unit, used for setting the operating parameters of the spectroscopic ellipsometer;
椭偏拟合模型构建单元,用于构建测量金属膜层的椭偏拟合模型;An ellipsometric fitting model building unit for constructing an ellipsometric fitting model for measuring metal film layers;
椭偏参量测量单元,用于利用所述光谱椭偏仪分别测量所述椭偏拟合模型的结构层所对应的椭偏参量;所述结构层包括硅衬底层、自然氧化硅层、非吸收介质层、过渡层、金属膜层、空气粗糙层以及空气层;其中,所述过渡层中的第二非吸收介层对应的椭偏参量与所述非吸收介质层对应的椭偏参量相同;The ellipsometric parameter measurement unit is used to measure the ellipsometric parameters corresponding to the structural layers of the ellipsometric fitting model by using the spectroscopic ellipsometer; the structural layers include a silicon substrate layer, a natural silicon oxide layer, a non-absorbing A medium layer, a transition layer, a metal film layer, an air roughness layer, and an air layer; wherein, the ellipsometric parameter corresponding to the second non-absorbing medium layer in the transition layer is the same as the ellipsometric parameter corresponding to the non-absorbing medium layer;
金属膜层数据获得单元,用于将所述结构层对应的椭偏参量与所述椭偏拟合模型进行拟合,得到所述金属膜层的光学常数及厚度数据。The metal film layer data acquisition unit is configured to fit the ellipsometric parameters corresponding to the structural layer with the ellipsometric fitting model to obtain the optical constant and thickness data of the metal film layer.
进一步的,所述操作参数包括:入射角参数、测量波长范围参数、测量波长的间隔参数以及参考表征波长参数中的至少一种;Further, the operating parameters include: at least one of an incident angle parameter, a measurement wavelength range parameter, a measurement wavelength interval parameter, and a reference characteristic wavelength parameter;
所述过渡层由第二非吸收介质层与第二金属膜层组成;The transition layer is composed of a second non-absorbing medium layer and a second metal film layer;
所述空气粗糙层由第三金属膜层与第二空气层组成。The rough air layer is composed of the third metal film layer and the second air layer.
采用本发明所述的利用光谱椭偏仪检测超薄金属膜的方法,能够对超薄的金属膜进行非破坏性、高精度和高灵敏度的检测,仪器配置简单且,具有较好的重现性。可集成到集成电路生产线中,适应集成电路的工艺控制及优化的检测要求,扩大了极限金属膜的椭偏测量范围。Adopting the method for detecting ultra-thin metal films using spectroscopic ellipsometry described in the present invention can perform non-destructive, high-precision and high-sensitivity detection of ultra-thin metal films, and the instrument configuration is simple and has good reproducibility sex. It can be integrated into the integrated circuit production line, adapt to the process control and optimized detection requirements of integrated circuits, and expand the ellipsometric measurement range of the limit metal film.
采用本发明所述的利用光谱椭偏仪的超薄金属膜的光学表征方法,能够对薄膜厚度低于10nm的金属膜进行非破坏性、高精度和高灵敏度的检测;仪器配置简单,容易操作,具有较好的重现性;同时不会损坏样品,避免了传统测量法对样品的损坏,而导致实验的不可重复性;另外,能够集成到集成电路生产线中,适应集成电路的工艺控制及优化的检测要求,扩大了极限金属膜的椭偏测量范围。Adopting the optical characterization method of the ultra-thin metal film using a spectroscopic ellipsometer according to the present invention can carry out non-destructive, high-precision and high-sensitivity detection on a metal film with a film thickness lower than 10 nm; the instrument configuration is simple and easy to operate , has good reproducibility; at the same time, it will not damage the sample, avoiding the damage of the sample by the traditional measurement method, which leads to the non-repeatability of the experiment; in addition, it can be integrated into the integrated circuit production line, adapting to the process control and The optimized detection requirements expand the ellipsometric measurement range of the limit metal film.
附图说明Description of drawings
为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施例或现有技术描述中所需要使用的附图作一简单地介绍,显而易见地,下面描述中的附图是本发明的一些实施例,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,还可以根据这些附图获取其他的附图。In order to more clearly illustrate the technical solutions in the embodiments of the present invention or the prior art, the following will briefly introduce the drawings that need to be used in the description of the embodiments or the prior art. Obviously, the accompanying drawings in the following description These are some embodiments of the present invention. For those skilled in the art, other drawings can also be obtained based on these drawings without creative effort.
图1为本发明实施例提供的一种利用光谱椭偏仪检测超薄金属膜的方法的流程示意图;Fig. 1 is a schematic flow chart of a method for detecting an ultra-thin metal film using a spectroscopic ellipsometer provided by an embodiment of the present invention;
图2为本发明实施例提供的一种利用光谱椭偏仪检测超薄金属膜的装置的结构示意图;Fig. 2 is a schematic structural diagram of a device for detecting ultra-thin metal films using a spectroscopic ellipsometer provided by an embodiment of the present invention;
图3为本发明实施例提供的一种利用光谱椭偏仪的超薄金属膜的光学表征方法的流程示意图;3 is a schematic flow diagram of an optical characterization method using a spectroscopic ellipsometer for an ultra-thin metal film provided by an embodiment of the present invention;
图4为本发明实施例提供的一种利用光谱椭偏仪的超薄金属膜的光学表征装置的结构示意图;4 is a schematic structural view of an optical characterization device using a spectroscopic ellipsometer for an ultra-thin metal film provided by an embodiment of the present invention;
图5a为本发明实施例提供的利用电子束蒸发在硅衬底、自然氧化硅层以及非吸收介质层组成的体系上蒸发超薄Pt膜与未蒸发超薄 Pt膜形成台阶的AFM形貌图;Fig. 5a is an AFM topography image of steps formed by evaporating an ultra-thin Pt film and an unevaporated ultra-thin Pt film on a silicon substrate, a natural silicon oxide layer, and a non-absorbing dielectric layer by electron beam evaporation provided by an embodiment of the present invention. ;
图5b为本发明实施例提供的利用电子束蒸发在硅衬底、自然氧化硅层以及非吸收介质层组成的体系上蒸发超薄Pt膜与未蒸发超薄 Pt膜形成的台阶的垂直高度曲线图;Figure 5b is the vertical height curve of steps formed by evaporating ultra-thin Pt films and non-evaporated ultra-thin Pt films on a system composed of silicon substrate, natural silicon oxide layer and non-absorbing dielectric layer by electron beam evaporation provided by the embodiment of the present invention picture;
图6为本发明实施例提供的在硅衬底、自然氧化硅层以及非吸收介质层组成的体系上蒸发超薄Pt膜的椭偏参量拟合图;Fig. 6 is a fitting diagram of ellipsometric parameters for evaporating an ultra-thin Pt film on a system composed of a silicon substrate, a natural silicon oxide layer and a non-absorbing medium layer provided by an embodiment of the present invention;
图7为本发明实施例提供的第一种椭偏拟合模型的结构图;7 is a structural diagram of the first ellipsometric fitting model provided by the embodiment of the present invention;
图8a为本发明实施例提供的利用电子束蒸发在硅衬底、自然氧化硅层及氧化硅SiO2层组成的体系上蒸发超薄Pt膜与未蒸发超薄Pt 膜形成台阶的AFM形貌图;Figure 8a is the AFM morphology of steps formed by evaporating an ultra-thin Pt film and an unevaporated ultra-thin Pt film on a system composed of a silicon substrate, a natural silicon oxide layer and a silicon oxide SiO2 layer by electron beam evaporation provided by an embodiment of the present invention picture;
图8b为本发明实施例提供的利用电子束蒸发在硅衬底、自然氧化硅层及氧化硅SiO2层组成的体系上蒸发超薄Pt膜与未蒸发超薄Pt 膜形成的台阶的垂直高度曲线图;Figure 8b is the vertical height of steps formed by evaporating an ultra-thin Pt film and an unevaporated ultra-thin Pt film on a system composed of a silicon substrate, a natural silicon oxide layer and a silicon oxide SiO2 layer by electron beam evaporation provided by an embodiment of the present invention Graph;
图9为本发明实施例提供的在硅衬底、自然氧化硅层及氧化硅 SiO2层组成的体系上蒸发超薄Pt膜的椭偏参量拟合图;Fig. 9 is an ellipsometric fitting diagram of evaporating an ultra-thin Pt film on a system composed of a silicon substrate, a natural silicon oxide layer and a silicon oxide SiO2 layer provided by an embodiment of the present invention;
图10为本发明实施例提供的第二种椭偏拟合模型的结构图。Fig. 10 is a structural diagram of the second ellipsometric fitting model provided by the embodiment of the present invention.
具体实施方式Detailed ways
为使本发明实施例的目的、技术方案和优点更加清楚,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进行清楚、完整地描述,显然,所描述的实施例是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有做出创造性劳动前提下所获取的所有其他实施例,都属于本发明保护的范围。In order to make the purpose, technical solutions and advantages of the embodiments of the present invention clearer, the technical solutions in the embodiments of the present invention will be clearly and completely described below in conjunction with the drawings in the embodiments of the present invention. Obviously, the described embodiments It is a part of embodiments of the present invention, but not all embodiments. Based on the embodiments of the present invention, 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.
本申请提出了一种基于光学椭偏测量技术精确测定超薄金属膜光学参数和厚度数据的方法,从而克服了目前常规使用的椭偏测量的局限性,实现厚度为10nm以下超薄金属膜的精确测定。这不仅拓展了椭偏仪的测量对象范围,而且丰富了椭偏测量方法,将积极推动和促进科学研究和工业生产中所需要的超薄金属膜测量技术的发展和进步。下面基于本发明所述的利用光谱椭偏仪检测超薄金属膜的方法,对其实施例进行详细描述。如图1所示,其为本发明实施例提供的一种利用光谱椭偏仪检测超薄金属膜的方法的流程示意图,具体实现过程包括以下步骤:This application proposes a method for accurately measuring the optical parameters and thickness data of ultra-thin metal films based on optical ellipsometry technology, thereby overcoming the limitations of conventionally used ellipsometry and realizing ultra-thin metal films with a thickness of less than 10nm Measured precisely. This not only expands the range of measurement objects of the ellipsometer, but also enriches the measurement methods of ellipsometry, which will actively promote and promote the development and progress of ultra-thin metal film measurement technology required in scientific research and industrial production. The following is a detailed description of the embodiment of the method for detecting an ultra-thin metal film using a spectroscopic ellipsometer according to the present invention. As shown in Figure 1, it is a schematic flow chart of a method for detecting an ultra-thin metal film using a spectroscopic ellipsometer provided by an embodiment of the present invention. The specific implementation process includes the following steps:
步骤101:构建硅衬底和自然氧化硅层组成的第一体系,利用光谱椭偏仪测量所述第一体系中硅衬底和自然氧化硅层的椭偏参量;根据所述椭偏参量,确定所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据。Step 101: Construct a first system consisting of a silicon substrate and a natural silicon oxide layer, and use a spectroscopic ellipsometer to measure the ellipsometric parameters of the silicon substrate and the natural silicon oxide layer in the first system; according to the ellipsometric parameters, The optical constant corresponding to the silicon substrate and the optical constant and thickness data corresponding to the natural silicon oxide layer are determined.
在本步骤中,利用光谱椭偏仪测量所述第一体系中硅衬底(Si 衬底)和自然氧化硅层的椭偏参量过程中,需要首先确定所述光谱椭偏仪的入射光的波长范围参数为190nm~2500nm以及所述入射光的入射角参数为45°~70°。In this step, in the process of measuring the ellipsometric parameters of the silicon substrate (Si substrate) and the natural silicon oxide layer in the first system using the spectroscopic ellipsometer, it is necessary to first determine the ratio of the incident light of the spectroscopic ellipsometer The wavelength range parameter is 190nm-2500nm and the incident angle parameter of the incident light is 45°-70°.
具体的,所述根据椭偏参量,确定所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,实现过程包括:构建所述第一体系对应的第一椭偏拟合模型,利用所述第一椭偏拟合模型对所述第一体系中硅衬底和自然氧化硅层的椭偏参量进行拟合,得到所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,并对数据进行记录存储;Specifically, according to the ellipsometric parameters, the optical constants corresponding to the silicon substrate and the optical constants and thickness data corresponding to the natural silicon oxide layer are determined, and the implementation process includes: constructing the first ellipsoid corresponding to the first system A partial fitting model, using the first ellipsometric fitting model to fit the ellipsometric parameters of the silicon substrate and the natural silicon oxide layer in the first system, to obtain the optical constants corresponding to the silicon substrate and the Describe the optical constant and thickness data corresponding to the natural silicon oxide layer, and record and store the data;
步骤102:在所述第一体系上制备非吸收介质层,构建硅衬底、自然氧化硅层及非吸收介质层组成的第二体系,利用光谱椭偏仪测量所述第二体系中非吸收介质层的椭偏参量;根据所述非吸收介质层的椭偏参量、所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,确定所述非吸收介质层的光学常数和厚度数据。Step 102: Prepare a non-absorbing medium layer on the first system, construct a second system consisting of a silicon substrate, a natural silicon oxide layer, and a non-absorbing medium layer, and measure the non-absorbing medium layer in the second system using a spectroscopic ellipsometer. The ellipsometric parameter of the medium layer; according to the ellipsometric parameter of the non-absorbing medium layer, the optical constant corresponding to the silicon substrate, and the optical constant and thickness data corresponding to the natural silicon oxide layer, determine the non-absorbing medium layer Optical constants and thickness data for .
在本步骤中,所述在第一体系上制备非吸收介质层具体实现方式包括:在硅衬底及自然氧化硅层上采用化学气相沉积、磁控溅射沉积以及电子束蒸发沉积中的任意一种或者两种方式制备非吸收介质层。其中,所述非吸收介质层为在椭偏仪测量光谱范围内对光是非吸收的介质材料,所述非吸收介质层包含SiO2膜、Si3N4膜以及MgF2膜等中任意一种;所述非吸收介质层的厚度数据为500nm~2um。In this step, the specific implementation of preparing the non-absorbing medium layer on the first system includes: using any of chemical vapor deposition, magnetron sputtering deposition and electron beam evaporation deposition on the silicon substrate and the natural silicon oxide layer. The non-absorbing medium layer is prepared in one or both ways. Wherein, the non-absorbing medium layer is a medium material that is non-absorbing to light within the spectral range of the ellipsometer measurement, and the non - absorbing medium layer includes any one of SiO2 film, Si3N4 film and MgF2 film, etc. ; The thickness data of the non-absorbing medium layer is 500nm-2um.
在具体实施过程中,利用光谱椭偏仪测量所述第二体系中非吸收介质层的椭偏参量的过程中,需要预先确定所述光谱椭偏仪的入射光的波长范围参数为190nm~2500nm以及所述入射光的入射角参数为45°~70°。In the specific implementation process, in the process of using the spectroscopic ellipsometer to measure the ellipsometric parameters of the non-absorbing medium layer in the second system, it is necessary to pre-determine that the wavelength range parameter of the incident light of the spectroscopic ellipsometer is 190nm-2500nm And the incident angle parameter of the incident light is 45°-70°.
具体的,所述根据非吸收介质层的椭偏参量、所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,确定所述非吸收介质层的光学常数和厚度数据,实现过程包括:构建所述第二体系对应的第二椭偏拟合模型,利用所述第二椭偏拟合模型对所述第二体系中非吸收介质层的椭偏参量进行拟合,得到所述非吸收介质层的光学常数和厚度数据,并对数据进行记录存储;Specifically, according to the ellipsometric parameters of the non-absorbing medium layer, the optical constants corresponding to the silicon substrate, and the optical constants and thickness data corresponding to the natural silicon oxide layer, the optical constants and the thickness of the non-absorbing medium layer are determined. Thickness data, the implementation process includes: constructing a second ellipsometric fitting model corresponding to the second system, using the second ellipsometric fitting model to simulate the ellipsometric parameters of the non-absorbing medium layer in the second system combined to obtain the optical constant and thickness data of the non-absorbing medium layer, and record and store the data;
步骤103:在所述第二体系上制备金属膜层,构建硅衬底、自然氧化硅层、非吸收介质层及金属膜层组成的第三体系,利用光谱椭偏仪测量所述第三体系中金属膜层的椭偏参量;根据所述金属膜层的椭偏参量、所述硅衬底对应的光学常数、所述自然氧化硅层对应的光学常数和厚度数据以及所述非吸收介质层的光学常数和厚度数据,确定所述金属膜层的光学常数和厚度数据。Step 103: Prepare a metal film layer on the second system, construct a third system consisting of a silicon substrate, a natural silicon oxide layer, a non-absorbing medium layer, and a metal film layer, and measure the third system using a spectroscopic ellipsometer The ellipsometric parameters of the metal film layer; according to the ellipsometric parameters of the metal film layer, the corresponding optical constants of the silicon substrate, the corresponding optical constants and thickness data of the natural silicon oxide layer, and the non-absorbing medium layer The optical constant and thickness data of the metal film layer are determined.
在本步骤中,所述在第二体系上制备金属膜层具体实现方式包括:在硅衬底、自然氧化硅层及非吸收介质层上采用化学气相沉积、磁控溅射沉积以及电子束蒸发沉积中的任意一种或者两种方式制备金属膜层。In this step, the specific implementation of preparing the metal film layer on the second system includes: using chemical vapor deposition, magnetron sputtering deposition and electron beam evaporation on the silicon substrate, natural silicon oxide layer and non-absorbing medium layer Either one or two methods of deposition are used to prepare metal film layers.
在具体实施过程中,利用光谱椭偏仪测量所述第三体系中金属膜层的椭偏参量的过程中,同样需要预先确定所述光谱椭偏仪的入射光的波长范围参数为190nm~2500nm以及所述入射光的入射角参数为 45°~70°。In the specific implementation process, in the process of using the spectroscopic ellipsometer to measure the ellipsometric parameters of the metal film layer in the third system, it is also necessary to predetermine that the wavelength range parameter of the incident light of the spectroscopic ellipsometer is 190nm-2500nm And the incident angle parameter of the incident light is 45°-70°.
具体的,所述根据所述金属膜层的椭偏参量、所述硅衬底对应的光学常数、所述自然氧化硅层对应的光学常数和厚度数据以及所述非吸收介质层的光学常数和厚度数据,确定所述金属膜层的光学常数和厚度数据,实现过程包括:构建所述第三体系对应的第三椭偏拟合模型,利用所述第三椭偏拟合模型对所述第三体系中金属膜层的椭偏参量进行拟合,得到所述金属膜层的光学常数和厚度数据,并对数据进行记录存储。其中,所述金属膜层包括金、铂、钯、钛等中的任意一种金属元素,所述金属膜层的厚度数据小于10nm。Specifically, according to the ellipsometric parameters of the metal film layer, the optical constants corresponding to the silicon substrate, the optical constants and thickness data corresponding to the natural silicon oxide layer, and the optical constants and Thickness data, determining the optical constant and thickness data of the metal film layer, the implementation process includes: constructing a third ellipsometric fitting model corresponding to the third system, using the third ellipsometric fitting model to The ellipsometric parameters of the metal film layer in the three systems are fitted to obtain the optical constant and thickness data of the metal film layer, and the data are recorded and stored. Wherein, the metal film layer includes any metal element among gold, platinum, palladium, titanium, etc., and the thickness data of the metal film layer is less than 10 nm.
在一个具体实施例中,采用光谱椭偏仪对金属膜层Pt(厚度约为 3nm)进行检测,其中,光谱椭偏仪的入射角可设置为70°,波长范围可设置为380nm至930nm,非吸收介质层为氮化硅(Si3N4)膜,具体方法如下:In a specific embodiment, a spectroscopic ellipsometer is used to detect the metal film layer Pt (thickness is about 3nm), wherein, the incident angle of the spectroscopic ellipsometer can be set to 70°, and the wavelength range can be set to 380nm to 930nm, The non-absorbing medium layer is a silicon nitride (Si 3 N 4 ) film, and the specific method is as follows:
(1)构建由Si衬底和自然氧化硅层组成的第一体系:可选取 n-Si(100)衬底作为Si衬底和自然氧化硅层组成的第一体系(体系1),利用光谱椭偏仪测量第一体系,获得第一体系中的Si衬底和自然氧化硅层的椭偏参量,计算并记录所述第一体系中的Si衬底和自然氧化硅层的光学常数及所述第一体系中的所述自然氧化硅层的厚度数据。在具体实施过程中,所计算的自然氧化硅层的厚度数据为1.27nm;当波长为633nm时,所计算的自然氧化硅层的折射率为1.5274以及消光系数为0。(1) Construct the first system composed of Si substrate and natural silicon oxide layer: n-Si(100) substrate can be selected as the first system (system 1) composed of Si substrate and natural silicon oxide layer, and the spectral The ellipsometer measures the first system, obtains the ellipsometric parameters of the Si substrate and the natural silicon oxide layer in the first system, and calculates and records the optical constants and the obtained values of the Si substrate and the natural silicon oxide layer in the first system. The thickness data of the natural silicon oxide layer in the first system. In the specific implementation process, the calculated thickness data of the natural silicon oxide layer is 1.27 nm; when the wavelength is 633 nm, the calculated refractive index of the natural silicon oxide layer is 1.5274 and the extinction coefficient is 0.
(2)构建制备Si衬底、自然氧化硅层和非吸收介质层(比如氮化硅(Si3N4)层或氮化硅(Si3N4)膜)组成的第二体系:可利用化学气相沉积法在第一体系上方制备厚度为1um的氮化硅(Si3N4)膜得到第二体系(即体系2),利用光谱椭偏仪测量该第二体系中的氮化硅(Si3N4)膜的椭偏参量,带入所记录的自然氧化硅层的光学常数和厚度,从而计算并记录所述第二体系中的氮化硅(Si3N4)膜的光学常数及厚度。其中,所计算的氮化硅(Si3N4)膜的厚度为947.66nm;当波长为633nm时,所计算的氮化硅(Si3N4)膜的折射率为1.9722 以及消光系数为0。(2) Construct the second system consisting of Si substrate, natural silicon oxide layer and non-absorbing dielectric layer (such as silicon nitride (Si 3 N 4 ) layer or silicon nitride (Si 3 N 4 ) film): available A silicon nitride (Si 3 N 4 ) film with a thickness of 1um was prepared on the first system by chemical vapor deposition to obtain the second system (i.e. system 2), and the silicon nitride in the second system ( Si 3 N 4 ) film's ellipsometric parameter, brought into the recorded optical constant and thickness of the natural silicon oxide layer, thereby calculating and recording the optical constant and the optical constant of the silicon nitride (Si 3 N 4 ) film in the second system thickness. Among them, the calculated thickness of the silicon nitride (Si 3 N 4 ) film is 947.66nm; when the wavelength is 633nm, the calculated refractive index of the silicon nitride (Si 3 N 4 ) film is 1.9722 and the extinction coefficient is 0 .
(3)制备Si衬底、自然氧化硅层、非吸收介质层体系以及金属膜层(比如铂Pt层或铂Pt膜)组成的第三体系(即体系3)。利用高真空电子束蒸发法在第二体系上方蒸发厚度约为3nm的铂Pt膜得到第三体系,利用光谱椭偏仪测量该第三体系中铂Pt膜的椭偏参量,带入所记录的第一体系的自然氧化硅层的光学常数和厚度以及第二体系的中的氮化硅(Si3N4)膜所述光学常数及所述厚度,从而计算并记录所述第三体系中的铂Pt膜的光学常数及厚度。其中,所计算的铂Pt膜的厚度为3.15nm;当波长为633nm时,所计算的铂Pt膜的折射率为2.2818以及消光系数为4.77632。(3) Prepare a third system (system 3) consisting of Si substrate, natural silicon oxide layer, non-absorbing medium layer system and metal film layer (such as platinum Pt layer or platinum Pt film). The third system was obtained by evaporating a platinum Pt film with a thickness of about 3nm above the second system by high vacuum electron beam evaporation method. The ellipsometric parameters of the platinum Pt film in the third system were measured by spectroscopic ellipsometer, and the recorded first The optical constant and thickness of the natural silicon oxide layer in one system and the optical constant and the thickness of the silicon nitride (Si 3 N 4 ) film in the second system, so as to calculate and record the platinum in the third system Optical constants and thickness of the Pt film. Wherein, the calculated thickness of the platinum Pt film is 3.15 nm; when the wavelength is 633 nm, the calculated refractive index of the platinum Pt film is 2.2818 and the extinction coefficient is 4.77632.
如图5(a)所示,其中虚线左侧为在硅衬底、自然氧化硅层、氮化硅(Si3N4)层体系上蒸发了超薄铂Pt膜,虚线右侧为并未在硅衬底、自然氧化硅层以及氮化硅(Si3N4)层组成的第二体系上蒸发超薄Pt膜。如图5(b)所示,利用电子束蒸发在Si衬底、自然氧化硅层及氮化硅(Si3N4)层组成的第二体系上蒸发超薄Pt膜与未蒸发超薄Pt膜形成台阶的垂直高度曲线图。从图5(a)和5(b)中可以看出利用高真空电子束蒸发系统蒸发的铂Pt膜的厚度约为2.954nm。采用原子力显微镜(AFM)测量金属膜的厚度(dAFM),与椭偏仪拟合出的厚度(dEI)进行比较,计算厚度偏差(|dEl-dAFM|/dAFM×100) 为6.9%。As shown in Figure 5(a), the left side of the dotted line is the ultra-thin platinum Pt film evaporated on the silicon substrate, natural silicon oxide layer, and silicon nitride (Si 3 N 4 ) layer system, and the right side of the dotted line is not An ultra-thin Pt film was evaporated on a second system composed of a silicon substrate, a natural silicon oxide layer and a silicon nitride (Si 3 N 4 ) layer. As shown in Figure 5(b), electron beam evaporation was used to evaporate ultra-thin Pt film and non-evaporated ultra-thin Pt film on the second system composed of Si substrate, natural silicon oxide layer and silicon nitride (Si 3 N 4 ) layer Vertical height plot of film-forming steps. It can be seen from Figures 5(a) and 5(b) that the thickness of the platinum Pt film evaporated by the high vacuum electron beam evaporation system is about 2.954nm. The thickness of the metal film (dAFM) was measured by an atomic force microscope (AFM), and compared with the thickness (dEI) fitted by the ellipsometer, the calculated thickness deviation (|dEl-dAFM|/dAFM×100) was 6.9%.
如图7所示,其为本发明实施例所提供的第一椭偏拟合模型的结构图。该第一椭偏拟合模型对应的结构层包括:Si衬底层(Si Lengosci)、自然氧化硅层(SiO2(native))、非吸收介质层(Si3N4-TL)、过渡层(Pt/Si3N4)、金属膜层(Pt(platiunum)-DL#1)、空气粗糙层(Roughness-Air/Pt(Platiunu…))、以及空气层(Air)。其中,利用化学气相沉积法在Si衬底上制备氮化硅(Si3N4)膜,厚度为 1000nm;利用高真空电子束蒸发法在氮化硅(Si3N4)膜上方蒸发厚度约为3nm的铂Pt膜。Si衬底层为Leng Oscilator色散模型;自然氧化硅层为Cauchy色散模型;非吸收介质层为Si3N4膜的Tauc-Lorentz 色散模型;过渡层为Si3N4层和Pt层的混合层,其为Bruggeman有效近似模型;铂Pt膜为Drude-Lorentz Oscilator色散模型;空气粗糙层为Pt层和空气层的混合层,其为Bruggeman有效近似模型。As shown in FIG. 7 , it is a structural diagram of the first ellipsometric fitting model provided by the embodiment of the present invention. The structural layers corresponding to the first ellipsometric fitting model include: Si substrate layer (Si Lengosci), natural silicon oxide layer (SiO 2 (native)), non-absorbing dielectric layer (Si 3 N 4 -TL), transition layer ( Pt/Si 3 N 4 ), metal film layer (Pt(platiunum)-DL#1), air roughness layer (Roughness-Air/Pt(Platiunu...)), and air layer (Air). Among them, a silicon nitride (Si 3 N 4 ) film was prepared on a Si substrate by chemical vapor deposition with a thickness of 1000 nm; a high vacuum electron beam evaporation method was used to evaporate a thickness of about 3nm platinum Pt film. The Si substrate layer is the Leng Oscilator dispersion model; the natural silicon oxide layer is the Cauchy dispersion model; the non-absorbing medium layer is the Tauc-Lorentz dispersion model of the Si 3 N 4 film; the transition layer is a mixed layer of the Si 3 N 4 layer and the Pt layer, It is a Bruggeman effective approximation model; the platinum Pt film is a Drude-Lorentz Oscilator dispersion model; the air rough layer is a mixed layer of Pt layer and air layer, which is a Bruggeman effective approximation model.
在另一个具体实施例中,采用光谱椭偏仪对金属膜Pt(厚度约为 3nm)进行检测,其中,光谱椭偏仪的入射角设置为70°,波长范围设置为380nm-930nm,非吸收介质层为氧化硅(SiO2),具体方法如下:In another specific embodiment, a spectroscopic ellipsometer is used to detect the metal film Pt (thickness is about 3nm), wherein, the incident angle of the spectroscopic ellipsometer is set to 70°, the wavelength range is set to 380nm-930nm, and the non-absorbing The dielectric layer is silicon oxide (SiO 2 ), and the specific method is as follows:
(1)构建Si衬底和自然氧化硅层组成的第一体系:可选取n-Si (100)衬底作为Si衬底和自然氧化硅层组成的第一体系(体系1),利用光谱椭偏仪测量第一体系,获得第一体系中的Si衬底和自然氧化硅层的椭偏参量,计算并记录所述第一体系中的Si衬底和自然氧化硅层的光学常数及所述第一体系中的所述自然氧化硅层的厚度数据。其中,所计算的自然氧化硅层的厚度为1.27nm;当波长为633nm 时,所计算的自然氧化硅层的折射率为1.5274以及消光系数为0。(1) Construct the first system composed of Si substrate and natural silicon oxide layer: n-Si (100) substrate can be selected as the first system (system 1) composed of Si substrate and natural silicon oxide layer, and use spectral ellipsometry The polarimeter measures the first system, obtains the ellipsometric parameters of the Si substrate and the natural silicon oxide layer in the first system, and calculates and records the optical constants and the described optical constants of the Si substrate and the natural silicon oxide layer in the first system. Thickness data of the native silicon oxide layer in the first system. Wherein, the calculated thickness of the natural silicon oxide layer is 1.27 nm; when the wavelength is 633 nm, the calculated refractive index of the natural silicon oxide layer is 1.5274 and the extinction coefficient is 0.
(2)构建Si衬底、自然氧化硅层以及非吸收介质层组成的第二体系:利用化学气相沉积法在第一体系上方制备厚度为1um的氧化硅(SiO2)膜得到第二体系,利用光谱椭偏仪测量该第二体系中的氧化硅(SiO2)膜的椭偏参量,带入所记录的自然氧化硅层的光学常数和厚度,从而计算并记录所述第二体系中的氧化硅(SiO2)膜的光学常数及厚度。其中,所计算的氧化硅(SiO2)膜的厚度为1033.85nm;当波长为633nm时,所计算的氧化硅(SiO2)膜的折射率为1.4699 以及消光系数为0。(2) Construct the second system consisting of Si substrate, natural silicon oxide layer and non-absorbing dielectric layer: use chemical vapor deposition to prepare a silicon oxide (SiO 2 ) film with a thickness of 1um above the first system to obtain the second system, The ellipsometric parameters of the silicon oxide (SiO 2 ) film in the second system are measured by spectroscopic ellipsometer, and the optical constants and thicknesses of the recorded natural silicon oxide layer are taken into account to calculate and record the oxidation rate in the second system. Optical constants and thicknesses of silicon (SiO 2 ) films. Wherein, the calculated thickness of the silicon oxide (SiO 2 ) film is 1033.85 nm; when the wavelength is 633 nm, the calculated refractive index of the silicon oxide (SiO 2 ) film is 1.4699 and the extinction coefficient is 0.
(3)制备Si衬底、自然氧化硅层、非吸收介质层体系及金属膜层体系:可利用高真空电子束蒸发法在第二体系上方蒸发厚度为3nm 的铂Pt膜,得到第三体系,利用光谱椭偏仪测量该第三体系中铂Pt 膜的椭偏参量,带入所记录的第一体系的自然氧化硅层的光学常数和厚度以及第二体系的中的氧化硅(SiO2)膜所述光学常数及所述厚度,从而计算并记录所述第三体系中的铂Pt膜的光学常数及厚度。其中,所计算的铂Pt膜的厚度为3.815nm;当波长为633nm时,所计算的铂Pt膜的折射率为2.3426以及消光系数为4.20478。(3) Preparation of Si substrate, natural silicon oxide layer, non-absorbing medium layer system and metal film layer system: a platinum Pt film with a thickness of 3nm can be evaporated on the second system by high vacuum electron beam evaporation method to obtain the third system , using spectroscopic ellipsometer to measure the ellipsometric parameters of the platinum Pt film in the third system, the optical constant and thickness of the native silicon oxide layer in the first system and the silicon oxide (SiO 2 ) in the second system film the optical constant and the thickness, so as to calculate and record the optical constant and thickness of the platinum Pt film in the third system. Wherein, the calculated thickness of the platinum Pt film is 3.815 nm; when the wavelength is 633 nm, the calculated refractive index of the platinum Pt film is 2.3426 and the extinction coefficient is 4.20478.
如图8(a)所示,利用电子束蒸发在Si衬底、自然氧化硅层氧化硅(SiO2)组成的第一体系上蒸发超薄Pt膜与未蒸发超薄Pt膜形成的台阶的AFM形貌图。其中虚线左侧为在Si衬底、自然氧化硅层以及氧化硅(SiO2)层体系上蒸发了超薄Pt膜,虚线右侧为并未在 Si衬底、自然氧化硅层以及氧化硅(SiO2)层组成的第二体系上蒸发超薄Pt膜。如图8(b)所示,利用电子束蒸发在Si衬底、自然氧化硅层以及氧化硅(SiO2)层组成的第二体系上蒸发超薄Pt膜与未蒸发超薄Pt膜形成的台阶的垂直高度曲线图。从图8(a)和(b)中可以看出利用高真空电子束蒸发系统蒸发的铂Pt膜的厚度约为2.99nm。采用原子力显微镜(AFM)测量金属膜的厚度(dAFM),与椭偏仪拟合出的厚度(dEI)进行比较,计算厚度偏差(|dEl-dAFM|/dAFM×100) 为27%。As shown in Figure 8(a), the difference between the steps formed by evaporating ultra-thin Pt film and non-evaporated ultra-thin Pt film on the Si substrate and the first system composed of natural silicon oxide layer silicon oxide (SiO 2 ) by electron beam evaporation AFM topography. The left side of the dotted line is the ultra-thin Pt film evaporated on the Si substrate, natural silicon oxide layer and silicon oxide (SiO 2 ) layer system, and the right side of the dotted line is the ultra-thin Pt film that was not evaporated on the Si substrate, natural silicon oxide layer and silicon oxide (SiO 2 ) layer system. An ultrathin Pt film was evaporated on the second system composed of SiO 2 ) layer. As shown in Fig. 8(b), electron beam evaporation was used to evaporate ultra-thin Pt film and non-evaporated ultra-thin Pt film on the second system composed of Si substrate, natural silicon oxide layer and silicon oxide (SiO 2 ) layer. Vertical height graph of steps. From Figure 8(a) and (b), it can be seen that the thickness of the platinum Pt film evaporated by the high vacuum electron beam evaporation system is about 2.99nm. The thickness of the metal film (dAFM) was measured by an atomic force microscope (AFM), and compared with the thickness (dEI) fitted by the ellipsometer, the calculated thickness deviation (|dEl-dAFM|/dAFM×100) was 27%.
如图10所示,其为第二椭偏拟合模型的结构图。该第二椭偏拟合模型的结构层包括:Si衬底层(Si Leng osci)、自然氧化硅层 (SiO2(native))、非吸收介质层(Cau-SiO(CVD))、过渡层(Pt/SiO2)、金属膜层(Pt(platiunum)-DL#1)、空气粗糙层 (Roughness-Air/Pt(Platiunu…))、以及空气层(Air)。其中,利用化学气相沉积法在Si衬底上制备氧化硅(SiO2)膜,厚度为1000nm;利用高真空电子束蒸发法在氧化硅(SiO2)膜上方蒸发厚度约为3nm 的铂Pt膜。Si衬底层为Leng Oscilator色散模型;自然氧化硅层为 Cauchy色散模型;非吸收介质层为氧化硅(SiO2)膜的Cauchy色散模型;过渡层为SiO2层和Pt层的混合层,其为Bruggeman有效近似模型;铂Pt膜为Drude-Lorentz Oscilator色散模型;空气粗糙层为Pt层和空气层的混合层,其为Bruggeman有效近似模型。As shown in FIG. 10 , it is a structural diagram of the second ellipsometric fitting model. The structural layers of the second ellipsometric fitting model include: Si substrate layer (Si Leng osci), natural silicon oxide layer (SiO 2 (native)), non-absorbing dielectric layer (Cau-SiO (CVD)), transition layer ( Pt/SiO 2 ), metal film layer (Pt(platiunum)-DL#1), air roughness layer (Roughness-Air/Pt(Platiunu...)), and air layer (Air). Among them, a silicon oxide (SiO 2 ) film was prepared on a Si substrate by chemical vapor deposition, with a thickness of 1000 nm; a platinum Pt film with a thickness of about 3 nm was evaporated on the silicon oxide (SiO 2 ) film by high vacuum electron beam evaporation. . The Si substrate layer is the Leng Oscilator dispersion model; the natural silicon oxide layer is the Cauchy dispersion model; the non-absorbing medium layer is the Cauchy dispersion model of the silicon oxide (SiO 2 ) film; the transition layer is a mixed layer of SiO 2 layer and Pt layer, which is The Bruggeman effective approximation model; the platinum Pt film is the Drude-Lorentz Oscilator dispersion model; the air rough layer is the mixed layer of the Pt layer and the air layer, which is the Bruggeman effective approximation model.
如图6所示,其为在Si衬底、自然氧化硅层及氮化硅(Si3N4) 层组成的第二体系上蒸发超薄Pt膜的椭偏参量拟合图。如图9所示,其为在Si衬底/自然氧化硅层/氧化硅(SiO2)层体系上蒸发超薄Pt 膜的椭偏参量拟合图。从图6和图9可以看出,一个或多个计算步骤在数学上的拟合度达到极好,即均方误差EMA极低,因此可以说明此计算结果更符合铂Pt膜的真实形貌。As shown in FIG. 6 , it is an ellipsometric fitting diagram of an ultra-thin Pt film evaporated on a second system composed of a Si substrate, a natural silicon oxide layer and a silicon nitride (Si 3 N 4 ) layer. As shown in FIG. 9 , it is an ellipsometric fitting diagram of an ultra-thin Pt film evaporated on a Si substrate/natural silicon oxide layer/silicon oxide (SiO 2 ) layer system. It can be seen from Figure 6 and Figure 9 that one or more calculation steps have an excellent mathematical fit, that is, the mean square error EMA is extremely low, so it can be shown that the calculation results are more in line with the real morphology of the platinum Pt film .
采用本发明实施例所述的利用光谱椭偏仪检测超薄金属膜的方法,能够对薄膜厚度低于10nm的金属膜进行非破坏性、高精度和高灵敏度的检测,测得的金属厚度与实际厚度偏差很小,并且使光谱椭偏仪能够实现对厚度小于10nm的金属膜的检测与拟合,极大地提高了超厚金属膜检测的精度和灵敏度,扩大了可测金属膜的厚度范围。仪器配置简单,容易操作,测量结果稳定可靠,适用范围广泛,具有较好的重现性;同时不会损坏样品,避免了传统测量法对样品的损坏,而导致实验的不可重复性;另外,能够集成到集成电路生产线中,适应集成电路的工艺控制及优化的检测要求,扩大了极限金属膜的椭偏测量范围。Using the method for detecting ultra-thin metal films using spectroscopic ellipsometry described in the embodiments of the present invention, non-destructive, high-precision and high-sensitivity detection can be performed on metal films with a film thickness lower than 10 nm, and the measured metal thickness and The actual thickness deviation is very small, and enables the spectroscopic ellipsometer to detect and fit metal films with a thickness less than 10nm, greatly improving the accuracy and sensitivity of ultra-thick metal film detection, and expanding the thickness range of measurable metal films . The instrument configuration is simple, easy to operate, the measurement results are stable and reliable, the application range is wide, and it has good reproducibility; at the same time, it will not damage the sample, avoiding the damage to the sample caused by the traditional measurement method, which leads to the non-repeatability of the experiment; in addition, It can be integrated into the integrated circuit production line, adapt to the process control and optimized detection requirements of integrated circuits, and expand the ellipsometric measurement range of the limit metal film.
与上述提供的一种利用光谱椭偏仪检测超薄金属膜的方法相对应,本发明还提供一种利用光谱椭偏仪检测超薄金属膜的装置。由于该装置的实施例相似于上述方法实施例,所以描述得比较简单,相关之处请参见上述方法实施例部分的说明即可,下面描述的利用光谱椭偏仪检测超薄金属膜的装置的实施例仅是示意性的。请参考图2所示,其为本发明实施例提供的一种利用光谱椭偏仪检测超薄金属膜的装置的结构示意图。Corresponding to the method for detecting the ultra-thin metal film by using the spectroscopic ellipsometer provided above, the present invention also provides a device for detecting the ultra-thin metal film by using the spectroscopic ellipsometer. Since the embodiment of the device is similar to the above-mentioned method embodiment, it is relatively simple to describe, please refer to the description of the above-mentioned method embodiment part for relevant points, and the device for detecting ultra-thin metal films using a spectroscopic ellipsometer described below The examples are illustrative only. Please refer to FIG. 2 , which is a schematic structural diagram of a device for detecting an ultra-thin metal film using a spectroscopic ellipsometer according to an embodiment of the present invention.
本发明所述的一种利用光谱椭偏仪检测超薄金属膜的装置具体包括如下部分:A kind of device that utilizes spectroscopic ellipsometer to detect ultra-thin metal film according to the present invention specifically comprises the following parts:
第一体系参数确定单元201,用于构建硅衬底和自然氧化硅层组成的第一体系,利用光谱椭偏仪测量所述第一体系中硅衬底和自然氧化硅层的椭偏参量;根据所述椭偏参量,确定所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据;The first system
第二体系参数确定单元202,用于在所述第一体系上制备非吸收介质层,构建硅衬底、自然氧化硅层及非吸收介质层组成的第二体系,利用光谱椭偏仪测量所述第二体系中非吸收介质层的椭偏参量;根据所述非吸收介质层的椭偏参量、所述硅衬底对应的光学常数以及所述自然氧化硅层对应的光学常数和厚度数据,确定所述非吸收介质层的光学常数和厚度数据;The second system
第三体系参数确定单元203,用于在所述第二体系上制备金属膜层,构建硅衬底、自然氧化硅层、非吸收介质层及金属膜层组成的第三体系,利用光谱椭偏仪测量所述第三体系中金属膜层的椭偏参量;根据所述金属膜层的椭偏参量、所述硅衬底对应的光学常数、所述自然氧化硅层对应的光学常数和厚度数据以及所述非吸收介质层的光学常数和厚度数据,确定所述金属膜层的光学常数和厚度数据。The third system
采用本发明实施例所述的利用光谱椭偏仪检测超薄金属膜的装置,能够对薄膜厚度低于10nm的金属膜进行非破坏性、高精度和高灵敏度的检测,测得的金属厚度与实际厚度偏差很小,并且使光谱椭偏仪能够实现对厚度小于10nm的金属膜的检测与拟合,极大地提高了超薄金属膜检测的精度和灵敏度,扩大了可测金属膜的厚度范围。仪器配置简单,容易操作,测量结果稳定可靠,适用范围广泛,具有较好的重现性;同时不会损坏样品,避免了传统测量法对样品的损坏,而导致实验的不可重复性;另外,能够集成到集成电路生产线中,适应集成电路的工艺控制及优化的检测要求,扩大了极限金属膜的椭偏测量范围。Using the device for detecting ultra-thin metal films with a spectroscopic ellipsometer described in the embodiments of the present invention, non-destructive, high-precision and high-sensitivity detection can be performed on metal films with a film thickness lower than 10 nm, and the measured metal thickness is consistent with The actual thickness deviation is very small, and enables the spectroscopic ellipsometer to detect and fit metal films with a thickness less than 10nm, greatly improving the accuracy and sensitivity of ultra-thin metal film detection, and expanding the thickness range of measurable metal films . The instrument configuration is simple, easy to operate, the measurement results are stable and reliable, the application range is wide, and it has good reproducibility; at the same time, it will not damage the sample, avoiding the damage to the sample caused by the traditional measurement method, which leads to the non-repeatability of the experiment; in addition, It can be integrated into the integrated circuit production line, adapt to the process control and optimized detection requirements of integrated circuits, and expand the ellipsometric measurement range of the limit metal film.
下面基于本发明所述的利用光谱椭偏仪的超薄金属膜的光学表征方法,对其实施例进行详细描述。如图3所示,其为本发明实施例提供的一种利用光谱椭偏仪的超薄金属膜的光学表征方法的流程示意图,具体实现过程包括以下步骤:Based on the optical characterization method of ultra-thin metal film using spectroscopic ellipsometer according to the present invention, its embodiment will be described in detail below. As shown in FIG. 3 , it is a schematic flowchart of an optical characterization method using a spectroscopic ellipsometer for an ultra-thin metal film provided by an embodiment of the present invention. The specific implementation process includes the following steps:
步骤301:设定光谱椭偏仪的操作参数。其中,所述操作参数包括:入射角参数、测量波长范围参数、测量波长的间隔参数以及参考表征波长参数等中的至少一种。Step 301: Setting the operating parameters of the spectroscopic ellipsometer. Wherein, the operating parameters include: at least one of an incident angle parameter, a measurement wavelength range parameter, a measurement wavelength interval parameter, and a reference characteristic wavelength parameter.
步骤302:构建测量金属膜层的椭偏拟合模型。Step 302: Construct an ellipsometric fitting model for measuring the metal film layer.
步骤303:利用所述光谱椭偏仪分别测量所述椭偏拟合模型的结构层所对应的椭偏参量;所述结构层包括硅衬底层、自然氧化硅层、非吸收介质层、过渡层、金属膜层、空气粗糙层以及空气层;其中,所述过渡层中的第二非吸收介层对应的椭偏参量与所述非吸收介质层对应的椭偏参量相同。Step 303: Use the spectroscopic ellipsometer to measure the ellipsometric parameters corresponding to the structural layers of the ellipsometric fitting model; the structural layers include a silicon substrate layer, a natural silicon oxide layer, a non-absorbing medium layer, and a transition layer , a metal film layer, an air rough layer, and an air layer; wherein, the ellipsometric parameter corresponding to the second non-absorbing medium layer in the transition layer is the same as the ellipsometric parameter corresponding to the non-absorbing medium layer.
步骤304:将所述结构层对应的椭偏参量与所述椭偏拟合模型进行拟合,得到所述金属膜层的光学常数及厚度数据。Step 304: Fitting the ellipsometric parameters corresponding to the structural layer with the ellipsometric fitting model to obtain the optical constant and thickness data of the metal film layer.
其中,所述过渡层由第二非吸收介质层与第二金属膜层组成,所述过渡层为Bruggeman有效近似模型。需要的说明的是,在具体实施过程中,所述过渡层不限于Bruggeman有效近似模型,还可以为其他拟合模型,在此不做具体限定。Wherein, the transition layer is composed of a second non-absorbing medium layer and a second metal film layer, and the transition layer is a Bruggeman effective approximate model. It should be noted that, in a specific implementation process, the transition layer is not limited to the Bruggeman effective approximation model, and may also be other fitting models, which are not specifically limited here.
所述空气粗糙层由第三金属膜层与第二空气层组成,所述过渡层为Bruggeman有效近似模型。需要的说明的是,在具体实施过程中,所述空气粗糙层不限于Bruggeman有效近似模型,还可以为其他拟合模型,在此不做具体限定。The rough air layer is composed of a third metal film layer and a second air layer, and the transition layer is a Bruggeman effective approximation model. It should be noted that, in the specific implementation process, the rough air layer is not limited to the Bruggeman effective approximation model, but can also be other fitting models, which are not specifically limited here.
采用本发明实施例所述的利用光谱椭偏仪的超薄金属膜的光学表征方法,能够对薄膜厚度低于10nm的金属膜进行非破坏性、高精度和高灵敏度的光学性质表征;仪器配置简单,容易操作,具有较好的重现性;同时不会损坏样品,避免了传统测量法对样品的损坏,而导致实验的不可重复性;另外,能够集成到集成电路生产线中,适应集成电路的工艺控制及优化的检测要求,扩大了极限金属膜的椭偏测量范围。Using the optical characterization method of the ultra-thin metal film using spectroscopic ellipsometer described in the embodiment of the present invention, it is possible to perform non-destructive, high-precision and high-sensitivity optical property characterization of the metal film with a film thickness of less than 10 nm; instrument configuration Simple, easy to operate, and has good reproducibility; at the same time, it will not damage the sample, avoiding the damage to the sample caused by the traditional measurement method, which leads to the unrepeatability of the experiment; in addition, it can be integrated into the integrated circuit production line, suitable for integrated circuit The process control and optimized detection requirements have expanded the ellipsometric measurement range of the limit metal film.
与上述提供的一种利用光谱椭偏仪的超薄金属膜的光学表征方法相对应,本发明还提供一种利用光谱椭偏仪的超薄金属膜的光学表征装置。由于该装置的实施例相似于上述方法实施例,所以描述得比较简单,相关之处请参见上述方法实施例部分的说明即可,下面描述的利用光谱椭偏仪的超薄金属膜的光学表征装置的实施例仅是示意性的。请参考图4所示,其为本发明实施例提供的一种利用光谱椭偏仪的超薄金属膜的光学表征装置的结构示意图。Corresponding to the optical characterization method of the ultra-thin metal film using the spectroscopic ellipsometer provided above, the present invention also provides an optical characterization device of the ultra-thin metal film using the spectroscopic ellipsometer. Since the embodiment of the device is similar to the above-mentioned method embodiment, the description is relatively simple. Please refer to the description of the above-mentioned method embodiment for the relevant parts. The optical characterization of the ultra-thin metal film using the spectroscopic ellipsometer described below The embodiments of the device are illustrative only. Please refer to FIG. 4 , which is a schematic structural diagram of an optical characterization device using a spectroscopic ellipsometer for an ultra-thin metal film provided by an embodiment of the present invention.
本发明所述的一种利用光谱椭偏仪的超薄金属膜的光学表征装置具体包括如下部分:An optical characterization device of an ultra-thin metal film using a spectroscopic ellipsometer according to the present invention specifically includes the following parts:
操作参数设定单元401,用于设定光谱椭偏仪的操作参数。An operating
椭偏拟合模型构建单元402,用于构建测量金属膜层的椭偏拟合模型。The ellipsometric fitting
椭偏参量测量单元403,用于利用所述光谱椭偏仪分别测量所述椭偏拟合模型的结构层所对应的椭偏参量;所述结构层包括硅衬底层、自然氧化硅层、非吸收介质层、过渡层、金属膜层、空气粗糙层以及空气层;其中,所述过渡层中的第二非吸收介层对应的椭偏参量与所述非吸收介质层对应的椭偏参量相同。The ellipsometric
金属膜层数据获得单元404,用于将所述结构层对应的椭偏参量与所述椭偏拟合模型进行拟合,得到所述金属膜层的光学常数及厚度数据。The metal film layer
采用本发明实施例所述的利用光谱椭偏仪的超薄金属膜的光学表征装置,能够对薄膜厚度低于10nm的金属膜进行非破坏性、高精度和高灵敏度的光学性质表征;仪器配置简单,容易操作,具有较好的重现性;同时不会损坏样品,避免了传统测量法对样品的损坏,而导致实验的不可重复性;另外,能够集成到集成电路生产线中,适应集成电路的工艺控制及优化的检测要求,扩大了极限金属膜的椭偏测量范围。Using the optical characterization device for ultra-thin metal films using spectroscopic ellipsometer described in the embodiments of the present invention, it is possible to perform non-destructive, high-precision and high-sensitivity optical property characterization of metal films with a film thickness of less than 10 nm; instrument configuration Simple, easy to operate, and has good reproducibility; at the same time, it will not damage the sample, avoiding the damage to the sample caused by the traditional measurement method, which leads to the unrepeatability of the experiment; in addition, it can be integrated into the integrated circuit production line, suitable for integrated circuit The process control and optimized detection requirements have expanded the ellipsometric measurement range of the limit metal film.
以上实施例仅用以说明本发明的技术方案而非对其进行限制,本方法旨在利用光学椭偏仪提高各种弱信号超薄膜的测量精度和灵敏度(包括超薄膜如亚纳米厚度的金属膜或其他膜系等弱信号体系),在不背离本发明精神及其实质的情况下,熟悉本领域的技术人员当可根据本发明作出各种相应的改变和变形,但这些相应的改变和变形都应属于本发明所附的权利要求的保护范围。Above embodiment is only in order to illustrate technical scheme of the present invention and is not limited to it, and this method aims at utilizing optical ellipsometer to improve the measurement accuracy and the sensitivity of various weak signal ultra-thin films (comprising ultra-thin films such as sub-nanometer thickness metals Weak signal systems such as films or other film systems), without departing from the spirit and essence of the present invention, those skilled in the art can make various corresponding changes and deformations according to the present invention, but these corresponding changes and All deformations should belong to the protection scope of the appended claims of the present invention.
还应当注释的是,在一些可替代实施方式中,框中注释的功能可以不按附图中注释的顺序发生。例如,连续示出的两个框实际上可以基本上同时执行,或者这些框有时可以以相反的顺序执行,这取决于所涉及的功能。可以设想其他步骤和方法,其在功能、逻辑或效果上等同于所图示的附图的一个或多个框或其部分。It should also be noted that, in some alternative implementations, the functions noted in the block may occur out of the order noted in the figures. For example, two blocks shown in succession may, in fact, be executed substantially concurrently, or the blocks may sometimes be executed in the reverse order, depending upon the functionality involved. Other steps and methods may be conceived that are equivalent in function, logic, or effect to one or more blocks of the illustrated figures, or portions thereof.
尽管可以在流程图和/或框图中采用各种箭头类型和线类型,但是应当理解它们不限制相对应实施例的范围。实际上,一些箭头或其他连接器可以仅用于指示所描绘实施例的逻辑流程。例如,箭头可以指示所描绘的实施例的枚举步骤之间的未指定持续时间的等待或监视时段。还将会注释的是,框图和/或流程图的每个框以及框图和/或流程图中的框的组合,能够由执行特定功能或操作的基于专用硬件的系统,或专用硬件和代码的组合来实现。Although various arrow types and line types may be employed in flowcharts and/or block diagrams, it should be understood that they do not limit the scope of the corresponding embodiments. In fact, some arrows or other connectors may merely be used to indicate the logical flow of the depicted embodiments. For example, an arrow may indicate a waiting or monitoring period of unspecified duration between enumerated steps of the depicted embodiment. It will also be noted that each block of the block diagrams and/or flowcharts, and combinations of blocks in the block diagrams and/or flowcharts, can be implemented by a dedicated hardware-based system that performs the specified function or operation, or by a combination of dedicated hardware and code. combination to achieve.
虽然本说明书包含许多具体的实现细节,但是这些不应当被解释为对任何发明或所要求保护的内容的范围的限制,而是对具体发明的具体实现所特有的特征的描述。在本说明书中在单独实现的上下文中描述的某些特征也可以在单个实现方式中组合实现。相反地,在单个实现的上下文中描述的各种特征也可以单独地或以任何合适的子组合在多个实现方式中实现。此外,虽然以上可以将特征描述为以某些组合起作用并且甚至最初如此要求保护,但是来自要求保护的组合的一个或多个特征在一些情况下可以从该组合中删除,并且要求保护的组合可以针对子组合或子组合的变体。While this specification contains many specific implementation details, these should not be construed as limitations on the scope of any inventions or of what may be claimed, but rather as descriptions of features that are specific to particular implementations of particular inventions. Certain features that are described in this specification in the context of separate implementations can also be implemented in combination in a single implementation. Conversely, various features that are described in the context of a single implementation can also be implemented in multiple implementations separately or in any suitable subcombination. Furthermore, although features above may be described as functioning in certain combinations and even initially claimed as such, one or more features from a claimed combination may in some cases be deleted from that combination and the claimed combination Can target subgroups or variations of subgroups.
对本公开中描述的实现的各种修改对本领域技术人员来说是显而易见的,并且在不脱离本公开的精神或范围的情况下,这里定义的一般原理可以应用于其它实现。因此,权利要求书不希望限于本文所示的实现方式,而是应符合与本文所揭示内容、原理和新颖特征一致的最广泛范围。Various modifications to the implementations described in this disclosure will be readily apparent to those skilled in the art, and the generic principles defined herein may be applied to other implementations without departing from the spirit or scope of the disclosure. Thus, the claims are not intended to be limited to the implementations shown herein but are to be accorded the widest scope consistent with the teachings, principles and novel features disclosed herein.
最后应说明的是:以上实施例仅用以说明本发明的技术方案,而非对其限制;尽管参照前述实施例对本发明进行了详细的说明,本领域的普通技术人员应当理解:其依然可以对前述各实施例所记载的技术方案进行修改,或者对其中部分技术特征进行等同替换;而这些修改或者替换,并不使相应技术方案的本质脱离本发明各实施例技术方案的精神和范围。Finally, it should be noted that: the above embodiments are only used to illustrate the technical solutions of the present invention, rather than to limit them; although the present invention has been described in detail with reference to the foregoing embodiments, those of ordinary skill in the art should understand that: it can still be Modifications are made to the technical solutions described in the foregoing embodiments, or equivalent replacements are made to some of the technical features; and these modifications or replacements do not make the essence of the corresponding technical solutions deviate from the spirit and scope of the technical solutions of the various embodiments of the present invention.
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