CN112097626A - A method for measuring the thickness of metal thin films based on resistance method - Google Patents
A method for measuring the thickness of metal thin films based on resistance method Download PDFInfo
- Publication number
- CN112097626A CN112097626A CN202011150197.9A CN202011150197A CN112097626A CN 112097626 A CN112097626 A CN 112097626A CN 202011150197 A CN202011150197 A CN 202011150197A CN 112097626 A CN112097626 A CN 112097626A
- Authority
- CN
- China
- Prior art keywords
- film
- thickness
- resistance
- standard
- thin film
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B7/00—Measuring arrangements characterised by the use of electric or magnetic techniques
- G01B7/02—Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness
- G01B7/06—Measuring arrangements characterised by the use of electric or magnetic techniques for measuring length, width or thickness for measuring thickness
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L22/00—Testing or measuring during manufacture or treatment; Reliability measurements, i.e. testing of parts without further processing to modify the parts as such; Structural arrangements therefor
- H01L22/10—Measuring as part of the manufacturing process
- H01L22/12—Measuring as part of the manufacturing process for structural parameters, e.g. thickness, line width, refractive index, temperature, warp, bond strength, defects, optical inspection, electrical measurement of structural dimensions, metallurgic measurement of diffusions
Landscapes
- Engineering & Computer Science (AREA)
- Manufacturing & Machinery (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
- Measurement Of Resistance Or Impedance (AREA)
Abstract
本发明提出一种基于电阻法的金属薄膜厚度测量方法,所述测量方法包括取得待测工件金属薄膜的电阻值数据曲线的方法;所述电阻值数据曲线为反映金属薄膜电阻值与金属薄膜厚度对应关系的电阻‑厚度标准曲线;在测量金属薄膜厚度时,根据待测金属薄膜的电阻值,从电阻‑厚度标准曲线得到与该电阻值对应的金属薄膜厚度;本发明操作简单,所能测量的厚度范围广,且本方法属于非接触式测量,不会对待测样品造成损坏,属于无损检测技术。
The present invention provides a method for measuring the thickness of a metal thin film based on a resistance method. The measuring method includes a method for obtaining a resistance value data curve of the metal thin film of a workpiece to be measured; the resistance value data curve reflects the resistance value of the metal thin film and the thickness of the metal thin film. The resistance-thickness standard curve of the corresponding relationship; when measuring the thickness of the metal film, according to the resistance value of the metal film to be measured, the metal film thickness corresponding to the resistance value is obtained from the resistance-thickness standard curve; the present invention is simple to operate and can measure It has a wide range of thickness, and this method belongs to non-contact measurement, which will not cause damage to the sample to be tested, and belongs to non-destructive testing technology.
Description
技术领域technical field
本发明涉及半导体制造领域,尤其是一种基于电阻法的金属薄膜厚度测量方法。The invention relates to the field of semiconductor manufacturing, in particular to a method for measuring the thickness of a metal thin film based on a resistance method.
背景技术Background technique
近年来,随着技术的进步,光电器件、激光器件、微电子器件、集成电路等各种半导体器件朝着微型化方向发展,其基础材料金属电极的厚度也越来越薄。通常把厚度低于1μm以下的材料称为薄膜材料,金属薄膜的厚度在很大程度上会影响其力学、光学、电学、磁学等物理性质,从而影响半导体器件的性能,因此简单、迅速、低成本且精确地测量金属薄膜厚度具有非常重要的实际意义。In recent years, with the advancement of technology, various semiconductor devices such as optoelectronic devices, laser devices, microelectronic devices, integrated circuits, etc. are developing towards the direction of miniaturization, and the thickness of the metal electrodes of their basic materials is getting thinner and thinner. Materials with a thickness of less than 1 μm are usually referred to as thin-film materials. The thickness of metal thin films will largely affect its physical properties such as mechanics, optics, electricity, and magnetism, thereby affecting the performance of semiconductor devices. Low-cost and accurate measurement of metal film thickness is of great practical importance.
目前金属薄膜厚度的测量方法主要有机械测量法、光学测量法和电学测量法等。At present, the measurement methods of metal film thickness mainly include mechanical measurement method, optical measurement method and electrical measurement method.
早期的机械测量法是机械式探针法,也称作轮廓法,典型代表设备有台阶仪。该方法利用微小高精度机械触针(一般只有几个微米)接触待测薄膜的表面,在物体表面运动来感知表面轮廓的变化,有薄膜覆盖的样品表面与没有薄膜覆盖的样品表面之间的高度差为薄膜厚度。该方法具有稳定性好,测量范围大等优点。但该方法是基于机械运动的探针,其精度受限于所用探针的大小;此外最严重的是探针在样品表面移动会划伤薄膜表面,是有损检测。The early mechanical measurement method is the mechanical probe method, also known as the profile method, and the typical representative equipment is a step meter. This method uses a tiny high-precision mechanical stylus (usually only a few microns) to contact the surface of the film to be tested, and moves on the surface of the object to sense the change of the surface profile. The height difference is the film thickness. The method has the advantages of good stability and large measurement range. However, this method is based on the mechanical movement of the probe, and its accuracy is limited by the size of the probe used; in addition, the most serious is that the probe moves on the sample surface, which will scratch the surface of the film, which is a destructive detection.
为了避免接触,发展了扫描探针显微法,它是应用扫描探针显微镜对薄膜进行相关参数测量,原子力显微镜就是最具代表性的扫描探针显微镜,原子力显微镜的探针被放置于微悬臂上,利用光学杠杆原理测出微悬臂在探针与薄膜原子的相互作用力下的形变,从而测得薄膜表面的形貌。具有高分辨力,无损测量等优点。但由于该方法是利用光学杠杆原理来测量微悬臂的形变,容易受到光电噪声、振动等因素影响;并且设备比较昂贵,测试成本较高。In order to avoid contact, scanning probe microscopy was developed, which is to use scanning probe microscopy to measure related parameters of thin films. AFM is the most representative scanning probe microscope. The probe of atomic force microscopy is placed on a microcantilever. On the above, the deformation of the microcantilever under the interaction force between the probe and the film atoms is measured by the principle of optical lever, so as to measure the topography of the film surface. It has the advantages of high resolution and non-destructive measurement. However, because this method uses the optical lever principle to measure the deformation of the micro-cantilever, it is easily affected by factors such as photoelectric noise and vibration; and the equipment is relatively expensive and the test cost is high.
光学测量法的测量原理是利用光学偏振、干涉特性,其中椭圆偏振法应用比较多,其典型代表设备有椭偏仪。当偏振光从空气入射到薄膜后,其反射的光线的偏振成分会随着薄膜厚度,入射角大小等改变,通过检测和分析入射光与反射光偏振态的变化来反演推导薄膜的厚度。该方法具有无损、非接触、高精度、高灵敏度的特点。但是椭圆偏振法存在一个膜厚周期,只有在该周期内使用椭圆偏振法才能够测得精确的薄膜厚度值,如果测量的范围超过该周期,则薄膜的厚度将有多个不确定值,因此椭圆偏振法测量的薄膜厚度范围一般从1nm到1μm,且以10nm左右的薄膜厚度测量为最佳;此外,该方法是一种间接测量法,依靠对色散模型的拟合得到薄膜厚度,但色散模型的建立过程复杂而繁琐,会给测量结果带来很多不确定性。The measurement principle of the optical measurement method is to use the optical polarization and interference characteristics. Among them, the ellipsometry method is widely used, and its typical representative equipment is an ellipsometer. When the polarized light is incident on the film from the air, the polarization component of the reflected light will change with the thickness of the film, the angle of incidence, etc. The thickness of the film can be inverted and deduced by detecting and analyzing the changes in the polarization state of the incident light and the reflected light. The method has the characteristics of non-destructive, non-contact, high precision and high sensitivity. However, there is a film thickness period in ellipsometry, and only within this period can the exact film thickness value be measured by using ellipsometry. If the measurement range exceeds this period, the thickness of the film will have multiple uncertain values, so The film thickness measured by ellipsometry generally ranges from 1nm to 1μm, and the film thickness of about 10nm is the best; in addition, this method is an indirect measurement method, which relies on the fitting of the dispersion model to obtain the film thickness, but the dispersion The modeling process is complex and tedious, which will bring a lot of uncertainty to the measurement results.
相对其他方法,电学测量法精度相对较差,但其具有简单、迅速、低成本的优点,电学测量法主要包括电阻法、电容法和石英晶体法等。其中电阻法是一种较为简单的电学测量方法,其通常采用电桥测量样品两端电流电压,再推导出薄膜电阻值,但在测量时探针与薄膜接触压力较大容易划伤薄膜,接触压力较小会产生较大的接触电阻,两种情况都会导致测量数据不准确。Compared with other methods, the electrical measurement method has relatively poor accuracy, but it has the advantages of simplicity, rapidity and low cost. The electrical measurement methods mainly include resistance method, capacitance method and quartz crystal method. Among them, the resistance method is a relatively simple electrical measurement method. It usually uses an electric bridge to measure the current and voltage at both ends of the sample, and then deduces the film resistance value. However, the contact pressure between the probe and the film is large during the measurement, and the film is easily scratched. Lower pressure creates higher contact resistance, both of which can lead to inaccurate measurement data.
发明内容SUMMARY OF THE INVENTION
本发明提出一种基于电阻法的金属薄膜厚度测量方法,操作简单,所能测量的厚度范围广,且本方法属于非接触式测量,不会对待测样品造成损坏,属于无损检测技术。The invention provides a method for measuring the thickness of a metal thin film based on a resistance method, which is simple to operate and can measure a wide range of thicknesses, and the method belongs to non-contact measurement, which will not cause damage to the sample to be measured, and belongs to non-destructive testing technology.
本发明采用以下技术方案。The present invention adopts the following technical solutions.
一种基于电阻法的金属薄膜厚度测量方法,所述测量方法包括取得待测工件金属薄膜的电阻值数据曲线的方法;所述电阻值数据曲线为反映金属薄膜电阻值与金属薄膜厚度对应关系的电阻-厚度标准曲线;在测量金属薄膜厚度时,根据待测金属薄膜的电阻值,从电阻-厚度标准曲线得到与该电阻值对应的金属薄膜厚度。A method for measuring the thickness of a metal thin film based on a resistance method, the measuring method includes a method for obtaining a resistance value data curve of a metal thin film of a workpiece to be measured; Resistance-thickness standard curve; when measuring the thickness of the metal film, according to the resistance value of the metal film to be measured, the thickness of the metal film corresponding to the resistance value is obtained from the resistance-thickness standard curve.
所述金属薄膜设于工件的衬底上;所述取得待测工件金属薄膜的电阻值数据曲线的方法,包括以下步骤;The metal film is arranged on the substrate of the workpiece; the method for obtaining the resistance value data curve of the metal film of the workpiece to be measured includes the following steps;
步骤一、将衬底清洗干净,并烘干;Step 1. Clean the substrate and dry it;
步骤二、在衬底上加第一掩膜版,以掩膜工艺来在衬底上生长测量用的电极;Step 2, adding a first mask on the substrate to grow electrodes for measurement on the substrate by a mask process;
步骤三、去除掩膜版,在衬底上制备具有相同表面积且不同厚度的标准薄膜;并使薄膜与电极相接;Step 3, removing the mask, preparing standard thin films with the same surface area and different thicknesses on the substrate; connecting the thin films with the electrodes;
步骤四、测量标准薄膜的厚度以及相应的电阻值;Step 4: Measure the thickness of the standard film and the corresponding resistance value;
步骤五、对所得数据进行拟合,得到反映薄膜电阻与薄膜厚度关系的电阻-厚度标准曲线。Step 5: Fitting the obtained data to obtain a resistance-thickness standard curve reflecting the relationship between the film resistance and the film thickness.
在测量工件上的金属薄膜厚度时,先以步骤一至步骤二所述方法,在待测工件上生成电极,再在工件衬底上制备与电极相连的待测量金属薄膜;然后测量金属薄膜的电阻,根据测得的薄膜电阻,从电阻-厚度标准曲线查知金属薄膜的厚度。When measuring the thickness of the metal film on the workpiece, first use the methods described in steps 1 to 2 to generate electrodes on the workpiece to be measured, and then prepare the metal film to be measured connected to the electrode on the workpiece substrate; then measure the resistance of the metal film , according to the measured sheet resistance, find out the thickness of the metal film from the resistance-thickness standard curve.
所述步骤一中,衬底为表面平整的玻璃片或抛光硅片,当衬底为硅片时,硅片表面镀有绝缘层,所述绝缘层的成分为氧化硅、氮化硅、氧化铝中的一种或者多种的组合。In the first step, the substrate is a glass sheet or a polished silicon wafer with a flat surface. When the substrate is a silicon wafer, the surface of the silicon wafer is plated with an insulating layer, and the composition of the insulating layer is silicon oxide, silicon nitride, oxide A combination of one or more of aluminum.
所述步骤二中,测量用的电极包括阴极和阳极,其电极的材料成分为银、铜、金、铝中的一种或者多种的组合。In the second step, the electrodes used for measurement include a cathode and an anode, and the material components of the electrodes are one or a combination of silver, copper, gold, and aluminum.
所述步骤三中相同表面积但不同厚度的标准薄膜,其制备过程包括三种方法;The standard film with the same surface area but different thickness in the step 3, the preparation process includes three methods;
第一种方法,在薄膜生长前,使用第二掩膜版加于薄膜生长区处,以掩膜工艺来生长薄膜;In the first method, before the thin film is grown, a second mask is applied to the thin film growth area, and the thin film is grown by a mask process;
第二种方法,在薄膜生长后,若需提升测量精度,则对样品采用激光划片;In the second method, after the film is grown, if the measurement accuracy needs to be improved, laser scribing is used on the sample;
第三种方法,在薄膜生长后,若对测量精度要求不高,则对样品采用金刚刀划片。In the third method, after the film is grown, if the measurement accuracy is not high, a diamond knife is used for scribing the sample.
在步骤四中,用台阶仪或椭偏仪或原子力显微镜测量标准薄膜的厚度;用电桥测量标准薄膜的电阻。In step 4, measure the thickness of the standard thin film with a step meter, ellipsometer or atomic force microscope; measure the resistance of the standard thin film with an electric bridge.
所述电极、标准薄膜和待测量薄膜的生长工艺包括磁控溅射、热蒸发、电子束蒸发和原子层沉积;The growth process of the electrode, the standard film and the film to be measured includes magnetron sputtering, thermal evaporation, electron beam evaporation and atomic layer deposition;
在测量工件上的金属薄膜厚度时,若待测量金属薄膜的表面积与标准薄膜相同,则可以直接带入电阻-厚度标准曲线进行计算;若待测量金属薄膜的表面积与标准薄膜不相同,则通过下列公式将待测薄膜的电阻转换成等效标准薄膜电阻后,再带入电阻-厚度标准曲线;When measuring the thickness of the metal film on the workpiece, if the surface area of the metal film to be measured is the same as the standard film, it can be directly brought into the resistance-thickness standard curve for calculation; if the surface area of the metal film to be measured is different from the standard film, pass The following formula converts the resistance of the film to be measured into the equivalent standard film resistance, and then brings it into the resistance-thickness standard curve;
所述转换公式为 公式一;The conversion formula is formula one;
其中R1为等效标准薄膜电阻,R2待测薄膜电阻,l1为标准薄膜长度,a1为标准薄膜宽度,l2为标准薄膜长度,a2为标准薄膜宽度。Among them, R1 is the equivalent standard film resistance, R2 is the film resistance to be measured, l1 is the standard film length, a1 is the standard film width, l2 is the standard film length, and a2 is the standard film width.
待测量薄膜与标准薄膜的生长工艺一致。The growth process of the film to be measured is the same as that of the standard film.
与传统的电阻测量法相比,本发明具有的有益效果是:Compared with the traditional resistance measurement method, the present invention has the following beneficial effects:
1.由于在待测金属薄膜厚度的测量过程中,仅需要对样品进行电阻的测量,电阻测量设备种类非常多而且价格低廉,测试成本低,并且操作简单,容易推广。1. In the process of measuring the thickness of the metal film to be measured, only the resistance of the sample needs to be measured. There are many types of resistance measuring equipment, and the price is low, the test cost is low, and the operation is simple and easy to popularize.
2.由于本发明没有使用探针直接接触薄膜表面,属于非接触式测量,不会对待测样品造成损坏,属于无损检测技术。2. Since the present invention does not use the probe to directly contact the surface of the film, it belongs to non-contact measurement and will not cause damage to the sample to be tested, which is a non-destructive testing technology.
3.在待测样品表面尺寸方面,如果对测量精度要求较高,则采用激光划片,大大增加样品尺寸的精度;如果对测量精度要求不高,则采用金刚刀划片,操作非常简单,极大缩短测量时间。3. In terms of the surface size of the sample to be measured, if the measurement accuracy is high, laser scribing is used to greatly increase the accuracy of the sample size; if the measurement accuracy is not high, the diamond knife is used for scribing, and the operation is very simple. Greatly shorten the measurement time.
4.本发明能够测量的厚度范围非常广,从几纳米到几百纳米,测量误差可控制在10%以内。4. The thickness range that can be measured by the present invention is very wide, from a few nanometers to several hundreds of nanometers, and the measurement error can be controlled within 10%.
附图说明Description of drawings
下面结合附图和具体实施方式对本发明进一步详细的说明:The present invention will be described in further detail below in conjunction with the accompanying drawings and specific embodiments:
附图1是第一掩膜版的示意图;Accompanying drawing 1 is the schematic diagram of the first mask;
附图2是第二掩膜版的示意图;Accompanying drawing 2 is the schematic diagram of the second mask;
附图3是电阻-厚度标准曲线的示意图。Figure 3 is a schematic diagram of a resistance-thickness standard curve.
具体实施方式Detailed ways
如图所示,一种基于电阻法的金属薄膜厚度测量方法,所述测量方法包括取得待测工件金属薄膜的电阻值数据曲线的方法;所述电阻值数据曲线为反映金属薄膜电阻值与金属薄膜厚度对应关系的电阻-厚度标准曲线;在测量金属薄膜厚度时,根据待测金属薄膜的电阻值,从电阻-厚度标准曲线得到与该电阻值对应的金属薄膜厚度。As shown in the figure, a method for measuring the thickness of a metal thin film based on a resistance method, the measuring method includes a method of obtaining the resistance value data curve of the metal thin film of the workpiece to be measured; the resistance value data curve reflects the resistance value of the metal thin film and the metal thin film. The resistance-thickness standard curve of the film thickness correspondence; when measuring the metal film thickness, according to the resistance value of the metal film to be measured, the metal film thickness corresponding to the resistance value is obtained from the resistance-thickness standard curve.
所述金属薄膜设于工件的衬底上;所述取得待测工件金属薄膜的电阻值数据曲线的方法,包括以下步骤;The metal film is arranged on the substrate of the workpiece; the method for obtaining the resistance value data curve of the metal film of the workpiece to be measured includes the following steps;
步骤一、将衬底清洗干净,并烘干;Step 1. Clean the substrate and dry it;
步骤二、在衬底上加第一掩膜版,以掩膜工艺来在衬底上生长测量用的电极;Step 2, adding a first mask on the substrate to grow electrodes for measurement on the substrate by a mask process;
步骤三、去除掩膜版,在衬底上制备具有相同表面积且不同厚度的标准薄膜;并使薄膜与电极相接;Step 3, removing the mask, preparing standard thin films with the same surface area and different thicknesses on the substrate; connecting the thin films with the electrodes;
步骤四、测量标准薄膜的厚度以及相应的电阻值;Step 4: Measure the thickness of the standard film and the corresponding resistance value;
步骤五、对所得数据进行拟合,得到反映薄膜电阻与薄膜厚度关系的电阻-厚度标准曲线。Step 5: Fitting the obtained data to obtain a resistance-thickness standard curve reflecting the relationship between the film resistance and the film thickness.
在测量工件上的金属薄膜厚度时,先以步骤一至步骤二所述方法,在待测工件上生成电极,再在工件衬底上制备与电极相连的待测量金属薄膜;然后测量金属薄膜的电阻,根据测得的薄膜电阻,从电阻-厚度标准曲线查知金属薄膜的厚度。When measuring the thickness of the metal film on the workpiece, first use the methods described in steps 1 to 2 to generate electrodes on the workpiece to be measured, and then prepare the metal film to be measured connected to the electrode on the workpiece substrate; then measure the resistance of the metal film , according to the measured sheet resistance, find out the thickness of the metal film from the resistance-thickness standard curve.
所述步骤一中,衬底为表面平整的玻璃片或抛光硅片,当衬底为硅片时,硅片表面镀有绝缘层,所述绝缘层的成分为氧化硅、氮化硅、氧化铝中的一种或者多种的组合。In the first step, the substrate is a glass sheet or a polished silicon wafer with a flat surface. When the substrate is a silicon wafer, the surface of the silicon wafer is plated with an insulating layer, and the composition of the insulating layer is silicon oxide, silicon nitride, oxide A combination of one or more of aluminum.
所述步骤二中,测量用的电极包括阴极和阳极,其电极的材料成分为银、铜、金、铝中的一种或者多种的组合。In the second step, the electrodes used for measurement include a cathode and an anode, and the material components of the electrodes are one or a combination of silver, copper, gold, and aluminum.
所述步骤三中相同表面积但不同厚度的标准薄膜,其制备过程包括三种方法;The standard film with the same surface area but different thickness in the step 3, the preparation process includes three methods;
第一种方法,在薄膜生长前,使用第二掩膜版加于薄膜生长区处,以掩膜工艺来生长薄膜;In the first method, before the thin film is grown, a second mask is applied to the thin film growth area, and the thin film is grown by a mask process;
第二种方法,在薄膜生长后,若需提升测量精度,则对样品采用激光划片;In the second method, after the film is grown, if the measurement accuracy needs to be improved, laser scribing is used on the sample;
第三种方法,在薄膜生长后,若对测量精度要求不高,则对样品采用金刚刀划片。In the third method, after the film is grown, if the measurement accuracy is not high, a diamond knife is used for scribing the sample.
在步骤四中,用台阶仪或椭偏仪或原子力显微镜测量标准薄膜的厚度;用电桥测量标准薄膜的电阻。In step 4, measure the thickness of the standard thin film with a step meter, ellipsometer or atomic force microscope; measure the resistance of the standard thin film with an electric bridge.
所述电极、标准薄膜和待测量薄膜的生长工艺包括磁控溅射、热蒸发、电子束蒸发和原子层沉积;The growth process of the electrode, the standard film and the film to be measured includes magnetron sputtering, thermal evaporation, electron beam evaporation and atomic layer deposition;
在测量工件上的金属薄膜厚度时,若待测量金属薄膜的表面积与标准薄膜相同,则可以直接带入电阻-厚度标准曲线进行计算;若待测量金属薄膜的表面积与标准薄膜不相同,则通过下列公式将待测薄膜的电阻转换成等效标准薄膜电阻后,再带入电阻-厚度标准曲线;When measuring the thickness of the metal film on the workpiece, if the surface area of the metal film to be measured is the same as the standard film, it can be directly brought into the resistance-thickness standard curve for calculation; if the surface area of the metal film to be measured is different from the standard film, pass The following formula converts the resistance of the film to be measured into the equivalent standard film resistance, and then brings it into the resistance-thickness standard curve;
所述转换公式为 公式一;The conversion formula is formula one;
其中R1为等效标准薄膜电阻,R2待测薄膜电阻,l1为标准薄膜长度,a1为标准薄膜宽度,l2为标准薄膜长度,a2为标准薄膜宽度。Among them, R1 is the equivalent standard film resistance, R2 is the film resistance to be measured, l1 is the standard film length, a1 is the standard film width, l2 is the standard film length, and a2 is the standard film width.
待测量薄膜与标准薄膜的生长工艺一致。The growth process of the film to be measured is the same as that of the standard film.
实施例1:Example 1:
本例各步骤如下:The steps in this example are as follows:
1)选取表面平整的玻璃片为衬底,用丙酮、酒精超声清洗5分钟,用氮气枪吹干后烘干;1) Select a glass sheet with a flat surface as the substrate, ultrasonically clean it with acetone and alcohol for 5 minutes, dry it with a nitrogen gun, and then dry it;
2)将第一掩膜版置于玻璃衬底上,采用磁控溅射设备,生长厚度为1.5微米厚的银电极;2) Place the first mask on the glass substrate, and use magnetron sputtering equipment to grow silver electrodes with a thickness of 1.5 microns;
3)除去第一掩膜版,采用热蒸发设备,生长不同厚度的铜薄膜;3) Remove the first mask and use thermal evaporation equipment to grow copper films of different thicknesses;
4)用激光对铜薄膜进行划片,获得规整矩形表面;4) Scribing the copper film with a laser to obtain a regular rectangular surface;
5)用台阶仪测量薄膜的厚度,用电桥测量薄膜的电阻值;5) Use the step meter to measure the thickness of the film, and use the bridge to measure the resistance value of the film;
6)对所得数据进行拟合,得到铜薄膜电阻与薄膜厚度关系的标准曲线,见附图;6) Fitting the obtained data to obtain a standard curve of the relationship between copper film resistance and film thickness, see attached figure;
7)重复步骤2)和步骤4)制备待测铜薄膜电极;7) Repeat steps 2) and 4) to prepare the copper thin film electrode to be tested;
8)用电桥法测量待测铜薄膜的电阻,带入铜薄膜电阻-厚度标准曲线得到待测铜薄膜厚度的理论值,作为对比,用椭偏仪直接测量待测铜薄膜的厚度,对比结果见附表。8) Use the bridge method to measure the resistance of the copper film to be measured, and bring in the resistance-thickness standard curve of the copper film to obtain the theoretical value of the thickness of the copper film to be measured. As a comparison, use an ellipsometer to directly measure the thickness of the copper film to be measured. The results are shown in the attached table.
实施例2:Example 2:
本例各步骤如下:The steps in this example are as follows:
1)选取抛光硅为衬底,用标准RCA液清洗,用氮气枪吹干,采用PECVD设备在衬底沉积150nm厚的氮化硅薄膜为绝缘层;1) Select polished silicon as the substrate, clean it with standard RCA liquid, dry it with a nitrogen gun, and use PECVD equipment to deposit a 150nm-thick silicon nitride film on the substrate as an insulating layer;
2)将第一掩膜版置于衬底上,采用磁控溅射设备,生长厚度为1.2微米厚的银电极;2) Place the first mask on the substrate, and use magnetron sputtering equipment to grow silver electrodes with a thickness of 1.2 microns;
3)换上第二掩膜版,采用原子层沉积设备,生长不同厚度的铝薄膜;3) Replace the second mask, and use atomic layer deposition equipment to grow aluminum films of different thicknesses;
4)用台阶仪测量薄膜的厚度,用电桥测量薄膜的电阻值;4) Use the step meter to measure the thickness of the film, and use the bridge to measure the resistance value of the film;
5)对所得数据进行拟合,得到铝薄膜电阻与薄膜厚度关系的标准曲线;5) Fit the obtained data to obtain the standard curve of the relationship between the aluminum film resistance and the film thickness;
6)重复步骤2)制备待测铝薄膜电极,用激光对铝薄膜进行划片,获得规整矩形表面;6) Repeat step 2) to prepare the aluminum film electrode to be tested, and scribe the aluminum film with a laser to obtain a regular rectangular surface;
7)用电桥法测量待测铝薄膜的电阻,带入铝薄膜电阻-厚度标准曲线得到待测铝薄膜厚度的理论值,作为对比,用椭偏仪直接测量待测铝薄膜的厚度,对比结果见附表。7) Use the bridge method to measure the resistance of the aluminum film to be tested, and bring it into the standard curve of resistance-thickness of the aluminum film to obtain the theoretical value of the thickness of the aluminum film to be tested. As a comparison, use an ellipsometer to directly measure the thickness of the aluminum film to be tested. The results are shown in the attached table.
实施例1、2的附表如下The attached tables of Examples 1 and 2 are as follows
上述实施例中,电极材质优选银。In the above embodiment, the electrode material is preferably silver.
第一掩膜版中的矩形图案即生长后的电极形状。The rectangular pattern in the first mask is the electrode shape after growth.
第二掩膜版中狭长条形图案即生长后的各个标准薄膜,各个标准薄膜具有相同的表面积但不同的厚度。The elongated strip pattern in the second mask is each standard thin film after growth, and each standard thin film has the same surface area but different thicknesses.
第一掩膜版中的矩形图案也可换为与第二掩膜版中狭长条形图案对应的多对矩形或多对圆形。The rectangular patterns in the first mask can also be replaced with pairs of rectangles or pairs of circles corresponding to the long and narrow strip patterns in the second mask.
步骤一、二、三中所用的工件为样品,用于测量以获取电阻-厚度标准曲线。The workpieces used in steps 1, 2, and 3 are samples, which are used for measurement to obtain a resistance-thickness standard curve.
Claims (9)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202011150197.9A CN112097626A (en) | 2020-10-23 | 2020-10-23 | A method for measuring the thickness of metal thin films based on resistance method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202011150197.9A CN112097626A (en) | 2020-10-23 | 2020-10-23 | A method for measuring the thickness of metal thin films based on resistance method |
Publications (1)
Publication Number | Publication Date |
---|---|
CN112097626A true CN112097626A (en) | 2020-12-18 |
Family
ID=73786025
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN202011150197.9A Pending CN112097626A (en) | 2020-10-23 | 2020-10-23 | A method for measuring the thickness of metal thin films based on resistance method |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN112097626A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113267118A (en) * | 2021-06-23 | 2021-08-17 | 东南大学 | Semiconductor conductive film thickness online test structure and test method thereof |
CN113916767A (en) * | 2021-09-30 | 2022-01-11 | 华中科技大学 | A device and method for measuring atmospheric corrosion of nano-scale metallized film |
CN115682905A (en) * | 2022-12-16 | 2023-02-03 | 广州粤芯半导体技术有限公司 | Method and device for determining thickness of thin film and computer equipment |
CN116165070A (en) * | 2023-04-21 | 2023-05-26 | 长鑫存储技术有限公司 | Method and device for detecting Young's modulus of film |
Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2003108622A (en) * | 2001-09-27 | 2003-04-11 | Nec Corp | Wiring modeling method, wiring model, wiring model extraction method, and wiring design method |
US20080268557A1 (en) * | 2007-04-24 | 2008-10-30 | Nanya Technology Corp. | Method for measuring a thin film thickness |
CN102620642A (en) * | 2012-03-29 | 2012-08-01 | 中国科学院长春应用化学研究所 | Detection method of metal nanometer film thickness |
CN106643587A (en) * | 2016-09-14 | 2017-05-10 | 西安交通大学 | Microwave transmission method-based metal film thickness measuring method |
CN107328808A (en) * | 2017-06-30 | 2017-11-07 | 西安工业大学 | Substrate and preparation and method of testing for testing semiconductive thin film Seebeck coefficient |
-
2020
- 2020-10-23 CN CN202011150197.9A patent/CN112097626A/en active Pending
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2003108622A (en) * | 2001-09-27 | 2003-04-11 | Nec Corp | Wiring modeling method, wiring model, wiring model extraction method, and wiring design method |
US20080268557A1 (en) * | 2007-04-24 | 2008-10-30 | Nanya Technology Corp. | Method for measuring a thin film thickness |
CN102620642A (en) * | 2012-03-29 | 2012-08-01 | 中国科学院长春应用化学研究所 | Detection method of metal nanometer film thickness |
CN106643587A (en) * | 2016-09-14 | 2017-05-10 | 西安交通大学 | Microwave transmission method-based metal film thickness measuring method |
CN107328808A (en) * | 2017-06-30 | 2017-11-07 | 西安工业大学 | Substrate and preparation and method of testing for testing semiconductive thin film Seebeck coefficient |
Non-Patent Citations (1)
Title |
---|
季振国等: "薄膜厚度对Au/ZnO/n~+-Si薄膜压敏电阻器阈值电压的影响", 《功能材料与器件学报》 * |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN113267118A (en) * | 2021-06-23 | 2021-08-17 | 东南大学 | Semiconductor conductive film thickness online test structure and test method thereof |
CN113916767A (en) * | 2021-09-30 | 2022-01-11 | 华中科技大学 | A device and method for measuring atmospheric corrosion of nano-scale metallized film |
CN115682905A (en) * | 2022-12-16 | 2023-02-03 | 广州粤芯半导体技术有限公司 | Method and device for determining thickness of thin film and computer equipment |
CN116165070A (en) * | 2023-04-21 | 2023-05-26 | 长鑫存储技术有限公司 | Method and device for detecting Young's modulus of film |
CN116165070B (en) * | 2023-04-21 | 2023-08-04 | 长鑫存储技术有限公司 | Method and device for detecting Young's modulus of film |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN112097626A (en) | A method for measuring the thickness of metal thin films based on resistance method | |
US20010011887A1 (en) | Micro-mechanical probes for charge sensing | |
Tam et al. | Precise measurements of a magnetostriction coefficient of a thin soft‐magnetic film deposited on a substrate | |
CN102099694A (en) | A multi-point probe for testing electrical properties and a method of producing a multi-point probe | |
JPH01262403A (en) | Probe and its manufacturing method | |
CN112113988A (en) | Electron microscope in-situ mechanical property testing chip and manufacturing method thereof | |
CN110672882B (en) | Method for detecting dielectric constant of material by using scanning probe | |
CN106441124A (en) | Novel method for measuring film thickness by time response based on laser-induced thermoelectricity voltage | |
JPH10170527A (en) | Cantilever and its manufacture | |
US6453263B1 (en) | Surface analysis using ellipsometry | |
Hasche et al. | Metrological characterization of nanometer film thickness standards for XRR and ellipsometry applications | |
CN110470441B (en) | Force-applying structure and method and application based thereon for measuring normal elastic constant of atomic force microscope probe | |
CN110470442B (en) | Normal elastic constant needle point nondestructive calibration device of atomic force microscope probe and use method | |
Láng et al. | Experimental determination of surface stress changes in electrochemical systems–possibilities and pitfalls | |
CN111609800B (en) | Method for determining value of line width standard sample based on spectrum ellipsometer | |
CN115684084A (en) | Method and system for non-destructive testing of uniformity of semiconductor thin film | |
Trujillo-Sevilla et al. | High speed roughness measurement on blank silicon wafers using wave front phase imaging | |
CN110542768A (en) | A processing method of micro-cantilever probe for ultra-low friction coefficient measurement | |
CN112992711A (en) | Method for measuring thickness of top silicon and buried oxide layer of ultra-thin SOI material | |
Mattsson | Characterization of supersmooth surfaces by light scattering techniques | |
CN104880161A (en) | Method for measuring solid material surface roughness by using elliptical polarization parameter | |
CN218481428U (en) | A subsurface multi-parameter nano standard template | |
Trujillo-Sevilla et al. | Roughness and nanotopography measurement of a Silicon Wafer using Wave Front Phase Imaging: High speed single image snapshot of entire wafer producing sub nm topography data | |
CN114674875B (en) | Method for measuring longitudinal effective piezoelectric coefficient of piezoelectric film | |
JP2008275552A (en) | Measuring method for embedment depth of metal film |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
RJ01 | Rejection of invention patent application after publication | ||
RJ01 | Rejection of invention patent application after publication |
Application publication date: 20201218 |