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CN115900996A - A method for measuring the temperature of a semiconductor device - Google Patents

A method for measuring the temperature of a semiconductor device Download PDF

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CN115900996A
CN115900996A CN202310141937.XA CN202310141937A CN115900996A CN 115900996 A CN115900996 A CN 115900996A CN 202310141937 A CN202310141937 A CN 202310141937A CN 115900996 A CN115900996 A CN 115900996A
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temperature
active surface
sensitive material
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fluorescent
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万坤
解靖飞
黄永
薛军帅
陈兴
王东
吴勇
龚子刚
艾月
韩超
李园
邵语嫣
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Wuhu Research Institute of Xidian University
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Abstract

本发明公开了一种半导体器件的温度测量方法,包括如下步骤:将荧光温敏材料与分散剂混合形成涂布溶液,并将涂布溶液涂敷于待检测器件的有源表面上;给待检测器件施加预设偏压,并获取荧光温敏材料在预设偏压下的荧光强度;根据荧光强度和荧光温敏材料的温敏荧光特性曲线得到待检测器件的有源表面温度;根据有源表面温度得到待检测器件内的空间电荷区处的温度。本发明中的方法,使用范围较广且温度检测精度较高。

Figure 202310141937

The invention discloses a method for measuring the temperature of a semiconductor device, which comprises the following steps: mixing a fluorescent temperature-sensitive material with a dispersant to form a coating solution, and coating the coating solution on an active surface of a device to be detected; The detection device applies a preset bias voltage, and obtains the fluorescence intensity of the fluorescent temperature-sensitive material under the preset bias voltage; obtains the active surface temperature of the device to be detected according to the fluorescence intensity and the temperature-sensitive fluorescence characteristic curve of the fluorescent temperature-sensitive material; The source surface temperature yields the temperature at the space charge region within the device to be inspected. The method in the invention has a wide application range and high temperature detection accuracy.

Figure 202310141937

Description

一种半导体器件的温度测量方法A method for measuring the temperature of a semiconductor device

技术领域technical field

本发明涉及半导体技术领域,尤其涉及到一种半导体器件的温度测量方法。The invention relates to the technical field of semiconductors, in particular to a method for measuring the temperature of a semiconductor device.

背景技术Background technique

随着电子产业的蓬勃发展,半导体行业对材料和器件的要求也越来越高,器件的尺寸也越来越小,这导致了器件功率密度的急剧上升,器件的自热效应明显,尤其是对于基于具有异质结(如AlGaN/GaN空间电荷区)、PN结以及金半结等空间电荷区的半导体器件,空间电荷区将会导致半导体器件内部的温度具有相对较高的升高,而器件内的温度过高将严重影响器件的电学特性,降低器件的可靠性,因此,在半导体器件应用之前,对半导体器件温度的进行测量进而对其进行性能评估非常必要。With the vigorous development of the electronics industry, the requirements of the semiconductor industry for materials and devices are getting higher and higher, and the size of the devices is getting smaller and smaller, which leads to a sharp increase in the power density of the device, and the self-heating effect of the device is obvious, especially for Based on semiconductor devices with space charge regions such as heterojunctions (such as AlGaN/GaN space charge regions), PN junctions, and gold half-junctions, the space charge region will cause a relatively high increase in the temperature inside the semiconductor device, and the device Excessive temperature inside will seriously affect the electrical characteristics of the device and reduce the reliability of the device. Therefore, before the application of the semiconductor device, it is necessary to measure the temperature of the semiconductor device and then evaluate its performance.

但是,现存的半导体器件测温方法均存在一定劣势,如,红外热成像测量适于应用在粗糙金属表面,光反射热成像测量适于应用在光滑金属化结构表面,标准拉曼测温适于应用在半导体表面(半导体器件内并不均为半导体表面,而是半导体表面、导电表面以及绝缘表面均可能具有),因而,提供一种适用范围较广且测量精度较高的半导体器件温度测量方法成为亟待解决的问题。However, the existing temperature measurement methods for semiconductor devices have certain disadvantages. For example, infrared thermal imaging measurement is suitable for rough metal surfaces, light reflection thermal imaging measurement is suitable for smooth metallized surface, and standard Raman temperature measurement is suitable for Applied on semiconductor surfaces (not all semiconductor devices have semiconductor surfaces, but semiconductor surfaces, conductive surfaces and insulating surfaces may all have), therefore, provide a method for measuring the temperature of semiconductor devices with a wide range of applications and high measurement accuracy become an urgent problem to be solved.

发明内容Contents of the invention

因此,为了解决现有技术中的上述问题,本发明提供一种可以应用于任何材料表面,并且具有较高的温度测量精度的半导体器件的温度测量方法。Therefore, in order to solve the above-mentioned problems in the prior art, the present invention provides a temperature measurement method of a semiconductor device that can be applied to any material surface and has high temperature measurement accuracy.

本发明提供的半导体器件的温度测量方法,包括如下步骤:The method for measuring the temperature of a semiconductor device provided by the invention comprises the following steps:

将荧光温敏材料与分散剂混合形成涂布溶液,并将涂布溶液涂敷于待检测器件的有源表面上;mixing the fluorescent temperature-sensitive material with a dispersant to form a coating solution, and coating the coating solution on the active surface of the device to be detected;

给待检测器件施加预设偏压,并获取荧光温敏材料在预设偏压下的荧光强度;Apply a preset bias voltage to the device to be detected, and obtain the fluorescence intensity of the fluorescent temperature-sensitive material under the preset bias voltage;

根据荧光强度和荧光温敏材料的温敏荧光特性曲线得到待检测器件的有源表面温度;According to the fluorescence intensity and the temperature-sensitive fluorescence characteristic curve of the fluorescent temperature-sensitive material, the active surface temperature of the device to be detected is obtained;

根据有源表面温度得到待检测器件内的空间电荷区处的温度。The temperature at the space charge region within the device to be inspected is derived from the active surface temperature.

在本发明的一种可能实现方式中,荧光温敏材料为稀土材料和温敏材料的复合材料。In a possible implementation manner of the present invention, the fluorescent temperature-sensitive material is a composite material of a rare earth material and a temperature-sensitive material.

在本发明的一种可能实现方式中,荧光温敏材料为Er3+和Li3Y(VO4)2的复合材料,或者为Eu3+和LuVO4的复合材料,或者为La2和MgTiO6的复合材料。In a possible implementation of the present invention, the fluorescent temperature-sensitive material is a composite material of Er 3+ and Li 3 Y(VO 4 ) 2 , or a composite material of Eu 3+ and LuVO 4 , or a composite material of La 2 and MgTiO 6 composite materials.

在本发明的一种可能实现方式中,温敏荧光特性曲线为荧光温敏材料在第一激发波长和第二激发波长下的荧光强度的比值随温度变化的曲线。In a possible implementation manner of the present invention, the temperature-sensitive fluorescence characteristic curve is a curve of the ratio of the fluorescence intensity of the fluorescent temperature-sensitive material at the first excitation wavelength to the second excitation wavelength as a function of temperature.

在本发明的一种可能实现方式中,根据有源表面温度得到待检测器件内的空间电荷区处的温度的步骤,具体包括:In a possible implementation of the present invention, the step of obtaining the temperature at the space charge region in the device to be detected according to the active surface temperature specifically includes:

获取待检测器件自空间电荷区处至有源表面的温度传导热量消耗;Obtain the heat consumption of the device to be detected from the temperature conduction from the space charge region to the active surface;

根据有源表面温度和温度传导热量消耗得到待检测器件内的空间电荷区处的温度。The temperature at the space charge region within the device to be inspected is derived from the active surface temperature and the thermal conduction heat dissipation.

在本发明的一种可能实现方式中,根据有源表面温度和温度传导热量消耗得到待检测器件内的空间电荷区处的温度的步骤中,计算公式为:In a possible implementation of the present invention, in the step of obtaining the temperature at the space charge region in the device to be detected according to the active surface temperature and the thermal conduction heat consumption, the calculation formula is:

Figure BDA0004087875430000031
Figure BDA0004087875430000031

其中,Q是指温度传导热量消耗,k是指有源表面和空间电荷区之间的结构层的导热率,A是指导热面积,T1是指空间电荷区处的温度,T2是指有源表面温度,d是指传导距离。Among them, Q refers to the temperature conduction heat consumption, k refers to the thermal conductivity of the structural layer between the active surface and the space charge region, A refers to the thermal area of the guide, T1 refers to the temperature at the space charge region, T2 refers to the active Surface temperature, d refers to the conduction distance.

在本发明的一种可能实现方式中,分散剂为挥发性试剂或者去离子水。In a possible implementation of the present invention, the dispersant is a volatile reagent or deionized water.

在本发明的一种可能实现方式中,半导体器件的温度测量方法还包括如下步骤:In a possible implementation of the present invention, the method for measuring the temperature of a semiconductor device further includes the following steps:

对待检测器件进行超声清洗,去除荧光温敏材料。Ultrasonic cleaning is performed on the device to be tested to remove fluorescent temperature-sensitive materials.

本发明提供的技术方案,具有如下优点:The technical scheme provided by the invention has the following advantages:

本发明提供的半导体器件的温度测量方法,通过将荧光强度随温度变化的荧光温敏材料与分散剂混合形成涂布溶液后,涂敷于待检测器件的有源表面(待检测器件的电极所在的表面)上,进而通过获取待检测器件被施加预设偏压后的荧光温敏材料的荧光强度,得到待检测器件的有源表面温度的方式,实现非接触式间接测温,摆脱了待检测器件表面材料类型和形貌的限制,适用范围较广、温度测量精度较高;同时,基于半导体器件内的空间电荷区是其核心自热点,因而,通过根据有源表面温度计算得到空间电荷区处的温度,能够为待检测器件的后续性能评估提供准确数据,提高了该半导体器件的温度测量方法的实用性。The method for measuring the temperature of a semiconductor device provided by the present invention is formed by mixing a fluorescent temperature-sensitive material whose fluorescence intensity changes with temperature and a dispersant to form a coating solution, and then coating it on the active surface of the device to be detected (where the electrodes of the device to be detected are located) On the surface of the device to be detected), and then obtain the active surface temperature of the device to be detected by obtaining the fluorescence intensity of the fluorescent temperature-sensitive material after the device to be detected is applied with a preset bias voltage, so as to realize non-contact indirect temperature measurement and get rid of the need to Detect the limitation of the surface material type and shape of the device, have a wide range of applications, and have high temperature measurement accuracy; at the same time, based on the space charge region in the semiconductor device is its core self-hot spot, therefore, the space charge is calculated based on the active surface temperature The temperature at the region can provide accurate data for the subsequent performance evaluation of the device to be tested, and improves the practicability of the method for measuring the temperature of the semiconductor device.

附图说明Description of drawings

为了更清楚地说明本发明具体实施方式或现有技术中的技术方案,下面将对具体实施方式或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图是本发明的一些实施方式,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得其他的附图。In order to more clearly illustrate the specific implementation of the present invention or the technical solutions in the prior art, the following will briefly introduce the accompanying drawings that need to be used in the specific implementation or description of the prior art. Obviously, the accompanying drawings in the following description The drawings show some implementations of the present invention, and those skilled in the art can obtain other drawings based on these drawings without any creative work.

图1为本发明实施例提供的一种半导体器件的温度测量方法的方法流程图;Fig. 1 is a method flowchart of a method for measuring the temperature of a semiconductor device provided by an embodiment of the present invention;

图2为本发明实施例提供的一种荧光温敏材料的温敏荧光特性曲线示意图。Fig. 2 is a schematic diagram of a temperature-sensitive fluorescence characteristic curve of a fluorescent temperature-sensitive material provided by an embodiment of the present invention.

具体实施方式Detailed ways

下面将结合附图对本发明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得的所有其他实施例,都属于本发明保护的范围。The technical solutions of the present invention will be clearly and completely described below in conjunction with the accompanying drawings. Apparently, the described embodiments are some of the embodiments of the present invention, but not all of them. 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.

在本发明的描述中,需要说明的是,术语“上”、“下”等指示的方位或位置关系为基于附图所示的方位或位置关系,仅是为了便于描述本发明和简化描述,而不是指示或暗示所指的装置或元件必须具有特定的方位、以特定的方位构造和操作,因此不能理解为对本发明的限制。此外,术语“第一”、“第二”、“第三”仅用于描述目的,而不能理解为指示或暗示相对重要性。In the description of the present invention, it should be noted that the orientation or positional relationship indicated by the terms "upper", "lower", etc. is based on the orientation or positional relationship shown in the drawings, and is only for the convenience of describing the present invention and simplifying the description. It is not intended to indicate or imply that the referred device or element must have a particular orientation, be constructed in a particular orientation, and operate in a particular orientation, and thus should not be construed as limiting the invention. In addition, the terms "first", "second", and "third" are used for descriptive purposes only, and should not be construed as indicating or implying relative importance.

图1为本实施例提供的一种半导体器件的温度测量方法的流程图,如图1所示,该方法包括如下步骤:Fig. 1 is a flow chart of a method for measuring the temperature of a semiconductor device provided in this embodiment, as shown in Fig. 1, the method includes the following steps:

S100:将荧光温敏材料与分散剂混合形成涂布溶液,并将涂布溶液涂敷于待检测器件的有源表面上。S100: Mix the fluorescent temperature-sensitive material and the dispersant to form a coating solution, and apply the coating solution on the active surface of the device to be detected.

本实施例中,荧光温敏材料是指(同一激发波长下)荧光强度随温度变化而变化的材料,具体地,荧光温敏材料可以为稀土材料和温敏材料的复合材料,如,Er3+和Li3Y(VO4)2的复合材料,或者为Eu3+和LuVO4的复合材料,或者为La2和MgTiO6的复合材料,等。In this embodiment, the fluorescent temperature-sensitive material refers to a material whose fluorescence intensity changes with temperature (under the same excitation wavelength). Specifically, the fluorescent temperature-sensitive material can be a composite material of a rare earth material and a temperature-sensitive material, such as Er 3 + and Li 3 Y(VO 4 ) 2 composite materials, or Eu 3+ and LuVO 4 composite materials, or La 2 and MgTiO 6 composite materials, etc.

本实施例中,荧光温敏材料与分散剂混合形成的涂布溶液为悬浊液即可,且为了减小分散剂对待检测器件表面和荧光温敏材料的影响,可以设置分散剂为无水乙醇、无水异丙醇等挥发性试剂,或者去离子水,且当分散剂为挥发性试剂时,下述步骤S200为在分散剂挥发后执行。In this embodiment, the coating solution formed by mixing the fluorescent temperature-sensitive material and the dispersant can be a suspension. Volatile reagents such as ethanol, anhydrous isopropanol, or deionized water, and when the dispersant is a volatile reagent, the following step S200 is performed after the dispersant volatilizes.

具体实施方式中,可以使用混匀仪混合荧光温敏材料和分散剂。In a specific embodiment, a mixer can be used to mix the fluorescent temperature-sensitive material and the dispersant.

本实施例中,有源表面是指待检测器件的电极所在的表面,且基于下述步骤S200中需要给待检测器件施加预设偏压,因而,此步骤中的涂布溶液涂敷于有源表面上的电极以外的区域。In this embodiment, the active surface refers to the surface where the electrodes of the device to be detected are located, and based on the need to apply a preset bias voltage to the device to be detected in the following step S200, the coating solution in this step is applied to the active surface. Areas other than electrodes on the source surface.

S200:给待检测器件施加预设偏压,并获取荧光温敏材料在预设偏压下的荧光强度。S200: Apply a preset bias voltage to the device to be detected, and obtain the fluorescence intensity of the fluorescent temperature-sensitive material under the preset bias voltage.

本实施例中,预设偏压可以为一个也可以为多个,其具体数量和数值为根据待检测器件在具体应用场景中的工作电压进行设置,在此不做限制。In this embodiment, there can be one or more preset bias voltages, the specific number and value of which are set according to the operating voltage of the device to be tested in a specific application scenario, and are not limited here.

具体实施时,可以先在显微光致发光光谱仪下进行探针台、电压电流源的搭建,然后将附有荧光温敏材料的待检测器件置于显微光致发光光谱仪的显微镜物镜下,并对焦成功后,将探针接触到待检测器件的电极上,通过电压电流源给器件施加预设偏压,进而获取荧光温敏材料的荧光强度。同时,此步骤中,可以使用一个激发波长激发荧光,对应得到一个荧光强度,也可以使用两个激发波长激发荧光,对应得到两个荧光强度。During specific implementation, the probe station and the voltage and current source can be built under the microphotoluminescence spectrometer first, and then the device to be detected with the fluorescent temperature-sensitive material is placed under the microscope objective of the microphotoluminescence spectrometer, After focusing successfully, touch the probe to the electrode of the device to be detected, apply a preset bias voltage to the device through a voltage and current source, and then obtain the fluorescence intensity of the fluorescent temperature-sensitive material. At the same time, in this step, one excitation wavelength can be used to excite fluorescence to obtain one fluorescence intensity, or two excitation wavelengths can be used to excite fluorescence to obtain two fluorescence intensities.

S300:根据荧光强度和荧光温敏材料的温敏荧光特性曲线得到待检测器件的有源表面温度。S300: Obtain the active surface temperature of the device to be detected according to the fluorescence intensity and the temperature-sensitive fluorescence characteristic curve of the fluorescent temperature-sensitive material.

本实施例中,荧光温敏材料的温敏荧光特性曲线可以为一个激发波长下,荧光温敏材料的荧光强度随温度变化的曲线,也可以为两个激发波长下,荧光温敏材料在第一激发波长和第二激发波长下的荧光强度的比值随温度变化的曲线(此时,此步骤中具体的也为根据荧光强度比值和荧光温敏材料的温敏荧光特性曲线得到待检测器件的有源表面温度)。以荧光温敏材料为Er3+和Li3Y(VO4)2的复合材料为例,第一激发波长可以为552nm,第二激发波长可以为524nm,此时,荧光温敏材料的温敏荧光特性曲线如图2所示。In this embodiment, the temperature-sensitive fluorescent characteristic curve of the fluorescent temperature-sensitive material can be a curve of the fluorescence intensity of the fluorescent temperature-sensitive material changing with temperature at one excitation wavelength, or it can be a curve of the fluorescent temperature-sensitive material at the second excitation wavelength at two excitation wavelengths. The curve of the ratio of the fluorescence intensity at the first excitation wavelength and the second excitation wavelength as a function of temperature (at this time, in this step, the specific method is also to obtain the temperature-sensitive fluorescence characteristic curve of the device to be detected according to the fluorescence intensity ratio and the temperature-sensitive fluorescence characteristic curve of the fluorescent temperature-sensitive material. active surface temperature). Taking the composite material of Er 3+ and Li 3 Y(VO 4 ) 2 as the fluorescent temperature-sensitive material as an example, the first excitation wavelength can be 552nm, and the second excitation wavelength can be 524nm. At this time, the temperature sensitivity of the fluorescent temperature-sensitive material The fluorescence characteristic curve is shown in Fig. 2 .

S400:根据有源表面温度得到待检测器件内的空间电荷区处的温度。S400: Obtain the temperature at the space charge region in the device to be detected according to the active surface temperature.

本实施例中,空间电荷区可以为PN结、异质结或者金半结等。In this embodiment, the space charge region may be a PN junction, a heterojunction, or a gold half junction.

综上,本实施例提供的半导体器件的温度测量方法,通过将荧光强度随温度变化的荧光温敏材料与分散剂混合形成涂布溶液后,涂敷于待检测器件的有源表面(待检测器件的电极所在的表面)上,进而通过获取待检测器件被施加预设偏压后的荧光温敏材料的荧光强度,得到待检测器件的有源表面温度的方式,实现非接触式间接测温,摆脱了待检测器件表面材料类型和形貌的限制,适用范围较广、温度测量精度较高;同时,基于半导体器件内的空间电荷区是其核心自热点,因而,通过根据有源表面温度计算得到空间电荷区处的温度,能够为待检测器件的后续性能评估提供准确数据,提高了该半导体器件的温度测量方法的实用性。To sum up, the method for measuring the temperature of a semiconductor device provided in this embodiment is to mix a fluorescent temperature-sensitive material whose fluorescence intensity changes with temperature with a dispersant to form a coating solution, and then apply it to the active surface of the device to be detected (to be detected) The surface where the electrode of the device is located), and then obtain the active surface temperature of the device to be detected by obtaining the fluorescence intensity of the fluorescent temperature-sensitive material after the device to be detected is applied with a preset bias voltage, so as to realize non-contact indirect temperature measurement , get rid of the limitations of the surface material type and shape of the device to be detected, and have a wide range of applications and high temperature measurement accuracy; at the same time, based on the space charge region in the semiconductor device is its core self-hot spot, therefore, according to the active surface temperature The calculated temperature at the space charge region can provide accurate data for the subsequent performance evaluation of the device to be detected, and improves the practicability of the method for measuring the temperature of the semiconductor device.

在本实施例的一种可能的具体实施方式中,步骤S400具体可以包括如下步骤:In a possible specific implementation manner of this embodiment, step S400 may specifically include the following steps:

S401:获取待检测器件自空间电荷区处至有源表面的温度传导热量消耗。S401: Obtain the heat consumption of the device to be detected by temperature conduction from the space charge region to the active surface.

具体地,此步骤中的温度传导热量消耗可以为对待检测器件进行仿真搭建后测量得到。Specifically, the temperature conduction heat consumption in this step can be measured after the device to be tested is simulated and built.

S402:根据有源表面温度和温度传导热量消耗得到待检测器件内的空间电荷区处的温度。S402: Obtain the temperature at the space charge region in the device to be detected according to the active surface temperature and the heat consumption by temperature conduction.

具体地,可以根据以下公式计算得到待检测器件内的空间电荷区处的温度:Specifically, the temperature at the space charge region in the device to be detected can be calculated according to the following formula:

Figure BDA0004087875430000071
Figure BDA0004087875430000071

其中,Q是指温度传导热量消耗,k是指有源表面和空间电荷区之间的结构层的导热率,A是指导热面积,T1是指空间电荷区处的温度,T2是指有源表面温度,d是指传导距离。Among them, Q refers to the temperature conduction heat consumption, k refers to the thermal conductivity of the structural layer between the active surface and the space charge region, A refers to the thermal area of the guide, T1 refers to the temperature at the space charge region, T2 refers to the active Surface temperature, d refers to the conduction distance.

在本实施例的另一种可能的具体实施方式中,为了进一步减小半导体器件的温度测量方法对待检测器件的影响,最终还原待检测器件的形貌,在具有上述步骤S100~步骤S400的基础上,如图1所示,该方法还可以包括下述步骤:In another possible specific implementation of this embodiment, in order to further reduce the influence of the semiconductor device temperature measurement method on the device to be detected, and finally restore the shape of the device to be detected, based on the above steps S100 to S400 On, as shown in Figure 1, the method may also include the following steps:

S500:对待检测器件进行超声清洗,去除荧光温敏材料。S500: Ultrasonic cleaning is performed on the device to be tested to remove fluorescent temperature-sensitive materials.

显然,上述实施例仅仅是为清楚地说明所作的举例,而并非对实施方式的限定。对于所属领域的普通技术人员来说,在上述说明的基础上还可以做出其它不同形式的变化或变动。这里无需也无法对所有的实施方式予以穷举。而由此所引伸出的显而易见的变化或变动仍处于本发明的保护范围之中。Apparently, the above-mentioned embodiments are only examples for clear description, rather than limiting the implementation. For those of ordinary skill in the art, other changes or changes in different forms can be made on the basis of the above description. It is not necessary and impossible to exhaustively list all the implementation manners here. However, the obvious changes or changes derived therefrom still fall within the scope of protection of the present invention.

Claims (8)

1. A method of measuring temperature of a semiconductor device, comprising the steps of:
mixing a fluorescent temperature-sensitive material with a dispersant to form a coating solution, and coating the coating solution on the active surface of a device to be detected;
applying a preset bias voltage to the device to be detected, and acquiring the fluorescence intensity of the fluorescent temperature-sensitive material under the preset bias voltage;
obtaining the active surface temperature of the device to be detected according to the fluorescence intensity and the temperature-sensitive fluorescence characteristic curve of the fluorescent temperature-sensitive material;
and obtaining the temperature of the space charge region in the device to be detected according to the active surface temperature.
2. The method for measuring the temperature of a semiconductor device according to claim 1, wherein the fluorescent temperature-sensitive material is a composite material of a rare earth material and a temperature-sensitive material.
3. The method for measuring the temperature of a semiconductor device according to claim 2, wherein the fluorescent temperature-sensitive material is Er 3+ And Li 3 Y(VO 4 ) 2 Or Eu, or 3+ And LuVO 4 Or La 2 And MgTiO 6 The composite material of (1).
4. The method for measuring temperature of a semiconductor device according to claim 1, wherein the temperature-sensitive fluorescence characteristic curve is a curve in which a ratio of fluorescence intensities of the fluorescent temperature-sensitive material at the first excitation wavelength and the second excitation wavelength changes with temperature.
5. The method according to claim 1, wherein the step of obtaining the temperature of the space charge region in the device to be tested according to the active surface temperature specifically comprises:
acquiring the temperature conduction heat consumption of the device to be detected from the space charge region to the active surface;
and obtaining the temperature of the space charge area in the device to be detected according to the active surface temperature and the temperature conduction heat consumption.
6. The method according to claim 5, wherein in the step of obtaining the temperature at the space charge region in the device to be detected based on the active surface temperature and the temperature conduction heat consumption, the calculation formula is:
Figure FDA0004087875410000021
wherein Q refers to the temperature conduction heat consumption, k refers to the thermal conductivity of the structural layer between the active surface and the space charge region, a refers to the thermal conduction area, T1 refers to the temperature at the space charge region, T2 refers to the active surface temperature, and d refers to the conduction distance.
7. The method according to claim 1, wherein the dispersant is a volatile agent or deionized water.
8. The method for measuring the temperature of the semiconductor device according to claim 7, further comprising the steps of:
and carrying out ultrasonic cleaning on the device to be detected, and removing the fluorescent temperature-sensitive material.
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Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001004460A (en) * 1999-06-25 2001-01-12 Osaka Gas Co Ltd Method and apparatus for measuring temperature and temperature-sensitive coating
JP2001272277A (en) * 2000-03-27 2001-10-05 Osaka Gas Co Ltd Method for measuring surface temperature of object
CN104634466A (en) * 2013-11-14 2015-05-20 北京华峰测控技术有限公司 Junction temperature simulation circuit for semiconductor power devices
CN105241575A (en) * 2015-09-10 2016-01-13 南昌航空大学 Intensity ratio temperature measurement method based on broadband fluorescence spectrum
CN111238661A (en) * 2020-03-17 2020-06-05 北京科易达知识产权服务有限公司 Non-contact temperature measuring method and device based on fluorescent afterglow
CN114213878A (en) * 2021-11-26 2022-03-22 西安交通大学 Temperature indicating coating based on fluorescence temperature-sensitive characteristic and preparation method thereof

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2001004460A (en) * 1999-06-25 2001-01-12 Osaka Gas Co Ltd Method and apparatus for measuring temperature and temperature-sensitive coating
JP2001272277A (en) * 2000-03-27 2001-10-05 Osaka Gas Co Ltd Method for measuring surface temperature of object
CN104634466A (en) * 2013-11-14 2015-05-20 北京华峰测控技术有限公司 Junction temperature simulation circuit for semiconductor power devices
CN105241575A (en) * 2015-09-10 2016-01-13 南昌航空大学 Intensity ratio temperature measurement method based on broadband fluorescence spectrum
CN111238661A (en) * 2020-03-17 2020-06-05 北京科易达知识产权服务有限公司 Non-contact temperature measuring method and device based on fluorescent afterglow
CN114213878A (en) * 2021-11-26 2022-03-22 西安交通大学 Temperature indicating coating based on fluorescence temperature-sensitive characteristic and preparation method thereof

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
光电器件: "基于倒装焊芯片的功率型LED热特性分析", 光电器件, vol. 33, no. 3, 30 June 2012 (2012-06-30), pages 321 *

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