CN116298750A - A method for non-destructive characterization of semiconductor device microstructure damage - Google Patents

A method for non-destructive characterization of semiconductor device microstructure damage Download PDF

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CN116298750A
CN116298750A CN202310163377.8A CN202310163377A CN116298750A CN 116298750 A CN116298750 A CN 116298750A CN 202310163377 A CN202310163377 A CN 202310163377A CN 116298750 A CN116298750 A CN 116298750A
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张亚民
温茜
孟宪伟
冯士维
彭飞
杨洁
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Abstract

The invention discloses a nondestructive characterization method for damage of a micro-region structure of a semiconductor device, which is characterized in that a certain electrical bias condition is applied to the device to be tested, transient curves of leakage current changing along with time before and after the stress action of the device to be tested are respectively collected by a testing instrument, the time constant of the damage position of the device is extracted from the transient curves by using a Bayesian iterative time constant extraction method, the time constant of the damage position of the device is presented in a peak spectrum form by combining a peak spectrum time constant extraction technology, and the spectrum valued characterization is carried out by using an amplitude spectrum technology on the basis, so that the evolution process of the damage of the invisible micro-region structure in the device under the stress action is converted into visual spectral line movement, and the accurate positioning, damage degree and spectral valued quantitative characterization of the evolution process of the damage of the micro-region structure of the device are realized.

Description

一种半导体器件微区结构损伤无损表征的方法A method for non-destructive characterization of semiconductor device microstructure damage

技术领域technical field

本发明涉及半导体器件测试表征领域,主要应用于半导体器件微区结构损伤无损表征。The invention relates to the field of testing and characterization of semiconductor devices, and is mainly applied to the non-destructive characterization of semiconductor device micro-region structure damage.

背景技术Background technique

宽禁带半导体器件,具有高击穿电压、高输出功率和高可靠性等优良特性,在高频大功率领域显示出优异的性能。然而受器件异质结构和材料生长条件的影响,器件在高温、动态强场、电应力作用下,器件有源区极易诱发陷阱,然而陷阱问题的存在限制了其性能的进一步提高和广泛应用,因此了解器件微区结构损伤位置、损伤程度、损伤演化过程及规律,是有效分析微区结构损伤机理和进行器件可靠设计的前提,亟需开展半导体器件微区结构损伤无损表征技术研究,实现半导体器件微区结构损伤的非破坏性测量、精准定位和演化过程量化表征。Wide bandgap semiconductor devices have excellent characteristics such as high breakdown voltage, high output power and high reliability, and show excellent performance in the field of high frequency and high power. However, affected by the heterogeneous structure of the device and the growth conditions of the material, the active region of the device is very easy to induce traps under the action of high temperature, dynamic strong field, and electrical stress. However, the existence of traps limits the further improvement of its performance and its wide application. Therefore, understanding the damage location, damage degree, damage evolution process and law of the device microstructure is the prerequisite for effective analysis of the microstructure damage mechanism and reliable design of the device. Non-destructive measurement, precise location and quantitative characterization of the evolution process of semiconductor device microstructure damage.

发明内容Contents of the invention

本发明的技术目的在于,基于漏极瞬态电流变化与半导体器件微区结构损伤之间的关系,提出了一种半导体器件微区结构损伤无损表征方法,该方法贝叶斯迭代反卷积的时间常数提取技术,分析时间常数和峰值谱变化,实现半导体器件微区结构损伤无损表征、精准定位和演化过程量化表征。The technical purpose of the present invention is to propose a non-destructive characterization method for semiconductor device microstructure damage based on the relationship between drain transient current changes and semiconductor device microstructure damage. The Bayesian iterative deconvolution of the method Time constant extraction technology, analysis of time constant and peak spectrum changes, to achieve non-destructive characterization of semiconductor device microstructure damage, precise positioning and quantitative characterization of evolution process.

半导体器件损伤带来的缺陷捕获和释放电子过程直接影响其电流变化。漏-源电极之间电流瞬态变化与器件微区损伤之间存在映射关系。基于该映射关系,通过采集器件损伤前后的漏极电流瞬态变化曲线,利用贝叶斯迭代反卷积时间常数提取方法电流瞬态曲线时间常数提取,并在此基础上通过对时间常数谱进行积分,获取不同位置发生损伤对漏极电流变化的贡献,并以谱线的形式表现出来。通过分析损伤前后漏极瞬态曲线,将器件内部不可见的微区结构损伤的演化过程转变为可视化的谱线移动,实现器件微区结构损伤的精准定位、损伤程度和演化过程的谱值化量化表征。The defect capture and release electron process caused by the damage of semiconductor device directly affects its current change. There is a mapping relationship between the transient change of the current between the drain and the source electrode and the damage of the micro-region of the device. Based on the mapping relationship, by collecting the transient change curve of the drain current before and after the device damage, the time constant of the current transient curve is extracted by using the Bayesian iterative deconvolution time constant extraction method, and on this basis, the time constant spectrum is extracted Integrate to obtain the contribution of damage at different positions to the change of drain current, and express it in the form of spectral lines. By analyzing the drain transient curve before and after the damage, the evolution process of the invisible microstructure damage inside the device is transformed into a visualized spectral line movement, and the precise positioning of the device microstructure damage, the damage degree and the spectral value of the evolution process are realized Quantitative representation.

本发明采用的技术方案为一种半导体器件微区结构损伤无损表征的方法,可将应力作用对器件的损伤程度与器件损伤前进行对比,精准表征器件损伤程度及损伤位置的变化情况。The technical solution adopted in the present invention is a method for non-destructive characterization of semiconductor device microstructure damage, which can compare the degree of damage to the device by stress with that before the device is damaged, and accurately characterize the change of the degree of device damage and the location of the damage.

S1搭建一瞬态电流测试系统,如图2所示,采集应力(高温、高压等)作用前后器件漏电流的瞬态变化曲线。电流测试系统的精度可达毫秒量级,测量瞬态电流响应中需要在测量过程前对器件损伤部位先施加一个陷阱填充阶段,在填充阶段施加较大的电应力,使器件损伤部位即陷阱被充分填充,然后迅速切换至小的测量偏置下(测量阶段),监控电子从陷阱中释放的过程,即可采集到漏电流IDS随时间的变化曲线。选择一被测器件,将被测器件放置温度为T0的恒温平台,对器件施加上述说明中的电学偏置条件,以采集漏电流IDS随时间的变化曲线。S1 builds a transient current test system, as shown in Figure 2, to collect the transient change curves of device leakage current before and after stress (high temperature, high voltage, etc.). The accuracy of the current test system can reach the order of milliseconds. In the measurement of the transient current response, it is necessary to apply a trap filling stage to the damaged part of the device before the measurement process. In the filling stage, a large electrical stress is applied to make the damaged part of the device, that is, the trap Fully fill, then quickly switch to a small measurement bias (measurement phase), monitor the process of releasing electrons from the trap, and then collect the curve of leakage current I DS versus time. Select a device under test, place the device under test on a constant temperature platform with a temperature of T0, and apply the electrical bias conditions in the above description to the device to collect the change curve of the leakage current I DS with time.

S2在采集到瞬态漏极电流响应后,为了提取到器件损伤位置(陷阱)的核心信息,对瞬态漏极电流响应曲线进一步处理,得到陷阱的时间常数谱,基于贝叶斯反卷积的时间常数提取方法经过多次迭代计算可将曲线幅值变化较平缓区域即峰值被强信号的峰值湮没而难以识别的区域或高度重叠峰值区域等极其不易分辨区域精准区分开,并且能有效地凸显出器件损伤位置(陷阱)的时间常数峰值。S2 After collecting the transient drain current response, in order to extract the core information of the device damage position (trap), the transient drain current response curve is further processed to obtain the time constant spectrum of the trap, based on Bayesian deconvolution The time constant extraction method can accurately distinguish the area where the curve amplitude changes more gently, that is, the area where the peak value is annihilated by the peak value of the strong signal and is difficult to identify, or the area with highly overlapping peaks, which is extremely difficult to distinguish after multiple iterative calculations, and can effectively Highlights time constant peaks at device damage sites (traps).

陷阱信息以e指数变化形式存在于瞬态电流响应中,如式(1)所示The trap information exists in the transient current response in the form of e exponential change, as shown in formula (1)

Figure BDA0004094979000000031
Figure BDA0004094979000000031

τi为第i个陷阱的时间常数,ΔIi为其影响电流变化的幅值。时间常数谱主要用来提取陷阱的特征时间常数τi,并以峰值谱的形式展示出来,其峰值的横坐标即为陷阱时间常数。τ i is the time constant of the i-th trap, and ΔI i is the magnitude of its influence on the current change. The time constant spectrum is mainly used to extract the characteristic time constant τ i of the trap, and display it in the form of peak spectrum, and the abscissa of the peak value is the trap time constant.

首先,引入对数时间变量:First, introduce the logarithmic time variable:

z=lnt (2)z=lnt (2)

然后,陷阱的时间常数谱如下式:Then, the time constant spectrum of the trap is as follows:

Figure BDA0004094979000000032
Figure BDA0004094979000000032

ΔI(z)即为时间常数谱,则瞬态电流Ids(t)被描述为:ΔI(z) is the time constant spectrum, then the transient current I ds (t) is described as:

Figure BDA0004094979000000033
Figure BDA0004094979000000033

与式(1)相比较,(4)是沟道瞬态电流的积分形式。结合式(2),瞬态电流被转换为:Compared with formula (1), (4) is the integral form of channel transient current. Combined with equation (2), the transient current is converted to:

Figure BDA0004094979000000034
Figure BDA0004094979000000034

这是ΔI(τ)的卷积型积分方程。在式(3.5)的两侧对z进行微分的结果为:This is a convolution type integral equation of ΔI(τ). The result of differentiating z on both sides of equation (3.5) is:

Figure BDA0004094979000000035
Figure BDA0004094979000000035

定义函数W(z)如下:Define the function W(z) as follows:

W(z)=exp(z-exp(z)) (7)W(z)=exp(z-exp(z)) (7)

Figure BDA0004094979000000036
的表达式为:but
Figure BDA0004094979000000036
The expression is:

Figure BDA0004094979000000037
Figure BDA0004094979000000037

Figure BDA0004094979000000038
为卷积运算符,则时间常数谱ΔI(z)为:
Figure BDA0004094979000000038
is a convolution operator, then the time constant spectrum ΔI(z) is:

Figure BDA0004094979000000041
Figure BDA0004094979000000041

至此,时间常数谱可以由贝叶斯反卷积求解得到。所有的器件损伤位置(陷阱)时间常数以峰值谱的形式呈现出来,峰值谱包络线围成的面积与漏源电流的变化量相对应,时间常数谱峰值对应横坐标为器件损伤位置(陷阱)的时间常数,纵坐标为器件损伤位置(陷阱)引起漏源电流的相对变化量。So far, the time constant spectrum can be solved by Bayesian deconvolution. The time constants of all device damage locations (trap) are presented in the form of peak spectrum. The area enclosed by the peak spectrum envelope corresponds to the variation of the drain-source current, and the abscissa corresponding to the peak value of the time constant spectrum is the device damage location (trap). ), the ordinate is the relative change in the drain-source current caused by the device damage location (trap).

S3根据峰值和漏极电流总的变化量,累加时间常数谱的y值,使每个时间点对应的y值等于前面所有时间点(包括该时间点)y值的累加值,即令

Figure BDA0004094979000000042
再将x轴数值与y轴数值互换得到积分幅值谱。S3 accumulates the y value of the time constant spectrum according to the total variation of the peak value and the drain current, so that the y value corresponding to each time point is equal to the cumulative value of the y value of all previous time points (including this time point), that is,
Figure BDA0004094979000000042
Then exchange the x-axis value with the y-axis value to obtain the integral amplitude spectrum.

S4对积分幅值谱一阶求导得到微分幅值谱。微分幅值谱中峰值之间的差值即为陷阱的绝对作用强度,即全部作用强度之和等于总的瞬态电流响应的变化。可以更直观精确的表征器件微区结构损伤的位置及损伤程度。此外,微分幅值谱的峰值纵坐标代表着该类型陷阱的“独立程度”,即这类陷阱的时间常数与其他陷阱的远近。S4 calculates the first-order derivative of the integrated amplitude spectrum to obtain the differential amplitude spectrum. The difference between the peaks in the differential amplitude spectrum is the absolute action strength of the trap, that is, the sum of all action strengths is equal to the change in the total transient current response. It can more intuitively and accurately characterize the damage location and damage degree of the device microstructure. In addition, the peak ordinate of the differential amplitude spectrum represents the "degree of independence" of this type of trap, that is, how close the time constant of this type of trap is to other traps.

全部表征过程如图1所示,表征过程包括:瞬态漏极电流采集与修正、时间常数提取、峰值谱表征、幅值谱表征。The entire characterization process is shown in Figure 1. The characterization process includes: transient drain current acquisition and correction, time constant extraction, peak spectrum characterization, and amplitude spectrum characterization.

附图说明Description of drawings

图1器件微区结构损伤表征过程示意图。Fig. 1 Schematic diagram of the device microstructure damage characterization process.

图2器件瞬态电流测试系统。Figure 2 Device transient current test system.

图3瞬态漏电流测量系统硬件架构和电学偏置时序图。Figure 3 The hardware architecture and electrical bias timing diagram of the transient leakage current measurement system.

图4应力引起器件微区结构损伤的谱值化表征方法示意图。Fig. 4 Schematic diagram of spectral value characterization method for stress-induced device microstructure damage.

具体实施方式Detailed ways

以下结合附图和实施例对本发明进行详细说明。The present invention will be described in detail below in conjunction with the accompanying drawings and embodiments.

以GaN HEMT为例,将器件放置在温度为T0的恒温平台,采集漏电流IDS随时间的变化曲线。器件损伤位置(陷阱)释放电子(detrapping)过程漏电流瞬态响应表征:填充阶段,在漏极接入直流电压,电压为V0,源极接地,栅极接反向偏电压V1,填充时间为T1;测量阶段,对填充完的被测器件立即施加一个小的激励信号,即栅极电压为0V,源极接入小电压V2,使器件填充阶段俘获的电子能够被充分释放,测试时间为T2。由于示例中所使用的GaNHEMT为耗尽型器件,若栅极漏极皆处于正偏状态,漏电流超过允许的最大沟道电流时器件极易损坏。因此需要单独的两路时序脉冲分别控制栅极和漏极的工作状态。GaN HEMT瞬态漏电流测量系统硬件架构和电学偏置时序图如图3所示。将这一器件施加一定应力(如电应力、高温应力等)条件后,将应力作用后的器件放置温度为T0的恒温平台,施加与应力作用前相同的电学偏置条件,再次测试器件漏电流随时间变化的瞬态曲线,应力作用前后漏电流随时间变化的瞬态曲线如图4(a)所示。Taking GaN HEMT as an example, the device is placed on a constant temperature platform with a temperature of T0, and the curve of the leakage current IDS changing with time is collected. Leakage current transient response characterization during device damage (trap) release of electrons (detrapping): In the filling stage, a DC voltage is connected to the drain, the voltage is V0, the source is grounded, the gate is connected to the reverse bias voltage V1, and the filling time is T1; In the measurement stage, a small excitation signal is immediately applied to the filled device under test, that is, the gate voltage is 0V, and the source is connected to a small voltage V2, so that the electrons captured in the device filling stage can be fully released, and the test time is T2. Since the GaNHEMT used in the example is a depletion-type device, if the gate and drain are both in a forward-biased state, the device will be easily damaged when the leakage current exceeds the maximum allowable channel current. Therefore, two separate timing pulses are required to control the working states of the gate and the drain respectively. The hardware architecture and electrical bias timing diagram of the GaN HEMT transient leakage current measurement system are shown in Figure 3. After applying a certain stress (such as electrical stress, high temperature stress, etc.) to this device, place the stress-applied device on a constant temperature platform with a temperature of T0, apply the same electrical bias conditions as before the stress, and test the leakage current of the device again The transient curve changing with time, the transient curve of leakage current changing with time before and after the stress is shown in Fig. 4(a).

在采集到被测器件损伤前后瞬态漏极电流响应后,对瞬态漏极电流响应曲线进一步处理得到时间常数谱,基于贝叶斯反卷积的时间常数提取方法从时间常数谱中提取器件陷阱位置的时间常数和相对峰值并以峰值谱的形式呈现出来。峰值谱包络线围成的面积与漏源电流的变化量相对应,如图4(b)所示,存在3处时间常数峰值谱,即DP1、DP2和DP3,根据峰值和漏极电流总的变化量,我们可以大致估算对比出器件应力作用前后即损伤前后器件DP1的位置和损伤程度并无变化,DP2的峰值位置从6s左右移动到3s左右损伤程度明显增大,DP3的峰值位置从360s左右移动到240s左右,损伤程度也明显增大。After collecting the transient drain current response before and after the damage of the device under test, the transient drain current response curve is further processed to obtain the time constant spectrum, and the time constant extraction method based on Bayesian deconvolution extracts the device from the time constant spectrum The time constants and relative peaks of the trap locations are presented as a peak spectrum. The area enclosed by the peak spectrum envelope corresponds to the variation of the drain-source current, as shown in Figure 4(b), there are three time constant peak spectra, namely DP1, DP2 and DP3, according to the total peak and drain current We can roughly estimate and compare the position and damage degree of the device DP1 before and after the stress of the device, that is, before and after the damage. The peak position of DP2 moves from about 6s to about 3s. From around 360s to around 240s, the degree of damage also increased significantly.

由于峰值谱表征不能直观定量观察到器件损伤程度的量化表征,因此在此基础上可以利用幅值谱技术实现器件损伤的谱值化表征,采用基于贝叶斯反卷积的提取方法提取得到时间常数谱,累加时间常数谱的y值,使每个时间点对应的y值等于前面所有时间点(包括该时间点)y值的累加值,即令

Figure BDA0004094979000000061
再将x轴数值与y轴数值互换得到积分幅值谱,可以直观定量分析应力作用前后器件3处损伤位置漏电的变化量,如图4(c)所示。Since the peak spectrum characterization cannot directly and quantitatively observe the quantitative characterization of the damage degree of the device, on this basis, the amplitude spectrum technology can be used to realize the spectral value characterization of the device damage, and the extraction method based on Bayesian deconvolution is used to extract the time Constant spectrum, accumulating the y value of the time constant spectrum, so that the y value corresponding to each time point is equal to the cumulative value of the y value of all previous time points (including this time point), that is,
Figure BDA0004094979000000061
Then exchange the x-axis value with the y-axis value to obtain the integrated amplitude spectrum, which can intuitively and quantitatively analyze the change of leakage at the three damaged positions of the device before and after stress, as shown in Figure 4(c).

对积分幅值谱一阶求导得到微分幅值谱。此方法可以更准确直观的表征应力损伤前后3处器件损伤引起的漏极电流变化量以及器件损伤程度和损伤位置的演化过程,如图4(d)所示。The differential amplitude spectrum is obtained by first deriving the integral amplitude spectrum. This method can more accurately and intuitively characterize the drain current variation caused by the three device damages before and after the stress damage, as well as the evolution process of the device damage degree and damage location, as shown in Figure 4(d).

本发明中,通过实时采集漏极电流的变化,对瞬态漏极电流响应曲线进一步处理,基于贝叶斯反卷积的时间常数提取方法实现了陷阱时间常数谱的准确获取,并在此基础上实现了利用幅值谱技术实现器件微区损伤的谱值化表征。基于上述表征过程,对器件施加不同应力类型,例如高温、强场等等,分别在施加应力前(损伤前)和应力施加一段时间后(损伤后)提取峰值谱和幅值谱,可将器件内部不可见的微区结构损伤的演化过程转变为直观定性可视化的谱线移动,通过对比分析应力施加前后峰值谱线和幅值谱的移动,获取应力类型、施加强度、持续时间等对器件微区结构损伤位置及损伤程度的影响,如图4所示。In the present invention, by collecting the change of the drain current in real time, the transient drain current response curve is further processed, and the time constant extraction method based on Bayesian deconvolution realizes the accurate acquisition of the trap time constant spectrum, and based on this The spectral value characterization of device micro-area damage is realized by using the amplitude spectrum technology. Based on the above characterization process, different stress types are applied to the device, such as high temperature, strong field, etc., and the peak spectrum and amplitude spectrum are extracted respectively before the stress is applied (before damage) and after a period of stress (after damage), and the device can be The evolution process of internal invisible microstructure damage is transformed into intuitive qualitative and visualized spectral line movement. By comparing and analyzing the movement of the peak spectral line and amplitude spectrum before and after stress application, the effects of stress type, applied intensity, and duration on the device microstructure can be obtained. The influence of the damage location and damage degree of the zone structure is shown in Fig. 4.

Claims (3)

1. The method is characterized in that the method is based on a Bayesian iterative deconvolution time constant extraction technology, analyzes time constants and peak spectrum changes, and realizes nondestructive characterization, accurate positioning and quantitative characterization of evolution process of the micro-area structural damage of the semiconductor device;
mapping relation exists between current transient change between drain and source electrodes and damage of a micro-area of the device; based on the mapping relation, the drain current transient change curve before and after the damage of the device is acquired, the current transient curve time constant is extracted by using a Bayesian iterative deconvolution time constant extraction method, and the contribution of the damage at different positions to the drain current change is acquired by integrating a time constant spectrum on the basis, and is shown in a spectral line form; by analyzing the transient curves of the drain electrodes before and after the damage, the evolution process of the invisible micro-region structural damage in the device is converted into visual spectral line movement, and the accurate positioning of the damage of the micro-region structural damage of the device, the damage degree and the spectral value quantitative characterization of the evolution process are realized.
2. The method for nondestructive characterization of micro-area structural damage of a semiconductor device according to claim 1, wherein S1 is used for constructing a transient current test system and collecting transient change curves of leakage current of the device before and after stress action; the accuracy of the current test system reaches millisecond level, a trap filling stage is required to be applied to a damaged part of the device before a measurement process in transient current response is measured, larger electric stress is applied in the filling stage, the damaged part of the device, namely the trap, is fully filled, then the device is switched to a small measurement bias, and the process of releasing electrons from the trap is monitored, so that a change curve of leakage current IDS along with time can be acquired; selecting a tested device, placing the tested device on a constant temperature platform with the temperature of T0, and applying an electrical bias condition to the device so as to acquire a change curve of leakage current IDS along with time;
s2, after transient drain current response is acquired, processing a transient drain current response curve to obtain a time constant spectrum of a trap, and accurately distinguishing a region with a more gentle curve amplitude change through repeated iterative computation by a time constant extraction method based on Bayesian deconvolution, wherein a time constant peak value of a device damage position can be highlighted;
trap information exists in transient current response in an e-exponential variation form as shown in a formula (1)
Figure FDA0004094978990000011
τ i Time constant, ΔI, for the ith trap i For which the amplitude of the current change is affected; time constant spectrum for extracting characteristic time constant tau of trap i The time constant is displayed in the form of peak value spectrum, and the abscissa of the peak value is the trap time constant;
first, a logarithmic time variable is introduced:
z=lnt (2)
then, the time constant spectrum of the trap is as follows:
Figure FDA0004094978990000012
Δi (z) is the time constant spectrum, then the transient current Ids (t) is described as:
Figure FDA0004094978990000013
compared to equation (1), equation (4) is an integrated version of the channel transient current; in combination with equation (2), the transient current is converted into:
Figure FDA0004094978990000021
this is the convolution integral equation for Δi (τ); the result of differentiating z on both sides of equation (5) is:
Figure FDA0004094978990000022
the definition function W (z) is as follows:
W(z)=exp(z-exp(z)) (7)
then
Figure FDA0004094978990000023
The expression of (2) is:
Figure FDA0004094978990000024
Figure FDA0004094978990000027
as a convolution operator, the time constant spectrum Δi (z) is:
Figure FDA0004094978990000025
the time constant spectrum is obtained by solving the Bayes deconvolution; the time constant of the damaged position of the device is presented in the form of a peak spectrum, the area enclosed by the envelope curve of the peak spectrum corresponds to the variation of the drain-source current, the abscissa corresponding to the peak value of the time constant spectrum is the time constant of the damaged position of the device, and the ordinate is the relative variation of the drain-source current caused by the damaged position of the device;
s3, accumulating the y value of the time constant spectrum according to the total variation of the peak value and the drain current to enable the y value corresponding to each time point to be equal to the accumulated value of the y values of all the previous time points, namely
Figure FDA0004094978990000026
Exchanging the x-axis value with the y-axis value to obtain an integral amplitude spectrum;
s4, first-order derivation is carried out on the integral amplitude spectrum to obtain a differential amplitude spectrum; the difference value between peak values in the differential amplitude spectrum is the absolute action intensity of the trap, namely the sum of all action intensities is equal to the change of the total transient current response, and the position and the damage degree of the damage of the micro-area structure of the device are intuitively and accurately represented; the ordinate of the peak of the differential amplitude spectrum represents the degree of independence of this type of trap.
3. The method for nondestructive characterization of semiconductor device micro-area structure damage of claim 2 wherein the characterization of S4 comprises: transient drain current collection and correction, time constant extraction, peak spectrum characterization and amplitude spectrum characterization.
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Publication number Priority date Publication date Assignee Title
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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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