CN115047022A - Time domain reconstruction method and system for thermal diffusion process - Google Patents

Time domain reconstruction method and system for thermal diffusion process Download PDF

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CN115047022A
CN115047022A CN202210960652.4A CN202210960652A CN115047022A CN 115047022 A CN115047022 A CN 115047022A CN 202210960652 A CN202210960652 A CN 202210960652A CN 115047022 A CN115047022 A CN 115047022A
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张家晨
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Hefei Lock In Optical Technology Co ltd
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Abstract

The invention provides a time domain reconstruction method and a time domain reconstruction system in a thermal diffusion process, wherein the method comprises the following steps: applying an excitation signal to a sample, and emitting an infrared signal at a sample test point; collecting infrared signals of the sample test point, and calculating to obtain delay phase information based on the collected infrared signals; performing Fourier expansion on the periodic function of the excitation signal to construct a prediction function of the infrared signal intensity value of the sample test point; determining an amplitude parameter and a phase parameter of the prediction function based on the infrared signal of the sample test point and corresponding delay phase information; and sampling the sample test point according to the prediction function to obtain a thermal diffusion image of the sample test point. The invention can overcome the defects that the phase-locked thermal infrared imager detection technology is easily interfered by external noise and is difficult to interpret.

Description

Time domain reconstruction method and system for thermal diffusion process
Technical Field
The invention relates to the field of image processing, in particular to a time domain reconstruction method and a time domain reconstruction system for a thermal diffusion process.
Background
In the information age, electronic products have been widely used. The electronic product itself is composed of electronic components such as a logic operation device (CPU), a memory device (magnetic disk), and the like. In the production process of these electronic components and after a failure occurs in use for a certain period of time, it is necessary to detect them, and therefore, a method of detecting a failure of these electronic components is very important.
In recent years, nondestructive detection means are simple and efficient, and a phase-locked thermal infrared imager measurement method is taken as a main representative. The phase-locked thermal infrared imager detection technology adopts an exciting source to heat a tested piece, observes and records the infrared signal change on the surface of a material through a thermal infrared imager, and converts the infrared signal change into a visible temperature image, thereby judging and detecting the defects of a sample.
However, the detection technology of the phase-locked thermal infrared imager in the prior art is easily interfered by internal and external noise, so that the infrared flaw detection image has low contrast, high noise content and the like, and is difficult to interpret.
Disclosure of Invention
The technical problem solved by the technical scheme of the invention is as follows: the method solves the problems that the phase-locked thermal infrared imager detection technology is easily interfered by external noise and is difficult to interpret.
In order to solve the above technical problem, a technical solution of the present invention provides a time domain reconstruction method for a thermal diffusion process, including:
applying an excitation signal to a sample, wherein the excitation signal is a periodic signal, and the sample is excited by the excitation signal to emit an infrared signal at a sample test point;
collecting infrared signals of the sample test point, and calculating to obtain delay phase information based on the collected infrared signals;
performing Fourier expansion on the periodic function of the excitation signal, and constructing a prediction function of the infrared signal intensity value of the sample test point, wherein the prediction function comprises an amplitude parameter and a phase parameter;
determining an amplitude parameter and a phase parameter of the prediction function based on the periodic infrared signal of the sample test point and the delay phase information;
and sampling the sample test point according to the prediction function to obtain a thermal diffusion image of the sample test point.
Optionally, the excitation signal is a square wave signal, and the fourier expansion of the periodic function of the excitation signal includes:
fourier expansion is performed on the periodic function of the excitation signal based on the waveform of the square wave signal.
Optionally, the fourier expanding the periodic function of the excitation signal includes:
expressing the periodic function based on a trigonometric function; alternatively, the first and second electrodes may be,
the periodic function is expressed based on a trigonometric function and a combination of trigonometric functions.
Optionally, the prediction function is:
Figure 916851DEST_PATH_IMAGE001
wherein t is a time, A is the amplitude parameter,
Figure 240516DEST_PATH_IMAGE002
for the purpose of said phase parameter(s),
Figure 551412DEST_PATH_IMAGE003
in the form of a circular frequency, the frequency of the circular frequency,
Figure 353146DEST_PATH_IMAGE004
,f c is the phase locked frequency.
Optionally, the prediction function is:
Figure 308464DEST_PATH_IMAGE005
wherein t is time, C is a constant,
Figure 150167DEST_PATH_IMAGE006
for the parameters of the higher order terms corresponding to the fourier expansion,
Figure 89305DEST_PATH_IMAGE007
for the amplitude parameter corresponding to the higher order term parameter,
Figure 350522DEST_PATH_IMAGE008
for the phase parameter corresponding to the higher order term,
Figure 222663DEST_PATH_IMAGE003
is the phase lock frequency.
Optionally, the prediction function is:
Figure 294655DEST_PATH_IMAGE009
wherein t is a time, C is a constant,
Figure 658771DEST_PATH_IMAGE006
for the parameters of the higher order terms corresponding to the fourier expansion,
Figure 127274DEST_PATH_IMAGE010
is the maximum amplitude parameter of the excitation signal waveform,
Figure 994867DEST_PATH_IMAGE011
is the excitation signal waveform duty cycle parameter,
Figure 644286DEST_PATH_IMAGE003
in the form of a circular frequency, the frequency of the circular frequency,
Figure 775926DEST_PATH_IMAGE004
,f c is the phase locked frequency.
Optionally, the acquiring the infrared signal and the corresponding delay phase information of the sample test point includes:
and carrying out single measurement on the sample test point through a phase-locked infrared camera, and determining the infrared signal and the corresponding delay phase information of the sample test point.
Optionally, the sampling the sample test point according to the prediction function to obtain the thermal diffusion image of the sample test point includes:
setting the thermal diffusion image time required to be acquired in the period based on the period of the excitation signal;
and generating a thermal diffusion image of the corresponding sample test point at each moment according to the prediction function.
Optionally, the sampling the sample test point according to the prediction function to obtain the thermal diffusion image of the sample test point includes:
determining a sample sampling period according to the heating starting time of the sample test point;
setting the thermal diffusion image time required to be acquired in the period based on the sampling period;
and generating a thermal diffusion image of the corresponding sample test point at each moment according to the prediction function.
Optionally, the time domain reconstruction method further includes:
and synthesizing a thermal diffusion dynamic image of the sample based on the thermal diffusion image at the corresponding moment of the sample test point.
Optionally, the sample is an MOS tube, an IGBT tube, or a wire.
In order to solve the above technical problem, a time domain reconstruction system for a thermal diffusion process is further provided in the technical solution of the present invention, and includes:
the excitation unit is suitable for applying an excitation signal to a sample, the excitation signal is a periodic signal, and the sample is excited by the excitation signal to emit an infrared signal at a sample test point;
the acquisition unit is suitable for acquiring the infrared signals of the sample test points;
the computing unit is suitable for computing delay phase information based on the collected infrared signals;
the construction unit is suitable for performing Fourier expansion on the periodic function of the excitation signal and constructing a prediction function of the infrared signal intensity value of the sample test point, wherein the prediction function comprises an amplitude parameter and a phase parameter;
the determining unit is suitable for determining the amplitude parameter and the phase parameter of the prediction function based on the infrared signal of the sample test point and the delay phase information;
and the sampling unit is suitable for sampling the sample test point according to the prediction function so as to obtain a thermal diffusion image of the sample test point.
Optionally, the time domain reconstruction system of the thermal diffusion process further includes:
and the synthesis unit is suitable for synthesizing the thermal diffusion dynamic image of the sample based on the thermal diffusion image at the corresponding moment of the sample test point.
The technical scheme of the invention at least comprises the following beneficial effects:
the technical scheme of the invention can collect the infrared signals and the corresponding delay phase information of the sample test points based on the phase-locked thermal infrared imager detection technology, construct a prediction function of the infrared signal intensity value of the sample test points through the Fourier expansion of excitation signal waves, determine the amplitude parameters and the phase parameters of the prediction function through the collected infrared signals and the corresponding delay phase information, and sample the sample test points based on the constructed prediction function to obtain the thermal diffusion images of the sample test points; through the construction of the prediction function and the resampling of the test points, the defects that a phase-locked thermal infrared imager detection sample is easily interfered by external noise and is difficult to interpret in the prior art can be overcome.
The technical scheme of the invention can effectively restore the process that the temperature distribution on the sample dynamically changes along with the time, can obtain the time domain reconstruction result by applying the excitation signal with fixed frequency to carry out single phase-locked infrared measurement without multiple measurements, and has the advantages of simple, rapid and reliable measurement method, visual and concise measurement result and the like.
According to the technical scheme, Fourier expansion is carried out on the waveform of the excitation signal, a prediction function based on the infrared signal intensity of the sample test point is constructed, and the algorithm is simple and reliable, requires a small storage space and has the advantage of low cost.
In an optional technical scheme of the invention, a scheme for measuring and sampling test points at different positions of a sample is also provided. Due to the fact that time sequences of hot spots of test points at different positions of the sample are different, the technical scheme of the invention can periodically reflect the heating sequence of the different positions of the sample, so that the conduction process of the hot spots in the sample can be dynamically presented, great convenience is brought to detection and analysis of subsequent data, and material properties of different areas on an electronic device and depth information of fault positions in the device are further represented.
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Other features, objects and advantages of the invention will become more apparent upon reading of the detailed description of non-limiting embodiments with reference to the following drawings:
fig. 1 is a schematic flow chart illustrating steps of a time domain reconstruction method for a thermal diffusion process according to an embodiment of the present invention;
FIG. 2 is a schematic waveform diagram of an excitation signal provided by the present invention;
FIG. 3 is a schematic structural diagram of a collection and computer system for applying an excitation signal to a sample according to an embodiment of the present invention;
fig. 4 is a schematic flow chart illustrating steps of a time domain reconstruction method of another thermal diffusion process according to an embodiment of the present invention;
FIG. 5 is a schematic diagram of a periodic temperature profile for time domain reconstruction in a thermal diffusion process of an MOS transistor according to the present invention;
FIG. 6 is a schematic flow chart of an algorithm for synthesizing a sample image in a period containing high-order terms according to the present invention;
fig. 7 is a schematic diagram of a periodic temperature distribution image for time domain reconstruction in the thermal diffusion process of the IGBT tube according to the technical solution of the present invention;
fig. 8 is a schematic diagram of a periodic temperature distribution image for time domain reconstruction of a thermal diffusion process of a nickel-titanium alloy wire according to the technical solution of the present invention.
Detailed Description
In order to better and clearly show the technical scheme of the invention, the invention is further described with reference to the attached drawings.
The phase-locked infrared thermal imager detection technology can apply periodic excitation signals to electronic components in the production process or the use process, a periodic heat source is formed on the electronic components to be detected, and images related to the heating process of the electronic components to be detected are obtained through image processing of the acquired infrared signals. According to the technical scheme, the time domain reconstruction is carried out on the heating process of the sample in a period by measuring the intensity information and the delay phase information of the infrared image of the periodically heated sample, the relation between the temperature distribution on the sample and the time in the period is displayed, and the thermal diffusion image of the sample test point is formed.
The present embodiment provides a time domain reconstruction method of a thermal diffusion process as shown in fig. 1, which includes the following steps:
step S100, applying an excitation signal to a sample, wherein the excitation signal is a periodic signal, and the sample is excited by the excitation signal to emit an infrared signal at a sample test point.
In this step, the sample may be an electronic component, such as a MOS transistor, an IGBT transistor, or a wire, during production or during use.
In theory, the excitation signal can be applied to the embodiment of the present invention as long as it is a periodic signal, and it is convenient and appropriate to select the excitation signal as a square wave signal. Fig. 2 illustrates that three square wave signals with different duty ratios (respectively, square wave signals with 80%, 50%, 20%) can be used as the excitation signal waveform of step S100.
Referring to fig. 3, when an excitation signal is applied to a sample, test points at different positions of the sample are excited by a current (i.e., the excitation signal), and an infrared signal is generated. An infrared camera can be used to obtain the infrared signals of the various test points of the sample. It should be noted that fig. 3 only shows that the excitation signal is a current by way of example, but in practice, the excitation sources such as voltage, radiation, stress, etc. are all replaceable and usable, and the present embodiment does not limit the specific signal form of the excitation signal.
The infrared camera obtains the heating condition of each test point, and the heating condition is different due to different positions of the test points. The test point may be a sample position corresponding to a sample pixel point in the image corresponding to the image generated by the infrared camera.
And S101, acquiring infrared signals of the sample test point, and calculating to obtain delay phase information based on the acquired infrared signals.
With continued reference to fig. 3, an infrared camera may be used to acquire infrared signals collected at various test points of the sample. Because the excitation signal is periodic, a periodic heat source is formed on each test point of the sample, and the infrared signal intensity and the delay phase information of the heating position on the sample are calculated through image processing of the collected infrared signal. The infrared camera has a synchronization process with the excitation source (schematically shown as current in fig. 3) at the time of acquisition, thereby generating and obtaining delayed phase information of the infrared signal.
And S102, performing Fourier expansion on the periodic function of the excitation signal, and constructing a prediction function of the infrared signal intensity value of the sample test point, wherein the prediction function comprises an amplitude parameter and a phase parameter.
In step S102, any periodic function can be fourier-expanded, so that fourier expansion can be used for the periodic function expression of the excitation signal, that is, the periodic waveform of the excitation signal is described by a trigonometric series, and a prediction function of the infrared signal intensity value of the sample test point is constructed by the infrared signal intensity of the test point and the corresponding delay phase information obtained in step S101. Further, the prediction function may be calculated by calculating a functional expression in which the infrared signal intensity value of each test point of the sample varies periodically with time. Specifically, a prediction function of the sample test point can be constructed by using a trigonometric function and a periodic amplitude value and a delayed phase value of the infrared signal intensity value of the corresponding test point based on Fourier expansion of the periodic function of the excitation signal.
In the present embodiment, the prediction function may be a trigonometric function simulating a change in signal intensity with time according to the waveform of the excitation signal. Since the prediction function is expressed by fourier expansion based on the waveform of the excitation signal, an arbitrary trigonometric function expression and a combination of trigonometric functions may be used, such as a sin function may be typically applicable. Other forms of trigonometric functions, such as cos functions, tan · cos functions and combinations of other trigonometric functions, may also be used, essentially identical to the result obtained with sin functions without any distinction. In the case that the excitation signal is a square wave signal, the fourier transform theory proves that any periodic square wave function can be represented by the sum of a series of trigonometric functions, and therefore the construction method of the prediction function under the square wave signal is the same.
Specifically, the prediction function may be:
Figure 660836DEST_PATH_IMAGE001
Figure 914094DEST_PATH_IMAGE012
can be a function of the periodic variation of the infrared signal intensity value of a test point of the sample with time, wherein t is the time when the infrared signal intensity value of the test point varies, A is an amplitude parameter of the infrared signal intensity value of the test point,
Figure 859048DEST_PATH_IMAGE002
a delay phase parameter for the infrared signal strength at the test point,
Figure 319460DEST_PATH_IMAGE003
in the form of a circular frequency, the frequency of the circular frequency,
Figure 8062DEST_PATH_IMAGE004
,f c the phase-locked frequency of the infrared camera for collecting the infrared signal parameters of the test point.
Specifically, the prediction function may also consider a higher-order term of fourier expansion of the waveform of the test point excitation signal, so that the following function may also be applied as the prediction function model:
Figure 115826DEST_PATH_IMAGE013
Figure 109977DEST_PATH_IMAGE014
may be a function of the periodic variation of the infrared signal intensity value of a test point of the sample with time, where t is the time at which the infrared signal intensity value of the test point varies, C is a constant,
Figure 139244DEST_PATH_IMAGE006
the parameters of the higher order terms for the fourier expansion of the corresponding function,
Figure 225011DEST_PATH_IMAGE007
the amplitude parameter of the infrared signal intensity of the test point corresponding to the parameter of the high-order item,
Figure 794140DEST_PATH_IMAGE008
the delay phase parameter corresponding to the higher-order term of the infrared signal intensity of the test point,
Figure 80896DEST_PATH_IMAGE003
in the form of a circular frequency, the frequency of the circular frequency,
Figure 987672DEST_PATH_IMAGE004
,f c the phase-locked frequency of the infrared camera for collecting the infrared signal parameters of the test point.
Specifically, the prediction function may also consider the duty ratio of the excitation signal waveform in consideration of a high-order term of fourier expansion of the excitation signal waveform of the test point, and with reference to fig. 2, in the case of excitation signal waveforms with different duty ratios, a duty ratio parameter may be added to the prediction function to perfect the accuracy of the prediction model, so that the following function may also be applied to the prediction function model of this embodiment:
Figure 486917DEST_PATH_IMAGE015
Figure 639113DEST_PATH_IMAGE016
may be a function of the periodic variation of the infrared signal intensity value of a test point of the sample with time, where t is the time at which the infrared signal intensity value of the test point varies, C is a constant,
Figure 955825DEST_PATH_IMAGE006
the parameters of the higher order terms for the fourier expansion of the corresponding function,
Figure 490843DEST_PATH_IMAGE010
is the maximum amplitude parameter of the infrared signal strength of the test point,
Figure 587587DEST_PATH_IMAGE011
for the excitation signal waveform duty cycle parameter,
Figure 134237DEST_PATH_IMAGE003
in the form of a circular frequency, the frequency of the circular frequency,
Figure 28375DEST_PATH_IMAGE004
,f c the phase-locked frequency of the infrared camera for collecting the infrared signal parameters of the test point.
Step S103, determining the amplitude parameter and the phase parameter of the prediction function based on the infrared signal of the sample test point and the corresponding delay phase information.
In step S103, based on the prediction function constructed in step S102, a single measurement may be performed on each sample test point by using the phase-locked infrared camera, and the infrared signal and the corresponding delay phase information of the sample test point are determined, so as to determine the parameters in the prediction function.
E.g. for prediction functions
Figure 788040DEST_PATH_IMAGE017
If the excitation signal introduced into the sample is set to be a fixed frequency
Figure 550459DEST_PATH_IMAGE018
The square wave current can obtain the amplitude A and the delayed phase value of the infrared signal intensity of each test point on the sample measured by the phase-locked infrared camera
Figure 76250DEST_PATH_IMAGE002
(ii) a At this time, the known circular frequency is
Figure 141289DEST_PATH_IMAGE003
Figure 647969DEST_PATH_IMAGE004
,f c If the phase-locked frequency of the infrared camera is adopted, a function expression that the infrared signal intensity value of each test point in the sample changes periodically along with time can be obtained through calculation, namely
Figure 699233DEST_PATH_IMAGE001
As yet another example, for a prediction function
Figure 610688DEST_PATH_IMAGE019
Prediction function
Figure 595698DEST_PATH_IMAGE019
The process of more finely reducing the sample heating, many higher order terms of the fourier expansion are also taken into account. By performing a single measurement with a phase-locked infrared camera, it can be determined in turn
Figure 592604DEST_PATH_IMAGE019
A in (1) 1 ,A 2 ,A 3 … (i.e. the
Figure 696826DEST_PATH_IMAGE007
) And
Figure 197208DEST_PATH_IMAGE020
Figure 601120DEST_PATH_IMAGE021
Figure 448772DEST_PATH_IMAGE022
… (i.e. the
Figure 310679DEST_PATH_IMAGE008
) And (5) waiting for parameters, and obtaining a prediction function parameter value of the pixel point in the infrared image of the sample along with the change of time.
As another example, for a prediction function
Figure 55782DEST_PATH_IMAGE023
Prediction function
Figure 630595DEST_PATH_IMAGE024
The waveform duty cycle of the sample test point excitation signal is also considered, and the waveform duty cycle parameters are known. In fact, the prediction function
Figure 336514DEST_PATH_IMAGE025
Based on predictive functions
Figure 267692DEST_PATH_IMAGE019
And the waveform duty cycle is taken into account. Prediction function
Figure 999457DEST_PATH_IMAGE019
Is/are as follows
Figure 748101DEST_PATH_IMAGE007
Is composed of
Figure 941316DEST_PATH_IMAGE026
Figure 204414DEST_PATH_IMAGE008
Is composed of
Figure 799474DEST_PATH_IMAGE027
Constructed as a prediction function
Figure 719020DEST_PATH_IMAGE023
Figure 524165DEST_PATH_IMAGE010
For square-wave amplitude, to be identifiable sequentially by a single measurement of the infrared camera
Figure 190288DEST_PATH_IMAGE007
Figure 905435DEST_PATH_IMAGE008
Carry-in-return prediction function
Figure 995881DEST_PATH_IMAGE019
Can be reduced to obtain a signal with any duty ratio to obtain a prediction function
Figure 898109DEST_PATH_IMAGE023
The parameter (c) of (c). Prediction function
Figure 893223DEST_PATH_IMAGE028
The duty cycle of (2) is adjustable. By passing
Figure 728455DEST_PATH_IMAGE011
The parameter adjusts the waveform duty ratio parameter, the duty ratio is large,
Figure 661907DEST_PATH_IMAGE011
the value is large and ranges from 0% to 100%. At the moment, the signal frequency is not changed, and the power of the excitation signal can be adjusted through the duty ratio parameter. For example, the excitation signal in FIG. 2 is a square wave signal corresponding to a duty cycle parameter of 80% of the square wave signal
Figure 379327DEST_PATH_IMAGE011
Is 80%, corresponding to the duty ratio parameter of 50% square wave signal
Figure 305695DEST_PATH_IMAGE011
Is 50%, corresponding to the duty ratio parameter of 20% square wave signal
Figure 822582DEST_PATH_IMAGE011
The content was 20%.
And step S104, sampling the sample test point according to the prediction function to obtain a thermal diffusion image of the sample test point.
Based on step S104, with reference to fig. 3, according to the calculated prediction function, an image integer to be presented by the sample test point in the next period of the excitation signal may be preset by the computer, and the computer is configured to generate the thermal diffusion image of the test point in the period based on the prediction function.
Specifically, the sampling the sample test point according to the prediction function to obtain the thermal diffusion image of the sample test point includes:
setting the thermal diffusion image time required to be acquired in the period based on the period of applying the excitation signal to the sample test point;
and generating a thermal diffusion image of the corresponding sample test point at each moment according to the prediction function.
According to the process, the method can correspond to a computer to generate pixel points in the thermal diffusion image of the sample test point, the pixel points set the number of the image frames to be presented in one period of the sample test point to be N according to the heating process of the prediction function in the period, and the N is a natural number which is larger than or equal to zero.
For prediction functions
Figure 723673DEST_PATH_IMAGE029
And setting i as an index value for generating a sample thermal diffusion image, wherein the image comprises pixel values of a plurality of sample test points, and i is a natural number which is greater than or equal to zero and less than or equal to N. The pixel value of the sample thermal diffusion image can be determined by the following function
Figure 53023DEST_PATH_IMAGE030
Obtaining:
Figure 799393DEST_PATH_IMAGE031
Figure 343638DEST_PATH_IMAGE032
in the prediction function
Figure 943859DEST_PATH_IMAGE029
On the basis of
Figure 432609DEST_PATH_IMAGE033
Of course, for the prediction function
Figure 779408DEST_PATH_IMAGE029
Or taking values at N moments in a period and predicting a function
Figure 912580DEST_PATH_IMAGE029
And acquiring the image pixel value at the temperature distribution value at each moment. If a heating period is T =0.53s, a temperature distribution image at the time T of 0s, 0.11s, 0.21s, 0.32s, 0.43s, 0.53s is taken.
For other prediction function models, the image dereferencing process is similar, and is not described herein again.
Because the sample test points are multiple and can correspond to pixel points in a computer image, each pixel point has a heating process in a period according to a prediction function, and the heating process of each test point (which also corresponds to a pixel point in a computer) has different heating starting realization according to different test point positions, sampling the sample test points according to the prediction function to obtain the thermal diffusion image of the sample test points can also comprise:
determining a sample sampling period according to the heating starting time of the sample test point;
setting the thermal diffusion image time required to be acquired in the period based on the heating period of the sample test point;
and generating a thermal diffusion image of the corresponding sample test point at each moment according to the prediction function.
For prediction functions
Figure 955141DEST_PATH_IMAGE029
Setting i as an index value for generating a sample thermal diffusion image, wherein the image comprises pixel values of a plurality of sample test points, and the pixel values of the sample thermal diffusion image can be determined by the following function
Figure 416341DEST_PATH_IMAGE030
Obtaining:
Figure 832410DEST_PATH_IMAGE034
aiming at different time starting points of the heating process of the sample, the evolution of the heating process of the pixel point of the sample image can be simulated by the left and right movement of the value i in the interval, and the value i can be
Figure 145055DEST_PATH_IMAGE035
And x is an arbitrary value, namely a dynamic change value of the heating time starting point of the analog pixel point.
For other prediction function models, the image dereferencing process is similar, and is not described herein again. By simulating different time sequences of hot spots at different positions of the sample test point in the periodic heating process through the sample image pixel points, the heating sequence of the sample at different positions in the periodic heating process can be visually reflected, so that the conduction process of the hot spots in the sample can be dynamically presented, and great convenience is brought to the analysis of subsequent data.
According to the technical scheme, the intensity information and the delay phase information of each pixel point on the image of the tested sample are obtained by using a phase-locked infrared camera or other imaging equipment related to the applied periodic excitation signal, and parameter values such as amplitude parameters, phase parameters and the like in a trigonometric function formula are determined according to the intensity information and the delay phase information. After the amplitude, the phase value and the like of each pixel point in the formula are determined, a series of images of which the intensity value of each pixel point changes along with time are obtained by properly sampling the formula.
The present embodiment further provides a time domain reconstruction method of the thermal diffusion process as shown in fig. 4, which includes, in addition to the steps S100 to S104, the following steps:
and step S105, synthesizing a thermal diffusion dynamic image of the sample based on the thermal diffusion image of the sample at the corresponding moment of the test point.
By superimposing the sample photograph on the sample thermal diffusion image generated in steps S100 to S104, the heating conditions of different positions (i.e., the test points and the corresponding sample pixel points) of the sample can be synthesized, and a dynamic video can be synthesized to show the change of the temperature distribution of the sample after the sample is periodically excited.
The following provides an example of practical application to a device under test based on the time domain reconstruction method of the thermal diffusion process of the present embodiment.
The object to be measured is a metal oxide semiconductor field effect transistor (MOS tube) with broken grid, and the MOS tube is fed with fixed frequency by constant current source
Figure 90008DEST_PATH_IMAGE018
Square wave current (here square wave current is the excitation signal in the measurement).
Based on the test system shown in fig. 3, a square wave signal is applied to the sample MOS transistor through the excitation signal (the current in fig. 3), and the amplitude a and the delayed phase value of each pixel point on the image measured by the phase-locked infrared camera are obtained
Figure 428717DEST_PATH_IMAGE002
And inputting the data into a computer to execute the time domain reconstruction method step flow of the embodiment.
The known phase-locked infrared camera has a circular frequency of
Figure 382898DEST_PATH_IMAGE003
(
Figure 357239DEST_PATH_IMAGE004
),f c If the phase-locked frequency of the infrared camera is adopted, a function expression that the pixel value (namely, the infrared signal intensity value) of each pixel point of the MOS tube thermal diffusion image periodically changes along with time can be obtained by calculation is
Figure 473094DEST_PATH_IMAGE001
Setting the number of image frames to be presented in a period as N, generating N infrared images by a computer, wherein the value of the pixel value of the same pixel in each image is
Figure 299099DEST_PATH_IMAGE036
Wherein
Figure 116357DEST_PATH_IMAGE037
Taking values to generate index values for images
Figure 688415DEST_PATH_IMAGE038
. Fig. 5 illustrates a temperature distribution image at a time when T takes values of 0s, 0.11s, 0.21s, 0.32s, 0.43s, 0.53s during one heating period (e.g., T =0.53 s), the x-axis and the y-axis in the image illustrating pixels (pixels), and the grayscale value illustrating the temperature unit kelvin (K).
In this example, N =6 is taken as an example, N may be any positive integer in principle, and the larger N is, the more slowly the temperature distribution changes at every two times during the heat generation of the sample becomes. And finally, the images are sequentially synthesized into a complete animation by the computer, and the whole process of heating the object to be measured (namely the MOS tube) can be restored through the animation.
The above example only considers the case where the first order term (fundamental frequency) of the infrared result is phase locked when the duty cycle of the periodic excitation signal is 50%. If a more refined reduction of the process in which the sample is heated is desired, many higher order terms are also taken into account. The prediction function of the change of the pixel value of the pixel point in the infrared image of the sample along with the time can be as follows:
Figure 240750DEST_PATH_IMAGE039
wherein C is a constant, ensure
Figure 25822DEST_PATH_IMAGE040
. The fourier transform theory proves that any periodic square wave function can be represented by the sum of a series of trigonometric functions. A can be determined in sequence by performing a single measurement with a phase-locked infrared camera 1 ,A 2 ,A 3 … (i.e. the
Figure 180860DEST_PATH_IMAGE007
) And
Figure 263217DEST_PATH_IMAGE041
Figure 720874DEST_PATH_IMAGE042
Figure 862749DEST_PATH_IMAGE043
… (i.e. the
Figure 696844DEST_PATH_IMAGE008
) Equal parameters, at this time
Figure 899286DEST_PATH_IMAGE037
Pixel point value of sheet image is based on prediction function
Figure 808073DEST_PATH_IMAGE044
As a function of i
Figure 689441DEST_PATH_IMAGE045
Figure 796068DEST_PATH_IMAGE046
The computer-implemented flowchart of the algorithm, as shown in fig. 6, is an intra-period sample image synthesis algorithm containing high-order terms, and includes:
at the beginning, namely: the computer initializes i, i = 0;
capturing patterns, i.e. based on
Figure 587438DEST_PATH_IMAGE045
Acquiring a sample image at initialization of i =0, after which i = 1;
computing
Figure 915127DEST_PATH_IMAGE047
And
Figure 34524DEST_PATH_IMAGE048
i.e. by calculating A 1 ,A 2 ,A 3 …(
Figure 944842DEST_PATH_IMAGE007
) And
Figure 718281DEST_PATH_IMAGE041
Figure 219801DEST_PATH_IMAGE042
Figure 216707DEST_PATH_IMAGE043
…(
Figure 930716DEST_PATH_IMAGE008
) Generating a sample image of the current i value;
judging whether i reaches a preset order, namely checking whether the current i value is N;
if so, i = N, determining that i reaches a preset order, and synthesizing a video based on N images of the sample in the period;
if not, i = i +1, and the calculation continues under the current i value
Figure 693748DEST_PATH_IMAGE047
And
Figure 366169DEST_PATH_IMAGE048
and continuing to generate a sample image of the current i value.
Similarly, if the measured object is an IGBT, applying a periodic high-voltage excitation signal to both ends of the collector and emitter of the IGBT, applying a square-wave signal to the IGBT based on the test system shown in fig. 3 through the excitation signal, and obtaining the amplitude a and the delay phase value of each pixel point on the image measured by the phase-locked infrared camera
Figure 460158DEST_PATH_IMAGE002
And inputting the data into a computer to execute the time domain reconstruction method step flow of the embodiment. The known phase-locked infrared camera has a circular frequency of
Figure 234649DEST_PATH_IMAGE003
Then, a function expression of the periodic change of the pixel value (i.e. the infrared signal intensity value) of each pixel point of the thermal diffusion image of the IGBT tube with time can be calculated as
Figure 855117DEST_PATH_IMAGE001
Setting the number of image frames to be presented in a period to be N, generating N infrared images by a computer, wherein the value of the pixel value of the same pixel in each image is
Figure 432860DEST_PATH_IMAGE036
Wherein
Figure 404358DEST_PATH_IMAGE037
Taking values to generate index values for images
Figure 581874DEST_PATH_IMAGE038
. Fig. 7 illustrates a temperature distribution image at a time when T takes 0s, 0.53s, 1.07s, 1.6s, 2.13s, 2.67s in one heating period (e.g., T =2.67 s), the x-axis and the y-axis in the image illustrating pixels (pixels), and the grayscale value illustrating the temperature unit kelvin (K).
Similarly, if the measured object is a nitinol wire through which a periodic current flows, based on the test system shown in fig. 3, square signals are applied to the two ends of the sample wire through the excitation signal to obtain the amplitude a and the delay phase value of each pixel point on the image measured by the phase-locked infrared camera
Figure 322428DEST_PATH_IMAGE002
And inputting the data into a computer to execute the time domain reconstruction method step flow of the embodiment. The known phase-locked infrared camera has a circular frequency of
Figure 71072DEST_PATH_IMAGE003
Then, the pixel value (i.e. infrared signal intensity value) of each pixel point of the metal wire thermal diffusion image can be calculatedThe function expression of the time periodic variation is
Figure 264288DEST_PATH_IMAGE001
Setting the number of image frames to be presented in a period to be N, generating N infrared images by a computer, wherein the value of the pixel value of the same pixel in each image is
Figure 392299DEST_PATH_IMAGE036
Wherein
Figure 862726DEST_PATH_IMAGE037
Taking values to generate index values for images
Figure 782272DEST_PATH_IMAGE038
. Fig. 8 illustrates a temperature distribution image at the time of T taking 0s, 0.11s, 0.21s, 0.32s, 0.43s, 0.53s during a heating period (e.g., T =0.53 s), the x-axis and y-axis in the image illustrating pixels (pixels), and the grayscale value illustrating the temperature unit kelvin (K).
In particular, in the above examples of different samples, prediction functions were used
Figure 459853DEST_PATH_IMAGE049
As a sampling function model, but based on the embodiment of the technical solution of the present invention, if a prediction function is adopted
Figure 123047DEST_PATH_IMAGE050
Figure 431668DEST_PATH_IMAGE051
Fourier expansion functions such as equal trigonometric functions or combinations of trigonometric functions are possible. And will not be described in detail herein.
Because the trigonometric function has periodicity, when the computer is used for carrying out analog sampling on the sample test point based on the prediction function model to synthesize the pixel value of the sample pixel pointPrediction function
Figure 522115DEST_PATH_IMAGE049
Figure 438992DEST_PATH_IMAGE050
Figure 781242DEST_PATH_IMAGE051
When the functions further simulate the image, the generated functions
Figure 350895DEST_PATH_IMAGE052
Figure 343734DEST_PATH_IMAGE053
Figure 998838DEST_PATH_IMAGE054
Etc. are all in the prediction function
Figure 331730DEST_PATH_IMAGE055
The conversion is obtained, i is greater than or equal to 0 and less than or equal to N as a typical representation, in fact, because the trigonometric function has periodicity, i can be greater than or equal to 0-x and less than or equal to N-x, x is a deviation value of the heating time of the sample test point corresponding to the pixel point on the period, namely, the whole value interval of i can move left and right, the time starting points of the heating process of the sample are different, but the evolution process of the heating process of the sample along with the time is completely the same, and the description is omitted here.
The sample is an MOS tube, an IGBT tube, or a metal wire, but the sample of the present embodiment may be other electronic components, and the present embodiment is not illustrated.
By the technical scheme of the embodiment, the time sequence of hot spots at different positions can be simulated in the process that the sample is excited by an excitation signal and periodically heated, the intensity information and the delay phase information of the infrared signal at the test point are calculated and obtained based on the infrared signal measured by phase-locked infrared, and the heating sequence of the sample at different positions in the periodic heating process can be visually reflected through the dynamic image and the pixel value change of the pixel point of the dynamic image, so that the conduction process of the hot spot in the sample can be dynamically presented, and great convenience is brought to the analysis of subsequent data.
The sequence of the heating points of the sample can represent the material properties of different areas on the electronic component and the depth information of the fault position in the component. According to the technical scheme, a sample thermal diffusion dynamic image is generated by a series of sample thermal diffusion images and sample images which are obtained by performing analog sampling synthesis on a prediction function based on periodic excitation signal frequency Fourier expansion, and the whole process of heating of different positions of a sample can be efficiently and simply obtained.
The foregoing description of specific embodiments of the present invention has been presented. It is to be understood that the present invention is not limited to the specific embodiments described above, and that various changes and modifications may be made by one skilled in the art within the scope of the appended claims without departing from the spirit of the invention.

Claims (13)

1. A method for time domain reconstruction of a thermal diffusion process, comprising:
applying an excitation signal to a sample, wherein the excitation signal is a periodic signal, and the sample is excited by the excitation signal to emit an infrared signal at a sample test point;
collecting infrared signals of the sample test point, and calculating to obtain delay phase information based on the collected infrared signals;
performing Fourier expansion on the periodic function of the excitation signal, and constructing a prediction function of the infrared signal intensity value of the sample test point, wherein the prediction function comprises an amplitude parameter and a phase parameter;
determining an amplitude parameter and a phase parameter of the prediction function based on the periodic infrared signal of the sample test point and the delay phase information;
and sampling the sample test point according to the prediction function to obtain a thermal diffusion image of the sample test point.
2. The time-domain reconstruction method of claim 1, wherein the excitation signal is a square wave signal, and the fourier expanding the periodic function of the excitation signal comprises:
fourier expansion is performed on the periodic function of the excitation signal based on the waveform of the square wave signal.
3. The time-domain reconstruction method of claim 1 or 2, wherein said fourier expanding the periodic function of the excitation signal comprises:
expressing the periodic function based on a trigonometric function; alternatively, the first and second electrodes may be,
the periodic function is expressed based on a combination of a trigonometric function and a trigonometric function.
4. The time-domain reconstruction method of claim 1 or 2, wherein the prediction function is:
Figure DEST_PATH_IMAGE001
wherein t is a time, A is the amplitude parameter,
Figure 675030DEST_PATH_IMAGE002
for the purpose of said phase parameter(s),
Figure 61012DEST_PATH_IMAGE003
in the form of a circular frequency, the frequency of the circular frequency,
Figure 797674DEST_PATH_IMAGE004
,f c is the phase locked frequency.
5. The time-domain reconstruction method of claim 1 or 2, wherein the prediction function is:
Figure 599407DEST_PATH_IMAGE005
wherein t is time, C is a constant,
Figure 898933DEST_PATH_IMAGE006
for the parameters of the higher order terms corresponding to the fourier expansion,
Figure 469198DEST_PATH_IMAGE007
for the amplitude parameter corresponding to the higher order term parameter,
Figure 18122DEST_PATH_IMAGE008
for the phase parameter corresponding to the higher order term,
Figure 982403DEST_PATH_IMAGE003
is the phase-locked frequency.
6. The time-domain reconstruction method of claim 1 or 2, wherein the prediction function is:
Figure 605277DEST_PATH_IMAGE009
wherein t is a time, C is a constant,
Figure 2236DEST_PATH_IMAGE006
for the parameters of the higher order terms corresponding to the fourier expansion,
Figure 444980DEST_PATH_IMAGE010
is the maximum amplitude parameter of the excitation signal waveform,
Figure 201234DEST_PATH_IMAGE011
is the excitation signal waveform duty cycle parameter,
Figure 927881DEST_PATH_IMAGE003
in the form of a circular frequency, the frequency of the circular frequency,
Figure 701933DEST_PATH_IMAGE004
,f c is the phase locked frequency.
7. The time domain reconstruction method of claim 1, wherein said acquiring infrared signals and corresponding delay phase information for the sample test point comprises:
and carrying out single measurement on the sample test point through a phase-locked infrared camera, and determining the infrared signal and the corresponding delay phase information of the sample test point.
8. The time-domain reconstruction method of claim 1, wherein said sampling the sample test point according to the prediction function to obtain a thermal diffusion image of the sample test point comprises:
setting the thermal diffusion image time required to be acquired in the period based on the period of the excitation signal;
and generating a thermal diffusion image of the corresponding sample test point at each moment according to the prediction function.
9. The time-domain reconstruction method of claim 1, wherein the sample site has a plurality of sample sites, and wherein sampling the sample site according to the prediction function to obtain the thermal diffusion image of the sample site comprises:
determining a sample sampling period according to the heating starting time of the sample test point;
setting the thermal diffusion image time required to be acquired in the period based on the sampling period;
and generating a thermal diffusion image of the corresponding sample test point at each moment according to the prediction function.
10. The time-domain reconstruction method of any of claims 1, 8, and 9, further comprising:
and synthesizing a thermal diffusion dynamic image of the sample based on the thermal diffusion image at the corresponding moment of the sample test point.
11. The time domain reconstruction method of claim 1, wherein the sample is a MOS transistor, an IGBT transistor, or a wire.
12. A time domain reconstruction system for a thermal diffusion process, comprising:
the excitation unit is suitable for applying an excitation signal to a sample, the excitation signal is a periodic signal, and the sample is excited by the excitation signal to emit an infrared signal at a sample test point;
the acquisition unit is suitable for acquiring the infrared signals of the sample test points;
the computing unit is suitable for computing delay phase information based on the collected infrared signals;
the construction unit is suitable for performing Fourier expansion on the periodic function of the excitation signal and constructing a prediction function of the infrared signal intensity value of the sample test point, wherein the prediction function comprises an amplitude parameter and a phase parameter;
the determining unit is suitable for determining the amplitude parameter and the phase parameter of the prediction function based on the infrared signal of the sample test point and the delay phase information;
and the sampling unit is suitable for sampling the sample test point according to the prediction function so as to obtain a thermal diffusion image of the sample test point.
13. The time-domain reconstruction system of the thermal diffusion process of claim 12, further comprising:
and the synthesis unit is suitable for synthesizing the thermal diffusion dynamic image of the sample based on the thermal diffusion image at the corresponding moment of the sample test point.
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