CN106483550A - A kind of simulation spectrum curve emulation mode - Google Patents

A kind of simulation spectrum curve emulation mode Download PDF

Info

Publication number
CN106483550A
CN106483550A CN201510539124.1A CN201510539124A CN106483550A CN 106483550 A CN106483550 A CN 106483550A CN 201510539124 A CN201510539124 A CN 201510539124A CN 106483550 A CN106483550 A CN 106483550A
Authority
CN
China
Prior art keywords
spectrum curve
nuclear
simulation
actual
random number
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201510539124.1A
Other languages
Chinese (zh)
Other versions
CN106483550B (en
Inventor
易良碧
余国刚
王礼
涂小芳
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Array Microelectronics Ltd
Original Assignee
Individual
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Individual filed Critical Individual
Priority to CN201811086619.3A priority Critical patent/CN109239763B/en
Priority to CN201811085398.8A priority patent/CN109271707B/en
Priority to CN201510539124.1A priority patent/CN106483550B/en
Priority to CN201811085406.9A priority patent/CN109086555B/en
Publication of CN106483550A publication Critical patent/CN106483550A/en
Application granted granted Critical
Publication of CN106483550B publication Critical patent/CN106483550B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Management, Administration, Business Operations System, And Electronic Commerce (AREA)
  • Measurement Of Radiation (AREA)
  • Complex Calculations (AREA)

Abstract

The present invention relates to a kind of simulation spectrum curve emulation mode, comprise the steps:Step S1, obtains actual nuclear spectrum curve chart;Step S2, is processed to actual nuclear spectrum curve chart to obtain simulation spectrum curve;The simulation spectrum curve emulation mode of the present invention by carrying out Curves Recognition and spectrum curve quantizing to actual nuclear spectrum curve chart, thus obtaining the numerical value (i.e. the counting rate of the energy level of nuclear spectrum and each energy level) of spectrum curve each point, again the random number with regard to each nuclear level is obtained by this group numerical value of the random direct sampling of DSMC, thus simulating the randomness of nuclear decay process, finally more described random number is carried out with statistical disposition obtain simulating spectrum curve, determine reliability and the accuracy of imitative nuclear signal generator by inverting comparative simulation spectrum curve and actual spectrum curve.

Description

A kind of simulation spectrum curve emulation mode
Technical field
The present invention relates to a kind of nuclear energy field, more particularly, to a kind of simulation spectrum curve emulation mode.
Background technology
Nuclear decay process is random generation in time, and decay process release ray (energy) is also random , the analysis but time interval that it is occurred and energy value take statistics, can learn that nuclear decay process has following Characteristic:Approximate obedience exponential in the time interval that nuclear decay occurs;Nuclear decay process externally discharges The approximate Gaussian distributed of energy (i.e. power spectrum).
Above characteristic is had based on nuclear decay process, the imitative nuclear signal generator of traditional approach is to obey difference The random number of distribution simulating nuclear signal feature, that is, to obey exponential random number simulation nuclear signal in the time Interval statistical characteristic;Statistical property in amplitude for the nuclear signal is simulated with random numbers of Gaussian distribution.But only to take It is inapt for simulating statistical property on amplitude for the nuclear signal from the random number of Gauss distribution, and simulation obtains High phase distribution curve and actual spectrum curve there is larger error it is impossible to reflection nuclear signal spy exactly Property;Meanwhile, the power spectrum statistical property of each nucleic is not quite similar, therefore the amplitude to variety classes nucleic Simulated behavior then need produce different parameters random numbers of Gaussian distribution matching, this is unpractiaca, It is difficult in the operating process of border.
In view of a variety of drawbacks that traditional imitative nuclear signal generator exists, set forth herein one kind completely newly side Method is in order to solve problem above.
Content of the invention
It is an object of the invention to provide a kind of simulation spectrum curve emulation mode, to realize nuclear energy spectral line is carried out Emulation.
In order to solve above-mentioned technical problem, the invention provides a kind of simulation spectrum curve emulation mode, it is special Levy and be, comprise the steps:Step S1, obtains actual nuclear spectrum curve chart;And step S2, to reality Border nuclear spectrum curve chart is processed to obtain simulation spectrum curve.
Further, described simulation spectrum curve emulation mode also includes:Step S3, compares simulation by inverting Spectrum curve and actual spectrum curve, to obtain the error between simulation spectrum curve and actual spectrum curve.
Further, in step S2, actual nuclear spectrum curve chart is processed to obtain the side of simulation spectrum curve Method includes:Step S21, carries out Curves Recognition and spectrum curve quantizes to actual nuclear spectrum curve chart, with Obtain the numerical value of spectrum curve each point;Step S22, by this group number of the random direct sampling of DSMC It is worth to the random number with regard to each nuclear level, to simulate the randomness of nuclear decay process;And step S23, right Described random number carries out statistical disposition and obtains described simulation spectrum curve.
Further, in described step S21, actual nuclear spectrum curve chart is carried out with Curves Recognition and by spectrum curve The method of the numerical value to obtain spectrum curve each point of quantizing includes:Actual nuclear energy is respectively set a song to music the image of line chart Again actual spectrum curve figure is shown after filtered denoising, and the actual spectrum curve according to display Each key point that figure copies this nuclear energy spectral curve obtains spectrum curve data, to set up spectrum curve data base; Or by actual nuclear energy respectively set a song to music line chart image is filtered, noise reduction pretreatment, Curves Recognition, curvilinear characteristic carry Take, and carry out interpolation processing to improve and to repair each point data of disappearance spectrum curve, can be set a song to music with setting up Line data base.
Further, in step S22 by this group numerical value of the random direct sampling of DSMC obtain with regard to The random number of each nuclear level is included with the method simulating the randomness of nuclear decay process:Nuclear signal time statistics is special Property simulation;And nuclear signal amplitude statistics simulated behavior.
Further, the method for described nuclear signal time statistical property simulation includes:By obeying exponential Random number realizes the simulation of nuclear signal time statistical property, wherein
The random number of exponential by (0,1] equally distributed random number by inverse function method conversion obtain, and (0,1] uniform random number is suitable to try to achieve by linear congruential method.
Further, the method for described nuclear signal amplitude statistics simulated behavior includes:
By to actual nuclear spectrum Curves Recognition and digitized obtains each energy level amplitude and counting rate, then by covering Special Caro method direct sampling simultaneously exports described random number;Wherein
Identification digitized process to actual nuclear energy spectral curve include:
Step S221, is filtered to actual spectrum curve figure, noise reduction;
Step S222, by maximum kind between split-run obtain threshold value, and spectrum curve figure is carried out at binaryzation Reason, then be coordinate by the numerical value that pixel scanning method extracts each point on spectrum curve;
Step S223, is repaired to spectrum curve and is quantized.
Further, described by DSMC direct sampling and the method that exports described random number, that is,
By each point value on DSMC direct sampling spectrum curve and curve, a series of to obtain Random number, thus to simulate the randomness of nuclear decay process.
Further, the method in described step S221, actual spectrum curve figure being filtered, that is, to actual energy Line chart of setting a song to music carries out Wiener filtering process, to filter the Gaussian noise of spectrum curve in figure.
Further, in described step S223, spectrum curve is repaired and the method that quantized is included:Pass through Cubic spline interpolation filling up during spectrum curve feature extraction the data point of disappearance, and by sitting Target ratio expands stretches to obtain the numerical value of each point on spectrum curve figure.
The invention has the beneficial effects as follows, the simulation spectrum curve emulation mode of the present invention is by actual nuclear spectrum Curve chart carries out Curves Recognition and spectrum curve quantizes, thus obtaining the numerical value of spectrum curve each point (i.e. The energy level of nuclear spectrum and the counting rate of each energy level), then pass through this group number of the random direct sampling of DSMC Value is to obtain the random number with regard to each nuclear level, thus simulating the randomness of nuclear decay process, finally again to institute State random number and carry out statistical disposition and obtain simulating spectrum curve, by inverting comparative simulation spectrum curve with actual Spectrum curve is to determine reliability and the accuracy of imitative nuclear signal generator.
Brief description
The present invention is further described with reference to the accompanying drawings and examples.
Fig. 1 is the theory diagram of the simulation spectrum curve emulation mode of the present invention;
Fig. 2 is the simulation spectrum curve emulation mode flow chart of the present invention;
Fig. 3 be the present invention described step S2 in actual nuclear spectrum curve chart is processed to obtain simulation energy The method flow diagram of spectral curve;
Fig. 4 is generation n=10000 involved in the present invention (0,1) uniform random number scattergram;
Fig. 5 is the exponential random-number distribution figure of the present invention;
Fig. 6 is that 1000 group squares that above exponential random number span is evenly dividing of the present invention are gone forward side by side The cartogram of row statistics;
Fig. 7 is the spectrum curve characteristic pattern extracting of the present invention;
Fig. 8 is the spectrum curve Preliminary Simulation design sketch of the present invention;
Fig. 9 is the design sketch after the cubic spline interpolation of the present invention;
Figure 10 is that this spectrum curve that finally gives of the present invention simulates design sketch;
Figure 11 shows the design sketch of the simulation random generating process of nuclear signal;
Figure 12 shows using DSMC direct sampling final effect figure.
Specific embodiment
In conjunction with the accompanying drawings, the present invention is further detailed explanation.These accompanying drawings are the schematic diagram of simplification, The basic structure of the present invention is only described in a schematic way, therefore it only shows the composition relevant with the present invention.
As shown in figure 1, the simulation spectrum curve emulation mode of the present invention is by entering to actual nuclear spectrum curve chart Spectrum curve simultaneously quantizes by row Curves Recognition, thus obtaining numerical value (the i.e. nuclear spectrum of spectrum curve each point Energy level and the counting rate of each energy level), then obtained by this group numerical value of the random direct sampling of DSMC With regard to the random number of each nuclear level, thus simulating the randomness of nuclear decay process, finally again to described random number Carry out statistical disposition to obtain simulating spectrum curve, by inverting comparative simulation spectrum curve and actual spectrum curve To determine reliability and the accuracy of imitative nuclear signal generator.
The specific embodiment of the present invention is as illustrated in the examples below.
As shown in Fig. 2 a kind of simulation spectrum curve emulation mode of the present invention, comprise the steps:
Step S1, obtains actual nuclear spectrum curve chart;
Step S2, is processed to actual nuclear spectrum curve chart to obtain simulation spectrum curve.
Optionally, described simulation spectrum curve emulation mode also includes:
Step S3, compares simulation spectrum curve and actual spectrum curve by inverting, can be set a song to music with obtaining simulation Error between line and actual spectrum curve.
Further, as shown in figure 3, being processed to actual nuclear spectrum curve chart in described step S2 to obtain The method of simulation spectrum curve includes:
Step S21, carries out Curves Recognition and spectrum curve quantizes, to obtain to actual nuclear spectrum curve chart The numerical value of spectrum curve each point;Step S22, is obtained by this group numerical value of the random direct sampling of DSMC To the random number with regard to each nuclear level, to simulate the randomness of nuclear decay process;And step S23, to described Random number carries out statistical disposition and obtains described simulation spectrum curve.
Specifically, in described step S21, actual nuclear spectrum curve chart is carried out with Curves Recognition and by spectrum curve The method of the numerical value to obtain spectrum curve each point of quantizing includes:
Actual nuclear energy is respectively set a song to music line chart the filtered denoising of image after actual spectrum curve figure is carried out Display, and obtain and can set a song to music according to each key point that the actual spectrum curve figure of display copies this nuclear energy spectral curve Line number evidence, to set up spectrum curve data base;Or by actual nuclear energy respectively set a song to music line chart image filtered, fall Make an uproar pretreatment, Curves Recognition, curvilinear characteristic extract, and carry out interpolation processing with improve and repair disappearance energy Each point data of spectral curve, to set up spectrum curve data base.
Wherein, closed by this group numerical value of the random direct sampling of DSMC in described step S22 Random number in each nuclear level is included with the method simulating the randomness of nuclear decay process:The nuclear signal time counts Simulated behavior and nuclear signal amplitude statistics simulated behavior.
The method of described nuclear signal time statistical property simulation includes:Random number by obedience exponential is real Existing nuclear signal time statistical property simulation, the wherein random number of exponential by (0,1] equally distributed random Number is converted by inverse function method and obtains, and (0,1] uniform random number is suitable to try to achieve by linear congruential method.
Specifically, tried to achieve by linear congruential method (0,1] method of uniform random number is as follows:
The recurrence formula of linear congruential method is as follows:
xi+1≡λxi+c(mod M) (1)
Wherein λ, c are constant.The initial x choosing1Referred to as seed, has one to be fixed the generation quality of random number Ring, its value is respectively 1~216Choose between=65535.For the ease of using on computers, generally take
M=2S, wherein S is binary maximum possible number of significant digit in computer.
Fig. 4 be take 10000 (0,1] random-number distribution situation
The production method of exponential random number, that is, exponential random number can be realized by inverse function method, specifically Process is as follows:
If the distribution function of stochastic variable X obeys exponential:
F (x)=1-e-ax, x >=0 (3)
Wherein, a is a time constant, and e is the nature truth of a matter.
Permissible by above formula, F (x) ∈ [0,1), and monotone decreasing in domain of definition, therefore function F (x) is in 0~+∞ Must there is inverse function, seek its inverse function:
Due to 0 < 1-F (x)≤1, therefore above formula can be reduced to
Can be learnt by meeting by formula (5) (0,1] equally distributed Random sampling obtain obeying exponential with Machine number x.
TakeThe exponential being produced by inverse function method by the equal distribution random numbers of above unit is random Number scattergram such as Fig. 5.Above exponential random number span is evenly dividing with 1000 group squares and carries out Statistics, final cartogram is as shown in Figure 6.
The method of described nuclear signal amplitude statistics simulated behavior includes:By to actual nuclear spectrum Curves Recognition simultaneously Digitized obtains each energy level amplitude and counting rate, then by DSMC direct sampling and export described with Machine number;Wherein identification digitized process to actual nuclear energy spectral curve include:
Step S221, is filtered to actual spectrum curve figure, noise reduction;Step S222, by between maximum kind Split-run obtains threshold value, and spectrum curve figure is carried out binary conversion treatment, then is extracted by pixel scanning method On spectrum curve, the numerical value of each point is coordinate;Step S223, is repaired to spectrum curve and is quantized.
Specifically, described by DSMC direct sampling and the method that exports described random number, that is, lead to Cross each point value on DSMC direct sampling spectrum curve and curve, a series of random to obtain Random number, thus to simulate the randomness of nuclear decay process.
The method in described step S221, actual spectrum curve figure being filtered, that is, to actual spectrum curve figure Carry out Wiener filtering process, to filter the Gaussian noise of spectrum curve in figure, thus reducing noise as far as possible The interference bringing.
The specific implementation process of the method for described nuclear signal amplitude statistics simulated behavior is as follows:
In described step S221, actual spectrum curve figure is filtered, the specific implementation step of noise reduction as follows:
By Wiener filtering, actual spectrum curve figure is filtered, noise reduction process, i.e. described Wiener filter For a kind of linear filter, and also it is a kind of based on minimum mean square error criterion, the optimum to stationary process Estimator.
Hypothesis Wiener filter input signal is s (t), superimposed noise n (t).Output signal x (t) passes through wave filter g (t) Obtained by following convolution algorithm:
X (t)=g (t) * (s (t)+n (t)) (6)
For signal x (t) estimating it is desirable to be equal to s (t).
Its error is:E (t)=s (t+d)-x (t) (7)
Variance is:e2(t)=s2(t+d)-2s(t+d)x(t)+x2(t) (8)
Wherein s (t+d) is desired wave filter output.
X (t) is write as convolution integral, that is,
Square error can be calculated is:
Wherein RsIt is the auto-correlation function of s (t), RxIt is the auto-correlation function of x (t), RxsIt is x (t) and s (t) from phase Close function.The final purpose of Wiener filtering is exactly to seek optimum g (t) so that E (e2) minimum.
In described step S222 by maximum kind between split-run obtain threshold value, and spectrum curve figure is carried out two-value Change is processed, then is coordinate by the numerical value that pixel scanning method extracts each point on spectrum curve;
The specific algorithm process of maximum variance between clusters is as follows:
If the gray value of piece image is 1~m, wherein the pixel number for i for the gray value is ni, N represents figure As pixel sum, then the probability that gray value occurs for i is:
Making gray value be more than threshold value k is c1Group, i.e. c1={ 1~k }, that gray value is more than threshold value k is then c2Group, c2={ k+1~m }, then C1And C2The probability occurring is respectively:
It is calculated C1And C2Gray average be:
Wherein,So can obtain:
μr1·μ12·μ2(16)
The variances sigma between two groups thus can be calculated2For:σ2(k)=ω11r)222r)2(17)
Formula (16) is substituted into formula (17) can obtain:σ2(k)=ω2ω221)2
So optimal threshold T*=Arg max { σ2(k) }, 0≤k < m-1 (18)
Try to achieve segmentation threshold T*=0.6353.
That in described step S223, spectrum curve is repaired and quantized comprises the following steps that:
It is the number extracting each point on nuclear energy spectral curve after the filtered denoising of actual nuclear spectrum curve chart, binaryzation Value is coordinate, need to extract spectrum curve feature, and curve is quantized.Detailed process is as follows:
First, Straight Line Identification, that is, pass through to scan the row and column of nuclear energy spectral curve binary map, identify nuclear spectrum The straight line of in figure;
Secondly, fixed point, is judged horizontal stroke, the vertical coordinate of spectrum curve place coordinate system by the straight line identifying, and Positioning initial point, typically from top to bottom, scans from left to right, and the straight line identifying is just horizontal, vertical seat Mark;
3rd, spectrum curve feature extraction.For reduce image in frame and coordinate pair curve impact, need by Frame filters.Again the point (two that pixel is 0 line by line or is scanned by column by pixel scan method after filtering frame In value image, black is 0, and white is 1).
Finally, curve quantizes.After extracting curve, arrived by calculating the spectrum curve available point scanning The row of scan origin and stringer distance determine that this pixel, in the position of in figure, is sat finally by being multiplied by expand Target scale factor obtains the coordinate figure of this pixel.
Final extraction spectrum curve characteristic effect is as shown in Figure 7.
And spectrum curve Preliminary Simulation effect is as shown in Figure 8.
Further, can be seen that from Fig. 7 and Fig. 8, the spectrum curve figure of the simulation obtaining is than proper energy spectral curve Lack in the data of some points.For truly reflecting actual spectrum curve characteristic as far as possible, need to scarce The data lost carries out filling up reparation.
Specifically, described being filled up by cubic spline interpolation is lacked during spectrum curve feature extraction The data point lost, and the numerical value obtaining each point on spectrum curve figure is stretched by the ratio expansion of coordinate, to realize The data of disappearance is filled up effectively and repairs.
Described cubic spline interpolation is filling up during spectrum curve feature extraction the data point of disappearance Specific algorithm is as follows:
Piecewise function S (x) on interval of definition [a, b], if meet:
1. S (x) is in each subinterval [xi, xi+1] on be a cubic polynomial function;
2. S (x) has continuous second dervative on entirely interval [a, b].
Then S (x) is called with regard to a=x on interval [a, b]0< x1< ... < xnOne cubic spline function of=b. Thus cubic spline interpolation problem is:N+1 node x of given function g (x)0, x1..., xnObtain function y0, y1..., yn, seek cubic spline function S (x) so as to meet:
S(xj)=yj, j=0,1 ..., n (19)
Wherein, function S (x) is referred to as the cubic spline functions of g (x).
If S (x) is three sample spline interpolation functions of f (x), then must be fulfilled for following condition:
1. interpolation condition, that is,
S(xj)=yj, j=0,1 ..., n-1
2. the condition of continuity, that is,
3. the first derivative condition of continuity, that is,
4. the second dervative condition of continuity, that is,
Design sketch after cubic spline interpolation, as shown in figure 9, can be seen by its partial enlarged drawing, Data point after cubic spline interpolation is more smooth, more approaches actual value.
Actual nuclear spectrum curve simulation effect, that is, to actual nuclear spectrum curve chart after above-mentioned image procossing, Obtain this spectrum curve simulation design sketch eventually as shown in Figure 10.
Specifically, by each point value on DSMC direct sampling spectrum curve and curve, to obtain Obtain a series of random randoms number, thus to simulate the randomness of nuclear decay process.
Figure 11 shows the design sketch of the simulation random generating process of nuclear signal;
Figure 12 shows that (this figure is by actual spectrum curve using DSMC direct sampling final effect figure Figure obtains energy level and this array of counting rate after quantizing after, random sampling procedure counting obtains.This figure It is suitable to prove by the reasonability of Monte-Carlo step and accuracy).
Obtain simulating the numerical value of each point on spectrum curve and curve by numbers above image processing process (abscissa is road location Channel, and vertical coordinate is counting rate Count), more directly taken out with DSMC This group data of sample just can obtain a series of random energy levels, and (energy level such as but not limited to passes through multichannel analyzer Quantization obtains, and described road location refers to what the energy of nuclear decay process release obtained after multichannel analyzer quantization) Random number, thus to simulate the randomness of nuclear decay process.Finally more described random number is counted, can To obtain simulating spectrum curve figure, so on the one hand can be with the reliability of checking system and accuracy, the opposing party Face can also inverting in multichannel analyzer, in order to demarcate the accuracy of multichannel analyzer.
Using DSMC, probability P (A)=p (unknown) that certain event A is occurred, it is simulated meter Calculate, circular:
(1) carry out n times and repeat independent sampling test, calculating event A frequency is nA.
Introduce stochastic variable Xi, represent event A frequency in i & lt test, order
Then have
(2) event A that calculates repeats the occurrence frequency f in independent sampling test in n timesN, it is
(3) when N is fully big, with probability fNEstimated value as probability P (A)=pFor
(4) require estimated valueFor the unbiased esti-mator of probability P (A)=p, that is,
And direct sampling, that is, to nuclear signal, the characteristic on time and amplitude is with two groups of obedience different distributions Random number simulating, and random number is discrete, discontinuous.For the sampling of discrete random sequence, Direct sampling method is ideal.
The concrete sampling process of discrete distribution direct sampling method is as follows:
If the span of discrete random variable X is Xi(i=0,1,2,3 ...), its probability distribution is
P (X=Xi)=Pi(i=0,1,2,3 ...).Wherein Pi>=0,
(1) produce equally distributed random number r on (0,1) interval;
(2) try to achieve positive integer n=0,1,2... so that r meets
(3) sample value extracting discrete random variable X is X=Xn.And work as 0<r≤P0When X=X0
(4) repeat step (1), (2), (3) are until extracting n sample value.
Due to producing (0,1) if equally distributed random number r is in intervalProbability be
I.e. eventThe probability occurring is equal to event X=XnThe probability occurring.
Again because random number r obeys being uniformly distributed on (0,1), its probability density function is
Its distribution function is as follows:
Therefore it is X=x that the random number r producing draws sample valuenProbability be
It follows that (X=X is drawn into by direct sampling methodn) probability be equivalent to random number XnIn random number sequence Row X1, X2... XnThe frequency occurring.
Can be by following proof for direct sampling method reliability:
If X is discontinuous variable, its probability distribution is Pi=P { X=Xi, wherein i=1,2 ....X respectively with PiObtain Xi, thenEvent | X-E (X) | >=ε represents that stochastic variable X obtains all satisfactions Inequality | Xi- E (X) | the probable value X of >=εi, then
Due to event X=XiThe probability that (i=0,1,2 ... N) occurs is pi(0<pi<1), then X ≠ XiGeneral Rate is then 1-pi, and each X=XiThe probability occurring is constant, and each sampling resultses are with other each extractions Result is unrelated.Therefore X=XiIndividual event is a bernoulli experiment, then sampling n time, then weigh primary for n Nu Li tests.If making event A (X=Xi) number of times that occurs is nA, i.e. nA~B (n, p).Due to X1, X2..., XnIt is n stochastic variable that is separate and obeying the 0-1 distribution that parameter is p, and
HaveD (Xi)=p (1-p), i=1,2 ... n.Giving any ε > 0 then has
Be can be derived from by (4.31) formula
And
Therefore can be derived from
Abbreviation obtains
I.e. when the frequency n extracting is bigger, after sampling, the number of times of event A appearance and the frequency ratio of population of samples are got over The probability occurring close to event A.
Extracting its error of random number by direct sampling is:
OrderTherefore
I.e.It is the unbiased esti-mator of p,
I.e. the number of times of sampling n is bigger, estimated valueCloser to theoretical value p.
With the above-mentioned desirable embodiment according to the present invention for enlightenment, by above-mentioned description, related work Personnel can carry out various change and modification completely in the range of without departing from this invention technological thought. The technical scope of this invention is not limited to content in description it is necessary to according to right To determine its technical scope.

Claims (10)

1. a kind of simulation spectrum curve emulation mode is it is characterised in that comprise the steps:
Step S1, obtains actual nuclear spectrum curve chart;
Step S2, is processed to actual nuclear spectrum curve chart to obtain simulation spectrum curve.
2. simulation spectrum curve emulation mode according to claim 1 is it is characterised in that described simulation Spectrum curve emulation mode also includes:
Step S3, compares simulation spectrum curve and actual spectrum curve by inverting, can be set a song to music with obtaining simulation Error between line and actual spectrum curve.
3. according to claim 1 and 2 simulation spectrum curve emulation mode it is characterised in that
In step S2, actual nuclear spectrum curve chart is processed and included with the method obtaining simulation spectrum curve:
Step S21, carries out Curves Recognition and spectrum curve quantizes, to obtain to actual nuclear spectrum curve chart The numerical value of spectrum curve each point;
Step S22, is obtained with regard to each nuclear level by this group numerical value of the random direct sampling of DSMC Random number, to simulate the randomness of nuclear decay process;
Step S23, carries out statistical disposition and obtains described simulation spectrum curve to described random number.
4. according to claim 3 simulation spectrum curve emulation mode it is characterised in that
In described step S21, actual nuclear spectrum curve chart is carried out Curves Recognition and by spectrum curve quantize with The method obtaining the numerical value of spectrum curve each point includes:
Actual nuclear energy is respectively set a song to music line chart the filtered denoising of image after actual spectrum curve figure is carried out Display, and obtain and can set a song to music according to each key point that the actual spectrum curve figure of display copies this nuclear energy spectral curve Line number evidence, to set up spectrum curve data base;Or
By actual nuclear energy respectively set a song to music line chart image is filtered, noise reduction pretreatment, Curves Recognition, curvilinear characteristic Extract, and carry out interpolation processing to improve and to repair each point data of disappearance spectrum curve, to set up power spectrum Diagram database.
5. according to claim 4 simulation spectrum curve emulation mode it is characterised in that
Obtained with regard to each nuclear level by this group numerical value of the random direct sampling of DSMC in step S22 Random number included with the method simulating the randomness of nuclear decay process:
Nuclear signal time statistical property is simulated;And nuclear signal amplitude statistics simulated behavior.
6. according to claim 5 simulation spectrum curve emulation mode it is characterised in that
The method of described nuclear signal time statistical property simulation includes:Random number by obedience exponential is real Existing nuclear signal time statistical property simulation, wherein
The random number of exponential by (0,1] equally distributed random number by inverse function method conversion obtain, and (0,1] uniform random number is suitable to try to achieve by linear congruential method.
7. simulation spectrum curve emulation mode according to claim 6 is it is characterised in that described core is believed The method of number amplitude statistics simulated behavior includes:
By to actual nuclear spectrum Curves Recognition and digitized obtains each energy level amplitude and counting rate, then by covering Special Caro method direct sampling simultaneously exports described random number;Wherein
Identification digitized process to actual nuclear energy spectral curve include:
Step S221, is filtered to actual spectrum curve figure, noise reduction;
Step S222, by maximum kind between split-run obtain threshold value, and spectrum curve figure is carried out at binaryzation Reason, then be coordinate by the numerical value that pixel scanning method extracts each point on spectrum curve;
Step S223, is repaired to spectrum curve and is quantized.
8. simulation spectrum curve emulation mode according to claim 7 is it is characterised in that described pass through DSMC direct sampling the method exporting described random number, that is,
By each point value on DSMC direct sampling spectrum curve and curve, a series of to obtain Random number, thus to simulate the randomness of nuclear decay process.
9. simulation spectrum curve emulation mode according to claim 8 is it is characterised in that described step The method in S221, actual spectrum curve figure being filtered, carries out Wiener filtering to actual spectrum curve figure Process, to filter the Gaussian noise of spectrum curve in figure.
10. according to claim 9 simulation spectrum curve emulation mode it is characterised in that
In described step S223, spectrum curve is repaired and is quantized including:By cubic spline interpolation To fill up during spectrum curve feature extraction the data point of disappearance, and expanded by the ratio of coordinate stretch with Obtain the numerical value of each point on spectrum curve figure.
CN201510539124.1A 2015-08-28 2015-08-28 A kind of simulation spectrum curve emulation mode Active CN106483550B (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
CN201811086619.3A CN109239763B (en) 2015-08-28 2015-08-28 Simulation method for simulating nuclear decay process by using simulated energy spectrum curve
CN201811085398.8A CN109271707B (en) 2015-08-28 2015-08-28 Simulation energy spectrum curve simulation method for simulating nuclear energy spectrum line
CN201510539124.1A CN106483550B (en) 2015-08-28 2015-08-28 A kind of simulation spectrum curve emulation mode
CN201811085406.9A CN109086555B (en) 2015-08-28 2015-08-28 Simulation method for simulating energy spectrum curve by adopting Monte Carlo method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201510539124.1A CN106483550B (en) 2015-08-28 2015-08-28 A kind of simulation spectrum curve emulation mode

Related Child Applications (3)

Application Number Title Priority Date Filing Date
CN201811085406.9A Division CN109086555B (en) 2015-08-28 2015-08-28 Simulation method for simulating energy spectrum curve by adopting Monte Carlo method
CN201811085398.8A Division CN109271707B (en) 2015-08-28 2015-08-28 Simulation energy spectrum curve simulation method for simulating nuclear energy spectrum line
CN201811086619.3A Division CN109239763B (en) 2015-08-28 2015-08-28 Simulation method for simulating nuclear decay process by using simulated energy spectrum curve

Publications (2)

Publication Number Publication Date
CN106483550A true CN106483550A (en) 2017-03-08
CN106483550B CN106483550B (en) 2018-09-18

Family

ID=58234736

Family Applications (4)

Application Number Title Priority Date Filing Date
CN201811085398.8A Active CN109271707B (en) 2015-08-28 2015-08-28 Simulation energy spectrum curve simulation method for simulating nuclear energy spectrum line
CN201811086619.3A Active CN109239763B (en) 2015-08-28 2015-08-28 Simulation method for simulating nuclear decay process by using simulated energy spectrum curve
CN201811085406.9A Active CN109086555B (en) 2015-08-28 2015-08-28 Simulation method for simulating energy spectrum curve by adopting Monte Carlo method
CN201510539124.1A Active CN106483550B (en) 2015-08-28 2015-08-28 A kind of simulation spectrum curve emulation mode

Family Applications Before (3)

Application Number Title Priority Date Filing Date
CN201811085398.8A Active CN109271707B (en) 2015-08-28 2015-08-28 Simulation energy spectrum curve simulation method for simulating nuclear energy spectrum line
CN201811086619.3A Active CN109239763B (en) 2015-08-28 2015-08-28 Simulation method for simulating nuclear decay process by using simulated energy spectrum curve
CN201811085406.9A Active CN109086555B (en) 2015-08-28 2015-08-28 Simulation method for simulating energy spectrum curve by adopting Monte Carlo method

Country Status (1)

Country Link
CN (4) CN109271707B (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108416355A (en) * 2018-03-09 2018-08-17 浙江大学 A kind of acquisition method of the industry spot creation data based on machine vision
CN111276195A (en) * 2020-01-20 2020-06-12 深圳大榆树科技有限公司 Method for calculating number of compounds in gel energy spectrum by using maximum inter-class variance method
CN112462676A (en) * 2021-01-27 2021-03-09 泛华检测技术有限公司 Device capable of simulating overlapped nuclear pulse signal generation and control method thereof
CN112462675A (en) * 2021-01-27 2021-03-09 泛华检测技术有限公司 Cascaded dual-index nuclear pulse signal generating device and control method thereof

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111273337B (en) * 2020-02-27 2022-11-29 成都工贸职业技术学院 Nuclear energy spectrum processing method based on Monte Carlo pulse interpolation method
CN111553111B (en) * 2020-04-30 2023-03-28 成都航空职业技术学院 Digital imitation nuclear signal generator based on MCNP
CN114422041B (en) * 2021-12-23 2023-03-24 中国原子能科学研究院 Nuclear signal simulation method, device, terminal and storage medium
CN114241846A (en) * 2021-12-24 2022-03-25 西安恒律模训科技发展有限公司 Simulation gamma radioactive nuclide identification training method and system thereof

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN201233446Y (en) * 2008-07-14 2009-05-06 成都理工大学 Arbitrary nuclear power spectrum generator
CN102073060A (en) * 2009-11-24 2011-05-25 成都理工大学 Simulation method for random properties of nuclear signals
CN102353972A (en) * 2011-07-01 2012-02-15 成都理工大学 Multimode digital multichannel spectrometer
CN102902958A (en) * 2012-09-19 2013-01-30 四川大学 Digital nuclear signal processing and multi-parameter nuclear information acquisition method based on image recognition
CN104316954A (en) * 2014-09-28 2015-01-28 中国石油大学(华东) Nuclear physics experiment simulation system and method for carrying out energy spectrum measurement experiment and intensity measurement experiment by using the nuclear physics experiment simulation system

Family Cites Families (17)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4633088A (en) * 1985-04-08 1986-12-30 Packard Instrument Co., Inc. Reverse sum quench measurement using a liquid scintillation counter
AUPO427796A0 (en) * 1996-12-20 1997-01-23 University Of Queensland, The Computer simulation of magnetic resonance spectra employing homotopy
JP4309733B2 (en) * 2003-09-29 2009-08-05 株式会社東芝 Combustion calculation method and combustion calculation program
US7411188B2 (en) * 2005-07-11 2008-08-12 Revera Incorporated Method and system for non-destructive distribution profiling of an element in a film
CN102177444B (en) * 2008-10-10 2014-07-09 皇家飞利浦电子股份有限公司 Practical SPECT calibration method for quantification of nuclides with high-energy contributions
CN201622351U (en) * 2009-11-18 2010-11-03 成都理工大学 Nuclear signal random characteristic simulator
WO2011123837A2 (en) * 2010-04-01 2011-10-06 University Of Georgia Research Foundation, Inc. Method and system using computer simulation for the quantitative analysis of glycan biosynthesis
CN102298652B (en) * 2010-06-23 2013-02-27 成都理工大学 Method for simulating energy spectrum drift during radioactive measurement
JP2012037305A (en) * 2010-08-05 2012-02-23 Fujita Corp Sequential nonlinear earthquake response analysis method for foundation and storage medium with analysis program stored thereon
DE102011055075B4 (en) * 2010-11-05 2013-04-18 Stefan Brühl A method and apparatus for the preliminary planning of a medical ion beam therapy and apparatus for performing a medical ion beam therapy
CN102928866B (en) * 2011-08-09 2015-05-20 中国辐射防护研究院 Method for measuring spectrum and accumulated dose of neutrons by utilizing passive detector
CN103091701B (en) * 2011-10-28 2015-09-30 中国原子能科学研究院 Multipurpose flight time equipment for measuring quality of cold neutron beam
CN102916683B (en) * 2012-10-18 2016-09-14 成都理工大学 A kind of Parameter-adjustablenuclear nuclear pulse simulation method
CN103076622B (en) * 2012-10-31 2016-08-17 成都理工大学 A kind of production method of spectrum stabilization stochastic signal
WO2014090297A1 (en) * 2012-12-12 2014-06-19 Qatar Foundation System and method for the simulation of metabolic profiles
US10593436B2 (en) * 2013-11-21 2020-03-17 Terrapower, Llc Method and system for generating a nuclear reactor core loading distribution
CN103853929B (en) * 2014-03-17 2016-06-15 东华理工大学 A kind of based on the low resolution gamma spectrum inversion analysis system and method covering card response matrix

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN201233446Y (en) * 2008-07-14 2009-05-06 成都理工大学 Arbitrary nuclear power spectrum generator
CN102073060A (en) * 2009-11-24 2011-05-25 成都理工大学 Simulation method for random properties of nuclear signals
CN102353972A (en) * 2011-07-01 2012-02-15 成都理工大学 Multimode digital multichannel spectrometer
CN102353972B (en) * 2011-07-01 2013-04-10 成都理工大学 Multimode digital multichannel spectrometer
CN102902958A (en) * 2012-09-19 2013-01-30 四川大学 Digital nuclear signal processing and multi-parameter nuclear information acquisition method based on image recognition
CN104316954A (en) * 2014-09-28 2015-01-28 中国石油大学(华东) Nuclear physics experiment simulation system and method for carrying out energy spectrum measurement experiment and intensity measurement experiment by using the nuclear physics experiment simulation system

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
万东阳 等: "《数字核信号图形化识别和处理研究》", 《第十六届全国核电子学与核探测技术学术年会》 *
谭承君 等: "《基于随机抽样的核脉冲信号发生器的研究》", 《原子能科学技术》 *
霍建文 等: "《任意分布的高速仿核信号发生器》", 《核电子学与探测技术》 *

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN108416355A (en) * 2018-03-09 2018-08-17 浙江大学 A kind of acquisition method of the industry spot creation data based on machine vision
CN111276195A (en) * 2020-01-20 2020-06-12 深圳大榆树科技有限公司 Method for calculating number of compounds in gel energy spectrum by using maximum inter-class variance method
CN111276195B (en) * 2020-01-20 2023-09-19 深圳大榆树科技有限公司 Method for calculating number of gel energy spectrogram compounds by using maximum inter-class variance method
CN112462676A (en) * 2021-01-27 2021-03-09 泛华检测技术有限公司 Device capable of simulating overlapped nuclear pulse signal generation and control method thereof
CN112462675A (en) * 2021-01-27 2021-03-09 泛华检测技术有限公司 Cascaded dual-index nuclear pulse signal generating device and control method thereof
CN112462675B (en) * 2021-01-27 2021-05-07 泛华检测技术有限公司 Cascaded dual-index nuclear pulse signal generating device and control method thereof

Also Published As

Publication number Publication date
CN109239763A (en) 2019-01-18
CN109086555B (en) 2022-04-19
CN109271707B (en) 2022-04-19
CN106483550B (en) 2018-09-18
CN109239763B (en) 2022-04-19
CN109086555A (en) 2018-12-25
CN109271707A (en) 2019-01-25

Similar Documents

Publication Publication Date Title
CN106483550A (en) A kind of simulation spectrum curve emulation mode
CN106483842A (en) A kind of high-precision intelligent is imitated nuclear signal and system and its method of work is occurred
CN106483551B (en) A kind of imitative nuclear signal generator and its working method
CN104134204B (en) Image definition evaluation method and image definition evaluation device based on sparse representation
Venema et al. A stochastic iterative amplitude adjusted Fourier transform algorithm with improved accuracy
CN109784410B (en) Characteristic extraction and classification method for ship radiation noise signals
CN110059845B (en) Metering device clock error trend prediction method based on time sequence evolution gene model
CN108181613B (en) Non-uniform quantitative sorting method for sequence difference values of PRI (pulse repetition index) jittering signals
CN108681689B (en) Frame rate enhanced gait recognition method and device based on generation of confrontation network
CN108776582A (en) A kind of true random number sequence production method based on quantum tunneling effect
Szarka III et al. On the equivalence of the Bernoulli and geometric CUSUM charts
CN112989361A (en) Model security detection method based on generation countermeasure network
CN109597123B (en) Effective signal detection method and system
CN116432703B (en) Pulse height estimation method, system and terminal based on composite neural network model
CN106483867A (en) There is system processor, system and method for work in imitative nuclear signal
CN112183260A (en) One-way valve fault diagnosis method based on total variation noise reduction and RQA
CN114553606B (en) Industrial control network intrusion detection method and system
CN107886113B (en) Electromagnetic spectrum noise extraction and filtering method based on chi-square test
CN114972330A (en) Workpiece surface roughness detection optimization method based on improved histogram homogenization algorithm
CN111008356A (en) WTSVD algorithm-based background-subtracted gamma energy spectrum set analysis method
Rao et al. An Automatic CADI’s Ionogram Scaling Software Tool for Large Ionograms Data Analytics
CN111931412A (en) Underwater target noise LOFAR spectrogram simulation method based on generative countermeasure network
CN112508862A (en) Method for enhancing magneto-optical image of crack by improving GAN
CN110988802A (en) Radar radiation source identification system based on signal scale decomposition
CN114638851B (en) Image segmentation method, system and storage medium based on generation countermeasure network

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
TA01 Transfer of patent application right

Effective date of registration: 20180821

Address after: 610000 1 East three road, Erxian bridge, Chengdu, Sichuan

Applicant after: Chengdu University of Technology

Address before: 213000 Hohai University, Xinbei District, Changzhou, Jiangsu

Applicant before: Yi Liangbi

TA01 Transfer of patent application right
GR01 Patent grant
GR01 Patent grant
TR01 Transfer of patent right

Effective date of registration: 20240218

Address after: 201100 Room 201-202, Building E, No. 1618, Yishan Road, Minhang District, Shanghai

Patentee after: ARRAY MICROELECTRONICS LTD.

Country or region after: China

Address before: 610000 1 East three road, Erxian bridge, Chengdu, Sichuan

Patentee before: Chengdu University of Technology

Country or region before: China

TR01 Transfer of patent right