CN1799506A - Interation curative wave filtration combined weighted least squares positron emission tomography method - Google Patents

Interation curative wave filtration combined weighted least squares positron emission tomography method Download PDF

Info

Publication number
CN1799506A
CN1799506A CN 200510122610 CN200510122610A CN1799506A CN 1799506 A CN1799506 A CN 1799506A CN 200510122610 CN200510122610 CN 200510122610 CN 200510122610 A CN200510122610 A CN 200510122610A CN 1799506 A CN1799506 A CN 1799506A
Authority
CN
China
Prior art keywords
image
component
observed data
projection
data
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
CN 200510122610
Other languages
Chinese (zh)
Other versions
CN100387194C (en
Inventor
周健
罗立民
李松毅
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.)
Southeast University
Original Assignee
Southeast University
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 Southeast University filed Critical Southeast University
Priority to CNB200510122610XA priority Critical patent/CN100387194C/en
Publication of CN1799506A publication Critical patent/CN1799506A/en
Application granted granted Critical
Publication of CN100387194C publication Critical patent/CN100387194C/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Landscapes

  • Image Processing (AREA)

Abstract

The invention discloses an image-forming method of weighting curvature flow filtering during the least square iterating for constructing image of positive electron emitting tomography, firstly getting observing data, determining the scale of original image, comparing each component in the observing data with 1, dividing each component in the error variance and filtering the intermediate image with curvature flow and getting the filtered image as original image, repeating this course until the image reconstructed image contracted and getting the finished image; the invention adding curvature flow filtering in the least square iterating depending on the current feature of PET image-forming, through which to inhibit pattern noise and improve the image quality; the invention is characterized by the simple process, fast treating speed and good effect for inhibiting the background disturb.

Description

The interation curative wave filtration combined weighted least squares positron emission tomography method
Technical field
The invention belongs to positron emission tomography (PET:Positron emission tomography) technical field of imaging, the invention particularly relates to a kind of interation curative wave filtration combined weighted least squares positron emission tomography method that is used to make up image.
Background technology
In modern PET imaging system, the precorrection that meets at random of original Poisson observed data is operated, especially postpone the window coincidence correction, become an essential important step.It can suppress the major part signal to noise ratio of coincident event (especially ambient interferences) raising observed data at random effectively.Yet because the processing of precorrection makes observed data not obey original Poisson statistics characteristic.Like this based on the method for estimation of original Poisson maximum likelihood not feasible.In this case, we consider weighted least require method usually.
The observed data model of existing least square method is:
y i = Σ j a ij f j + ϵ i - - - ( 1 )
Y wherein iI the number of photons that probe access detects of expression precorrection, 1≤i≤M, M are total probe access number; f jRepresent the number of photons that j pixel goes out to send, f j〉=0,1≤j≤N, N are total number of picture elements; a IjRepresent that photon energy that j pixel go out to send is by i the detected probability of probe access; ε iExpression is attached to the random error on the photon number that i probe access detect, its statistical property obedience zero-mean, and variance is d iNormal distribution.According to (1), the object function that we rebuild can be expressed as:
J ( f ) = arg min f ( y - Af ) T Σ - 1 ( y - Af ) , And Condition of Non-Negative Constrains: f 〉=0 (2)
Here y is by y i, the observed data vector that 1≤i≤M forms; F is by f j, the image vector that 1≤j≤N forms; A is by a IjSystem's probability matrix of the M * N that forms; ∑ is M * M weighting diagonal matrix, and i element on its diagonal is d i
Choosing of weighting matrix is extremely important, and its quality directly has influence on quality of reconstructed images.We can adopt following variance method of estimation:
d i=max(y i,1),1≤i≤M,(3)
Under Condition of Non-Negative Constrains, if image
Figure A20051012261000051
Separate for the weighted least-squares of object function (2), must satisfy the Kuhn-Tucker condition so:
a ) - - - f ^ j Σ i 1 d i a ij ( y i - Σ p a ip f ^ p ) = f ^ j Σ i 1 d i a ij y i , If f ^ j > 0 , j = 1 , Λ , N - - - ( 4 )
b ) - - - f ^ j Σ i 1 d i a ij ( y i - Σ p a ip f ^ p ) ≤ f ^ j Σ i 1 d i a ij y i , If f ^ j ≤ 0 , j = 1 , Λ , N - - - ( 5 )
We can directly obtain existing least square alternative manner according to (4):
f ^ j n + 1 = f ^ j n Σ i a ij y i / d i Σ i a ij Σ p a ip f ^ p n / d i , j = 1 , Λ , N , n = 0,1,2 , Λ - - - ( 6 )
N represents iterations herein.
Because the incompleteness of data for projection itself and the ill-posedness of method for reconstructing only use weighted least require method to can not get ideal reconstructed image to a great extent.Phenomenons such as it is rough that its result is easy to generate image, and noise is more obvious.Common practices is the regularization technology, considers simultaneously that promptly the regular terms relevant with image smoothing suppresses effect of noise.Yet the complexity of its realization is different with the difference of regular terms.For example, some regularization methods can bring good reconstruction effect, but realize comparatively complexity, and level and smooth dynamics is difficult to control.The introducing of regular terms can not suppress background noise preferably in addition.For the shortcoming of prior art is described, we are according to the template data shown in Figure 1 emulation that experimentizes.Fig. 2 has provided and has utilized emulated data, according to the result of existing weighted least require method reconstruction.We can find out significantly that reconstructed image is not ideal enough, and making an uproar phenomenon is comparatively obvious.Therefore how reconstructing high-quality PET image is one of problem that presses at present solution.
Summary of the invention
The invention provides a kind of interation curative wave filtration combined weighted least squares positron emission tomography method that can improve reconstructed image quality.
The present invention adopts following technical scheme:
A kind of interation curative wave filtration combined weighted least squares positron emission tomography method that is used to make up image, adopt the following step:
1) obtains observed data, write down its scale M, and it is kept at vectorial y=[y 1, Λ, y M] TIn; According to the dimensional requirement for the treatment of reconstructed image, determine the scale N of initial pictures, given its initial gray value is greater than 1, and it is kept at vector f=[f 1, Λ, f N] TIn,
2) according to the size of observed data y and initial pictures f, calculate the probability matrix A of system of M * N,
3) each component among the observed data y is carried out one by one with 1 relatively: if than 1 greatly then keep, littler than 1
Then be set to 1, and comparative result be kept among the vectorial d d=[d 1, Λ, d M] T, as the error variance of observed data,
4) with each component among the observed data y and the corresponding one by one observation data for projection that is divided by and obtains revising of each component among the error variance d y ~ : y ~ = [ y ~ 1 , Λ , y ~ M ] T , Wherein y ~ i = y i / d i , i=1,Λ,M,
5) with the transposition of the probability matrix A of system and the observed data of correction
Figure A20051012261000063
Multiplying each other obtains vectorial g, g = A T y ~ , g=[g 1,Λ,g N] T
6) probability matrix A of system and initial pictures f are multiplied each other, obtain forward projection p, p=[p 1, Λ, p M] T, again with each component among this forward projection p and the corresponding one by one forward projection that is divided by and obtains revising of each component among the error variance d p ~ : p ~ = [ p ~ 1 , Λ , p ~ M ] T , Wherein p ~ i = p i / d i , I=1, Λ, M utilizes transposition and this forward projection of the probability matrix A of system then
Figure A20051012261000067
Multiply each other and obtain the h of back projection: h = A T p ~ , h=[h 1,Λ,h N] T
7) each component of vectorial g and each component corresponding one by one being divided by among the h of back projection, obtained the image correction value
C:c=[c 1, Λ, c N] T, c wherein j=g j/ h j, j=1, Λ, N,
8) each component among this image correction value c is obtained intermediate image with corresponding one by one the multiplying each other of each component among the initial pictures f f ^ : f ^ = [ f ^ 1 , Λ , f ^ N ] T , Wherein f ^ j = c j × f j , j=1,Λ,N,
9) with intermediate image Carry out curvature flow filter at least one time, can obtain filtering image
Figure A20051012261000074
10) with this filtering image As initial pictures, turned back to for the 6th step, repeat the image convergence of this process after rebuilding, can obtain the image of final imaging.
The present invention is in conjunction with the characteristics of current PE T imaging data, and the drawback at existing method exists has proposed a kind of new solution: the interation curative wave filtration combined weighted least squares formation method.The present invention adds curvature flow filter mechanism in existing least square method iterative process, suppress making an uproar of image with this, improves the quality of image.
Compared with prior art, the outstanding effect that the present invention has is: realize comparatively simply, wherein the curvature flow filter process acts directly on the two dimensional image, needn't carry out conversion, so processing speed is very fast; The number of times that can regulate filtering to the control of the smoothness of required reconstructed image is accomplished.Because the filtering of curvature flow is a kind of preferable image filtering technique, it does not influence the original basic feature of image to smoothed image the time, such as the edge, and line, angle etc., therefore the image of rebuilding can keep due basic feature information in the original image equally; In addition, the ambient interferences that suppresses reconstructed image also there is good effect.
Fig. 3 has provided the result that the present invention rebuilds emulated data, wherein carries out Filtering Processing between 3 iteration.Itself and Fig. 2 are compared, and we can clearly find, the clear picture of rebuilding by method of the present invention, smooth can reflect the original feature of original image.
For effectiveness of the present invention there being a quantitative recognition, we weigh the quality of this formation method with the reconstructed image signal-to-noise ratio (SNR) Criterion.This criterion is defined as follows:
SNR ( dB ) = 10 lo g 10 ( | | f | | 2 | | f * - f | | 2 ) - - - ( 7 )
F wherein *Expression simulation modular view data.It is just high more to rebuild signal to noise ratio, illustrates that then formation method is good more.By calculating, we list the reconstruction signal to noise ratio of Fig. 2 and Fig. 3 respectively in the table 1, to make comparisons.
Table 1
Prior art The present invention
Rebuild signal to noise ratio (snr) 8.28dB 12.53dB
Obviously, can obtain higher signal to noise ratio with the method for the invention, its value exceeds 4dB nearly than existing weighted least require method.This has illustrated significantly that it is superior to the general property taken advantage of weighted least require method.
Table 2
Filter times 1 3 5 7 9
Rebuild signal to noise ratio (snr) 9.27dB 10.32dB 11.48dB 12.22dB 12.78dB
The present invention rebuilds signal to noise ratio to be increased and increases along with the number of times of filtering.But the amplitude that increases reduces gradually along with the increase of number of times, so filter times can control in certain scope, such as 10 times.Show that in addition the method that we invent converges to consistent reconstructed results the most at last.
In order further to verify the superiority of the method that we invent, we are illustrated with actual 3 clinical datas that obtain.Fig. 4, Fig. 5, Fig. 6 use the prior art reconstructed results.Clearly, picture quality is relatively poor, is not easy to clinical research.Fig. 7, Fig. 8 and Fig. 9 be corresponding diagram 4, Fig. 5 and Fig. 6 respectively, and they are the results with method imaging of the present invention.Therefrom we can clearly find, interation curative wave filtration combined weighted least squares method image quality of the present invention is quite superior, and it is not only level and smooth image has kept the edge, and also quite effective to suppressing ambient interferences.Therefore the present invention is more suitable for the clinical diagnosis needs.
Description of drawings
Fig. 1 is the thoracic cavity template image that is used for testing formation method
The result of Fig. 2 for rebuilding with existing weighted least require method
Fig. 3 is with the result's (3 filtering) after the imaging of the present invention
The result of Fig. 4 for clinical data 1 being carried out imaging with existing weighted least require method
The result of Fig. 5 for clinical data 2 being carried out imaging with existing weighted least require method
The result of Fig. 6 for clinical data 3 being carried out imaging with existing weighted least require method
The result (5 filtering) of Fig. 7 for clinical data 1 being carried out imaging with the present invention
The result (5 filtering) of Fig. 8 for clinical data 2 being carried out imaging with the present invention
The result (5 filtering) of Fig. 9 for clinical data 3 being carried out imaging with the present invention
The specific embodiment
The specific embodiment of the present invention is as follows:
1) obtains the observed data of carrying out coincidence correction at random, determine its scale M, and save as at vectorial y=[y 1, Λ, y M] TAccording to the dimensional requirement for the treatment of reconstructed image, determine the scale N of initial pictures, given its initial gray value is greater than 1, and it is kept at vector f=[f 1, Λ, f N] TIn.
2), calculate the probability matrix A of system of M * N according to the size of observed data y and initial pictures f.In order to calculate this system's probability matrix, we answer the geometry of known scanner, then can be according to certain method, and for example visual angle method (Angle of view) is calculated.
In practical situation, the observed data collection is from PET video picture scanner.For the quality of appraisal procedure, we also can generate the observed data that needs by computer simulation experiment.Here we illustrate with the PET thoracic cavity template of a Computer Simulation shown in Figure 1.This thoracic cavity template size is 128 * 128 PEL matrix, i.e. N=128 * 128.We suppose that the data for projection scale is M=192 * 192, and it represents 192 projection angles, and 192 probe access are arranged on each angle.We suppose that further passage and interchannel spacing are a pixel, are convenient to our computing system probability matrix A like this.
The method of coincidence correction is a lot of at random, and modern PET scanner all adopts and postpones the window coincidence correction.By its principle, we can make following emulation experiment to generate required observed data.We multiply each other with system's probability matrix and thoracic cavity template image earlier and obtain muting observed data, then all data summations are obtained total number of photons.Total number of photons is counted M divided by total probe access, estimate the average photon number that each probe access is caught.Get 25% random mark average (the 25%th, according to just before giving birth the empirical value of the analysis gained of data) as a setting of this meansigma methods.We add each noiseless observed data the average of the Poisson observation data for projection that this background random mark average is used as emulation.In conjunction with the Poisson PRNG on the computer, produce required uncorrected observation data for projection with this average.With same background random mark average, in conjunction with PRNG, we can simulate other one group of Poisson data and meet data at random as postponing window.Uncorrected observation data for projection is deducted the observation data for projection y that these delay window random mark data obtain final precorrection.
3) utilize observation data for projection y, the error variance d=[d of the method calculating observation data of being given in conjunction with formula (3) 1, Λ, d M] T
4) with each component among the observed data y and the corresponding one by one observation data for projection that is divided by and obtains revising of each component among the error variance d y ~ : y ~ = [ y ~ 1 , Λ , y ~ M ] T , Wherein y ~ i = y i / d i , i=1,Λ,M,
5) with the transposition of the probability matrix A of system and the observed data of correction Multiplying each other obtains vectorial g, that is: g = A T y ~ ,
g=[g 1,Λ,g N] T
6) probability matrix A of system and initial pictures f are multiplied each other, obtain forward projection p, p=[p 1, Λ, p M] T, again with each component among this forward projection p and the corresponding one by one forward projection that is divided by and obtains revising of each component among the error variance d p ~ : p ~ = [ p ~ 1 , Λ , p ~ M ] T , Wherein p ~ i = p i / d i , i=1,Λ,M。Utilize transposition and this forward projection of the probability matrix A of system then
Figure A20051012261000107
Multiply each other and obtain the h of back projection: h = A T p ~ ,
h=[h 1,Λ,h N] T
7) each component of vectorial g and each component corresponding one by one being divided by among the h of back projection, obtained image correction value c:c=[c 1, Λ, c N] T, c wherein j=g j/ h j, j=1, Λ, N,
8) each component among this image correction value c is obtained intermediate image with corresponding one by one the multiplying each other of each component among the initial pictures f f ^ : f ^ = [ f ^ 1 , Λ , f ^ N ] T , Wherein f ^ j = c j × f j , j=1,Λ,N,
9) middle image is carried out curvature flow filter: curvature flow filter can effectively be removed noise, but does not damage image original characteristics information, for example edge, line, angle etc.Its filtering can be represented with following partial differential equation:
∂ f ( h , v ; t ) ∂ t = ▿ · ( ▿ f ( h , v ; t ) | ▿ f ( h , v ; t ) | ) - - - ( 7 )
And boundary condition: Initial condition: f (h, v; 0)=f 0Here represents gradient operator; For the ease of difference, we use h, the level of v presentation video and the coordinate of vertical both direction; Ω is the image domain of definition; Ω is an image boundary, Be the boundary method vector; The t express time.Introducing time evolution step delta t (it is comparatively suitable to get Δ t=0.0005 here) also launches equation (7) the right item:
f t + 1 = f t + Δt × ( f hh t ( f v t ) 2 - 2 f hv t f h t f v t + f vv t ( f h t ) 2 ( f h t ) 2 + ( f v t ) 2 ) - - - ( 8 )
F wherein t≡ f (h, v; T); f h t ≡ ∂ f ( h , v ; t ) / ∂ h , f v t ≡ ∂ f ( h , v ; t ) / ∂ v Be the level of t moment function f and the single order partial derivative of vertical both direction; f hh t ≡ ∂ 2 f ( h , v ; t ) / ∂ h 2 , f hv t ≡ ∂ f ( h , v ; t ) / ∂ h ∂ v With
f vv t ≡ ∂ 2 f ( h , v ; t ) / ∂ v 2 Be second-order partial differential coefficient.
In practical situation, we consider discrete picture usually.For using formula (8) carries out filtering, we need introduce suitable difference scheme and come partial derivative in the replacement formula (8).Narration for convenience, we can suppose that image is that (square formation and the pixel pitch of K * K=N) are unit length 1 to K * K.Note (f h t) jBe function f (h, v; T) at point (h j, v j) (1≤h wherein j≤ K, 1≤v jThe single order partial derivative of≤h direction K) located, then it can be represented with following first-order difference:
( f h t ) j = f ( h j + 1 , v j ; t ) - f ( h j , v j ; t ) , j = 1 , Λ , N - - - ( 9 )
Wherein: h j=int[j/K]+1, v j=j-int[j/N] * N (int[x] the expression integer part of getting x) and j=(h j-1) * K+v jIn the same way, we can also obtain:
( f v t ) j = f ( h j , v j + 1 ; t ) - f ( h j , v j ; t ) , - - - ( 10 )
( f hh t ) j = f ( h j + 1 , v j ; t ) - 2 f ( h j , v j ; t ) + f ( h j - 1 , v j ; t ) , - - - ( 11 )
( f vv t ) j = f ( h j , v j + 1 ; t ) - 2 f ( h j , v j ; t ) + f ( h j , v j - 1 ; t ) , - - - ( 12 )
( f hv t ) j = ( f ( h j + 1 , v j + 1 ; t ) + f ( h j - 1 , v j - 1 ; t ) ) - ( f ( h j - 1 , v j + 1 ; t ) + f ( h j + 1 , v j - 1 ; t ) ) 4 - - - ( 13 )
Order in like manner f j t = f ( h j , v j ; t ) , j=1,Λ,N。We can be rewritten as (8) like this:
f j t + 1 = f j t + Δt × ( f hh t ) j ( f v t ) j 2 - 2 ( f hv t ) j ( f h t ) j ( f v t ) j + ( f vv t ) j ( f h t ) j 2 ( f h t ) j 2 + ( f v t ) j 2 , j = 1 , Λ , N , - - - ( 14 )
And t=0, Λ, t Max, t here MaxFor total time is filter times.For the image border, we do the edge replication processes, promptly for formula (9) to formula (13):
If h j-1≤0, then put h j-1 is 1; If v j-1≤0, then put v j-1 is 1;
If h j+ 1 〉=K then puts h j+ 1 is K; If v j+ 1 〉=K then puts v j+ 1 is K.
According to above-mentioned curvature flow filter principle, to middle image
Figure A20051012261000121
Carrying out curvature flow filter can followingly operate: total filter times t is set Max(general 1≤t Max≤ 10 is comparatively reasonable); Initial condition is set: f j 0 = f ^ j , J=1, Λ, N, and put t=0; By formula (14) carry out filtering, put t=t+1; Recurring formula (14) is until t=t MaxFinish.Final filtering result is kept at vector
Figure A20051012261000123
In, f ~ = [ f ~ 1 , Λ , f ~ N ] T .
10) with this filtering image
Figure A20051012261000125
As initial pictures f, turned back to for the 6th step, repeat the image convergence of this process after rebuilding, can obtain the image of final imaging.

Claims (1)

1. interation curative wave filtration combined weighted least squares positron emission tomography method that is used to make up image is characterized in that adopting the following step:
1) obtains observed data, write down its scale M, and it is kept at vectorial y=[y 1, Λ, y M] TIn; According to the dimensional requirement for the treatment of reconstructed image, determine the scale N of initial pictures, given its initial gray value is greater than 1, and it is kept at vector f=[f 1, Λ, f N] TIn,
2) according to the size of observed data y and initial pictures f, calculate the probability matrix A of system of M * N,
3) each component among the observed data y is carried out one by one with 1 relatively: if than 1 greatly then keep, then be set to 1 for a short time than 1, and comparative result be kept among the vectorial d d=[d 1, Λ, d M] T, as the error variance of observed data,
4) with each component among the observed data y and the corresponding one by one observation data for projection that is divided by and obtains revising of each component among the error variance d
Figure A2005101226100002C1
y ~ = [ y ~ 1 , Λ , y ~ M ] T , Wherein y ~ i = y i / d i , i=1,Λ,M,
5) with the transposition of the probability matrix A of system and the observed data of correction Multiplying each other obtains vectorial g, g = A T y ~ , g=[g 1,Λ,g N] T
6) probability matrix A of system and initial pictures f are multiplied each other, obtain forward projection p, p=[p 1, Λ, p M] T, again with each component among this forward projection p and the corresponding one by one forward projection that is divided by and obtains revising of each component among the error variance d
Figure A2005101226100002C6
p ~ = [ p ~ 1 , Λ , p ~ M ] T , Wherein p ~ i = p i / d i , I=1, Λ, M utilizes transposition and this forward projection of the probability matrix A of system then Multiply each other and obtain the h of back projection: h = A T p ~ , h=[h 1,Λ,h N] T
7) each component of vectorial g and each component corresponding one by one being divided by among the h of back projection, obtained image correction value c:c=[c 1, Λ, c N] T, c wherein j=g j/ h j, j=1, Λ, N,
8) each component among this image correction value c is obtained intermediate image with corresponding one by one the multiplying each other of each component among the initial pictures f
Figure A2005101226100003C1
f ^ = [ f ^ 1 , Λ , f ^ N ] T , Wherein f ^ j = c j × f j , j=1,Λ,N,
9) with intermediate image
Figure A2005101226100003C4
Carry out curvature flow filter at least one time, can obtain filtering image
10) with this filtering image
Figure A2005101226100003C6
As initial pictures, turned back to for the 6th step, repeat the image convergence of this process after rebuilding, can obtain the image of final imaging.
CNB200510122610XA 2005-11-29 2005-11-29 Interation curative wave filtration combined weighted least squares positron emission tomography method Expired - Fee Related CN100387194C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CNB200510122610XA CN100387194C (en) 2005-11-29 2005-11-29 Interation curative wave filtration combined weighted least squares positron emission tomography method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CNB200510122610XA CN100387194C (en) 2005-11-29 2005-11-29 Interation curative wave filtration combined weighted least squares positron emission tomography method

Publications (2)

Publication Number Publication Date
CN1799506A true CN1799506A (en) 2006-07-12
CN100387194C CN100387194C (en) 2008-05-14

Family

ID=36809874

Family Applications (1)

Application Number Title Priority Date Filing Date
CNB200510122610XA Expired - Fee Related CN100387194C (en) 2005-11-29 2005-11-29 Interation curative wave filtration combined weighted least squares positron emission tomography method

Country Status (1)

Country Link
CN (1) CN100387194C (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102184559A (en) * 2011-05-17 2011-09-14 刘华锋 Particle filtering-based method of reconstructing static PET (Positron Emission Tomograph) images
CN102254313A (en) * 2011-07-14 2011-11-23 浙江大学 Image defogging method based on restoration and fusion of images on foggy days

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1641700A (en) * 2005-01-06 2005-07-20 东南大学 Positive electron emitted computerised tomography full-variation weighted image method
CN1640361A (en) * 2005-01-06 2005-07-20 东南大学 Positive computerized tomography restoration method for multi-phase horizontal set

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102184559A (en) * 2011-05-17 2011-09-14 刘华锋 Particle filtering-based method of reconstructing static PET (Positron Emission Tomograph) images
CN102254313A (en) * 2011-07-14 2011-11-23 浙江大学 Image defogging method based on restoration and fusion of images on foggy days

Also Published As

Publication number Publication date
CN100387194C (en) 2008-05-14

Similar Documents

Publication Publication Date Title
WO2021232653A1 (en) Pet image reconstruction algorithm combining filtered back-projection algorithm and neural network
WO2021159948A1 (en) Deep learning-based low dose pet 3d reconstruction method
CN104751429B (en) A kind of low dosage power spectrum CT image processing methods based on dictionary learning
CN102968762B (en) Polyethylene glycol terephthalate (PET) reconstruction method based on sparsification and Poisson model
CN100508891C (en) Maximum posteriori optimizing image rebuilding method in PET imaging
Wang et al. FBP-Net for direct reconstruction of dynamic PET images
CN106846430B (en) Image reconstruction method
CN109712209A (en) The method for reconstructing of PET image, computer storage medium, computer equipment
CN109584324B (en) Positron Emission Tomography (PET) reconstruction method based on automatic encoder network
CN104574416B (en) A kind of low dosage power spectrum CT image de-noising methods
CN1924926A (en) Two-dimensional blur polymer based ultrasonic image division method
CN113256753B (en) PET image region-of-interest enhancement reconstruction method based on multitask learning constraint
CN101980302A (en) Projection data recovery-guided nonlocal mean low-dose CT reconstruction method
JP2013085960A5 (en) X-ray CT apparatus and image reconstruction system
CN103810735A (en) Statistical iterative reconstructing method for low-dose X-ray CT image
US20210366169A1 (en) Positron emission tomography image reconstruction method
CN110009613A (en) Low-dose CT imaging method, apparatus and system based on the dense network of depth
CN106204674A (en) The dynamic PET images method for reconstructing retrained based on structure dictionary and kinetic parameter dictionary joint sparse
CN112348936A (en) Low-dose cone-beam CT image reconstruction method based on deep learning
CN1640361A (en) Positive computerized tomography restoration method for multi-phase horizontal set
CN1641700A (en) Positive electron emitted computerised tomography full-variation weighted image method
CN102013108A (en) Regional spatial-temporal prior-based dynamic PET reconstruction method
CN106846427A (en) A kind of limited angle CT method for reconstructing based on the weighting full variation of anisotropy again
CN107958472A (en) PET imaging methods, device, equipment and storage medium based on sparse projection data
Michielsen et al. Patchwork reconstruction with resolution modeling for digital breast tomosynthesis

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
C17 Cessation of patent right
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20080514

Termination date: 20101129