CN108010100B - Single-scanning magnetic resonance quantitative T based on residual error network2Imaging reconstruction method - Google Patents

Single-scanning magnetic resonance quantitative T based on residual error network2Imaging reconstruction method Download PDF

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CN108010100B
CN108010100B CN201711287890.9A CN201711287890A CN108010100B CN 108010100 B CN108010100 B CN 108010100B CN 201711287890 A CN201711287890 A CN 201711287890A CN 108010100 B CN108010100 B CN 108010100B
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蔡淑惠
张俊
蔡聪波
廖璞
曾坤
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Xiamen University
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Abstract

Single-scanning magnetic resonance quantitative T based on residual error network2An imaging reconstruction method relates to a magnetic resonance imaging method. Using 4 small angles with the same deflection angleExcitation pulses, each excitation pulse being followed by an evolution time such that the transverse relaxation time T of each echo signal2Different. A shifting gradient in both the frequency-encoding and phase-encoding dimensions is applied after each excitation pulse so that the signals generated by different excitation pulses differ in their position in k-space. A plurality of echo signals with different transverse relaxation times are obtained in one sample. Then, the sampling signal is input into a trained residual error network after normalization, zero filling and fast Fourier transform to be reconstructed to obtain quantitative T2And (4) an image. The training data for the residual network is derived from the simulated data. Firstly, randomly generating a template, then simulating an experimental environment to sample to obtain an input image of a network, using the template as a label, and training to obtain a mapping relation between the input image and an output image.

Description

Single-scanning magnetic resonance quantitative T based on residual error network2Imaging reconstruction method
Technical Field
The invention relates to a magnetic resonance imaging method, in particular to a single-scanning magnetic resonance quantitative T based on a residual error network2Imaging (T)2mapping) reconstruction method.
Background
Magnetic resonance parametric imaging (e.g. T)1Imaging, T2Imaging and T2 *Imaging) can be readily used to provide quantitative information for characterizing specific tissue characteristics[1]. Quantitative imaging has many prominent features, the most obvious of which is the elimination of tissue property independent effects such as operator dependence, scan parameter differences, magnetic field spatial variations, and image scaling[2]. Quantitative T2Imaging has a wide range of clinical applications, involving early diagnosis of neurodegenerative diseases[3]Liver iron overload measurement[4]Myocardial infarction assessment[5]Quantification of labeled cells[6]Diagnosis of multiple sclerosis and epilepsy[7]And the like. Quantitative T2Imaging is gaining increasing attention in clinical Magnetic Resonance Imaging (MRI). Albeit upon transverse relaxationInter T2Can be obtained by fitting spin echo MRI data of multiple different echo Times (TE), but the longer scan time of spin echo MRI allows for quantitative T in the clinic2The image is challenging[8]. Furthermore, the longer scan time also allows for spin-echo MRI based quantification T2Images are susceptible to motion artifacts[9]. Single-scan quantitative T-imaging (EPI) based on multi-echo planar imaging has been proposed2The imaging method shows great advantages in functional magnetic resonance imaging[10,11]. However, the resulting image is susceptible to more signal attenuation and ghost artifacts than single echo sampling[12,13]. Other fast quantitative T2Imaging methods, e.g. gradient spin echo (GraSE) schemes[14]Still, a multi-echo spin-echo (MSE) strategy is employed, typically requiring several minutes[15,16]
Methods of planar imaging by overlapping echo separation (OLED) have been proposed[17]Can obtain high-quality quantitative T in single scan2Images whose temporal resolution is comparable to conventional single-scan EPI images. In addition, OLED planar imaging also shows contrast to motion artifacts and non-ideal B1Stronger resistance of the field. However, the previous sequence contained only two excitation pulses, and thus a measurable T2The range is very limited, which results in having a large T2The effect is poor in areas of range, such as cerebrospinal fluid (CSF). Therefore, we improve the OLED sequence with four excitation pulses to achieve a larger T2The measurement range. However, it is difficult to separate four overlapping echo signals by the conventional method.
Deep learning, a technique for discovering distributed features of data by combining lower level features to form more abstract higher level representation attribute classes or features, has shown explosive popularity with the availability of powerful GPUs in recent years[18]. In particular, Convolutional Neural Networks (CNN) have caused super-resolution (supe) of imagesr-resolution, SR) reconstruction[19]. Different network models, e.g. convolutional neural networks[20]Residual network (ResNet)[21]Deep-recursive convolutional network (DRCN)[22]An efficient sub-pixel convolutional neural network (ESPCN)[23]And generating a antagonistic network (GAN)[24]Have been applied to obtain high resolution images. Convolutional neural networks are becoming increasingly popular in medical imaging analysis of various problems.
Reference documents:
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[14]A.M.Sprinkart,J.A.Luetkens,F.J.Doerner,J.Gieseke,B.Schnackenburg,G. Schmitz,D.Thomas,R.Homsi,and W.Block,"Gradient Spin Echo(GraSE)imaging for fast myocardial T2mapping,"Journal of CardiovascularMagnetic Resonance,vol.17,no.1,pp.12-20, 2015.
[15]T.J.Sumpf,A.Petrovic,M.Uecker,F.Knoll,and J.Frahm,"Fast T2mapping with improved accuracy using undersampled spin-echo MRI and model-based reconstructions with a generating function,"IEEE Transactions onMedical Imaging,vol.33,no.12,pp.2213-2222,2014.
[16]N.Ben‐Eliezer,D.K.Sodickson,and K.T.Block,"Rapid and accurate T2mapping from multi–spin‐echo data using Bloch‐simulation‐basedreconstruction,"Magnetic Resonance in Medicine,vol.73,no.2,pp.809-817,2015.
[17]C.B.Cai,Y.Q.Zeng,Y.C.Zhuang,S.H.Cai,L.Chen,X.H.Ding,L.J.Bao,J.H.Zhong, and Z.Chen,"Single-shot T2mapping through Overlapping-echoDetachment(OLED)Planar Imaging,"IEEE Transactions on Biomedical Engineering,vol.64,no.10,pp.2450-2461,2017.
[18]S.S.Wang,Z.H.Su,L.Ying,X.Peng,S.Zhu,F.Liang,D.G.Feng,and D.Liang,"Accelerating magnetic resonance imaging via deep learning,"in2016 IEEE 13thInternational Symposium on Biomedical Imaging(ISBI),pp.514-517,2016.
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disclosure of Invention
The invention aims to obtain four echo signals in a single scanning and then reconstruct reliable quantitative T by using a deep learning method2Single-scanning magnetic resonance quantitative T based on residual error network of image2An imaging reconstruction method.
The invention comprises the following steps:
1) preparing an experimental sample, placing the sample to be tested on an experimental bed, fixing the sample, and conveying the experimental bed with the sample into a detection cavity of a magnetic resonance imager;
2) opening imager operation software on an operation table of a magnetic resonance imager, firstly carrying out region-of-interest positioning on an experimental sample, and then carrying out tuning, shimming, frequency correction and power correction;
3) importing a compiled OLED imaging sequence, and setting each parameter of a pulse sequence according to a specific experimental condition;
4) executing the OLED imaging sequence with the set parameters in the step 3), starting sampling, and executing the next step after data sampling is finished;
5) normalizing, zero filling and fast Fourier transform are carried out on the signals obtained in the step 4), and the signals of the k space are converted into an image domain;
6) generating a random template according to the characteristics of a sample to be tested, carrying out analog sampling on the random template by using analog software to obtain a k-space signal, and then carrying out normalization, zero filling and fast Fourier transform on the signal to obtain training data;
7) building a residual error network model by adopting a TensorFlow deep learning frame and Python, and setting relevant parameters for training;
8) adopting the data training network obtained in the step 6) until the data training network converges and reaches stability to obtain a trained network model, and then utilizing the trained network model to reconstruct the experimental data obtained in the step 5) to obtain reliable quantitative T2And (4) an image.
In the step 3), the OLED imaging sequence has the structure that an excitation pulse with a flip angle of α and a displacement gradient G are sequentially arranged1Excitation pulse with flip angle of α, shift gradient G2Excitation pulse with flip angle of α, shift gradient G3Excitation pulse with flip angle of α, shift gradient G4Refocusing pulse with flip angle of β and sampling echo chain;
4 deflection angles α excitation pulses in combination with 4 shift gradients G in the frequency encoding dimension (RO) and the phase encoding dimension (PE)1、G2、G3、G4Shifting 4 echo signals in the center of k space, and combining 4 angle excitation pulses with the layer selection gradient of a layer selection dimension (SS) to perform layer selection;
the sampling echo chain is composed of gradient chains respectively acting on a frequency encoding dimension and a phase encoding dimension, the gradient chain of the frequency encoding dimension is composed of a series of positive and negative gradients, and the gradient chain of the phase encoding dimension is composed of a series of phase encoding gradients with equal areas;
before sampling an echo chain, applying bias gradients in the directions of a frequency encoding dimension and a phase encoding dimension respectively, wherein the bias gradient area of the frequency encoding dimension is half of the area of the first frequency encoding gradient, the directions are opposite, the bias gradient area of the phase encoding dimension is half of the area of all the phase encoding gradients of the phase encoding dimension, and the directions are opposite.
In step 5), analyzing the signals obtained in step 4), theoretically deriving the nuclear spin evolution under the action of an OLED imaging sequence, wherein the observable signal intensity after the action of a refocusing pulse with a flip angle of β is in direct proportion to the following expression:
Figure BDA0001498831980000051
wherein the content of the first and second substances,
Figure BDA0001498831980000052
gamma is the spin magnetic ratio of the nuclear spin,
Figure BDA0001498831980000053
the position of the nuclear spins in real space; from the above formula, the sampling period has 4 echo signals modulated by different phases, and the 4 different modulation phases are θ4、(θ34)、(θ234) And (theta)1234)。
In the step 6), the random template is randomly generated in batches by using a computer according to the feature distribution of the experimental sample, and meanwhile, the complexity of the random template is ensured to be higher and can contain all the features of the experimental sample; in the simulation sampling process, the change of a real experimental environment is considered, and an unstable factor is added, so that the robustness of the network model to an unsatisfactory experimental environment is improved; the unstable factors include excitation pulse angle deviation, shift gradient deviation, noise, and the like.
In step 7), the residual network model mainly includes: the main structure of the network and the related training parameters, the objective function of the network model is:
Figure BDA0001498831980000054
wherein N is the number of training images in the same batch, f (-) is a training network, W and b are network parameters, x is an input image, y is a template corresponding to the input imagechangeIs a matrix with a value less than a certain threshold in y set as the threshold, ymaskIs calculated using Canny for yAnd (5) image edge information obtained by the sub-calculation.
In the step 8), the trained network model is trained by using a random template, so that the generalization is strong, and the method can be suitable for reconstruction of various samples.
The present invention increases the number of excitation pulses from 2 to 4 to expand the T in the OLED sequence2And improve the accuracy of the CSF region. The OLED image is reconstructed from the 4 overlapping echo signals using a deep learning technique, thereby circumventing the difficulties encountered with conventional methods.
The invention uses 4 excitation pulses with the same small-angle deflection angle, a period of evolution time is left after each excitation pulse, so that 4 echoes have different transverse relaxation times, a shift gradient is added after each excitation pulse, so that 4 echo signals are deviated in the center of a signal space (k space), and then the k space image data is reconstructed by using a deep learning method to obtain a quantitative T2And (4) an image. The method can obtain a reliable quantitative T in a single scanning2Images while ensuring a larger T2The measurement range.
Drawings
FIG. 1 is a sequence diagram of a single scan OLED imaging sequence employed in this patent.
FIG. 2 is the reconstructed quantification T2Residual network model for image usage. In fig. 2, the residual network model contains 3 sub-networks: an input network, a residual learning network and a reconstruction network. The input network takes the real and imaginary parts of the OLED image as input and is represented by a set of feature maps. The residual error learning network is a main component for solving the task of image reconstruction. The reconstruction network is used for reconstructing a plurality of characteristic maps into a quantitative T2And (4) an image.
FIG. 3 shows the quantification T of 3 layers of human brain2Imaging reconstruction results; in FIG. 3, the first column represents the amplitude map of SE, wherein 16 yellow circles represent selected regions of interest (ROI) numbered with numbers 1-16, respectively; the second column represents the original amplitude diagram of the OLED, i.e. the input of the network; the third column shows the quantification T of the OLED reconstruction2The image is the output of the network; the fourth column indicates SE fittingQuantitative of (2)2Imaging reference images.
Fig. 4 shows the statistics of 16 ROIs. In fig. 4, a is an OLED and b is SE.
Detailed Description
The invention is further illustrated by the following figures and specific examples.
The invention provides a single-scanning magnetic resonance quantitative T based on a residual error network2The imaging reconstruction method comprises the following steps in the specific implementation process:
(1) preparing an experimental sample, placing the sample to be detected on an experimental bed and fixing, and sending the experimental bed with the sample into a detection cavity of a magnetic resonance imager.
(2) And opening imager operation software on an operation table of the magnetic resonance imager, firstly carrying out region-of-interest positioning on the experimental sample, and then carrying out tuning, shimming, frequency correction and power correction.
(3) And importing a compiled OLED imaging sequence, and setting various parameters of the pulse sequence according to specific experimental conditions.
The OLED imaging sequence sequentially comprises an excitation pulse with a flip angle of α and a displacement gradient G1Excitation pulse with flip angle of α, shift gradient G2Excitation pulse with flip angle of α, shift gradient G3Excitation pulse with flip angle of α, shift gradient G4Refocusing pulse with flip angle β, sampling echo train.
The four small angle (α) excitation pulses incorporate four shift gradients G in the frequency encoding dimension (RO) and the phase encoding dimension (PE)1、G2、G3、G4Four echo signals are shifted in the center of k space, and four small-angle excitation pulses are combined with the layer selection gradient of a layer selection dimension (SS) to perform layer selection.
The sampling echo chain is composed of gradient chains respectively acting on a frequency encoding dimension and a phase encoding dimension, the gradient chain of the frequency encoding dimension is composed of a series of positive and negative gradients, and the gradient chain of the phase encoding dimension is composed of a series of phase encoding gradients with equal areas.
Before sampling an echo chain, applying bias gradients in the directions of a frequency encoding dimension and a phase encoding dimension respectively, wherein the bias gradient area of the frequency encoding dimension is half of the area of the first frequency encoding gradient, the directions are opposite, the bias gradient area of the phase encoding dimension is half of the area of all the phase encoding gradients of the phase encoding dimension, and the directions are opposite.
(4) And (4) executing the OLED imaging sequence with the set parameters in the step (3), starting sampling, and executing the next step after data sampling is completed.
(5) And (4) carrying out normalization, zero filling and fast Fourier transform on the signals obtained in the step (4) to convert the signals of the k space into an image domain.
The obtained signal is analyzed, and the nuclear spin evolution under the action of an OLED imaging sequence is theoretically deduced, the observable signal intensity after the action of a refocusing pulse with the flip angle of β is in direct proportion to the following expression:
Figure BDA0001498831980000071
Figure BDA0001498831980000072
gamma is the spin magnetic ratio of the nuclear spin,
Figure BDA0001498831980000073
the position of the nuclear spins in real space; from the above formula, the sampling period has four echo signals modulated by different phases, and the four different modulation phases are theta4、(θ34)、(θ234) And (theta)1234)。
(6) Generating a random template according to the characteristics of an experimental sample, carrying out analog sampling on the template by using SPROM software developed by a small group of people to obtain a k-space signal, and then carrying out normalization, zero filling and fast Fourier transform on the signal to obtain training data.
The random template is generated randomly in batches by using a computer according to the characteristic distribution of the experimental sample, and meanwhile, the complexity of the template is ensured to be higher, and all the characteristics of the experimental sample can be contained. In the simulation sampling process, the change of a real experimental environment is considered, and some unstable factors such as excitation pulse angle deviation, shift gradient deviation, noise and the like are added to improve the robustness of the network model to an unsatisfactory experimental environment.
(7) And (5) building a residual error network model by using a TensorFlow deep learning frame and Python, and setting relevant parameters for training.
The residual error network model mainly comprises: the body structure of the network and the associated training parameters. The objective function of the network model is:
Figure BDA0001498831980000081
where N is the number of training images in the same batch, f (-) is the training network, W and b are the network parameters, x is the input image, y is the template corresponding to the input image, y is the number of training images in the same batchchangeIs a matrix with a value of y less than 0.06 set to 0.06maskThe image edge information is obtained by Canny operator for y.
(8) Training a network by using the data obtained in the step (6) until the network converges and reaches a stable state to obtain a trained network model, and then reconstructing the experimental data obtained in the step (5) to obtain reliable quantitative T2And (4) an image.
The trained network model is trained by using the random template, so that the generalization is strong, and the method can be suitable for reconstruction of various samples.
Specific examples are given below:
quantification of T with single-scan magnetic resonance based on residual error network2The imaging reconstruction method was performed in human brain experiments to verify the feasibility of the invention. The experiment was performed under a human nmr 3T imager. On the operation table of the magnetic resonance imager, corresponding operation software in the imager is opened, the region of interest of the imaging object is firstly positioned, and then tuning, shimming, power and frequency correction are carried out. To evaluate the effectiveness of the method to obtain images, SE imaging experiments were performed as a comparison under the same environment. Then introduced intoThe compiled OLED imaging sequence (as shown in FIG. 1) sets the parameters of the pulse sequence according to the specific experimental situation, the experimental parameters of this embodiment are set as follows, the FOV of the imaging field is 22cm × 22cm, the excitation time of the 15 ° excitation pulse is 3ms, the excitation time of the 180 ° refocusing pulse is 3ms, the first echo time is 57.8ms, the second echo time is 83.9ms, the third echo time is 135.9ms, the fourth echo time is 162.1ms, the sampling points of the frequency coding dimension and the phase coding dimension are 192, after the above experimental parameters are set, the sampling is directly started, in FIG. 1, α is the excitation pulse flip angle, β is the refocusing pulse flip angle, G is the flip angle of the refocusing pulse β, and the parameters of the pulse sequence are set according to1、G2、G3And G4Four shift gradients in frequency encoding dimension and phase encoding dimension; gcrSelecting destruction gradients of 3 dimensions for the frequency encoding dimension, the phase encoding dimension and the level; TE1、TE2、TE3And TE4The time lengths of the 4 echoes respectively; the Ecoh1, Ecoh2, Ecoh3, and Ecoh4 are the center positions of 4 echo signals, respectively.
And (5) after the data sampling is finished, reconstructing the data according to the steps (5) to (8). The residual error network model used for reconstruction is shown in fig. 2, and comprises an input network, a residual error learning network and a reconstruction network. The input network takes the real part and the imaginary part of the OLED image as input and uses a group of characteristic maps for representation, the residual error learning network is a main component for solving the image reconstruction task, and the reconstruction network is used for reconstructing a plurality of characteristic maps into a quantitative T2And (4) an image. Reconstructed quantitative T2The image is shown in fig. 3, (a) is an anatomical image of a human brain acquired by a Spin Echo (SE) sequence, in which 16 regions marked by yellow circles are regions of interest (ROIs), which are numbered with numerals 1 to 16, respectively. (b) Is the original amplitude map acquired by the OLED sequence, in which the diagonal stripes are caused by overlapping the four echo signals. (c) Quantitative T derived from reconstruction of OLED data2And (4) an image. (d) Is a quantitative T fit by SE2And (4) an image. T for 16 interesting regions in the figure2The values are subjected to quantitative statistics, i.e. T for each region of interest2The values were averaged to obtain FIG. 4. The quantification T obtained with the OLED sequence can be seen in FIG. 32The image as a whole agreed with SE, and the statistical results in FIG. 4 also indicate T for 16 ROI regions2The values are all of better accuracy.
The invention uses 4 small angle excitation pulses with the same deflection angle, and there is a period of evolution time after each excitation pulse, so that the transverse relaxation time T of each echo signal2Different. At the same time, a shift gradient in both the frequency-encoding and phase-encoding dimensions is applied after each excitation pulse, so that the signals generated by different excitation pulses differ in their position in k-space. In this way, a plurality of echo signals with different transverse relaxation times are obtained in one sample. Then, the sampling signal is input into a trained residual error network after normalization, zero filling and fast Fourier transform to be reconstructed to obtain quantitative T2And (4) an image. The training data for the residual network is derived from the simulated data. Firstly, a template is randomly generated, then an experiment environment is simulated for sampling to obtain an input image of a network, the template is used as a label, and a mapping relation between the input image and an output image is obtained through training. The method provided by the invention can obtain reliable quantitative T in single scanning2And (4) an image.

Claims (6)

1. Single-scanning magnetic resonance quantitative T based on residual error network2An imaging reconstruction method, characterized by comprising the steps of:
1) preparing an experimental sample, placing the sample to be tested on an experimental bed, fixing the sample, and conveying the experimental bed with the sample into a detection cavity of a magnetic resonance imager;
2) opening imager operation software on an operation table of a magnetic resonance imager, firstly carrying out region-of-interest positioning on an experimental sample, and then carrying out tuning, shimming, frequency correction and power correction;
3) introducing a compiled OLED imaging sequence, and setting parameters of the pulse sequence according to specific experimental conditions, wherein the structure of the OLED imaging sequence comprises an excitation pulse with a flip angle of α and a shift gradient G1α flip angle excitation pulseImpact and shift gradient G2Excitation pulse with flip angle of α, shift gradient G3Excitation pulse with flip angle of α, shift gradient G4Refocusing pulse with flip angle of β, sampling echo chain, 4 excitation pulses with flip angle of α, and 4 shift gradients G in frequency coding dimension and phase coding dimension1、G2、G3、G4Shifting 4 echo signals in the center of k space, and performing slice selection by combining 4 excitation pulses with flip angles of α and a slice selection gradient of a slice selection dimension;
4) executing the OLED imaging sequence with the set parameters in the step 3), starting sampling, and executing the next step after data sampling is finished;
5) normalizing, zero filling and fast Fourier transform are carried out on the signals obtained in the step 4), and the signals of the k space are converted into an image domain;
6) generating a random template according to the characteristics of a sample to be tested, carrying out analog sampling on the random template by using analog software to obtain a k-space signal, and then carrying out normalization, zero filling and fast Fourier transform on the signal to obtain training data;
7) building a residual error network model by adopting a TensorFlow deep learning frame and Python, and setting relevant parameters for training; the residual network model comprises: the main structure of the network and the related training parameters, the objective function of the network model is:
wherein N is the number of training images in the same batch, f (-) is a training network, W and b are network parameters, x is an input image, y is a template corresponding to the input imagechangeIs a matrix with a value less than a certain threshold in y set as the threshold, ymaskImage edge information obtained by Canny operator for y;
8) training the network by adopting the data obtained in the step 6) until the network is converged and stable to obtain a trained network model, and then reconstructing the experimental data obtained in the step 5) by utilizing the trained network model to obtain the network modelBy quantitative T2And (4) an image.
2. Single-scan magnetic resonance quantitative T based on residual error network as claimed in claim 12The imaging reconstruction method is characterized in that in step 3), the sampling echo chain is composed of gradient chains respectively acting on a frequency encoding dimension and a phase encoding dimension, the gradient chain of the frequency encoding dimension is composed of a series of positive and negative gradients, and the gradient chain of the phase encoding dimension is composed of a series of gradients of the phase encoding dimension with equal areas.
3. Single-scan magnetic resonance quantitative T based on residual error network as claimed in claim 12The imaging reconstruction method is characterized in that in step 3), before sampling an echo chain, offset gradients are respectively applied to the directions of a frequency encoding dimension and a phase encoding dimension, the area of the offset gradient of the frequency encoding dimension is half of the area of the first frequency encoding gradient, the directions are opposite, the area of the offset gradient of the phase encoding dimension is half of the area of all the phase encoding gradients of the phase encoding dimension, and the directions are opposite.
4. Single-scan magnetic resonance quantitative T based on residual error network as claimed in claim 12The imaging reconstruction method is characterized in that in the step 5), the signals obtained in the step 4) are analyzed, the theoretical derivation is carried out on the nuclear spin evolution under the action of an OLED imaging sequence, and the observed signal intensity after the action of a refocusing pulse with the flip angle of β is in direct proportion to the following expression:
Figure FDA0002304366590000021
wherein the content of the first and second substances,
Figure FDA0002304366590000022
gamma is the spin magnetic ratio of the nuclear spin,
Figure FDA0002304366590000023
the position of the nuclear spins in real space; obtaining the sampling period from the above equationThere are 4 echo signals modulated with different phases, the 4 different modulation phases being theta4、(θ34)、(θ234) And (theta)1234)。
5. Single-scan magnetic resonance quantitative T based on residual error network as claimed in claim 12The imaging reconstruction method is characterized in that in the step 6), the random template is randomly generated in batches by using a computer according to the characteristic distribution of the experimental sample, the random template contains all the characteristics of the experimental sample, and an unstable factor is added to improve the robustness of the network model to an unsatisfactory experimental environment; the instability factors include excitation pulse angle deviation, shift gradient deviation, and noise.
6. Single-scan magnetic resonance quantitative T based on residual error network as claimed in claim 12The imaging reconstruction method is characterized in that in the step 8), the trained network model is suitable for reconstruction of various samples.
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