Peizhou Huang1, Brendan Eck2, Ruiying Liu3, Hongyu Li3, Mingrui Yang2, Jeehun Kim2, Xiaoliang Zhang1, Xiaojuan Li2, and Leslie Ying1,3
1Biomedical Engineering, State University of New York at Buffalo, Buffalo, NY, United States, 2Lerner Research Institute, Cleveland Clinic, Cleveland, OH, United States, 3Electrical Engineering, State University of New York at Buffalo, Buffalo, NY, United States
Synopsis
Keywords: MR Fingerprinting, MR Fingerprinting
Motivation: MR fingerprinting (MRF) conventional reconstruction methods need a substantial reconstruction time and memory space. We aim to propose a novel deep-learning method for accelerated MRF reconstruction.
Goal(s): To achieve more accurate quantification reconstruction for T1 and T2 from highly undersampled MRF data.
Approach: A novel training process was also proposed to construct reliable training data with noise-like aliasing artifacts boosted by Transformer network without need to know the structure information.
Results: Experimental results demonstrate that the proposed method achieves more accurate quantification for T1 and T2 than pattern matching and DRONE.
Impact: The proposed method can
generate more accurate quantitative maps for highly accelerated MRF data that
enable clinical use in real application. In addition, the proposed training
process is robust to different structures in the image to be reconstructed.
Introduction
MR Fingerprinting (MRF) [1] represents an
innovative approach to quantitative magnetic resonance imaging, facilitating
the concurrent measurement of various tissue properties. A principal challenge
faced by MRF pertains to pronounced noise and artifacts in image series
generated from highly undersampled data frames which lead to large quantitative
map errors. Several algorithms have been developed to estimate quantitative
maps more accurately [2-5] but suffers reconstruction time and memory space. Recent
studies have explored deep learning techniques to address these challenges [6,7].
For example, DRONE [6] built a 3-layer fully connected neural network to learn
tissue parameters from signal evolutions. However, the improvement is still
limited when the data is highly undersampled. In this study, we propose a
transformer network to learn the tissue parameter, leveraging the long-range dependency
in the time evolution of MRF signals. To train the network more effectively, we
also propose a novel method to generate training data with aliasing artifacts. Experimental results demonstrate that the
proposed method achieves more accurate quantification for T1 and T2 than pattern
matching and DRONE.Method
The MRF sequence uses a 3D Cartesian trajectory with
readout in kx and a variable density circular Cartesian undersampling pattern
in ky-kz [8]. The MRF acquisition consists of 500 time frames that are acquired
using fast imaging with steady-state free precession [9]. All acquisitions used
a matrix size of 96×96×24. In this work, a transformer encoder network [10] is
used to estimate the (T1, T2) values from MRF signals. The transformer
encoder consists of L layers of Multihead Self-Attention (MSA) and Feed Forward
blocks, as shown in Figure 1.
To improve the training process, we also propose a
novel approach to construct training data for the deep network. Different from
DRONE, where random noise was added to the elements in the dictionary to
generate training data, our method can simulate the aliasing artifacts on MRF
signals to make the training data closer to the testing ones. To generate the
training data, first, similar to conventional MRF, a dictionary is generated for 1569 (T1, T2) pairs,
consisting of T1 in the range of 100 to 2000 ms with increments of 50 ms, T2 in
the range of 5 to 200 with increments of 5 ms, and T1 greater or equal to T2. Secondly,
we construct a 3D image, each of whose voxel has its (T1, T2) pair taken
randomly from those in the dictionary.
Thereby, with the corresponding signal evolution for each voxel, we can obtain
500 frames of 3D fully sampled images. Thirdly, each voxel intensity is
multiplied by a proton density value randomly generated from a Gaussian
distribution tailored to the tissue characteristic of the image to be
reconstructed [11,12]. This proton density value is time-independent. In the
fourth step, a 3D Fourier transform is performed for each image frame to simulate
MRF acquisition with the above-mentioned sequence and Cartesian undersampling
in ky-kz. Finally, Zero-filled
3D Fourier reconstruction is performed for all time frames to obtain the MRF time
evolution signal with spatial aliasing artifacts. We then use such MRF signal
contaminated by artifacts as the input of the network, and the corresponding
(T1,T2) pair as the target to train a neural network. It is worth noting that
the random image does not have any spatial structure. The purpose of
constructing an image is to simulate the noise-like aliasing artifacts added to
the clean MRF signals. The training data generation and transformer
architecture are illustrated in Fig. 1.
To evaluate the performance of the trained network,
we
constructed a cylinder phantom and five digital
knee phantoms using the in vivo data from volunteers. The MRF acquisition using
the same above-mentioned sequence was simulated with an acceleration factor of
15. The corresponding MRF signal at each voxel was then put into the trained
neural network to estimate the (T1, T2) values for that voxel. The final
quantitative maps were reconstructed after all voxels were processed. Results
Figures
2 and 3 show the reconstructed T1 and T2 maps of the cylinder
phantom and digital knee phantom, respectively, using direct matching MRF [1], an
FCN (as used in DRONE [6]), and proposed transformer network. The difference
map shows that proposed method can generate more accurate quantitative maps
than pattern matching and is robust to different structures in the image.Conclusion
In this study, we proposed a transform
network and a novel training process for MRF using deep learning. Experimental results demonstrate that our
method can achieve accurate and robust T1 and T2 quantifications than existing
methods.Acknowledgements
This
work was supported in part by NIH/NIAMS
R01AR077452 and NIH/NIA K25AG070321.References
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