Haipeng Xu1, Tao Gong2, and Lin Chen1
1Department of Electronic Science, Fujian Provincial Key Laboratory of Plasma and Magnetic Resonance, School of Electronic Science and Engineering, National Model Microelectronics College, Xiamen University, Xiamen, China, 2Departments of Radiology, Shandong Provincial Hospital Affiliated to Shandong First Medical University, Jinan, Shandong, China
Synopsis
Keywords: CEST / APT / NOE, CEST & MT
Motivation: CEST MRI requires the collection of multiple saturated images with different saturation offsets, resulting in prolonged scan times, which hinders its clinical applications.
Goal(s): we aim to reduce the scan time of CEST MRI by recovering the undersampled Z-spectrum to full-sampling counterpart using data-driven Z-spectral compressed sensing method.
Approach: The modified U-Net was employed for Z-spectral recovery. Training data were generated using Bloch equation. Numerical simulations and in vivo experiments on rat brains were conducted to validate the proposed method.
Results: The results demonstrate that our method outperformed conventional interpolation methods, and threefold undersampling rate can be achieved without discernible degradation in quantification.
Impact: The
proposed method can efficiently reduce the scan time of CEST MRI, potentially
facilitating its clinical applications.
Introduction
CEST
MRI is a versatile technique that provides valuable diagnostic insights for
various diseases, including tumors, neurodegeneration diseases, and ischemic
stroke. Conventional CEST experiments acquire multiple saturated images with
different saturation offsets, leading to prolonged scan time, which hinders its
clinical applications. Furthermore, the long scan time also makes CEST MRI
vulnerable to motion artifacts and degrades quantification reliability.
Various
methods have been developed to accelerate CEST imaging, including fast readout1,
parallel imaging2, and compressed sensing3 (CS) in the
k-space domain. Recently, exploiting sparsity in the Z-spectrum domain has
attracted significant attention in accelerating CEST MRI4. In this
study, we proposed a data-driven deep learning method, named Z-spectral CS for short, to fully exploit the sparsity
in the Z-spectrum domain and recover the undersampled Z-spectrum to its
full-sampling counterpart. The proposed method was validated through numerical
simulations and in vivo rat brain experiments.Methods
The
neural network used in this study is a modified U-Net, consisting of an
encoder-decoder network with multi-scale skip connections and 1D convolution,
as shown in Fig. 1. The input and output are undersampled Z-spectrum and fully
sampled Z-spectrum, both with the same dimension size of 1 × W, where W
refers to the number of frequency offsets. For the input, missing data were set
to zero. We adopted the modified U-Net with four scales. Each scale features a
skip connection between the downsampling and upsampling operations. The channel
numbers for the four scales are C, 2C, 4C, and 8C,
respectively, corresponding to feature maps with dimensions of C × W,
2C × W/2, 4C × W/4, and 8C × W/8.
In this study, we adopted C=64 and W=51.
The training data were generated using the
five-pool Bloch-McConnell equation (i.e. bulk water, NOE, Amide, MT, and
creatine) with frequency offsets ranging from -5 to 5 ppm. Various combinations
of different experimental parameters, including concentration, exchange rate,
T1, and T2, saturation
power and duration, and different magnetic field strength, were considered. The
in vivo rat experiments were performed on a 9.4T Bruker scanner. The linear and
pchip interpolation methods, accomplished by Matlab's built-in functions, were
performed for comparison.Results and Discussion
In
neural network training, the Adam optimizer is employed to minimize the mean
squared error (MSE) loss function, the neural network was converged after 80
epochs.
The
performance of the proposed method with different acceleration factors was
demonstrated in Fig. 2. From the results, Z-CS outperformed the other two
comparison methods in both root mean square error (RMSE) and difference
evaluation. The interpolation methods show inferior performance around 0 ppm due to the significant
signal variation in this region. This is because these methods rely on the
local smoothness assumption, which becomes invalid around 0 ppm.
In contrast, Z-CS recovered the full Z-spectrum with better fidelity even
around 0 ppm, indicating that the neural network successfully learned the prior
information embedded in the Z-spectrum. Similar results were also observed in
the in vivo rat brain experiment with an acceleration factor of R=3, as shown
in Fig. 3.
The five-pool Lorentzian fitting was
performed to quantify the Z-spectrum recovered by different methods, and the
results are shown in Fig. 4. The difference maps, along with statistical
analyses, are presented in Fig. 5. The results indicate that our method yields
satisfactory quantification accuracy with an acceleration factor of R=3. The modified U-Net
is known for its ability to recover missing data by leveraging features
extracted from different levels, making it well-suited for Z-spectral
compressed sensing, as demonstrated in this study. As a data-driven method, the
accuracy of the proposed method highly depends on the training data. In this
study, the five-pool Bloch-McConnell equation was adopted to generate training
data, which is sufficient for the conditions of this study. In more complex
situations, the use of the Bloch-McConnell equation with additional
exchangeable pools is recommended.Conclusion
In
this study, a data-driven Z-Spectral compressed sensing based on a modified
U-Net was proposed to accelerate CEST MRI without discernible compromise in
quantification accuracy, potentially facilitating the clinical applications of
CEST MRI.Acknowledgements
This work is supported by the National Natural
Science Foundation of China, Grant/Award Number:82302151; Shenzhen Science and
Technology Program, Grant/Award Number: JCYJ20220818101213029; Fujian Province
Science and Technology Project, Grant/Award Number: 2022J05013; Xiamen
University Nanqiang Outstanding Talents Program.References
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