Runke Wang1, Yu Chen1, Suhao Qiu1, and Yuan Feng1
1School of Biomedical Engineering, Shanghai Jiao Tong University, Shanghai, China
Synopsis
Algorithms providing accurate
estimation of shear modulus and identification of tissue boundary are always
desired for magnetic resonance elastography (MRE). In this study, we proposed a
model-based neural network (MNN) embedding classic direct inversion (DI) and local
frequency estimation (LFE). Convolution layers with Inception-like structure were applied for
preprocessing, while postprocessing was implemented with a U-net structure. Additionally, DI and LFE algorithms were encapsulated as layers
transforming wave images to shear modulus maps. The network performance was tested
using a phantom with an inclusion. Compared with conventional algorithms,
MNN provided modulus estimation with 5-fold higher contrast-to-noise ratio
with clear boundaries.
Introduction
Shear modulus eastimation
is crucial for MR elastography (MRE)1. Conventional algorithms based on the Navier-Stokes equation
provide several strategies for modulus estimation, including direct inversion
(DI), local frequency estimation (LFE), and nonlinear inversion (NLI)2. Recent studies showed deep learning-based methods trained on
simulated data could provide higher robustness and time-efficiency for modulus
estimation3,4. In
addition, it is shown that LFE algorithm combined with a neural network
outperformed the conventional significantly5. In this study, we propose a neural network based on physics models,
aiming to achieve higher precision of modulus estimation and boundaries
identification.Methods
The
proposed network is based on a GAN structure, consisting of a DI and LFE-based
generator, a general discriminator, and an NLI-based discriminator (Figure 1). For
the generator, three blocks with different structures are established, which
are designed for preprocessing, inversion and postprocessing respectively. In
the preprocessing block, convolution layers with different filter sizes and
initial weights are set up and coalesced by the following CNN structure. In the
inversion block, DI and LFE algorithms are applied to achieve the domain
transformation from wave images to stiffness maps, respectively. The results
are then merged by a CNN structure. To calibrate the fused modulus map, a
Unet-based structure is applied in the last stage. The errors of modulus
estimation and boundaries identification are corrected in this block. Finally, the
loss function for the training of the generator is described as:
$$Loss_G =\min_{\theta_0}{ {\left \| f_G(U_{acq},\theta_0) - G_{label} \right \|}_1 }$$
where $$$U_{acq}$$$ is the acquired wave image as network input, $$$G_{label}$$$ is the reference shear modulus map. $$$f_G(\cdot)$$$ denotes the output of the proposed generator, while $$$\theta_0$$$ is the trainable parameters of the generator.
In
addition, two discriminators are applied to improve the calculation accuracy. The
first one is a conventional discriminator adopted from the pix2pix model, which
enhances details in stiffness maps6. In the second discriminator, the simulation
network is a pretrained model which estimates a wave image from a stiffness map
based on the Helmholtz equation and a Unet-based structure. The difference
between the estimated and acquired wave images indicating calculation errors of
the generator is minimized. The discriminators are trained by optimizing the
following loss functions:
$$Loss_D = Loss_{D1}+Loss_{D2}$$
$$Loss_{D1} = \min_{G_{est},\theta_1}{ {\left \| f_{D1}(G_{est},\theta_1) - \mathbf{M} _{fake} \right \|}_2^2 + {\left \| f_{D1}(G_{label},\theta_1) - \mathbf{M} _{real} \right \|}_2^2}$$
$$Loss_{D2} = \min_{G_{est}}{ {\left \| f_{D2}(G_{est}) - U_{acq} \right \|}_2^2}$$
where $$$\mathbf{M} _{fake}$$$ and $$$\mathbf{M} _{real}$$$ are matrices with
single element 0 or 1, respectively. $$$G_{est}$$$ is the stiffness map estimated by the generator. $$$f_{D1}(\cdot)$$$ and $$$f_{D2}(\cdot)$$$ denotes the results of two discriminators.
Over
5000 wave images were simulated by COMSOL as the training dataset, while MRE
data of a gel phantom with a stiffer inclusion was acquired with a 40/60Hz
vibration (Figure 2). For comparison, a pix2pix model was also trained with the
prepared dataset to evaluate the generalization capability of the proposed
method.Results and Discussion
Results
from MNN outperformed that from DI and LFE . The boundary of the inclusion was relatively sharp with the pix2pix model or the proposed method, while noticeable
artifacts covered the target in the results of DI and LFE (Figure 3A). In addition, the RMSE decreased
to 0.025 by over 90%, while the CNR rose up to 46 by 3 times (Figure 3B).
Compared with DI and LFE, the
Dice coefficient of MNN was 10% higher . (Figure 3B). The results indicated that the deep learning-based
methods provided higher
estimation accuracy and better boundary
identification.
In
the experiment of acquired wave images, the results demonstrated the limitation
of the data-driven model (pix2pix). Nonnegligible
artifacts appeared and the wrong
size of the inclusion was estimated (Figure 4A). In contrast,
the proposed method showed better generalization
ability. The CNR coefficient of MNN achieved an
over 30% increase, while the Dice coefficient kept a high level for all test conditions (Figure 4B). Since
the stiffness estimation was
accomplished by DI and LFE
layers, we observed a better
generalization of MNN.Conclusion
In
this study, we proposed a physics model-based neural network for modulus
estimation. DI and LFE algorithms were encapsulated as
layers transforming wave images to shear modulus maps. We were able to achieve improved estimation
accuracy with enhanced generalization capability. Results showed the potential
of MNN in a variety of MRE applications.Acknowledgements
Funding
support from grant 31870941 from National Natural Science Foundation of China
(NSFC) and grant 19441907700 from Shanghai Science and Technology Committee
(STCSM) are acknowledged.References
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