4497

Perturbation Robust: Deep Adversarial-Equilibrium Unfolding Network for Magnetic Resonance Image Reconstruction
Tian Zhou1, Zhuoxu Cui1, Kun Shang1, and Dong Liang1
1Shenzhen Institute of Advanced Technology,Chinese Academy of Sciences, Shenzhen, China

Synopsis

Keywords: AI/ML Image Reconstruction, Data Processing

Motivation: Deep unfolding neural networks had attained great success in solving tasks of magnetic resonance image (MRI) reconstruction.

Goal(s): However, minor perturbation in MR signals can result in significant distortions such as some artifacts of the reconstructed images via previous deep unfolding methods.

Approach: This paper proposes a deep equilibrium unfolding network based on adversarial learning to improve robustness of unfolding networks.

Results: Experiment results demonstrate that the proposed method obtains better reconstructed MR images compared with baseline-networks when some artifacts exist in under-sampled multi-channel k-space data.

Impact: We propose a robust method for MRI reconstruction against artefacts in k-space data.

Introduction:

Recently, deep unfolding methods1,2 had been exploited in the field of MRI reconstruction beyond black-box end-to-end networks, due to their better performance and be more explainable. Although these unfolding methods can produce excellent reconstructed MR images, the networks themself are often non-robust3 and lead to severe artifacts despite only some perturbations mixed in the sampled k-space data.
To reduce the artifacts in reconstructed MR images, we propose a deep adversarial-equilibrium learning method. As a consensus, modeling artifacts in MR image is often challenging and inaccurate, therefore, the perturbation which leads to the worst reconstructed result is taken consideration into adversarial learning for improving the robustness to artifacts. Furthermore, the idea of deep equilibrium (DEQ) networks4,5 is used to ensure the convergence of adversarial learning networks.

Method

Traditional unfolding methods in MRI reconstruction can be modeling as following
$$ \min \|\boldsymbol{M} * f f t(\boldsymbol{c s m} * \boldsymbol{x})-\boldsymbol{x}\|_2^2+\lambda R(\boldsymbol{x}) $$
where $$$\boldsymbol{M}$$$ denotes the binary matrix of under-sampling pattern, $$$ f f t$$$ represents operator of Fast Fourier Transform, $$$\boldsymbol{csm}$$$ is a mapping estimation of different channels and transform the image-domain image into a multi-channel estimated image via Hadamard product. $$$ R(\boldsymbol{x})$$$ represents regularization constraint for describing prior of MR images, $$$\lambda$$$ is the penalty of regularizer. $$$\boldsymbol{x}$$$ and $$$\boldsymbol{b}$$$ represents MR image to be reconstructed and under-sampled multi-channel k-space signal respectively.
To solve this model, iteration process in unfolding methods often can be formulated as
$$\boldsymbol{x}^{k+1}=\operatorname{Net}\left(\boldsymbol{x}^k-\boldsymbol{A}^T(\boldsymbol{A} \boldsymbol{x}-\boldsymbol{b})\right)$$
where $$$\operatorname{Net}$$$ can be different flexible network, $$$\boldsymbol{A}$$$ represents forward operator and $$$\boldsymbol{Ax}$$$ can be described as $$$\boldsymbol{M} * f f t(\boldsymbol{c s m} * \boldsymbol{x})$$$ , correspondingly, $$$\boldsymbol{A}^T$$$ denotes the adjoint operator.
Adversarial learning6 plays an essential role in reconstruction against artifacts, specifically, we consider the worst condition in reconstruction, which is formulated as
$$ \min _\theta \max _\varphi\left\|\boldsymbol{A} f_\theta\left(\boldsymbol{A} \boldsymbol{x} ; \boldsymbol{b}+\delta_{\varphi}(\boldsymbol{b})\right)-\boldsymbol{b}\right\|+\left\|f_\theta(\boldsymbol{A} \boldsymbol{x} ; \boldsymbol{y})-\boldsymbol{x}_{g t}\right\| \\ \text { s.t. }\left\|\delta_{\varphi}(\boldsymbol{b})\right\| \leq \varepsilon $$
$$$ f_\theta$$$ represents the reconstruction net, and $$$\delta_{\varphi}$$$ is a neural network to learn the worst perturbation to disrupt the reconstruction result as much as possible.
DEQ can be simply described as $$$\boldsymbol{x}^{\infty} = f\left(\boldsymbol{x}^{\infty}, \boldsymbol{b}\right)$$$, superscript represents the number of iterations, Anderson acceleration is utilized to figure out this the fixed point separately for example in a batch, the mapping relationship from $$$\boldsymbol{x}^{k}$$$ to $$$\boldsymbol{x}^{k+1}$$$ denotes as $$$ f$$$
$$\boldsymbol{x}^{k+1}=\sum_1^m \alpha_i * f\left(\boldsymbol{x}^{k-i+1}, \boldsymbol{b}\right)$$
where $$$\boldsymbol{\alpha}=\min _{\boldsymbol{\alpha}}\|\boldsymbol{G} \boldsymbol{\alpha}\|_2^2$$$, subject to $$$\mathbf{1}^T \boldsymbol{\alpha}=1$$$, and $$$\boldsymbol{G}$$$ is a matrix whose $$$\mathrm{i}$$$-th column is the (vectorized) residual $$$f\left(\boldsymbol{x}^{k-i}, \boldsymbol{b}\right)-\boldsymbol{x}^{k-i}$$$, with $$$i=0, \cdots, m-1$$$. Furthermore, it can also extend the iterations to either a generalized updating form
$$\boldsymbol{x}^{k+1}=(1-\beta) \sum_1^m \alpha_i * \boldsymbol{x}^{k-i+1}+\beta \sum_1^m \alpha_i * f\left(\boldsymbol{x}^{k-i+1}, \boldsymbol{b}\right)$$
according to chain rule, $$$\frac{\partial l}{\partial \theta}=\left(\frac{\partial\boldsymbol{x}^{\infty}}{\partial \theta}\right)^T \frac{\partial l}{\partial\boldsymbol{x}^{\infty}}$$$, and it can be extended as
$$\frac{\partial l}{\partial \theta}=\left(\frac{\partial f_\theta\left(\boldsymbol{x}^{\infty}, \boldsymbol{b}\right)}{\partial \theta}\right)^T\left(\boldsymbol{I}-\left.\frac{\partial f_\theta(\boldsymbol{x}, \boldsymbol{b})}{\partial \boldsymbol{x}}\right|_{x=x^{\infty}}\right)^{-T} \frac{\partial l}{\partial \boldsymbol{x}}$$
We conducted experiments on the public fastMRI dataset7, and randomly select 28 individuals for training, 4 individuals for test. The proposed method can be applicable to different unfolding networks, ISTA-net8 is taken as a basic method for MRI reconstruction in our experiment, and four fully- connected layers is utilized as the perturbation net. Framework of the proposed model is shown in Figure.1.

Result

To assess the robustness of different methods, we added different levels of simulated artifacts9, specifically, from 0 to 15% Frobenius norm of under-sampled k-space signal, to the under-sampled multi-channel MR signals in k-space at 4× acceleration shown in Figure.1. Furthermore, ISTA-net8 (baseline), ISTA-net with the worst perturbation adversarial learning, ISTA-net with DEQ architecture, and ISTA-net with both two modules are compared in the experiment, shown in Figure.2 and Figure.3, to display the improvement of quality and robustness of reconstructed MR image brought by adversarial learning and DEQ architecture. Furthermore, we add results of simple IFFT reconstruction by fully-sampled k-space signal with different levels of simulated artifacts to eliminate the influence of the sampling pattern in Figure.2.

Conclusion

The result demonstrates that the proposed method, which considers the worst perturbation in k-space, improve the performance both in quality and robustness of reconstructed MR images.

Acknowledgements

This work was partially supported by the National Natural Science Foundation of China (61871373, 62271474, 81830056, 61771463, U1805261, 81729003, 81901736, 12026603, 62206273 and 81971611, 12001180), the National Key R&D Program of China (2023YFB3811400),the Strategic Priority Research Program of Chinese Academy of Sciences (XDB25000000 and XDC07040000), the High-level Talent Program in Pearl River Talent Plan of Guangdong Province (2019QN01Y986), the Key Laboratory for Magnetic Resonance and Multimodality Imaging of Guangdong Province (2023B1212060052), the Science and Technology Plan Program of Guangzhou (202007030002), the Key Field R&D Program of Guangdong Province (2018B030335001), the Shenzhen Science and Technology Program, Grant Award (JCYJ20210324115810030), and the Shenzhen Science and Technology Program (Grant No. KQTD20180413181834876, and KCXF20211020163408012).

References

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[2] D. Liang, J. Cheng, Z. Ke, and L. Ying, “Deep Magnetic Resonance Image Reconstruction: Inverse Problems Meet Neural Networks,” IEEE Signal Process. Mag., vol. 37, pp. 141–151, 2020, doi: 10.1109/MSP.2019.2950557.

[3] V. Antun, F. Renna, C. Poon, B. Adcock, and A. C. Hansen, “On instabilities of deep learning in image reconstruction and the potential costs of AI,” Proc. Natl. Acad. Sci. U. S. A., vol. 117, no. 48, pp. 30088–30095, 2020, doi: 10.1073/pnas.1907377117.

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[6] D. Gilton, G. Ongie, and R. Willett, “Deep Equilibrium Architectures for Inverse Problems in Imaging,” IEEE Trans. Comput. Imaging, vol. 7, pp. 1123–113file:///C:/Users/zhoutian/Desktop/ismrm/kn, 2021, doi: 10.1109/TCI.2021.3118944.

[7] F. Knoll et al., “FastMRI: A publicly available raw k-space and DICOM dataset of knee images for accelerated MR image reconstruction using machine learning,” Radiol. Artif. Intell., vol. 2, no. 1, 2020, doi: 10.1148/ryai.2020190007.

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Figures

Figure.1 Framework of Deep Equilibrium-Adversarial Unfolding Network

Figure.2 Reconstructed MR images and error mapping via different methods with the increase of simulated artifacts.

Figure.3 Values of nmse/psnr/ssim via different methods with the increase of simulated artifacts.

Proc. Intl. Soc. Mag. Reson. Med. 32 (2024)
4497
DOI: https://doi.org/10.58530/2024/4497