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Accelerated Multi-Echo Gradient Echo Imaging using Locally-Low Rank Regularization
Mirco Grosser1,2 and Tobias Knopp1,2
1Section for Biomedical Imaging, University Medical Center Hamburg-Eppendorf, Hamburg, Germany, 2Institute for Biomedical Imaging, Technical University Hamburg, Hamburg, Germany

Synopsis

Reconstruction methods for multi-contrast MRI often employ a low-rank constraint to reconstruct images from highly undersampled data. For multi-echo gradient echo sequences such a constraint is hard to impose due off-resonance-induced oscillations of the time signals. In this work we show that spatio-temporal correlations can be exploited efficiently using locally low rank regularization. Based on this observation we develop a locally-low rank regularized reconstruction scheme and test it on a multi-echo gradient echo dataset of a human brain. In our tests the proposed method shows significantly improved image quality compared to regular compressed sensing reconstructions.

Introduction

Multi-echo gradient echo (MEGRE) sequences are a common tool in MRI with a variety of applications such as R2*- and quantitative susceptibility mapping (QSM). For other multi-contrast MRI sequences, strong acceleration can be achieved by exploiting correlations between the temporal signals for different tissue parameters. This translates into a low-rank constraint for the Casorati matrix of the images to be determined [1]. As a matter of fact, aforementioned low rank-property does not hold for MEGRE images due to the B0-induced time evolution of the image phase. Here we demonstrate that spatio-temporal correlations can be exploited when considering local image patches. As a result, we formulate image reconstruction as a locally low rank regularized (LLR) inverse problem [2,3] and show its effectiveness in comparison to standard compressed-sensing reconstructions.

Methods

In MEGRE MRI , the magnitude signal in a given voxel shows an approximately exponential decay. However, B0-inhomogeneity leads to a temporally oscillating phase, which makes it hard to find a low rank representation for the different signal evolutions in the image series. On the other hand, voxels within a small patch typically experience similar values of inhomogeneity, which makes it possible to find a low rank representation. To demonstrate this, we used the in-vivo brain dataset (measured on a GE scanner) accompanying the MEDI toolbox [4,5]. Fig. 1 shows the normalized singular values of both the global Casorati matrix and the Casorati matrix for two image patches. The former also suggests that a representation with lower rank can be found for signals similar to the magnitude signal. Based on those observations, we formulate the following reconstruction problem
$$ \underset{\mathbf{x}}{\operatorname{argmin}} \parallel \mathbf{y}-\mathbf{E}\mathbf{\Phi}\mathbf{x} \parallel_2^2 + \lambda\sum_{\mathbf{r}} L(R_{\mathbf{r}}\mathbf{x})$$
Here $$$\mathbf{E}$$$ denotes the signal encoding operator and $$$\mathbf{y}$$$ denotes the measured k-space signal. Analogously to [1], $$$R_{\mathbf{r}}$$$ extracts blocks around location $$$\mathbf{r}$$$ and reshapes them into the columns of the associated Casorati matrix. As a surrogate of the rank, $$$L$$$ denotes the logdet penalty of the singular-values, which was proposed in [4]. Although being non-convex the latter was observed to show superior results compared to the convex nuclear norm. Finally, we include the diagonal operator $$$\mathbf{\Phi}$$$ which multiplies each entry in $$$\mathbf{x}$$$ with an estimate of the image phase for the associated voxel and echo. As discussed before, this leads to a more compact representation of the spatio-temporal signals. In summary, the proposed method starts by solving (1) for $$$\mathbf{\Phi}_0 = \mathbf{1}$$$. Then the solution can be refined by updating the phase estimate $$$\mathbf{\Phi}_1$$$ and solving the new form of problem (1). In order to test the proposed method, the complex-valued brain dataset used before was Fourier transformed into k-space. The data was retrospectively undersampled using a variable density poisson disk pattern with a fully sampled calibration area of size 24x24. Finally, the multi contrast image series was reconstructed using the proposed method with and without updating the phase estimate. For comparison we also performed a compressed sensing (CS) reconstruction with ℓ1 regularization in the Wavelet domain.

Results

Fig. 2. shows the reconstructed magnitude images for the first and the last echo of the image series. The Wavelet-based CS reconstruction shows blurring and severe artifacts. For the proposed method, the reconstruction quality is increased. This is also reflected in the normalized root mean squared deviation (NRMSD), which is shown in the figure for each contrast. Incorporating the image phase into the imaging operator, leads to a further reduction in NRMSD and a reduced amount of perceivable noise.

Discussion

Our results demonstrate that LLR regularization is a powerful prior for the reconstruction of MRGRE image data. This can be justified by the fact that the underlying B0 map typically has a smooth structure. As a consequence neighboring voxels show a similar oscillatory behavior. By incorporating a prior phase estimate into the imaging operator, the images to reconstruct show more resemblance to the magnitude signals, which explains the additional increase in reconstruction quality. Note that the reconstruction problem (1) can be solved efficiently using ADMM [6]. Moreover, the successive reconstructions can be initialized with the previous image estimate. Thus, obtaining a phase estimate only leads to a moderate increase in reconstruction time.

Conclusion

A new image reconstruction was developed, which exploits signal correlations through LLR regularization. In particular, this method is suited for MEGRE sequences, where the image signals are no longer contained in a global low rank subspace. In comparison to standard CS methods, it allows successful image reconstruction at larger undersampling factors. Thus, the proposed method has the potential to further accelerate MRI applications such as R2*-mapping and QSM.

Acknowledgements

No acknowledgement found.

References

[1] Velikina, J., et al., MRM, 70(5), 1263-1273, (2012)

[2] Zhang, T., et al., MRM, 73(2), 655-661, (2015)

[3] Tamir, J., et al., MRM, 77(1), 180-195, (2017)

[4] Wang, Y., & Liu, T. , MRM, 73(1), 82-101, (2015)

[5] http://pre.weill.cornell.edu/mri/pages/qsmreview.html

[6] Boyd, S. et al., Foundations and Trends® in Machine Learning, 3(1), 1-122,(2011)

Figures

Fig 1. Magnitude of the first and the 9th echo of the MEGRE brain image series (a). (b) shows the singular values for the Casorati matrix formed from the complex valued signals (top) and from the modulus of the signals (bottom). The same quantities are shown for the two image patches marked in (a)

Fig 2. Reconstructed images using Wavelet ℓ1-regularization (left column), the proposed LLR regularized method (middle column) and the proposed LLR regularized method with phase adaption (right column). The numbers in each image denote the NRMSD with respect to the fully sampled reference.

Proc. Intl. Soc. Mag. Reson. Med. 28 (2020)
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