Magnetic Resonance Spectroscopic Imaging (MRSI) is a valuable tool to characterize metabolic concentrations and changes in several spatial locations in a single recording. However, the long acquisition time of conventional three-dimensional (3D) MRSI limits its practical application. Non-uniformly sampled 3D echo planar spectroscopic imaging (EPSI) has been proposed to accelerate the scan time, combined with compressed sensing (CS) to retain reconstruction fidelity. We apply the novel approach of reconstructing 3D EPSI data by applying TV, Wavelet-$$$\ell_{1}$$$, and TV + Wavelet-$$$\ell_{1}$$$ CS-based regularization on both the combined spectral and two undersampled spatial dimensions. These three reconstruction methods were evaluated in both simulated and in retrospectively undersampled data of a brain phantom.
CS reconstruction was performed using the Split-Bregman7 algorithm with three different types of sparsifying transforms applied on the y-z-f space for each point along the readout direction x, namely TV-, Wavelet-$$$\ell_{1}$$$-, and TV+Wavelet-$$$\ell_{1}$$$-based regularization. In addition to spatial sparsity, this approach exploits the increased sparsity available in the spectral domain with respect to the TV and/or wavelet transforms. The minimization is cast as $$ \min_{u} \mu\frac{1}{2}∥Fu−y∥^{2}_{2}+λTV(u)+γ∥Wu∥_{1} \quad \text{subject to} \quad ∥Fu−y∥^{2}_{2}<σ^{2}$$ where $$$ F $$$ is the undersampled Fourier transform, $$$ u $$$ is the desired data in y-z-f space, $$$ y $$$ is the acquired data in ky-kz-t, W is the wavelet transform (Daubechies 4, level 5), and $$$ \sigma $$$ is an estimate of the noise. The parameters $$$ \lambda $$$ and $$$ \gamma $$$ are set to zero to remove the $$$ TV $$$ or $$$ \|W \cdot \|_{1} $$$ regularization terms, respectively. Each reconstruction was run for 300 iterations or until the stopping criterion was satisfied. The regularization parameters were scaled according to the undersampled data, with the ratios $$$\mu:\lambda:\gamma \approx 1:0.01:0.01. $$$
A 3D EPSI sequence was used to acquire a fully sampled brain phantom data set on a 3T scanner with the following parameters: FOV = 240×240×120 mm3 , matrix = 32×32×8, spectral bandwidth = 1190 Hz, number of spectral points = 256, TE = 41ms, TR = 1.5s, number of averages = 8. This data was retrospectively undersampled along the spatial ky-kz dimensions at acceleration factors of 2x, 3x, 4x, and 5x. A 3D virtual phantom was created using a 32×32×8 Shepp-Logan spatial profile, in which each voxel contained a 256-length FID generated using the GAMMA library8. Simulated metabolites included NAA, Cr3.0, Ch, Glx, mI, and Cr3.9. This virtual data was undersampled at 2x, 3x, 4x, and 5x.
Reconstruction performance was quantified using the normalized root-mean-square error (nRMSE) of metabolite concentrations and ratios, and was qualitatively evaluated with comparisons of spatial maps and spectra.
This study evaluates the novel approach of reconstructing 3D EPSI data by applying the TV and wavelet transforms on the three-dimension spectral-spatial set y-z-f, in which y-z are the undersampled dimensions. Results from the reconstructed spectra, metabolite ratios, and spatial metabolite maps generally indicate that Wavelet-$$$\ell_{1}$$$ regularization performs less optimally than regularization involving the TV term. As seen in Figures 3 and 4, the combination of TV + Wavelet-$$$\ell_{1}$$$ leads to lower nRMSE values in comparison to TV alone, while Wavelet-$$$ \ell_{1} $$$ regularization retains higher nRMSE's. The spectral quality and accuracy of metabolite maps are consistent with these trends. Both TV and TV + Wavelet-$$$\ell_{1}$$$ methods produce similar results, though the latter is more robust to higher acceleration factors, as indicated in Figures 3 and 4.
1. Mansfield P. Spatial mapping of the chemical shift in NMR. Magnetic Resonance in Medicine, 1984; 1(3): 370-386.
2. Posse S. et al. High Speed 1H Spectroscopic Imaging in Human Brain by Echo Planar Spatial-Spectral Encoding. Magnetic Resonance in Medicine, 1995; 33(1):34-40.
3. Furuyama JK, Wilson NE, Burns BL, Nagarajan R, Margolis DJ, Thomas MA. Application of Compressed Sensing to Multidimensional Spectroscopic Imaging in Human Prostate. Magnetic Resonance in Medicine, 2012; 67:1499-1505.
4. Cao P, Wu E. Accelerating Phase-Encoded Proton MR Spectroscopic Imaging by Compressed Sensing. Journal of Magnetic Resonance Imaging, 2015; 41:487-495.
5. Askin NC, Atis B, Ozturk-Isik E. Accelerated phosphorus magnetic resonance spectroscopic imaging using compressed sensing. 2012 Annual International Conference of the IEEE Engineering in Medicine and Biology Society, pp. 1106-1109, IEEE, 2012.
6. Geethanath S. et al. Compressive Sensing Could Accelerate 1H Metabolic Imaging in the Clinic. Radiology, 2012; 262(3): 985-994.
7. Goldstein T, Osher S. The Split Bregman Method for L1-Regularized Problems. SIAM J. Imaging Sciences, 2009; 2(2):323-343.
8. Smith S, Levante T, Meier BH, Ernst RR. Computer simulations in magnetic resonance. An object-oriented programming approach. Journal of Magnetic Resonance, Series A 1994; 106:75-105.