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Regularized Image Domain Split Slice-GRAPPA for Simultaneous Multi-Slice Diffusion MR Imaging
SeyyedKazem HashemizadehKolowri1, Rong-Rong Chen1, Ganesh Adluru2,3, and Edward V. R. DiBella1,2,3
1Electrical and Computer Engineering, University of Utah, SALT LAKE CITY, UT, United States, 2Radiology and Imaging Science, University of Utah, SALT LAKE CITY, UT, United States, 3Biomedical Engineering, University of Utah, SALT LAKE CITY, UT, United States

Synopsis

Simultaneous multi-slice (SMS) acquisition combined with blipped controlled aliasing in parallel imaging is commonly used to accelerate diffusion imaging with single-shot EPI sequences. In this work, we propose a new method, termed regularized image domain split slice-GRAPPA (RI-SSG), which allows an efficient image domain implementation of SSG coupled with total variation regularization to improve the quality of SMS reconstruction. We process two single-shot EPI datasets acquired using diffusion protocol of Human Connectome Project in Aging to evaluate performance of SMS reconstructions. The RI-SSG yields less noisy results than SENSE and SSG in estimating diffusion-weighted images and parametric maps of diffusion.

Introduction

Simultaneous multi-slice (SMS) acquisition combined with blipped controlled aliasing in parallel imaging (CAIPI)[1] is commonly used to accelerate diffusion imaging with single-shot EPI sequences. Sensitivity encoding (SENSE)[2] in image domain and slice-GRAPPA (SG)[1] in k-space are the basis for the most SMS reconstruction methods. In this work, we propose a new method, termed regularized image domain split slice-GRAPPA[3] (RI-SSG), which allows an efficient image domain implementation of SSG coupled with total variation (TV) regularization to improve the quality of SMS reconstruction for the estimation of diffusion-weighted images (DWIs) and parametric maps of diffusion.

Theory

Suppose that a set of multi-coil and multi-slice DWIs with $$$z = 1,\cdots,N_s$$$ simultaneous slices, $$$n=1,\cdots,N_d$$$ diffusion directions, and $$$i=1,\cdots,N_c$$$ coils are acquired. These DWIs which are the IFFT of k-space data are written as
$$m_{i,z,n}(x,y) =c_{i,z}(x,y)s_{z,n}(x,y), \quad (1)$$
where $$$(x,y)$$$ is pixel position, $$$s_{z,n}$$$ is the underlying magnetization image, and $$$c_{i,z}$$$ is the coil sensitivity. Assume that single slices are phase modulated using blipped-CAIPI[1], with superscript $$$(\phi_z)$$$ denoting phase modulation of slice $$$z$$$. Then, for the SMS image we have
$$r_{i,n}(x,y) =\sum_{z=1}^{N_s}m_{i,z,n}^{(\phi_z)}(x,y).\quad (2)$$

The SSG reconstruction using image domain kernels are described with following equations:
$$\widehat{m}_{i,z,n}^{(\phi_z)}(x,y) =\sum_{j=1}^{N_c} k_{i,z,j}(x,y)r_{j,n}(x,y). \quad (3)$$
By substituting (2) into (3) and separating slice of interest $$$z$$$ from other slices, we obtain
$$\widehat{m}_{i,z,n}^{(\phi_z)}(x,y) =\sum_{j=1}^{N_c}k_{i,z,j}(x,y)m_{j,z,n}^{(\phi_z)}(x,y)\\+\sum_{j=1}^{N_c}\sum_{z'=1,z'\neq z}^{N_s}k_{i,z,j}(x,y)m_{j,z',n}^{(\phi_{z'})}(x,y).\quad (4)$$
In the proposed RI-SSG, by assuming that kernels are slowly varying and hence by approximating them as piece-wise constant functions on small local neighborhoods (e.g., rectangular patches), we can solve (4) for kernel coefficients $$$k_{i,z,j}$$$. To control intra-slice artifacts and inter-slice leakages simultaneously, we let the first summation in (4) equal to $$$\widehat{m}_{i,z,n}^{(\phi_z)}(x,y)$$$ and the second summation be zero. For kernel training, we use (4) with b=0 images ($$$n=0$$$).Therefore, RI-SSG kernel training on a local patch $$$\Omega$$$ is written as
$$\begin{pmatrix} \vdots \\ \mathbf{0}\\ \mathbf{m}_{i,z,0}\\ \mathbf{0}\\ \vdots \end{pmatrix} = \begin{pmatrix} \mathbf{m}_{1,1,0} & \dots & \mathbf{m}_{N_c,1,0}\\ \vdots & \ddots &\vdots \\ \mathbf{m}_{1,z,0} & \dots & \mathbf{m}_{N_c,z,0} \\ \vdots & \ddots & \vdots \\ \mathbf{m}_{1,N_s,0} & \dots & \mathbf{m}_{N_c,N_s,0} \end{pmatrix} \begin{pmatrix} {k}_{i,z,1} \\ {k}_{i,z,2} \\ \vdots \\ {k}_{i,z,N_c} \end{pmatrix}\quad (5)$$
where $$$\mathbf{m}_{i,z,0}$$$ is the vectorized form of $$$\{m_{i,z,0}^{(\phi_z)}(x,y)|(x,y)\in\Omega\}$$$. Equation (5) is well conditioned when $$$|\Omega|\times N_s \gg N_c$$$. After kernel training, SMS reconstruction using RI-SSG is formulated as
$$\{\mathbf{s}_{z,n}^{\star}|_{z=1}^{N_s}|_{n=1}^{N_d}\} = \arg\min_{\{\mathbf{s}_{z,n}|_{z=1}^{N_s}|_{n=1}^{N_d}\}} \sum_{n=1}^{N_d}\sum_{z'=1}^{N_s} \left\| \overbrace{\sum_{i}\mathbf{c}_{i,z'}^{*}}^{\text{(C)}}\overbrace{\sum_{j}k_{i,z',j}}^{\text{(B)}}\overbrace{\mathbf{r}_{j,n}}^{\text{(A)}}-\overbrace{\sum_{i}\mathbf{c}_{i,z'}^{*}}^{\text{(C)}}\overbrace{\sum_{j}k_{i,z',j}}^{\text{(B)}}\overbrace{\sum_{z}\mathbf{c}_{j,z}\mathbf{s}_{z,n}}^{(\text{A}')}\right\|_2^2 \\+ \lambda\sum_{n=1}^{N_d}\sum_{z=1}^{N_s} \left( \left\|\nabla_x(\mathbf{s}_{z,n})\right\|_1 + \left\|\nabla_y(\mathbf{s}_{z,n})\right\|_1\right),\quad (6)$$
where $$$\mathbf{s}_{z,n}$$$, $$$\mathbf{c}_{i,z}$$$, and $$$\mathbf{r}_{j,n}$$$ are the vectorized form of $$$\{s_{z,n}^{(\phi_z)}(x,y)|(x,y)\in\Omega\}$$$, $$$\{c_{i,z}^{(\phi_z)}(x,y)|(x,y)\in\Omega\}$$$, and $$$\{r_{j,n}(x,y)|(x,y)\in\Omega\}$$$, respectively. We solve (6) independently for each $$$ \Omega$$$ to jointly estimate all simultaneous single slices. Directions can be reconstructed one at a time, or, with (6) regularization across directions could be included. The first term in (6) enforces data consistency, where (A) denotes acquired SMS images, (A') is the forward model using (1) and (2), (B) is de-aliasing of SMS images using RI-SSG kernels, and (C) is sensitivity-weighted coil combining. The second term imposes TV regularization on estimated single slices. The weighting parameter $$$\lambda$$$ adjusts trade-off between the two constraints.

Methods

Two single-shot EPI diffusion datasets were acquired using a Siemens 3T Prisma scanner from a normal volunteer and a stroke patient with informed consent and IRB approval. The first dataset was acquired without slice acceleration and SMS acquisition with $$$N_s$$$=4 was simulated subsequently. A 32-channel head coil was used to acquire two sessions of the diffusion protocol of Human Connectome Project in Aging (HCP-A)[4] with AP and PA phase-encoding. In each session, we acquired seven b=0, 46 DWIs of b=1500 s/mm$$$^2$$$, and 46 DWIs of b=3000 s/mm$$$^2$$$, with TE = 83.8 ms, TR = 13194 ms, number of slices = 92, voxel size = 1.5$$$\times$$$1.5 $$$\times$$$1.5 mm$$$^3$$$, matrix size = 140$$$\times$$$105, and partial Fourier 6/8. The second dataset was acquired with $$$N_s$$$=4, a 64-channel head coil, TE = 89.2 ms, TR = 3230 ms, number of slices = 23$$$\times$$$4. Other acquisition settings were the same as the first dataset. Each session took ~22 minutes for the first dataset, and ~5 minutes for the second dataset. Whitening of noise and EPI phase corrections were performed prior to SMS reconstructions. A single band non-diffusion scan was used for kernel training and sensitivity estimations. SMS reconstruction was performed using SENSE, SSG, and RI-SSG. For SSG k-space kernel sizes were 7$$$\times$$$7. For RI-SSG we set $$$\Omega$$$ to be 12$$$\times$$$12 patches with stride of 4 and reconstruction results in overlapping areas were averaged. Setting $$$\lambda$$$=10$$$^{-6}$$$, Projection onto Convex Sets (POCS)[5] was used to solve (6) with maximum number of iterations 10, and relaxation parameters of 0.075 and 0.1 for data fidelity and TV regularization, respectively. SMS reconstruction in image domain was evaluated using magnitude DWIs. Prior to model fitting, DWIs were processed using a pipeline consisting of ringing artifact removal, EPI susceptibility distortions correction (topup)[6], eddy current and subject motion corrections[6]. Model fitting was done using a standard approach[7] for DTI, and using accelerated microstructure imaging via convex optimization (AMICO)[8] for neurite orientation dispersion and density imaging (NODDI).

Results

The SMS reconstruction results for the two datasets are shown in Figures 1-3 and Figures 4-5, respectively.

Conclusions

In this work, we proposed a novel regularized image domain SSG method (RI-SSG) for SMS reconstruction that demonstrated less noisy DWIs and more accurate diffusion parametric maps than SENSE and SSG.

Acknowledgements

We thank Dr. Douglas Dean and Dr. Andrew Alexander for providing the diffusion processing pipeline and Darshan Shimpi for his assistance with the processing pipeline.

References

[1] Setsompop K., et al., Blipped-controlled aliasing in parallel imaging for simultaneous multi-slice echo planar imaging with reduced g-factor penalty. Magnetic Resonance in Medicine, 67(5):1210–1224, 2012.

[2] Larkman David J., et al., Use of multi-coil arrays for separation of signal from multiple slices simultaneously excited. Journal of Magnetic Resonance Imaging, 13(2):313–317, 2001.

[3] Cauley S. F., et al., Inter-slice leakage artifact reduction technique for simultaneous multi-slice acquisitions. Magnetic Resonance in Medicine, 72(1):93–102, 2014.

[4] Harms Michael P., et al., Extending the human connectome project across ages:Imaging protocols for the lifespan development and aging projects. NeuroImage, 183:972 – 984, 2018.

[5] Samsonov Alexei A., et al., Pocsense:Pocs-based reconstruction for sensitivity encoded magnetic resonance imaging. Magnetic Resonance in Medicine, 52(6):1397–1406, 2004.

[6] Jenkinson Mark, et al., Fsl. NeuroImage, 62(2):782 – 790, 2012. 20 YEARS OF fMRI.

[7] Garyfallidis Eleftherios, et al., Dipy, a library for the analysis of diffusion MRI data. Frontiers in Neuroinformatics, 8:8, 2014.

[8] Daducci Alessandro, et al., Accelerated microstructure imaging via convex optimization (AMICO) from diffusion MRI data. NeuroImage, 105:32 – 44, 2015.

Figures

Figure 1: Reconstructed DWIs (first dataset) using SENSE, SSG, and RI-SSG for b=1500 s/mm$$$^2$$$ and 3000 s/mm$$$^2$$$. Difference images, normalized root-mean-square-error (nRMSE), and structural similarity index (SSIM) are computed against fully sampled single slices. RI-SSG outperforms SSG and SENSE. While all methods have random-like errors, a darker difference image for RI-SSG is observed. Also, RI-SSG produces less noisy DWIs while preserving fine structural details. For b=3000 s/mm$$$^2$$$, the reconstruction quality degrades for all methods due to reduced SNR.

Figure 2: Estimated DTI maps (first dataset) including fractional anisotropy (FA) and FA-weighted color-coded primary eigenvector of diffusion tensors. The maps are smooth and difference images are relatively dark for all methods. This is because more than 90 DWIs with both AP and PA phase encoding were acquired while the DTI model fitting requires only a small number of diffusion directions. The error patterns are different in that while SSG and SENSE have slightly higher errors in corpus callosum and brain stem areas, the errors for RI-SSG are more uniform in the entire brain.

Figure 3: Estimated NODDI maps (first dataset) including the orientation dispersion index (ODI), intra-cellular volume fraction $$$v_{\text{ic}}$$$, and isotropic volume fraction $$$v_{\text{iso}}$$$. The ODI indicates the extent of dispersion in orientation of neurites, $$$v_{\text{ic}}$$$ measures neurite density, and $$$v_{\text{iso}}$$$ measures the extent of cerebrospinal fluid (CSF) in voxels. The difference images of all three maps are darker for RI-SSG than those of SSG and SENSE. This is more pronounced in areas with higher neurite density and CSF areas.

Figure 4: Estimated DWIs and corresponding DTI maps for the actual SMS acquisition (second dataset). RI-SSG results in less noisier DWIs compared to SENSE and SSG without compromising structural details. For b=3000 s/mm$$$^2$$$, due to reduced SNR, the quality of SMS reconstruction degrades for all methods. The DTI maps are smooth and similar for all three methods. This is consistent with our observation from the simulated SMS acquisition using the first dataset.

Figure 5: Estimated NODDI maps for the actual SMS acquisition (second dataset). For ODI maps, in areas with lower values we see similar estimations from the three methods while in areas with higher ODI differences are more pronounced. For $$$v_{\text{ic}}$$$, the maps are also similar in areas with lower neurite density. In comparison, for denser white matter areas, the $$$v_{\text{ic}}$$$ map from RI-SSG reveals more structural details while maps from SENSE and SSG are saturated. For $$$v_{\text{iso}}$$$ maps, a sharper contrast between CSF and non-CSF areas is observed for RI-SSG.

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