Hyunkyung Maeng1 and Jaeseok Park1,2
1Department of Biomedical Engineering, Sungkyunkwan University, Suwon, Korea, Republic of, 2Department of Intelligent Precision Healthcare Convergence, Sungkyunkwan University, Suwon, Korea, Republic of
Synopsis
Keywords: Data Acquisition, Diffusion Tensor Imaging, High resolution 3D DTI
To
propose an accelerated high resolution whole brain DTI and investigate its
feasibility (1.0$$$mm^3$$$ isotropic spatial resolution, imaging time ~ 15
min)
Introduction
Diffusion tensor imaging (DTI)1 is to provide information on anisotropic diffusivity and hence
characterize microscopic architecture. Nevertheless, it is still challenging to
achieve highly well-defined diffusion information in whole brain MRI due to
limited spatial resolution and prolonged imaging time. Whole brain DTI with
single-slab 3D imaging is promising method with high signal-to-noise ratio
(SNR) and no slab boundary artifact, but recent studies have some limitations
in terms of the low spatial resolution (>1 $$$mm^3$$$)2, insufficient whole
brain coverage, and low magnetic field strength (<3T)3. To address these issues, we first propose accelerated diffusion
weighted imaging using single-slab 3D segmented EPI with pseudo-linear random
sampling in k-q space to be capable of reduced scan time. Second, we combine locally
low rank constrained reconstruction to achieve artifact-free diffusion weighted
images by exploiting spatial-angular redundancies. Finally, we investigated the
feasibility of accelerated high resolution whole brain DTI on a 3T scanner
(1.0$$$mm^3$$$ isotropic spatial resolution, imaging time ~ 15 min).Methods
High resolution single-slab 3D EPI
To achieve our aim, a single-slab 3D
segmented EPI with pseudo-linear random sampling in k-q space was developed.
Fig 1 represents a schematic of the proposed single-slab 3D segmented EPI
(diffusion weighted imaging and phase navigator to correct shot-to-shot
variations) (Fig. 1a) and its corresponding incoherent encoding schemes in k-q
space (Figs. 1b, c). Especially, we use a grouped, pseudo-linear undersampling strategy with some physical
constraints which is employed to achieve incoherence and alleviate both
amplitude and phase modulation which occur considerably along the 3D
EPI readout simultaneously. With this grouping sampling schedule, the blip
gradient amplitudes in the ky and kz directions are physically constrained to achieve smooth
signal transition while avoiding abrupt gradient switching. Therefore, variable density
incoherent undersampled k-space can be acquired without significant k-space
modulation and is utilized for robust constrained reconstruction.
Spatial-angular low rank constrained
reconstruction
Missing signals were interpolated by
solving constrained optimization problem with spatial and angular, locally low
rank priors exploiting the fact that the different diffusion contrasts share
the brain structure in images. The formulation of the problem with additional
sparsity prior is:
$$\mathcal{J} \left \{ \mathrm{\mathbf{X}=\left( \mathbf{x}_0,...,\mathbf{x}_{N_d-1}\right)} \right \} = \lambda_p\sum_{p=0}^{N_p-1}\left\|\mathcal{R}_p\left ( \mathbf{X} \right ) \right\|_{*} + \lambda_{\Psi}\sum_{d=0}^{N_d-1}\left\|\Psi\left ( \mathbf{x_d} \right ) \right\|_{1} \\s.t. \quad \mathbf{Y} = \mathbf{F_u}\mathbf{S}\mathbf{P}\mathbf{X}$$
where $$$\mathbf{Y}$$$ denotes the acquired k-space signal; $$$\mathbf{P}$$$ is the phase
map for each shot and each diffusion direction; $$$\mathbf{S}$$$ is the sensitivity encoding
operator; $$$\mathbf{F_u}$$$ is the Fourier transform operator
with undersampling; $$$\mathbf{X}$$$ is the desired artifact-free DWI, which is $$$\mathbf{X} = \mathbf{vect}([\mathbf{x}_0,...,\mathbf{x}_{N_d-1}])$$$; $$$N_d$$$ is the number of diffusion
encoding directions; $$$N_s$$$ is the number of
shots in each DWI; $$$N_c$$$ is the number of coils. This problem is solved using variable
splitting methods under the framework of alternating direction approach.
Experiments
Experimental studies were performed in 15 healthy volunteers
on a 3T whole-body MR
scanner (Prisma, Siemens Healthineers, Erlangen, Germany) using the proposed, rapid
diffusion-weighted MR pulse sequence with a 52-channel head coil. The imaging
parameters were: TE = 64ms, field-of-view (FOV) = 230×200×150 $$$mm^3$$$, matrix size = 220×192×144, readout bandwidth = 1140
Hz/Pixel, echo train length (ETL) = 32, and Flip Angle =90◦. Electrocardiogram synchronization was used to minimize
periodic phase
incoherence
from cardiac motion. Six
diffusion-directions with b=1000s/$$$mm^2$$$ were acquired for DTI
study. In the prospective study, the reduction factor is 5.5 (total scan time:
15min). Additionally,
the 2D single-shot EPI with 1×1×2mm resolution
was acquired for comparison with the proposed method. Fractional anisotropy
maps were generated using FSL4.Results
Fig 2 shows the brain images reconstructed using a
conventional SENSE (without priors) and proposed method in the absence (‘before PC’) and presence (‘after PC’) of inter-shot 3D phase correction. The images with different
diffusion encoding directions were shown in different rows with SSIM. The
proposed method with inter-shot 3D phase correction reveals higher SSIM with
noise suppression. Fig 3 shows the repeated comparison with prospective
undersampled data (R =5.5, total scan time ~ 15min). DWIs, FA maps, and colored
FA maps are shown in different rows. White arrows indicate that the proposed
method can delineate the fine structures in DTI without noise amplification. Finally,
we report the comparison of whole brain DTI colored FA maps acquired using a conventional
2D single-shot EPI and the proposed method. The zoom-in images show the details
of the brain structure, and the proposed method is superior in preserving fine
details.Discussion and Conclusion
We successfully demonstrated that the
accelerated, 3D diffusion tensor imaging can be produced over the whole brain
roughly in 15 minutes without an apparent artifact and amplified noise. We need
to further investigate It is expected that the proposed method widens the
neurological and clinical utility of diffusion tensor imaging, although it
needs to be further investigated.Acknowledgements
This work is supported in part by NRF-2018M3C7A1056887, KMDF-202011B35, and KMDF-202011C20.References
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