Paul Dubovan1,2, Lars Kasper3, Kamil Uludag3,4, and Corey Baron1,2
1Medical Biophysics, Western University, London, ON, Canada, 2Center for Functional and Metabolic Mapping, Robarts Research Institute, London, ON, Canada, 3Techna Institute, University Health Network, Toronto, ON, Canada, 4Medical Biophysics, University of Toronto, Toronto, ON, Canada
Synopsis
Spiral diffusion images are known to
suffer from image distortions due to the enhanced sensitivity to magnetic field
inhomogeneities. Application of parallel imaging to accelerate readout times,
and inclusion of robust B0 field maps are two techniques that
generally contribute to spiral image improvements. In this work, the impact of
field map resolution and acceleration factors are investigated to identify
acquisition parameters that optimize image quality. A moderate acceleration
factor (3 or 4) coupled with a field map on the order of the imaging resolution
(1.5 mm in-plane) provided the best trade-off between geometric accuracy, blurring
reduction, and noise amplification.
Introduction
Single-shot spiral MRI is a rapid acquisition technique that offers
drastically shorter achievable echo times (TE) compared to EPI, which minimizes
signal loss from T2 decay leading to higher signal-to-noise ratios
(SNR)1. This can be particularly advantageous for diffusion MRI (dMRI)
which generally experiences lower SNR due to signal attenuation of moving water
molecules, and long diffusion encoding periods that prolong TE2. A limitation
which prevents the technique’s implementation in clinical practice is its
sensitivity to magnetic field inhomogeneities3, but recent work
using field monitoring with external probes and an expanded encoding model have
demonstrated the feasibility of high-quality spiral dMRI4. Static
field (B0) maps are essential in single-shot spiral brain imaging,
particularly at high field strengths, where images may suffer from
susceptibility-induced distortions caused by the paranasal sinuses5.
It is possible that field maps may be acquired at relatively low resolution
given the typically slow spatial variation of static field offsets, but the
trade-offs between B0 mapping resolution and single-shot spiral
reconstruction performance are not well understood. At the same time, the
deleterious effect of B0 inhomogeneity can be mitigated using undersampling.
In this work, we investigate the effects of varying B0 map
resolutions and acceleration factors on single-shot spiral dMRI image quality. Methods
A healthy patient was scanned on a 7T head-only MRI (Siemens). Single-shot spiral acquisitions
were performed at parallel imaging acceleration factors (R) of 2,3,4 and 5. A
single b=0 s/mm2 scan and 6 diffusion acquisitions using b = 1000
s/mm2 were acquired with each acceleration factor. Field maps were
acquired at 3 mm, 2 mm and 1.5 mm isotropic resolution. Remaining imaging parameters
were as follows: in-plane resolution = 1.5 x 1.5 mm2, 3 mm slice
thickness, TE = 33 ms, TR = 2500 ms, FOV = 192 x 192 mm2. To correct
for eddy current effects appearing during image acquisition, the spatially
varying field dynamics up to third order in space were measured after image
acquisitions using a field monitoring system (Skope) consisting of 16
transmit/receive 19F field probes, and were integrated into an
iterative expanded encoding model-base reconstruction with 30 iterations. The
pseudo multiple replica method was implemented to evaluate the noise
amplification for each R and B0 map resolution6.
Synthetic uncorrelated Gaussian noise was generated and added to the respective
k-space raw data prior to image reconstruction and repeated 100 times to
produce a stack of image replicas. Normalized noise standard deviation (SD) maps
were produced by calculating the SD of each pixel throughout the stack of images
and dividing the maps by the square root of the acceleration factor, which
accounts for the SNR loss due to fewer acquired signals6.Results
Increasing
the B0 map resolution is seen to make the largest impact near the
cortical surface (Figure 1). In Figures 2 and 3, increasing the B0
map resolution reduces blurring and artefacts for all acceleration rates.
Increasing R generally decreases blurring and decreases B0 artefacts
near the edge of the brain, particularly near the edge of the left frontal lobe
(top right); however, at extremely high acceleration, residual aliasing
artefacts are introduced near the center of the brain. Mean noise SD values
show slightly reduced noise amplification with larger acceleration factors, and
a generally low dependence on field map resolution (see Fig. 4). Discussion
The
higher resolution field maps lead to a reduction in blurring that is pronounced
for the acquisitions with longer readout times. For low resolution B0
maps, increasing acceleration can partially ameliorate artefacts and blurring,
but the best image quality is observed for the B0 resolution
matching the imaging resolution (1.5 mm) and moderate acceleration (R = 3 to
4). Notably, the B0 map resolution has no impact on blurring from T2*
decay during the readout, which is evidenced by the decreased blurring for the
highest B0 map resolution as the R is increased. At the highest
accelerations, residual undersampling artefacts become noticeable; however, the
degree of artefacts is much lower than what would be expected from EPI with
similar R, stemming from the two-dimensional nature of the aliasing point
spread function for spirals7.
Although visibly
reduced when using higher undersampling and high-resolution field maps, the
dark stripes present in the left frontal lobe remain an issue for all cases. The
field maps (Fig. 1) show excessive field offsets in the same region, which
suggests that the encoding matrix is ill conditioned in that region. The
unexpected trend for the noise SD to slightly decrease with increasing R is due
to the use of the same number of iterations in the reconstruction for all R.
This approach was used because there is no clear objective approach that we
know of to choose the number of iterations. Nevertheless, the number of
iterations balances the trade-off between residual artefacts and noise
amplification, and higher numbers of iterations are required as the encoding
matrix becomes less well conditioned with higher R. Alternatively, Tikhonov
regularization with a high number of iterations could be used to balance this
trade-off, but this requires lengthy reconstruction times. All things
considered, the results suggest a weak dependence of noise amplification on R,
in agreement with other recent findings7. Acknowledgements
This work has been supported by the Natural Sciences and Engineering Research Council of Canada (NSERC) and the Ontario Graduate Scholarship (OGS) Program.References
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