Marina Rakic1, Luis Miguel Lacerda1, Ahmad Beyh2, Pedro Luque-Laguna1, Rachel Barrett2, Francisco De Santiago Requejo1, Steven Williams1, Gareth Barker1, Fernando Zelaya1, and Flavio Dell'Acqua1,2
1Dept. of Neuroimaging, King's College London, London, United Kingdom, 2Dept. of Forensic and Neurodevelopmental Science, King's College London, London, United Kingdom
Synopsis
A well-known dilemma in DW-MRI acquisitions is to
determine the extent to which signal-to-noise ratio (SNR) can be can be
sacrificed in favour of higher spatial resolution on one hand, and in favour of
shorter acquisition time on the other. In this study we quantify the
reproducibility of spherical deconvolution results at 3 spatial resolutions
with and without denoising, as it is still unclear how denoising methods6 affect the uncertainty in subsequent diffusion model fitting and
whether it introduces or improves bias in modelled fibre direction.
PURPOSE
A
well-known dilemma in diffusion-weighted magnetic resonance imaging (DW-MRI)
acquisitions is to determine the extent to which signal-to-noise ratio (SNR) can
be can be sacrificed in favour of higher spatial resolution on one hand, and in
favour of shorter acquisition time on the other. Accelerated acquisition
methods have been introduced to reduce imaging time at a small expense of SNR and
various denoising methods in the pre-processing stage have been also recently suggested.
While several studies have evaluated the effects on signal-to-noise ratio (SNR)
of multiband MRI acquisition for different MRI modalities1–3, fewer studies have focused on the resulting
uncertainty of measures based on DW-MRI data4,5. In
addition, assessing the uncertainty at different spatial resolutions has
received very little attention. In this study we quantify the reproducibility
of spherical deconvolution results at 3 spatial resolutions with and without
denoising, as it is still unclear how denoising methods6 affect the uncertainty in subsequent diffusion model
fitting and whether it introduces or improves bias in modelled fibre direction.METHODS
Two datasets were
acquired with multi-band DW-MRI (MB=3) on a 3T MR750 GE scanner: dataset A contains
360(4x90) diffusion-weighted volumes and dataset B contains 180(2x90), acquired
at an isotropic resolution of 2mm, TE=72.0ms and b=2000s/mm2. Dataset B was also
acquired at 1.7mm and 1.5mm isotropic resolutions, with TE=73.9ms and TE=88.8ms,
respectively. Data was pre-processed using eddy
and topup (FSL software
7), with and without MPPCA denoising
6 performed prior to pre-processing. Residual bootstrap8 was used to obtain 600 synthetic signal realizations (500 considered
the lower limit for robust uncertainty estimation
9). Fibre orientation distribution (FOD) was estimated based on damped Richardson-Lucy
spherical deconvolution model
10. Generalized Jensen-Shannon divergence (JSD)
11 was calculated on 600 bootstrap FODs as a measure of FOD shape
reproducibility. Angular confidence interval of the 1st and 2nd
highest peak direction in each voxel was calculated for CI maps. The angular
bias maps were obtained by finding the angular difference between the highest
peak of FOD estimated on 360 DW volumes compared to 90 directions and denoised
90 directions.
RESULTS & DISCUSSION
JSD in Figure 1 is
an index of uncertainty of the overall FOD profile and it shows that higher
spatial resolution noticeably affects uncertainty of FODs in the 90 directions
dataset where higher JSD indicates lower reproducibility. JSD maps exhibit
spatial patterns similar to well known SNR maps9 of accelerated acquisition
sequences, since the variation in each FOD component is highly sensitive to
noise, which is amplified towards the centre of the brain, i.e. further away
from the receive coil. JSD maps show the reproducibility is efficiently
recovered by denoising the 90 DW directions data (row 2) and is comparable to
180 DW volumes (row 3). This is confirmed by JSD histogram distribution plots
(Figure 1), where the proportion of voxels in lower JSD ranges is higher in
denoised data, with most evident effect of denoising in 1.7mm spatial
resolution.
In Figure 2, CI
maps show increased angular uncertainty with higher spatial resolution. This
effect is more prominent for 90 directions compared to 180. Denoising 90
directions dataset results moderately improves angular confidence interval of
the 1st and 2nd peak. Unlike JSD maps, CI maps appear to follow the pattern of
white matter anisotropy suggesting the peak orientation angular error is
affected by noise as well as anatomical complexity. This could explain why the
effects of denoising are more prominent in reducing the shape uncertainty, and
less obvious in peak direction angular uncertainty.
Both,
JSD and CI, show the uncertainty of 90 DW-volumes dataset is brought closer to
the 180-directions dataset by MPPCA denoising method. Finally Figure 3 shows
the angular bias of 90 directions compared to reference dataset of 360
directions (i.e. more reliable) remains unchanged before and after denoising.
Tying these results together suggests the uncertainty in diffusion model
fitting is efficiently reduced with results comparable to doubling the number
of data, without systematically affecting the angular bias.
CONCLUSION
This study
investigates how increased resolution and denoising can affect uncertainty and
modelled fibre direction, which is an important consideration in both
deterministic and probabilistic tractography methods. The results suggest
denoising does not introduce any additional bias in the angle of modelled fibre
orientation. Given the reduced uncertainty results, if one wants to spend
imaging time in favour of higher spatial resolution, denoising is an efficient
solution and almost necessary. Acknowledgements
No acknowledgement found.References
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