Curtis N Wiens1, Chad T Harris1, Andrew T Curtis1, Philip J Beatty1, and Jeff A Stainsby1
1Research and Development, Synaptive Medical, Toronto, ON, Canada
Synopsis
This work examined the feasibility of diffusion tensor
imaging (DTI) at 0.5T, a technique performed almost exclusively at field
strengths of at least 1.5T. 2D
diffusion-weighted axial spin-echo echo-planar imaging and 3D T1
weighted acquisitions were performed in the NIST isotropic diffusion phantom, a
DTI phantom, and 5 healthy volunteers on a head-specific 0.5T MRI system. ADC measurements of the NIST phantom were in excellent
agreement with previously recorded 3T measurements while DTI processing and tractography performed
using Modus Plan was successful in all of the volunteers.
Introduction
Diffusion tensor imaging (DTI) is emerging as an important
tool for the pre-operative planning of neurosurgery1. Incorporation of DTI into neurosurgery has
been shown to offer many benefits including: reduced surgery durations, reduced prevalence
of seizures during surgery, improved surgical outcomes, and improved post-operative
survival2,3. Lower field strengths offer several advantages for
neurosurgical planning using DTI. The
reduction in geometric distortions at lower field strengths result in improved
spatial accuracy of fiber tracts.
Furthermore, a lower field strength offers a more compact system with
less weight and a more compact fringe field which could improve
accessibility. Despite these advantages,
evaluations of DTI at field strengths below 1.5T is extremely limited4. In this work, we leveraged the
high-performance gradient set of a small footprint, head-only MR system5
to demonstrate the feasibility of performing DTI at 0.5T.Methods
All imaging was performed on a head-specific 0.5T MR system equipped
with a 16 channel head coil5. This system contains a high-performance
gradient set with a maximum gradient strength and slew rate of 100mT/m and
400T/m/s per axis respectively.
NIST Isotropic Diffusion Phantom: 2D diffusion-weighted spin-echo
echo-planar imaging (diffusion EPI) were performed on a quantitative diffusion
phantom (High Precision Devices, Boulder, CO).
Parameters for the DTI acquisition were: in-plane resolution: 1.1x1.1mm,
slices =1, slice thickness = 5.0mm, b-value = 800mm/s2, diffusion
directions=24 (plus 4 b=0), TR=15s, TE=139ms, acceleration factor = 2, averages=2,
acquisition time = 14min. In accordance
with their guidelines, the phantom was filled with ice-water at 0°C to account
for the temperature dependence of ADC measurements. ADC measurements of were made by computing
the mean value throughout a circular region of interest within each vial.
DTI Phantom: Diffusion EPI and 3D gradient echo
acquisitions was performed on a DTI phantom previously described by Whitton et
al6. This phantom consists of
flexible fiber bundles with complex geometries including curved, kissing, and
interweaving. Parameters for the diffusion
acquisition were: in-plane resolution: 3.0x3.0mm, slice thickness = 3.0mm, b-value
= 800mm/s2, diffusion directions=60 (plus 8 b=0), TR=4.5s, TE=69ms, acceleration
factor = 2, averages=2, acquisition time = 10.3min. 3D gradient echo acquisition parameters: resolution=1.1x1.1x1.1, flip angle = 26°, TR = 11.2ms, TE =5.2ms.
In vivo: Diffusion
EPI and 3D gradient echo acquisitions were performed on 5 healthy volunteers with
informed consent in compliance with health and safety protocols.
Parameters for the diffusion acquisition were: in-plane resolution: 2.4x2.4mm,
slice thickness = 3.0mm, b-value = 800mm/s2, diffusion directions=52
(plus 8 b=0), TR=5.3s, TE=79ms, averages=2, acceleration factor = 2, acquisition
time = 10.6min. 3D gradient echo with the following
parameters: Resolution=1.1x1.1x1.1, Flip Angle = 26°, TR = 11.2ms, TE =5.2ms.
Reconstruction: Diffusion encoded images, apparent
diffusion coefficient (ADC) and fractional anisotropy (FA) maps were
reconstructed from the DTI acquisitions, correcting for gradient non-linearities7
and performing joint denoising processing8,9. In addition, fiber tractography was computed using Modus PlanTM
(Synaptive Medical, Toronto). This software performed image registration of DTI
and T1 weighted images and fiber tract creation and segmentation.Results
Figure 1 shows a PVP concentration schematic (a), ADC maps (b)
and measured and literature ADC values of the NIST isotropic diffusion
phantom. Good agreement between ADC values was demonstrated
between our measurements at 0.5T and previous measurements made at 3.0T10.
Schematics of the DTI phantom are shown in Figure 2a. Figure 2b shows tractography overlaid on T1-weighted
images for curved and interweaving fiber orientations. For each orientation, excellent alignment between
the tracts and the anatomical images is observed.
Figure 3 shows representative diffusion encoded images of one
subject. Figure 4 shows the ADC, FA, and
RGB of a center cut axial slice across all 5 volunteers. Figure 5 shows tractography results for one
of the subjects. Discussion
The ADC values obtained using the NIST isotropic diffusion
phantom were in good agreement with results obtained in a multi-center study at
3T. This is a promising result that
indicates that a 0.5T scanner can be used to obtain ADC measurements consistent
with higher field systems. However, further investigation would need to be done
to understand how measurement consistency at 0.5T compares to the consistency
observed in higher field systems.
A small pilot study involving 5 healthy volunteers was performed
to further demonstrate feasibility. In
this study, fat saturation preparation pulses were not applied as lower field
strength results in a less drastic chemical shift artifact. The combination of strong gradients and no
fat saturation allowed for improved sampling efficiency when compared to higher
field systems, partially alleviating some of the SNR constraints of a mid-field
system.Conclusions
Phantom and in-vivo results demonstrated that Diffusion Tensor Imaging can be successfully performed at 0.5T and used 1) to compute high quality ADC, FA and RGB maps and 2) by tractography software for fiber tractography and white matter segmentation. Acknowledgements
The authors would like to acknowledge Charles Cunningham and
Rachel Chan for lending us the NIST isotropic diffusion phantom.References
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