Claudia Calcagno1,2, Bram Coolen3, Bei Zhang1,2, Gilles Boeykens 3, Philip Robson1,2, Venkatesh Mani1,2, Aart J Nederveen3, Willem Mulder1,2, and Zahi Fayad1,2
1Department of Radiology, Icahn School of Medicine at Mount Sinai, New York, NY, United States, 2Translational and Molecular Imaging Institute, Icahn School of Medicine at Mount Sinai, New York, NY, United States, 3Department of Radiology, Academisch Medisch Centrum, Amsterdam, Netherlands
Synopsis
Accurate morphological
measurements and classification of carotid plaques require imaging with high
spatial resolution, and may benefit from the increased signal intrinsically
available on ultra-high field (7T) magnets. Several studies have already investigated
carotid vessel wall imaging at 7T and compared it with state-of-the-art 3T
protocols. These initial investigations have focused on 2
dimensional (2D), multi-slice imaging. Better than this approach, 3 dimensional
(3D) vessel wall imaging allows characterizing extensive vascular territories while
minimizing partial volume artifacts in plaque-prone regions, such as the
carotid bulb and bifurcation. Here, we demonstrated the feasibility of performing 3D carotid vessel wall imaging on a whole body 7T clinical magnet
using a custom made carotid coil. PURPOSE
Accurate morphological
measurements and classification of carotid atherosclerotic plaques require imaging with high
spatial resolution, and may therefore benefit from increased signal-to-noise
ratio (SNR) intrinsically available on ultra-high field (7T) systems
1-3. Several studies have already investigated
carotid vessel wall imaging at 7T and compared it with state-of-the-art 3T
protocols
1-3. These initial investigations have focused on 2D multi-slice
imaging. Better than this approach, 3D vessel wall imaging allows characterizing
extensive vascular territories while minimizing partial volume artifacts in
plaque-prone regions, such as the carotid bulb and bifurcation
4-5.
Here, we present our initial experience of 3D carotid vessel wall imaging on a
whole body 7T clinical magnet using a custom made carotid coil.
METHODS
MRI acquisition: 5 volunteers were imaged on a 7T whole body scanner (Siemens
Magnetom) using a dedicated, custom designed, 8 channel carotid coil (Figure 1). The coil consists of two
pads that lie on the left and right side of the neck. Each pad contains 2
transmit elements and 4 receive elements. After the acquisition of scout
images, a 3D time-of-flight (TOF) non contrast-enhanced, bright blood sequence
was acquired to identify the carotid arteries. Subsequently, black blood vessel
wall imaging was performed using 3D weighted SPACE (Sampling Perfection with
Application optimized Contrast using different flip angle Evolutions) with 5 different
acquisition settings as detailed in Table
1. Other relevant imaging parameters common to all 3D SPACE acquisitions
were: repetition time (TR) 1500 ms; echo time (TE) 100-106 ms; bandwidth
528-531 Hz/pixel; number of averages, 2; partial Fourier 6/8; echo train
duration: 200ms. No parallel imaging was used.
MRI analysis: Inner and outer vessel wall contours were delineated on axial slices
using Osirix software (http://www.osirix-viewer.com). Coronal acquisitions were reformatted in the axial
plane before analysis. An additional noise
region outside of the neck was also drawn. SNR in the vessel wall was
calculated as the signal intensity in the wall divided by the standard
deviation of the noise region in the same axial slice. Vessel wall to lumen
contrast-to-noise ratio (CNR) was calculated as the difference between vessel
wall and lumen SNR.
Statistical analysis: After checking for data normality (d’Agostino
and Pearson omnibus test), SNR and CNR measurements were compared among
different acquisitions using non-parametric tests. A Wilcoxon paired test was used to compare
SNR and CNR between 0.8 mm3 and 0.6 mm3 coronal T2W SPACE
with isotropic resolution, while a Friedman paired test was used to evaluate
difference between the 3 axial acquisitions (0.6, 0.5 and 0.4 mm2 with
anisotropic voxels). p values less than 0.05 were considered significant.
RESULTS
Images from all subjects
and all acquisitions were of sufficient image quality for further analysis.
Figure 2 shows curved multi-planar
reconstructions from the 0.8 and 0.6 mm
3 coronal acquisitions with
isotropic voxels, with zoomed in view of the carotid vessel wall at the bottom
(orange star indicates the vessel lumen). Figure
3 shows representative images from axial acquisitions (A, 0.6 mm
2; B,
0.5 mm
2; C, 0.4 mm
2),
and depicts examples of vessel wall (orange circle), lumen (green circle) and
noise (yellow circle) tracings. Average vessel wall SNR (0.8 mm
3:
20.7 +/- 11.18; 0.6 mm
3: 12.6 +/- 5.8) and vessel wall/lumen CNR (0.8
mm
3: 14.6 +/- 8.1; 0.6 mm
3: 9.0 +/- 4.5) measurements were
significantly different between the two coronal acquisitions with isotropic
voxels (
Figure 4). Vessel wall SNR was significantly different
between the 3 axial acquisitions (0.6 mm
2: 36.9 +/- 21.0; 0.5 mm
2:
25.3 +/- 11.5, 0.4 mm
2: 21.6 +/- 10.9) while CNR measurements
indicated no significant difference (0.6 mm
2: 22.4 +/- 13.1; 0.5 mm
2:
16.7 +/- 7.1, 0.4 mm
2: 15.1 +/- 7.7) (
Figure 4). In all cases SNR and CNR were comparable to values
reported in the literature for similar acquisitions performed on 3T magnets,
while achieving equivalent or higher spatial resolution.
DISCUSSION/CONCLUSIONS
In conclusion, we
demonstrate feasibility of 3D imaging of the carotid vessel wall at ultra-high
field using 3D T2W SPACE. SNR and CNR measurements indicate good image quality
and good vessel wall/lumen delineation even at high spatial resolution. These
results warrant investigation of these techniques in patients with carotid
artery disease, and the development of these protocols for multi-contrast and
quantitative imaging of the carotid vessel wall at 7T.
Acknowledgements
This work was supported by 2 R01HL071021 12.References
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