Arvin Arani1, Kevin J. Glaser1, Shivaram Poigai Arunachalam1, Phillip J. Rossman1, David S. Lake1, Joshua D. Trzasko1, Armando Manduca1, Kiaran P. McGee1, Richard L. Ehman1, and Philip A. Araoz1
1Mayo Clinic, Rochester, MN, United States
Synopsis
Noninvasive
stiffness imaging techniques (elastography) can image myocardial tissue
biomechanics in vivo. However, for cardiac magnetic resonance
elastography (MRE) techniques the optimal vibration frequency for in vivo
experiments is unknown. The purpose of this study was to determine the optimal
vibration frequency for cardiac MRE in healthy volunteers. Cardiac MRE
displacement fields can be imaged with mean OSS-SNR > 1.6 at frequencies as
high as 180Hz, however, mean OSS-SNR values and myocardial coverage was shown
to be highest at 140Hz across all subjects. This study motivates future
evaluation of high-frequency 3D MRE in patient populations.Purpose
Noninvasive
stiffness imaging techniques (elastography) can image myocardial tissue
biomechanics in vivo. However,
for cardiac magnetic resonance elastography (MRE) techniques the optimal
vibration frequency for in vivo
experiments is unknown. Since the myocardium is thinner than typical MRE shear
wavelengths, waveguide effects dominate the wave propagation, and incorrect
stiffness estimates will result if these are not accounted for. In principle, taking
the curl of the displacement field (1) will help reduce boundary
affects, but at the expense of noise amplification. Higher vibrational
frequencies imply higher resolution, but these attenuate quickly. Lower
frequencies penetrate deeper, but have stronger waveguide effects, and smaller
spatial derivatives with less tolerance to noise. The purpose of this study was to determine the optimal
vibration frequency for cardiac MRE in healthy volunteers.
Methods
3D
cardiac MRE was performed on 8 healthy volunteers. Vibration
was delivered to the heart with a passive drum driver (Figure 1A) in direct contact with the
volunteer’s skin, just to the left of the sternum and superior to the xiphoid process
(Figure 1B). To
establish a “no-motion” baseline measurement of noise, a full MRE exam without
the application of any vibrational motion was performed on one volunteer. Cardiac gating was performed by placing electrocardiography
leads on the back of the left shoulder of the
volunteers. Volunteers were imaged head first in the supine position. Imaging
was performed on a 1.5-Tesla closed-bore MR imager (Optima MR450W; GE
Healthcare, Milwaukee, WI, USA) in an oblique orientation to obtain long-axis MRE
images of the heart. Imaging was
conducted using a flow-compensated, cardiac-gated,
spin-echo, single-shot echo planar imaging MRE sequence, with vibration
frequencies of 80Hz, 100Hz, 140Hz, 180Hz and 220Hz; TR was matched to each
volunteer’s heart rate with electrocardiogram-gating, TE = 52-79ms depending on
frequency; FOV = 32 cm; 64x64 acquisition matrix; parallel imaging acceleration
factor = 2; 5 contiguous 5-mm-thick axial slices; 1-2 motion-encoding gradient
pairs; alternating x, y, z, and 0 motion-encoding gradient directions; and 4
phase offsets. The left ventricle of the heart was semi-automatically segmented
and the octahedral shear strain signal-to-noise ratio (OSS-SNR) (2) was calculated on the curl wave fields.
Results
The
out of plane component of the vector curl field, the corresponding elastograms
(magnitude of complex shear modulus |G*|), and a map of the voxels with OSS-SNR
> 1.6 on the curl data are shown in Figure 2 for a single volunteer over the 80-220 Hz
frequency sweep. The mean OSS-SNR (Figure 3A) and the
percentage of voxels with OSS-SNR > 1.6 (Figure 3B) over the entire myocardial volume were
calculated for each volunteer at each vibration frequency. The percentage of voxels that remain in the
“no-motion” and “motion” data sets as a function of OSS-SNR threshold for all
frequencies are shown in Figure
4A. The shaded grey region depicts the separation point between the
“motion” and “no motion data-sets”. The dashed cross-hair indicates the OSS-SNR
threshold of 1.6 where 95% of all “no motion” voxels are eliminated. For this
same subject the difference between |G*| of “motion” and “no motion” and the
ratio of |G*|“motion” over |G*|“no-motion” have been
plotted as a function of frequency in Figure 4B. In Figure 4 the boxes correspond to the 1st
and 3rd quartiles, the horizontal line in each box is the median value,
the ‘X’ corresponds to the maximum and minimum values, the small square in each
box is the mean value, and the error bars (whiskers) represent a single
standard deviation from the mean across all subjects. These plots show that at
all frequencies except for 220 Hz it was feasible for at least one volunteer to
have a mean OSS-SNR above 1.6. However, only the 140Hz frequency had a median
OSS-SNR over all subjects just over 1.6, and a mean OSS-SNR just below the 1.6
threshold, (square in box plot). The 140 Hz vibration frequency also
corresponded to having the highest percentage of voxels with OSS-SNR > 1.6.
Discussion
Cardiac
MRE displacement fields can be imaged with mean OSS-SNR > 1.6 at frequencies
as high as 180Hz, allowing for stiffness maps to be generated with direct
inversion algorithms. However,
octahedral shear strain signal to noise ratios and myocardial coverage was
shown to be highest at a frequency of 140Hz across all subjects. This study motivates future evaluation of
high-frequency 3D MRE in patient populations.
Acknowledgements
This study was supported by the National Institute of Health (NIH) grants 5R01HL115144 and EB001981.References
1. Sinkus
R. et al., Current medical imaging reviews 2012;8(1):56-63.
2. McGarry MD. et al., Physics in
medicine and biology 2011;56(13):N153-164.