Bernhard Gruber1,2, Arjan D. Hendriks 1, Cezar B.S. Alborahal3, Bas Brussen3, Tim Leiner1, Gustav Strijkers1, Dennis W. J. Klomp1,3, and Martijn Froeling1
1Department of Radiology, University Medical Center Utrecht, Utrecht, Netherlands, 2Institute of Biomedical Mechatronics, Johannes Kepler University, Linz, Austria, 3MR Coils B.V., Zaltbommel, Netherlands
Synopsis
High-density coil arrays can be used to accelerate
MRI. Here we present the results from measurement-based extrapolations of a 256
Channel Cardiac Array Coil obtained by 16 sequential scans of a 16 Channel Array
to assess acceleration performance and sensitivity constraints for 3T MRI. With
element sizes of 55 mm x 33 mm, tissue load remains dominant at the 3T Larmor
frequency of water, while SENSE accelerations can go up to 20-fold at low
g-factors. These results motivate the design of a 256 channel cardiac array for
accelerated 3T MRI.
Purpose
Todays Cardiac Magnetic Resonance Imaging (CMR) protocols can be extremely
time consuming, expensive, and uncomfortable for the patient. Particularly,
when including the realm of multi parametric MRI features that aid diagnosis.
In order to substantially accelerate the image acquisitions, high-density receiver
coil arrays1-3 may be used. Increasing the density of coils
coincides with reducing the coil size, which in turn will reduce tissue loading
and therefore can increase the noise figure of the MRI system. But, as long as tissue
load remains dominant, the density of the coils can be increased without
substantially adding noise4. In this study, we have investigated the use of high-density coil arrays for
accelerated5-7 cardiac MRI while assuring tissue load dominance. In
process of building the receiver chain, 16 sequential measurements with a
repositioned high density 16-channel receiver array are performed to obtain
coil sensitivity and noise correlations in a healthy volunteer to investigate
the possible acceleration performance of a 256 Channel Cardiac Coil Array at 3
Tesla.Methods
A 16-element (4 x 4) coil array was designed (MR Coils BV, Zaltbommel, the
Netherlands) with loop sizes of 55 mm in length and 33 mm in width (Fig. 1).
Individual Q-factor measurements were performed using an S12 measurement with
two pick-up probes weakly coupled (<<-30dB) to the loop. Unloaded and
loaded Q values were measured at different locations of the body.
Measurements were performed on a Philips 3T wide bore system with digital
receivers (Philips, Best, the Netherlands). Coil sensitivity maps were recorded
using the standard Philips reference scan (resolution = 6 mm isotropic, two
stacks: one obtained with 16 channels as receiver and one with the bodycoil as
receiver). A separate noise scan was obtained by switching off the RF transmit
power.
To simulate the expected improvement in
acceleration of the 256 Channel Cardiac Array, the measurements were repeated 16
times, each time with the array positioned at another location around the chest
of the patient. The 16 data sets of the array were spatially registered and
merged into a 256 by 256 array filling out only the diagonal 16 times 16
elements. The remaining part of the array is set to zero. G-factor maps are
calculated with SENSE accelerations in FH and LR using the aligned sensitivity
maps and the noise matrix.Results
The unloaded Q-factor was measured to be 603, while
the loaded Q-factor ranged from 53-98. The noise correlation matrix is shown in
Fig. 2. No noise correlation could be obtained for the cross terms outside the
16 element wide diagonal of the 256x256 matrix, due to absence of sufficient
receiver chains. Note the low noise correlation within the 16-element wide
diagonal. When merging the 16 images obtained with the 16 times 16 elements,
good penetration of the reception is obtained throughout the body (Fig. 3). SENSE
acceleration can go up to 5 in one dimension, or 4x5 in 2D acceleration (Fig. 4).Discussion
The results show that a 256 Channel Cardiac Coil
allows acceleration factors of up to 20 when accepting a g-factor of less than 2.
It should be noted that the results are obtained with only 16 elements
physically present during each scan. Consequently, potential couplings in a
full 256 Channel array have not been incorporated. However, it is expected that
these potential couplings will not effect our results substantially as the
elements within the 16 Channel array also show very low coupling.Conclusion
We have demonstrated that the coil element that can
be used for a high-density 256 Channel Cardiac Array remains in tissue load
dominance (6 to 11-fold). Moreover, coil couplings within the 4 x 4 array can
be very low. When neglecting potential noise cross correlation within the
remaining elements of the 256 Channel Array Coil, image acceleration of over 20
can be obtained with SENSE encoding. Consequently, these calculations
demonstrate the motivation to build the 256 Channel Cardiac Array Coil to
facilitate a boost in acceleration of the multi parametric cardiac MRI.Acknowledgements
No acknowledgement found.References
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