Mohamed Tachrount1, Bleddyn Woodward1, Emre Kopanoglu1, Michel Italiaander2, Denis Klomp2,3, Ian Driver1, and Richard Wise1
1CUBRIC, School of psychology, Cardiff University, Cardiff, United Kingdom, 2MR Coils, Zaltbommel, Netherlands, 3Department of Radiology, University Medical Center Utrecht, Utrecht, Netherlands
Synopsis
MRI at UHF is promising
for a variety of clinical applications however it is challenging because of B0
and B1 inhomogeneities and SAR limitations. To improve the RF efficiency in the
brain and the neck, a novel 8Tx/32Rx RF coil has been built by MR coils. Its performance
in terms of B1+ intensity and homogeneity at the brainstem/cerebellum and the
neck was assessed and compared with the standard Nova Medical 8Tx/32Rx coil. The
novel coil allows for a higher B1+ at the brainstem/cerebellum and the neck
where B1+ mapping and shimming need further optimisation for ASL application.
Introduction
MRI at ultra-high field (≥7T) is promising for a
variety of clinical applications due to the improved intrinsic signal-to-noise
ratio (SNR) and susceptibility induced contrast. However, it is technically
challenging due particularly to transmit field (B1+) inhomogeneities and
Specific Absorption Rate (SAR) limitations. The rapid drop of B1+ toward the
brainstem and the neck due to the limited extent of the standard head coils in
addition to the large B1+ and B0 inhomogeneities make clinical applications in those
regions much more challenging. Imaging brainstem and cerebellum as well as quantifying
blood flow using pseudo-Continuous Arterial Spin Labelling (pCASL) are applications
in which substantial B1+ is required in both the neck and the brain. To overcome
these pitfalls, different approaches have been adopted like designing novel
coils1, designing tailored RF pulses2 or parallel
transmit (pTx) techniques (RF shimming3,4 and transmit SENSE5,6
). In this work, the performance of a novel 8Tx/32Rx built by MRCoils (Zaltbommel,
The Netherlands) in terms of B1+ intensity and homogeneity at the brainstem/cerebellum
and the neck was assessed and compared with the standard Nova Medical 8Tx/32Rx
coil (Wilmington, USA).Materials and methods
Experiments
were performed on a whole-body Siemens 7 T scanner (Magnetom) equipped with an 8
channel pTx system with which we used the MRCoils 8Tx/32Rx and Nova 8Tx/32Rx
coils. Unlike the Nova coil, the MRCoils device is asymmetrical with three transmitting elements around the neck and 5 around
the (Fig1).
The B1+
shimming and mapping were performed first at the brainstem/cerebellum and then at
the neck (arterial spin labelling plane). As ASL requires optimal B1+ at both
neck and brain, additional B1+ maps were acquired within the brain. The
performance of the MRCoils coil was compared with the Nova coil. To perform
those measurements, ten healthy volunteers were imaged.
After the
standard B0 shimming and frequency adjustment, phase and magnitude images
corresponding of the individual transmitting elements were acquired using a Siemens
gradient-echo sequence (TE/TR=2.1/100ms, spatial resolution=3.1x3.1x5mm, TA=8s).
B1 maps were acquired using a Siemens multi-slice sequence based on turbo-flash
readout (TE/TR=1.9ms/10s, spatial resolution=3.1x3.1x5mm, TA=1min40s). The B1+
optimisation was based on phase only RF shimming. The images were transferred
to a separate computer on which a Matlab script was used to select ROIs and to
calculate phase corrections for each element.Results
Using the novel
coil, both sagittal and axial B1 maps before and after RF shimming depicted in
Fig2 show a clear improvement of RF homogeneity around brainstem/cerebellum. Compared
to Nova coil, an improvement of 65% (117° vs. 70°) of flip angle (FA) was
obtained (Fig3). RF shimming at both neck and brain are depicted in Fig4a for
sagittal and axial slices. RF shimming significantly enhanced B1+ intensity but
homogeneity still needs further improvement. When shimming in the neck, destructive
interferences and low B1+ intensities can be noticed on FA maps within the
brain. To improve B1+ within the brain, a further RF shimming was necessary as shown
in Fig5. Due to its symmetry, Nova coil transmits a more homogeneous B1+ in the
brain without RF shimming but it drops rapidly towards the
brainstem/cerebellum. For that coil, RF shimming at the neck did not improve
the intensity nor the homogeneity of B1+ and drastically deteriorates the
latter in the brain (Fig4b).Discussion
RF shimming with
the novel coil improved significantly both B1+ intensity and homogeneity at the
brainstem/cerebellum compared to the Nova coil. However, despite the
improvements, the intensity and the homogeneity of B1+ at the neck were not
optimal for applications like pCASL because of the adopted B1+ mapping and
shimming methods. Indeed, measuring B1+ maps of individual elements separately suffers
from a high degree of uncertainty in measuring FAs when the actual FA or the
SNR are low. In addition, phase only B1 shimming is sensitive to field
inhomogeneities and low SNR. Using a volumetric sequence like DREAM7
for B1+ mapping in combination with multiple interferometric measurements would
improve the sensitivity, reduce T2* effects, and drastically reduce the
acquisition time. Performing RF shimming using dedicated algorithms would
improve both B1+ intensity and homogeneity within the ROI3,8,9. Methods
like pCASL needing optimal B1+ within the neck and brain for the labelling and
the imaging respectively, would benefit from dynamic B1 shimming approaches that
switch between two sets of shimming coefficients during the same TR.Conclusion
Compared to the
8Tx/32Rx Nova coil, the new coil allows for a higher B1+ at the
brainstem/cerebellum and the neck where B1+ mapping and shimming need further
optimisation for ASL application.Acknowledgements
We would like to knowledge the Wellcome Trust Strategic Award for funding this research and Fabrizio Fasano (Siemens engineer) for his help.
References
1-
Gregor
Adriany, Pierre-Francois Van de Moortele, Johannes Ritter, Steen Moeller,
Edward J. Auerbach, Can Akgün, Carl J. Snyder, Thomas Vaughan, Kâmil Ugurbil, A
geometrically adjustable 16-channel transmit/receive transmission line array
for improved RF efficiency and parallel
imaging performance at 7 tesla, Magn. Reson. Med. 59 (3) (2008) 590–597
2-
Saekho
S, Yip CY, Noll DC, Boada FE, Stenger VA. Fast-kz three-dimensional tailored
radiofrequency pulse for reduced B1 inhomogeneity. Magn Reson Med
2006;55:719–724.
3-
Hoult
DI, Phil D. Sensitivity and power deposition in a high-field imaging
experiment. J Magn Reson Imaging 2000;12:46–67.
4-
Ibrahim
TS, Lee R, Baertlein BA, Abduljalil AM, Zhu H, Robitaille PM. Effect of RF coil
excitation on field inhomogeneity at ultra high fields: a
field optimized TEM
resonator. Magn Reson
Imaging 2001;19:1339–1347.
5-
Katscher
U, Bornert P, Leussler C, van den Brink JS. Transmit SENSE. Magn Reson Med
2003;49:144-150.
6-
Zhu
Y. Parallel excitation with an array of transmit coils. Magn Reson Med 2004;51:775–784.
7-
Nehrke
K, Versluis MJ, Webb A, Bornert P. Volumetric B1+ mapping of the brain at 7T
using DREAM. Magn Reson Med. 2014;71(1):246-56.
8-
Metzger
GJ, Snyder C, Akgun C, Vaughan T, Ugurbil K, Moortele P-FVd. Local B1+ shimming
for prostate imaging with transceiver arrays at 7T based on subject-dependent
transmit phase measurements. Magn Reson Med. 2008;59(2):396–40
9-
Deniz
CM, Alon L, Brown R, Daniel KS, Zhu Y. Specific Absorption Rate Benefits of
Including Measured Electric Field Interactions in Parallel Excitation Pulse
Design. Magn Reson Med. 2012;(67):164–174.