Jabrane Karkouri1, Saba Shirvani1, Tiger Zhang1, Dennis Klomp2, Martijn Lunenburg3, Ladislav Valkovic4, and Christopher T. Rodgers1
1Wolfson Brain Imaging Center, University of Cambridge, Cambridge, United Kingdom, 2Department of Radiology, University Medical Center Utrecht, Utrecht, Netherlands, 3Tesla Dynamic Coils, Zaltbommel, Netherlands, 4Oxford Centre for Clinical Magnetic Resonance Research, University of Oxford, Oxford, United Kingdom
Synopsis
We evaluated the performance of
two RF coil configurations for ultra-high field (7T) 31P-MRS
applications in the body. We tested: (A) a dipole Tx/Rx + loop Rx coil vs (B) a quadrature dual-loop Tx/Rx coil.
We assessed their relative performance by EM modelling simulations and through
phantom and in vivo cardiac scans. Both simulations and experimental
verifications indicate that there is notable improvement in terms of B1+
efficiency for the dipole+loop combination compared to quadrature loops.
We extrapolate these preliminary findings to predict the performance of the
dipole+loop combination if driven at 35kW total like our previous whole-body
birdcage coil.
Introduction
Ultra-high field
leads to a 2.5-fold increase in SNR [1] and increased spectral resolution [2]. The
use of dedicated receive-arrays further improves the SNR and extends coverage
to more of the heart at 7T. Array coils for cardiac 31P-MRS have mostly been using surface coils
for transmission. Surface coils’ radiofrequency (RF) transmit field strength (B1+) drops-off rapidly with increasing
distance from the coil to the volume of interest [3] which makes liver and
heart applications challenging. To
overcome one of the main technical challenges of significant B1+
signal dropouts at UHF, different RF coil designs have been introduced, that
counteract B1 field variations.
In this study we have compared
the performance of a dipole Tx/Rx + loop Rx RF coil with a quadrature dual-loop
Tx/Rx RF coil configurations for ultra-high field (7T) 31P-MRS
applications in the body. We assessed their relative performance through
simulations and through phantom field map acquisitions and in vivo cardiac
scans.Methods
Materials:
The surface quadrature Tx/Rx 1H/31P
loop coil consists of a1H loop (Frequency = 297.8 MHz) in the centre
of the coil and two 31P loops (Frequency = 1210.3 MHz) located on
the sides (Figure 1). The new prototype surface body coil dipole array contains
4 anterior and 4 posterior Tx/Rx 1H/31P dipoles. For in
vivo data acquisition, dipoles A3 and A4, as shown in Figure 1, have been
used for transmission.
Simulations:
We have performed EM simulations using CST Studio Suite 2020
to compare the transmit efficiency of the dipole design against a whole-body
birdcage transmit design (previously reported in Valkovic et al, PlosONE) in
terms of B1+ and depth. The coil B1+
efficiency was simulated over a homogenous numerical phantom and a human model
with values extracted for all “heart” voxels afterwards (Figure 2).
B1
map acquisition:
A 31P B1 map was acquired from the
surface body dipole array coil with a progressive saturation method on a 30 L
phosphorus phantom of phosphate concentration of 30 mM. A 3D gradient echo
sequence has been used with TR = 100 ms, TE = 5 ms, rectangular excitation
pulse of 10 ms length duration, 200 averages and various excitation pulse
voltages varying from 2 V to 51.9 V.
MRSI
acquisitions:
3D weighted CSI cardiac data has been
acquired on the heart of a healthy volunteer with TR 1s, matrix size 8x16x8,
FOV 220 mm, vector size 1024 points, spectral bandwidth 6 kHz and both dual
tuned 1H/31P quadrature loop surface transmit coil and
dipole array body coil. Acquisition times were 11 min 48 s.
Results
Figure 2 shows simulations of a B1+ evolution
with depth for the novel prototype dipole coil design and for a previous whole-body
birdcage coil design (Valkovic et al., PlosONE).
Figure 3 shows simulations of B1+ field distribution over a numerical phantom
and numerical model of human heart.
Figure 4 shows the acquired B1+ map of
the dipole array coil. At typical depths for the heart (5-10cm), B1+
values are about 0.1-0.2 Hz/V. At max power, which for this coil is 600 VRMS
(approx. 8kW), we would have a B1+ of about 3.5-7 uT. From Figure 2, at typical depths for the
heart, we have a B1+ of about 0.2-0.15 uT/sqrt(W). At maximum
power, this corresponds to a B1+ of about 3.7 – 4.9 uT
with an 8kW RF amplifier.
Figure 5 shows a spectrum acquired on the heart of healthy
man from a 3D CSI acquisition. All the expected cardiac metabolites are clearly
visible in this spectrum. The PCr/ATP ratio is as expected for a healthy
subject allowing for partial saturation and the usual levels of blood
contamination.Discussion
B1+ field map acquisitions agree with EM
modelling simulations for dipole coils. Simulations show that with a set of 4x
dipoles, good B1+ homogeneity is obtained right across
the chest, similar to our previous whole-body birdcage coil design [1]. Figure 3
shows that with a suitably upgraded RF power amplifier, this coil would have an
excellent liver and heart performances comparable to whole-body birdcage
designs but without the complexities of mechanical integration into the
existing bore liner or mechanical clashes with the standard patient table.
The B1+ field values measured in the
phantom agree with EM modelling simulations,
as shown in Figure 2. These first simulations and experiments make us confident
to proceed with planned liver and cardiac studies using this coil. Preliminary
human data are shown in Figure 5.Acknowledgements
This project has received funding from the European
Union’s Horizon 2020 research and innovation programme under grant
agreement No 801075. We would also like to acknowledge Tesla Dynamic Coils for
their work in constructing the surface dipole array coil as part of the NICI
consortium.
Christiopher
T. Rodgers and Ladislav Valkovic are funded by the Wellcome Trust and Royal
Society [098436/Z/12/B].
We acknowledge the NIHR Cambridge Biomedical Research
Centre and the MRC Clinical Research Infrastructure Award for 7T research.
References
[1] Rodgers,
Christopher T., et al. "Human cardiac 31P magnetic resonance spectroscopy
at 7 Tesla." Magnetic resonance in medicine 72.2 (2014):
304-315.
[2] Purvis, Lucian
AB, et al. "Phosphodiester content measured in human liver by in vivo 31P
MR spectroscopy at 7 tesla." Magnetic resonance in medicine 78.6
(2017): 2095-2105.
[3] Rodgers, Christopher T., and
Matthew D. Robson. "Receive array magnetic resonance spectroscopy:
whitened singular value decomposition (WSVD) gives optimal Bayesian
solution." Magnetic Resonance in Medicine: An Official Journal of the
International Society for Magnetic Resonance in Medicine 63.4 (2010):
881-891.
[4] Valkovič, Ladislav, et al. "Using
a whole-body 31P birdcage transmit coil and 16-element receive array for human
cardiac metabolic imaging at 7T." PLoS One 12.10 (2017):
e0187153.