Byeong-Yeul Lee1, Xiao-Hong Zhu1, Sebastian Rupprecht2, Michalel T. Lanagan3, Qing X. Yang2, and Wei Chen1
1Center for Magnetic Resonance Research, Department of Radiology, University of Minnesota Medical School, Minneapolis, MN, United States, 2Center for NMR Research, Department of Radiology, The Pennsylvania State College of Medicine, Hershey, PA, United States, 33Department of Engineering Science and Mechanics, The Pennsylvania State College of Engineering, University Park, PA, United States
Synopsis
X-nuclei MRS for human application
faces two challenges: high RF power requirement (thus, higher SAR) for
achieving the same RF pulse flip angle due to a relatively lower gyromagnetic ratio, and limit
of detection sensitivity (or SNR) even at high/ultrahigh field. In this work,
we report that by incorporating ultra-high dielectric constant (uHDC) material into
the RF head volume coil, huge RF transmit power reduction was observed in the
regions near the uHDC pads for 31P MRSI at 7T. Concomitantly, the B1
efficiency for acquiring the spectra was increased about 100%. Strikingly, up
to ~20% denoising effect was also observed with the uHDC material. Our results demonstrated
that incorporating uHDC with RF coil can significantly boost SNR and reduce SAR
in X-nuclei MRS applications; such improvements are beyond the gains obtainable
at very high field strength magnet that has approached to its technologic
limits.
Purpose
In vivo 31P MRSI
provides an important neuroimaging tool for studying high-energy phosphate
metabolisms, neuroenergetics and NAD redox state [1-2]. This study
was to investigate the efficacy and utility of ultra-high dielectric constant
(uHDC) technology for significantly improving SNR and reducing RF power
requirement for in vivo 31P
MRSI at ultrahigh field of 7T. Introduction
Increased RF power deposition or
specific absorption rate (SAR) has become a major safety concern and technical
hurdle at ultrahigh field despite its substantial improvement of the
spatial/temporal/spectral resolution with increased signal-to-noise ratio (SNR).
As one of the engineering solutions, incorporating high dielectric constant
(HDC) material into the RF coil at various magnetic fields has provided substantial
benefits for improving both the transmit efficiency (|B1+|) and receive sensitivity (|B1-|) [3-5].
Thus, our research aims were to 1) develop the ultrahigh HDC (uHDC) material using
advanced material science for MR imaging application, and 2) to quantitatively
investigate the B1 efficiency and sensitivity gain for 31P
MRS application at 7T on both phantom and in
vivo human brain validation. Here we present the first result of the B1
field improvements with the half-pipe uHDC material that was designed for the
human occipital lobe.Methods
uHDC Material: First,
given the operation frequency (120.3MHz for 31P at 7T) in
conjunction with a 31P TEM head volume coil configuration, the
ultrahigh effective permittivity constant (εeff = 1200)
material was made lead zirconium titanate (TRS, State College, PA, USA).
In particular, a half-pipe shape of the ceramic dielectric pad was successfully manufactured
for targeting local region of the human occipital lobe.
31P MRS: All 31P
MRS measurements were performed at 7.0T/90 cm bore human scanner (Siemens/Magnex)
with 31P-1H double-tuned RF volume coil; 1H channel
for anatomic imaging and B0 shimming, and 31P channel for
acquiring 3D 31P chemical shift imaging (CSI). A phantom 31P
MRS data were collected from a spherical container filled with inorganic
phosphate (Pi: 100 mM) and gadolinium contrast agent for shortening the T1 value of
Pi to ~300 ms. In
vivo 31P MRS data were also collected on the brains of two healthy
volunteers. The 3D 31P CSI data of the phantom were acquired with
Fourier Series Window (FSW) technique [6] (TR= 1s, FA= 90°, phase encode= 9x9x7, bandwidth= 5 kHz, FOV= 20x20x18
cm3, and pulse width = 1 ms). In
vivo 31P CSI data were acquired with slightly different parameters
of TR= 1.5s with an Ernst flip angle. Finally, spatial maps of relative B1+
(i.e., inversely proportional to the RF transmit voltage for reaching a 90° RF flip angle) and B1-
(proportional to the maximum signal at 90° flip angle) were calculated using fitting algorithm for
determining the integrals of phosphorous creatine (PCr) signal for in vivo data and Pi signal for phantom
data and their dependence on the variable RF pulse voltages. Noise was measured
from the signal-free regions of the spectra.Results and Discussion
Figure 1 displays the
experimental setup of the phantom and Fig. 2 shows both RF transmission
field (B1+) and reception field (B1-)
for acquiring 3D 31P CSI at 7T, which demonstrate large improvements
with the uHDC pads for Pi phantom. Such a significant B1 improvements
were also observed in human brain measurement showing an increased SNRs (more
than 200%) and reduced RF power requirement (more than 200% voltage reduction) in
the regions of interest near the uHDC pads as compared to that without pads (see
Fig. 3). Strikingly, noise levels were also significantly reduced in both
phantom (-20%) and in vivo case
(-15%) with the use of the uHDC material (see Fig. 4). The amplitude of the
denoising effect seems to depend on the configuration between the uHDC pad and
RF volume coil as well as the loading condition. These results provide compelling
evidence of the uHDC materials for improving B1 efficiency, consequentially
leading to SNR enhancements and SAR reduction. Based on the field-dependent SNR
of the PCr metabolite [7], a 200% SNR gain with the uHDC technique observed
at 7T is equivalent to a similar performance and SNR expected at > 15T without
additional concerns for SAR.Conclusion
Our results demonstrate
that a novel design of uHDC materials significantly improved both |B1+| and |B1-| for in vivo 31P MRS. Therefore, utilizing uHDC materials could
be an important and cost-effective engineering solution for overcoming high
specific absorption rate (SAR) and significantly gaining SNR at ultrahigh
fields, which will provide enormous benefits for in vivo
human applications including brain research.Acknowledgements
NIH grants: R01
NS057560, NS070839, MH111447; R24 MH106049, S10RR026783,
P41 EB015894, and P30 NS057091; and the AHC Faculty Research Development (FRD)
grant from the University of Minnesota.References
[1] Du et al, PNAS
105:6409-14 (2008); [2] Zhu et al, PNAS 112:2876-81 (2015); [3] Qing et al,
JMRI 38:435-440 (2013);
[4]
Lee et al., Proc. ISMRM; 23: 2382
(2016); [5] Rupprecht et al., Proc.
ISMRM; 23: 403 (2014); [6] Garwood et al.,
JMR 75:244-261 (1987); [7] Lu et al, NMR Biomed 27:1135-41
(2014).