Rita Schmidt1,2 and Andrew Webb1
1Leiden University Medical Center, Leiden, Netherlands, 2Neurobiology, Weizmann Institute of Science, Rehovot, Israel
Synopsis
Several studies have shown proof-of-principle implementations of
metamaterials for local RF transmit efficiency and sensitivity improvement. The
most common implementations are based on set of split-rings or set of wires. To
support a dual-band enhancement, the design here relies on a combination of the
mentioned above two types of metamaterials. Whereas in the original study we
focused on 7T 31P/1H dual-band implementation, in this
work we were interested to examine the possibility to extend it to much lower
frequencies, namely a dual-band metamaterial for 3T 23Na/1H
local signal enhancement. The implementation was examined in EM simulations and
in phantom experiments at 3 T.
Introduction
Several studies have shown proof-of-principle implementations of
metamaterials for local RF transmit efficiency and sensitivity improvement1-6.
The most common implementations are based on sets of split-rings3-4
or wires5, designed to be resonant or close to resonant at the
frequency of interest. In our recent studies, we implemented a hybrid metamaterial
based on a high permittivity substrate and set of conducting strips6.
We have also shown the feasibility of dual-band enhancement, with a set of long
strips producing the resonant mode for the low frequency band, and a set of
short strips (which behaves equivalently to split-rings) responsible for the
resonant modes for the high frequency band. Whereas in the original study7
we focused on 7T 31P/1H dual-band implementation, in the current
study we were interested to examine the possibility to extend it to much lower
frequencies, namely a dual-band metamaterial for 3T 23Na/1H
local signal enhancement. To implement such a metamaterial in a compact setup,
we used high permittivity material suspensions of BaTiO3 in water. The
implementation was examined via electromagnetic (EM) simulations and in phantom
experiments at 3 T. Methods
3D EM
simulations of the B1+ field were performed using FIT
(finite integration technique) software (CST Microwave Studio, Darmstadt,
Germany). All B1+ maps were normalized to an accepted
power of 1 Watt. The first steps in the design included an optimization study of
the resonant structures at 33.8 MHz and 128 MHz separately. The structure was
designed to have dimensions 16x31x1 cm3. The conducting strips were
implemented using copper strips in a zigzag shape (which allowed the resonant
mode to be achieved within the aforementioned structure dimension) and were
attached to a transparent plastic sheet, placed inside the pad. Once the
metasurfaces are optimized, a combined setup was produced with the long strips
on one side of the dielectric and the short strips on the other side, in
contact with the dielectric layer. The simulation showed that a coupling effect
between the metasurfaces reduces the efficiency of the higher frequency. A tilt
of the high frequency setup in-plane (by 10°) reduced this coupling, and
resonant modes for 23Na and 1H could be achieved. Figure
1 shows the geometry of the metasurface and the magnetic field distributions
for each band. The effect of the dielectric permittivity on the enhancement was
examined. Although a relative permittivity (εr) of 250 shows maximal
enhancement, the estimated actual permittivity used was slightly lower, εr
= 230. To improve the attainable enhancement, we added an extra BaTiO3
pad to the setup (as used in several works8 -18x18x1 cm3,
εr = 280) to increase the enhancement at the 1H
frequency. The phantom included one container of water with NaCl (0.1%) and another
container of white cheese (0.2% NaCl). The metasurface was placed on the
opposite side of the phantom from a commercial 23N
and 1H double-resonant surface coil
. Phantom images were acquired on a 3T Siemens TIM
TRIO scanner, including a low flip angle gradient-echo sequence for SNR
estimation for protons and a chemical shift imaging sequence for sodium. Scan
parameters are shown in the caption for Figure 3.
Results
Figure 1 shows the H-field resonant modes of the setup for
low and high frequencies. Figure 2 shows EM simulation in a full setup, which included
a surface-coil, a phantom and a metamaterial. Using metamaterial setup, the
maximal enhancement is achieved at εr=250 (which matched the
resonant mode). Simulation results of the implemented setup (using εr=230
and added BaTiO3 pad) show an enhancement of ~2 for 23Na
and ~2.5 for 1H in the vicinity of the metamaterial. Figure 3 shows
experimental results, where the SNR enhancement ratio (using square root of the
normalized intensity divided by the noise) show maximal enhancement of ~1.5 for
23Na and ~2.3 for 1H. The deviation between the simulated
and measured enhancement ratio for the 23Na can be due to the relatively
high partial volume in the 23Na scan. Conclusions
In this study, we designed a dual-band 23Na/1H
metametarial for local signal enhancement. This work has shown an improvement
in SNR of a factor of ~1.5 for 23Na and ~2.3 for 1H. Further
control and optimization is required to achieve a greater penetration of the
signal enhancement, especially for the 23Na frequency. Acknowledgements
No acknowledgement found.References
[1] Radu X. Metamaterials, 2009, 3(2),
90-99, [2] Hurshkainen A.A. et.al. J. Magn. Reson., 2016,269,
87-96, [3] Freire M. J et.al J. Magn.
Reson., 2010, 203, 81–90, [4] Algarin J.M.; et.al. J. Magn. Reson. , 2014,
247, 9-14, [5] Slobozhanyuk A.P. et.al. Adv. Mater., 2016, 28(9), 1832-1838, [6]
Schmidt R. et.al. Sci. Rep., 2017, 7, [7] Schmidt R., & Webb A. ACS
Appl. Mater. Interfaces, 2017, 9(40), 34618-34624, [8] Teeuwisse W.M. et.al. Magn. Reson. Med., 2012; 67, 912-918.