4296

Dual-nuclei metamaterial implementation for sodium and proton acquisition at 3 T
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.

Figures

Figure 1: Schematic setup of the hybrid metasurface, for low frequency band (a) and high frequency band (b). The dielectric substrate used here had εr =250. c) H-field of the resonant modes in a combined setup. The H-field is shown in two main cross-sections (XY and YZ planes). The maps are normalized to the maximal intensity in each case (“cool” colormap is used for 23Na and jet colormap for 1H).

Figure 2: Full setup EM simulation results. B1+ maps at 23Na frequency (a) and 1H frequency (b). The maps show B1+ for three setups: with double-tuned surface coil only, with the metamaterial structure (εr=230) placed underneath the sample on the opposite side to the surface coil, and with the metamaterial (εr=230) and extra BaTiO3 pad. The B1+ profile and enhancement ratio are shown at the 23Na frequency (c) and 1H frequency (d). The profiles are shown for three εr values (230,250,270) and for the actual experimental setup (εr=230 plus extra BaTiO3 pad).

Figure 3: Phantom experimental results. a) 1H image and the physical setup (surface coil on top, metasurface at the bottom). Images comparison for 23Na (b) and 1H (c) without and with the setup, respectively. SNR profiles and enhancement ratio for 23Na (d) and 1H (e ), respectively. The fit for surface-coil (shown in red) in d) used for NaCl concentration estimation. Scan parameters: 1H FOV 24x24 cm2, resolution 1.7 x 1.7 x 5.0 mm3, TR/TE 12/3.4 ms, flip angle 23°. The 23Na CSI scan parameters were FOV 20x20 cm2, phase encoding matrix 32x32, flip angle 45°, TR/TE 540/2.3 ms.

Proc. Intl. Soc. Mag. Reson. Med. 26 (2018)
4296