Joseph Busher1 and Mary P. McDougall1,2
1Biomedical Engineering, Texas A&M University, College Station, TX, United States, 2Electrical and Computer Engineering, Texas A&M University, College Station, TX, United States
Synopsis
Keywords: Non-Array RF Coils, Antennas & Waveguides, Non-Array RF Coils, Antennas & Waveguides
Multi-frequency coils are typically known to have substantial
losses as compared to their single-tuned counterparts. Here we investigate sensitivity tradeoffs
of triple-tuned (
1H-
23Na-
31P) trap designs on
receive coils in a tightly controlled experiment to isolate the sensitivity
effects of the traps. Triple-tuned LCC traps were shown to have
significant improvement in sensitivity for
23Na and
1H as
compared to an LC trap design. The increase came at the expense of
31P
sensitivity, however continued optimization of the trap design will likely
further improve the final experimental SNR.
Introduction
Multinuclear NMR experiments require the application
of specialized multi-tuned coils with high receive sensitivity to compensate
for the inherently low SNR (signal to noise ratio) of these X-nuclei. Several
approaches are taken to multi-nuclear tuning including nesting coils1-3, and switching designs4,5, but one of the
most common approaches is the use of traps6,7. Traps benefit from the elimination
of redundant coils of nested designs while still allowing for true simultaneous
multi-tuning which can enable applications that include proton decoupling and
the nuclear Overhauser effect. The use of LC trap circuits for multi-tuned
coils is well established6, and double-tuned
LCC traps more recently have been shown to increase efficiency by minimizing
the effects of the resistive losses of inductors7. To the authors’
knowledge the application of LCC traps has yet to be extended to triple-tuned
designs. The work presented here investigates the potential applications and
benefits of LC and LCC traps for triple-tuned receive coils.Methods
Triple-tuned 4cm diameter loop coils were designed for 1H
(200MHz), 31P (81MHz) and 23Na (53MHz) at 4.7T using 18AWG
polyurethane coated wires soldered to tune networks designed on milled 1oz
copper clad FR4 boards. Identical
board designs were used for all three configurations with traces appropriately
left open and shorted to remove the effects of varied board impedance on the
sensitivity measurements. Single-tuned reference coils were
coarsely tuned using fixed tuning capacitors (Passive Plus 1111C Series) and
finely tuned using variable trimmer capacitors (Sprague Goodman, SG3C Series)
using the circuit schematic shown in Fig. 1A. Triple-tuned networks were
designed using series LC traps (Fig. 1B), and series LCC traps (Fig. 1C) to
compare the benefits of a triple-tuned LCC network to those of an LC trap
design. Inductors were hand wound using 24AWG polyurethane coated wire with
varying diameters to achieve the desired inductance and positioned orthogonally
on the coil boards to limit coupling. To compare relative sensitivity of the
different tune networks a custom test platform was designed to place each coil
design repeatably in the same position over a phantom (Fig. 2A) of
physiological sodium and phosphorus concentrations (30 mM NaCl and 9.4 mM H3PO4).
Crossed (i.e. decoupled) double loop probes were used to measure the relative sensitivities
at a depth of 2.5 cm away from the coil (Fig. 2B) via an S21 measurement at
each resonant frequency of the coils.Results
Photographs of the coils with representative single-tuned (Fig. 3A),
triple-tuned LC (Fig. 3B) and triple-tuned LCC (Fig. 3C) traps are shown. Relative
sensitivity measurements (Table 1) show that LCC traps produce a roughly 4dB
improvement in sensitivity as compared to an LC design for 1H. When
compared to a single-tuned coil, the LC trap showed a 12.4 dB and 6 dB loss in
sensitivity for the lowest and middle frequency respectively whereas the LCC
trap design showed a 5.6 dB and 13.6 dB loss in sensitivity for the lowest and
middle frequency respectively. The test platform with decoupled double-loop
probes was used to consistently compare coil sensitivity, allowing for a
uniform comparison of relative coil sensitivities across the different coil/trap
designs and ensure any measured difference in sensitivity is a result of the
trap designs only.Discussion
While the frequency requirements of triple-tuned
circuits further constrain the valid inductance combinations in series traps,
complicating their optimization as compared to similar double-tuned experiments,
the implementation of LCC traps substantially improved the sensitivity at two
out of three frequencies in the triple-tuned configuration as compared to an
analogous LC trap design. Although this improvement is at the expense of the
middle frequency, the design increased sensitivity for the other two nuclei
allowed for a net improvement in sensitivity over the LC trap design. Quantification
of trap sensitivities can be further used to motivate/inform the number of
array elements necessary to recover the losses associated with the
triple-tuning circuitry. While implementation of multi-frequency matching
networks will be added for the final coil design, the methods used here for testing
the sensitivity without this added complexity allowed for a purer measure of
the effects of the trap design on the coil sensitivity. Further optimization of
the design is needed to improve sensitivity at the middle frequency, but
potential studies for varied inductance combinations and the possibility to
combine the LC and LCC traps for triple-tuning circuitry to maximize their
respective benefits offers tremendous potential.Conclusion
Two port measurements on resonant coils without the
additional matching network components, a physical platform for repeatable
measurements, and identically designed PCBs for the trap configurations likely
allowed for a more independent indicator of true trap performance. While it is
noted that matching networks will be needed in future works, these methods
allow for separate analysis of losses associated with each component of the
coil and allow for more thorough optimization of triple-tuned designs. While
further sensitivity improvements of trapping circuitry to benefit all
frequencies simultaneously is needed, the work here presents valuable insight
into the optimization of traps for simultaneously triple-tuned coils.Acknowledgements
The authors gratefully
acknowledge funding for this project provided by NIH grant number R01EBO28533.References
1. Busher,
J., Valle, E., Wright, S. M. & McDougall, M. P. in Proceedings from the ISMRM ESMRMB Joint Annual Meeting.
2. Augath,
M., Heiler, P., Kirsch, S. & Schad, L. R. In vivo 39K, 23Na and 1H MR
imaging using a triple resonant RF coil setup. Journal of Magnetic Resonance 200,
134-136 (2009).
3. Du,
F. et al. in 2019 IEEE International Conference on Real-time Computing and Robotics
(RCAR). 598-603 (IEEE).
4. Carrell,
T., Bosque, R. D., Wilcox, M. & McDougall, M. P. in Proceedings of the ISMRM 27th Annual Meeting.
5. Maunder,
A., Rao, M., Robb, F. & Wild, J. M. Comparison of MEMS switches and PIN
diodes for switched dual tuned RF coils. J
Magnetic resonance in medicine 80,
1746-1753 (2018).
6. Schnall,
M. D., Harihara Subramanian, V., Leigh, J. S. & Chance, B. A new
double-tuned probed for concurrent 1H and 31P NMR. Journal of Magnetic Resonance (1969) 65, 122-129, doi:10.1016/0022-2364(85)90380-4 (1985).
7. Meyerspeer, M., Seres Roig, E.,
Gruetter, R. & Magill, A. W. An improved trap design for decoupling
multinuclear RF coils. Magn Reson Med
72, 584-590, doi:10.1002/mrm.24931
(2014).