Zachary Colwell1, Djaudat Idiyatullin2, Lance DelaBarre2, Thomas Vaughan3, Michael Garwood2, and Sung-Min Sohn1
1School of Biological and Health Systems Engineering, Arizona State University, Tempe, AZ, United States, 2Center for Magnetic Resonance Research, Department of Radiology, University of Minnesota, Minneapolis, MN, United States, 3Zuckerman Institute, Columbia University, New York, NY, United States
Synopsis
Simultaneous Transmit and
Receive (STAR) requires high decoupling between the RF transmitter and receiver.
Current methods for this include, but are not limited to: geometric isolation,
active RF leakage cancellation and metamaterial decoupling. The presented
method uses a passive, four-port, tunable canceller circuit to achieve upwards
of 40 dB of isolation between a quadrature transmit coil pair and the single
receiving coil for a 1.5T system.
Introduction
Because STAR, also denoted as CEA1 for “Concurrent Excitation
and Acquisition” requires high transmitter-receiver isolation (greater than 70
dB), multiple layers of isolation are required to not overflow the dynamic
range of the pre-amplifier and to extract MR signals2. Geometric
coil decoupling and active RF leakage cancellation do not necessarily provide
enough isolation, and metamaterials tend to be bulky for the large wavelength
of 1.5T (64MHz Larmor frequency)3. Utilizing multiple layers of isolation (i.e.
using geometric decoupling along with a canceller circuit) pushes us closer to
STAR’s requirements. Another layer of isolation can thus come from a
transmitter-receiver canceller circuit based on microstrip coupled lines with passive,
tunable components when it is tuned to the target Larmor frequency.Methods
The system contains a
quadrature pair of transmit RF coil elements, a single receive coil element, a
hybrid coupler, a filter and the passive tunable canceller, as shown in figures
1 and 2. The canceller circuit consists of four ports: transmit-in,
transmit-out, receive-in and receive-out. The schematic is also shown in figure
2, where the circuit is composed of three sections: the transmit path, the
receive path and the cancellation path. Transmit-in and transmit-out are
directly connected via microstrip lines, as are receive-in and receive-out.
Transmit-in and receive-out are connected to the vector network analyzer to
measure S21 (isolation) and S11 (Tx return loss) on the
bench, while transmit-out and receive-in are connected to the RF coil elements.
Both the transmit and receive microstrip lines are coupled to another pair of
microstrip lines, which feed the cancellation path as a network of tunable
capacitors, inductors, and resistors. A narrowband analysis of this type of
network has been reported previously4 and 5. As these tunable
devices are varied, the sampled RF signal from the transmit line to the receive
line undergoes destructive interference through the cancellation path. This
destructive interference stems from the tuning of the amplitude of a
cancellation signal via resistors and the phase of the cancellation signal via
capacitors and inductors. The system is tuned when decoupling is maximized while
maintaining coil performance. Results and Discussion
Using Keysight’s ADS, the entire system was simulated with the coils and
a phantom model. Figure 3 shows the simulated results, where we can see the
return loss (S11) of the transmitting antenna to be approximately 35
dB with a decoupling factor (S21) of more than 50 dB. Figure 4 shows
the physical system data with and without the canceller present. With the canceller
added to the system and comparing the red dot-dash line to the black dot-dash line,
we get an increase in isolation from around 25 dB to 40 dB. The change in
transmit coil return loss from 40 dB to 35 dB is seen by comparing the solid
red line to the solid black line—a negligible difference in terms of transmit
power loss. The reason for such a flat and low return-loss plot with the canceller
bench test is due to the use of a quadrature setup, thus using a 3 dB hybrid
coupler feed with a higher bandwidth than the coil. In practice, 40 dB of
isolation can be achieved but not sustained due to coil tuning and loading sensitivity.
This sensitivity issue is currently being investigated by adding an active
matching circuit after the transmit-out port. Conclusion
High isolation between
the transmitter and receiver is critical for STAR. A passive and tunable canceller
provides a quick, simple, low cost, low power means of contributing to the
isolation stack with a nominal cancellation of 40 dB and without degradation to
transmitter power. The residual leakage signal after this canceller can be
removed in the digital domain after the preamplifier. In addition, this
decoupling technique would be useful for general purpose RF coil decoupling
between channels. Acknowledgements
No acknowledgement found.References
1. A. C. Özen, E. Atalar, J. G. Korvink, and M. Bock, “In vivo MRI with Concurrent Excitation
and Acquisition using Automated Active Analog Cancellation,” Sci. Rep., vol. 8, no. 1, pp.
1–12, 2018, doi: 10.1038/s41598-018-28894-w.
2. Sohn, S.‐M., Vaughan, J.T., Lagore, R.L., Garwood, M. and Idiyatullin, D. (2016), In vivo
MR imaging with simultaneous RF transmission and reception. Magn. Reson. Med., 76:
1932-1938. https://doi.org/10.1002/mrm.26464
3. Duan, G., Zhao, X., Anderson, S. W., & Zhang, X. (2019). Boosting magnetic resonance
imaging signal-to-noise ratio using magnetic metamaterials. Communications Physics, 2(1).
https://doi.org/10.1038/s42005-019-0135-7
4. K. Nishimoto, H. Makimura, T. Yanagi, Y. Nishioka, Y. Nofumi, and H. Miyashita,
“Narrowband/Wideband Decoupling Networks for Antenna Arrays and Exciation
Distribution Control,” IEEE.
5. S. -M. Sohn, A. Gopinath and J. T. Vaughan, "A Compact, High Power Capable, and Tunable
High Directivity Microstrip Coupler," in IEEE Transactions on Microwave Theory and
Techniques, vol. 64, no. 10, pp. 3217-3223, Oct. 2016, doi: 10.1109/TMTT.2016.2602835.