M. Arcan Erturk1 and Gregory J Metzger1
1Center for Magnetic Resonance Research, University of Minnesota, Minneapolis, MN, United States
Synopsis
Using endorectal
coils (ERC) in combination with external surface arrays (ESA) can improve the
SNR inside the prostate at 7.0T. When used in transmit, ERC can provide higher
B1+ levels at the expense of field uniformity. Here, we develop a novel
actively-tuned ERC that can be used both in “transmit” and “receive-only” modes
utilizing the high B1+ of the ERC and field uniformity of the ESA inside the
prostate. Transmit capabilities of this approach are investigated using
simulations in a human model. Prostate
MRI is acquired using the combined ESA+ERC approach to demonstrate the
feasibility for translational studies at 7.0T.Introduction
Endorectal
coils (ERC) can improve the SNR inside the prostate at 7.0T, and are primarily advantageous
when used in receive-only mode in combination with an external surface array
(ESA) [1]. When used for field transmission alone or in
combination with an ESA, ERC can provide higher B1+ fields in the prostate at
the expense of field uniformity compared to ESA-only excitation. The ability to
dynamically control the tuning state of the ERC would permit the coil to be
detuned (i.e. turned off) during transmit for more controlled/homogeneous B1+
performance or tuned (i.e. turned on) for combined transmit for peak B1+
performance. Here, we develop an actively-tuned
ERC that can be used both as a transmitter and a receive-only coil in
combination with an ESA for improved prostate MRI capabilities at 7.0T.
Methods
Choke inductors and PIN diodes were added to a rigid
two-channel ERC [2] to enable tuning/detuning capabilities
(Figure 1.a). The ERC was tuned to 7.0T (297.2MHz) by applying a 100mA DC bias,
for use as a transmitter and/or receiver (Figure 1.b). By blocking the current,
the PIN diodes act as open circuits and the ERC becomes “invisible” to the ESA-only
excitation (Figure 1.c). The physical implementation of the actively-tuned ERC
and the sterilizable housing are shown in Figure 1.e. The hardware components, connections
and switching of the ERC between tuned/detuned states are explained in Figure
2.
Fourteen channels of a 16-channel combined loop-dipole
transceiver array (six-loops, eight-dipoles) were used as the ESA. The remaining
two ESA channels (two-loops) were terminated with 50Ω to accommodate the ERC
channels.
The ERC was modeled both in a tuned and detuned state
with the ESA to determine the excitation scheme in different operating modes
(i.e. ESA alone or ERC+ESA). EM-field distributions of each coil element were
computed using an FDTD solver in SEMCAD software (SPEAG, Zurich, Switzerland)
to investigate shim-dependent B1+ and SAR distributions. Peak
1g-averaged SAR around the rectum and 10g-averaged SAR inside the pelvis were
calculated using virtual-observation points [3].
A consented healthy
subject was scanned under an IRB approved protocol. Scanning was performed on a
whole-body Magnetom 7.0T system (Siemens Healthcare, Erlangen, Germany) using
the ESA combined with the actively-tuned ERC.
Results
Simulated transmit performance metrics of the ESA+ERC
combined and ESA-only excitations are shown in Figure 3. Depending on the
amplitude/phase settings, 1g-averaged SAR around the rectum or 10g-averaged SAR
around the skin can be the limiting factor for RF safety (Figure 3.a). The coefficient
of variation (CV) of the B1+ magnitude inside the prostate is plotted in Figure
3.b, and demonstrates, as expected, that the ESA-only excitation can provide a
more uniform field distribution (i.e. excitation scheme 2). ESA+ERC combined
excitation can provide >40% higher B1+ SAR efficiency compared to the ESA
alone (Figure 4.b). Using a B1+ shim with a tradeoff between homogeneity and
efficiency (i.e. Scheme 1, Shim B), uniformity of the ESA+ERC excitation can be
improved at the expense of transmit efficiency (Figure 4) compared to a pure
efficiency solution (scheme 1, shim A). Anatomical turbo spin-echo MRI of the
prostate at 0.4mm2 in-plane resolution are shown in Figure 5. Images
in Figure 5.a-b are acquired with ESA-only (i.e. Scheme 2) and Figure 5.c is acquired with
ESA+ERC (i.e. Scheme 1, Shim B) combined excitation.
Discussion/Conclusion
Traditionally, DC bias is used to detune receive-only
coils during RF transmission, but here this approach was not applicable because
high RF currents during ERC transmission might activate the PIN diodes and
force the coil into “detuned” state even if the intention was to have it
“tuned”. Therefore an “inverse” logic is employed, and the ERC is
actively-tuned by applying a DC bias. Series PIN diodes reduced the SNR of the
ERC by 0.2dB.
In receive-only mode, the ERC is virtually “invisible” to
the ESA-excitation; without accomplishing this, coupling can cause
unpredictable field inhomogeneities close to the ERC. Combined ESA+ERC
excitation can improve the B1+ transmit and SAR efficiencies compared to
ESA-only excitation. Achieving high B1+ SAR efficiency is crucial for enabling
SAR-intensive pulse sequences (i.e. turbo spin-echo, spectroscopy). Dynamically
alternating between different shim solutions for individual RF pulses [4] can improve performance. For example, Scheme
1 (combined ERC+ESA) would be used for B1+ insensitive pulses such as adiabatic
refocusing [5, 6] while other pulses including lipid
suppression, water suppression and excitation could use Scheme 2 (ESA-only). The
current in vivo imaging only demonstrated that the physical realizing of the
coil works in MRI, however exploiting and characterizing the advantages of dynamic
switching within specific acquisition protocols is currently under investigation.
Acknowledgements
Supported by: NCI R01 CA155268, NIBIB
P41 EB015894. References
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