Matthias Malzacher1, Nadia Paschke1, Jorge Chacon-Caldera1, and Lothar R. Schad1
1Computer Assisted Clinical Medicine,Medical Faculty Mannheim, Heidelberg University, Mannheim, Germany
Synopsis
23Na MRI keeps increasingly
demonstrating diagnostic value in a multitude of studies and clinical
applications due to its capability to provide information on tissue viability. In
order to co-register 23Na and 1H MR images, a double
resonant 23Na/1H RF system is the optimal solution. In
this work we present a clinical double-resonant RF system consisting of a
shielded 23Na BC coil, a 16 channel 23Na Rx array and a
local 1H Helmholtz coil inside the shielded 23Na BC coil.
The complete system is demonstrated in EM simulations and initial feasibility
measurements are performed.
Introduction
23Na-sodium MRI keeps increasingly
demonstrating diagnostic value in a multitude of studies and clinical
applications due to its capability to provide information on tissue viability[1,2]. Yet, sodium MRI suffers from weak SNR and low abundance of sodium in
the human body.Therefore, 1H MR images are needed for morphological
information to compensate for the poor resolution of sodium MRI. In order to
co-register 23Na and 1H MR images, a double resonant 23Na/1H
RF system is the optimal solution. Since clinical scanners do not support
X-nuclei hardware integrated in the MR system, local coils have to enable
combined proton and X-nuclei MRI. In this work we present a clinical
double-resonant RF system consisting of a shielded 23Na BC coil[3],
a 16 channel 23Na Rx array and a local 1H Helmholtz coil
inside the shielded 23Na BC coil. The complete system is
demonstrated in EM simulations and initial feasibility measurements are
performed.
Methods
Simulation:
EM fields were calculated using FEM simulations (CST – Computer Simulation
Technology GmbH) with a tetrahedral mesh. Mesh refinement converged for all
simulations to at least 5% for all S-parameters at the resonance frequency
32.586 MHz (23Na) and 123.2 MHz (1H).
23Na Tx:
A quadrature driven 16-legged asymmetric 23Na was modeled following reference[3].
23Na Rx:
A 16 channel 23Na Rx only array was designed with 8 posterior
and 8 anterior channels to be used for the abdomen. The Rx elements were decoupled
iteratively using EM simulations. Each Rx coil was split twice and a 1H
trap was added. The H-fields of the 23Na Rx channels were combined using the
matched filter approach[4].
1H TxRx:
The 1H TxRx coil was constructed as a Helmholtz coil covering
the FoV of the 23Na Rx array. Each loop of the Helmholtz coil was
equally split 16 times.
Phantom:
Four cylindrical phantoms were used with diameter = 115 mm,
length = 205 mm, σ = 0.91 S/m
and ε = 80.
The simulation setup of the different coils separately and the complete
simulation setup are shown in Figure 1 a).
Measurement:
For initial feasibility measurements, the posterior part of
the setup consisting of an 8 channel 23Na Rx only coil
(Figure 2) combined with one 1H TxRx posterior coil was built using
the dimensions of the EM simulation. Four cylindrical phantoms (Siemens
Healthineers, dimensions and solution as described above) were used for phantom
measurements.
We used a density adapted 3D radial sequence[5] for sodium imaging (TE/TR/FA=0.54ms/50ms/54°,
8500 projections, FoV=(450mm)3, resolution=(6mm)3, TRO=20ms),
and a 2D gradient echo sequence for proton imaging (TE/TR/FA=10ms/358ms/90°,
FoV=450mm², matrix=256²,Res = 1.75 mm, slice=5mm).
The reference scan was acquired using the 23Na BC coil stand alone
in TxRx mode.
In order to protect the detuning PIN diodes of the 23Na BC coil it stayed
resonant during the 1H measurement but the 23Na Rx array
was detuned.
For SNR calculation a noise scan was performed
using the same parameters as for the signal scan but without Tx power applied.
The 23Na Rx channels were combined identical to the simulation
using the matched filter approach.Results
Simulation:
The center coronal planes of the simulated B1-maps (normalized
to 1W accepted power) are shown
in Figure 1 b). The 23Na array showed a 2-fold B1-field
increase compared to the 23Na BC coil. The 23Na array
yielded an up to 6-fold higher B1-field compared to the 23Na
BC coil near the Rx coils.
The 1H TxRx coil covered almost the whole FoV of the 23Na
Rx array but showed a slightly unbalanced behavior in the longitudinal
direction.
Measurement:
The center coronal planes of the SNR measurements are shown in Figure
3. Consistent with the simulations, the 8 channel 23Na Rx only array
already achieved a 2-fold SNR increase in the coronal plane and an up to 6-fold
SNR increase near the Rx coils compared to the 23Na BC coil.
The 1H SNR map revealed a similar
FoV as the 23Na Rx only array.
Yet, the coil profile was unbalanced in longitudinal direction.Discussion & Conclusion
A double resonant 1H/23Na whole-body RF setup was demonstrated
for clinical MRI at 3T. The feasibility of a 16 channel 23Na Rx only
array combined with a 1H Helmholtz coil inside a 23Na BC
coil was proven in simulation. A 2-6 fold improvement of the 23Na
array was achieved over the whole FoV in simulation. This performance could also be
reproduced in initial SNR measurements of a reduced setup.
Yet, the rudimentary 1H coil revealed an unbalanced coil profile and
low SNR. Future research should focus on getting 1H performance near
to a clinical level. The RF setup should additionally be evaluated in in-vivo scans.Acknowledgements
No acknowledgement found.References
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