Georgiy Solomakha1, Stanislav Glybovski2, Alexander J.E. Raaijmakers3, Constantin Simovski 4, Alexander Popugaev5, Irina Melchakova2, Pavel Belov2, and Redha Abdeddaim6
1Depatment of Nanophotonics and metamaterials, ITMO University, Saint-Petersburg, Russian Federation, 2Nanophotonics and metamaterials, ITMO University, Saint-Petersburg, Russian Federation, 3Department of Radiology, UMC Utrecht, Utrecht, Netherlands, 4Electronics and Nanoengineering, Aalto University, School of Electrical Engineering, Helsinki, Finland, 5RF and SatCom Systems, Fraunhofer Institute for Integrated Circuits IIS, Erlangen, Germany, 6CNRS, Institut Fresnel, Aix-Marseille Universite, Marsel, France
Synopsis
In this work, we
demonstrate a new RF-coil for 7 Tesla ultrahigh field MRI with two orthogonal
channels to achieve better SAR and SNR of images. The first phase of the work
involves numerical study of different multimode structures consisting of coupled
electrical dipoles to form a radiofrequency coil that may operate both as a
surface loop [1] or a single radiative electrical dipole [2] depending on the
driven channel.
Introduction
Imaging of a human body at ultrahigh
fields (7 T and higher) requires advanced coil arrays. To achieve maximum B1 in
a region of interest (ROI) in transmit and maximum SNR in receive, antenna
elements of these arrays should preferably create circularly polarizaed RF
magnetic field (i.e. operate in the quadrature regime). To enhance performance
of body imaging at such high static fields, especially for deeply located ROIs,
on should design array elements as radiative antennas that enable wave
propagation inside tissues. In ultrahigh field MRI dipole antennas have proven
themselves as coils creating maximum B1 in the center of a human pelvis normalized by an
accepted Tx power and by maximum local SAR [1]. So far, the best performance has been shown
by FDAs (Fractioned Dipole Antennas) [2]. The FDA is a resonant dipole antenna,
miniaturized using multiple quasi-lumped inductors. To create a quadrature coil
the FDA was later equipped with a loop antenna fed by a separate orthogonal
channel [3] (so called dipole-loop antenna). This dual-channel array element configuration
allows to achieve better B1 performance with RF-shimming and reduce maximum
local SAR in complex RF-shimming procedures. In this work, we present an alternative radiative
array element with two orthogonal channels, where two identical coupled dipoles
are combined. By independent excitation of the even and the odd modes of the coupled
dipoles we can create two different field distributions in the ROI very similar
to ones created by a dipole-loop antenna. In this work, the performance of the
proposed array element was investigated by numerical simulations and on-bench
experiments including magnetic field measurements.Methods
The
experimental dual-dipole array element was built of two identical fractioned
dipole antennas both made on RO4003 PCB with 0.803 mm thickness. To excite the modes
independently, the inputs of the dipoles were connected to the outputs of a ratrace
coupler. The latter is a four-port device, with two input and two output ports.
If one input port is fed, the signal is splitted between the output ports with
zero phase shift and equal amplitudes. If the other input port is fed, the
signal is splitted with equal amplitudes, but a 180-degrees phase shift. Outputs
of the coupler are fully isolated, which allow the two modes of the dipoles to
be excited independently. A schematic view of the coil model made in CST Microwave
Studio is presented in Fig. 1a.
The proposed dual-dipole
coil was compared to the dipole-loop coil from [3] taken as a reference. The CST model of the reference coil is shown in
Fig. 1b. Frequency-domain FEM simulation was performed to calculate magnetic
fields and SAR distributions for a given transmit power applied to both
channels. To prove the simulation results we measured H-field distributions in an
anechoic chamber using a near-field scanner at the depth of 6 cm inside a water-salt
phantom. The fractionated dipoles in the proposed coil were similar to one in
the dipole-loop coil and had the length of 30 cm with 5-cm fractions all made
on a common PCB.
In the experiment both
channels of the proposed coil were matched at 298 MHz. The same was done for
the reference coil. In the field measurements the same power was applied to
both the compared coils. Results
The
simulated H-fields both the proposed dual-dipole coil (even and odd mode
channels) and for the reference dipole-loop coil (dipole and loop channels) are
presented in Fig. 2. The measurement results are also presented in Fig. 2 with
markers. The field distributions were normalized to the maximum field created
by the proposed antenna.
As
follows from Fig. 2, the proposed coil (using the even mode) provides 25%
higher RF magnetic field level for the given power than the dipole-loop coil
(the dipole is driven). The odd mode provides practically the same magnetic
field for the given power at the depth of 6 cm. The measured coupling between
the ports of the proposed coil was -23 dB. The simulated B1+ per square root of
maximum SAR level was the same for the compared coils. The measurement results
are in good agreement with simulations.Conclusion
A
new array element suitable for Tx/Rx with possibility of a quadrature
excitation for body imaging at 7 T has been proposed and demonstrated. The
proposed design based on two coupled dipoles exhibited similar RF-fields as the
dipole-loop coil, but with 25% higher transmit efficiency of the even mode due
to higher radiation resistance of a double dipole. The future work consists in
testing the proposed design in an array configuration under RF-shimming.Acknowledgements
This suppored by European
Union’s Horizon 2020 research and innovation
programme under grant agreement No 736937.References
[1] Raaijmakers AJ et al. NMR Biomed. 2016; 29: 1122–1130
[2] Raaijmakers AJ et al. Magn Reson Med. 2016 Mar;75(3):1366-74
[3] Arcan
Erturk et al.v Magn Reson Med. 2017 Feb;77(2):884-894.