Qi Duan1, Natalia Gudino1, and Hellmut Merkle1
1Laboratory of Functional and Molecular Imaging, National Institute of Neurological Disorders and Stroke, National Institutes of Health, Bethesda, MD, United States
Synopsis
In this work, we propose concepts of transmit arrays
based on combination of monopole and dipole antennas and their variations for high
field imaging. Based on these concepts, transmit arrays for a variety of applications
can be derived based on parameters such as desired and possible transmit
field-of-view, number of available transmit ports, etc. For illustration
purpose, a special case of the second order array, a.k.a. the Trident antenna,
was built for spine or posterior cortex imaging and tested on phantom at a 7T
scanner.Purpose
Recent advances in RF transmission for MRI suggested
that at high field (7 T or higher), electric antennas could be used as an
alternative transmitters. In this work, we propose general concepts of “Multi-pole
antenna array”, which combines monopole, dipole antennas, and their variations
to form a transmit array for various purpose. The general concept was first
explained. For demonstration purpose, several examples of second order array,
i.e. quadrature antenna array, were proposed. In this study one example, the
Trident antenna, was built and tested both for spine imaging and cortex imaging
on human mimicking phantoms at 7 T.
Methods
The multi-pole array can be composed by monopoles,
dipoles, and their combinations. Figure 1 shows some of these examples, among
which monopole and “bident” (a bent dipole) have roughly half of the
field-of-view (FOV) in comparison with a dipole. These basic building blocks
can be used to build higher order array, based on the number of available
transmit ports and target transmit FOV (as shown in Figure 1).
Quadrature antenna arrays for second-order multi-pole
implementations on a single transmit scanner are shown in Figure 2. The
effectiveness of dipole array implementation has already been shown previously
for spine imaging1 at 7 T. The
other arrays, which have roughly half of FOVs, have the potential to be used
for brain imaging particularly at 7 T or higher fields. In all implementations, the scanner transmit
power is split by a single hybrid to drive two antennas; additional phase delay
can be added in one of the ports to realize field steering.
For demonstration purpose, two trident antennas, one
for spine and one for posterior cortex, were implemented as a transmit receive
antenna and tested on gel phantoms2 mimicking dielectric properties of target tissues at
7 T (Figure 3), the length of the monopole was about 240 mm, whereas each arm
of the dipole is about 225 mm. The reflection coefficient, S11, for
the trident was better than -24 dB.
MR experiments were performed on a Siemens Magnetom
7T-830-AS scanner. To demonstrate the field steering capability,
cables with different phase delays were inserted between the balun and the
90-deg port of the hybrid while axial gradient-echo (GRE) images were acquired
at the center of the trident.
Results and Discussions
GRE images from the dipole spine array as well as the
two tridents are shown in Figure 4, with all arrays used as transmit-receive
coils. Images with three different phase delays were selected for each array: one
has minimum intensity in the middle of the array (left), one has maximum
intensity at that location (right), and one phase delay in between (middle). Field
steering capability is clearly demonstrated.
Similar to the circular dipole3, the bident antenna shares some similarities with circular
dipole or even loop coil to some extent, e.g. the possibility of overlapping
for decoupling, and the transmit field twisting observed. This fact can be
taken into consideration when designing higher order arrays for reducing
inter-channel coupling. Although it has be shown that circular dipole could
possibly achieve similar performance with a dipole at the center3, similar investigation for the bident should be
performed in the future.
Inter-channel coupling could be another issue for
antenna array in general. In principle it can be reduced to some extent with
careful geometric layout. In addition, the heavy loading could improve the directionality
of the antenna thus may help to reduce the issue. Given the transmitters at
high field are usually low-Q, other tricks like slightly detuning could further
reduce the coupling. Additional benchtop testing or simulation could be needed
for further investigation. Nevertheless, it has been shown previously1 that moderate coupling is tolerable in some
situation.
In general, construction of a dipole or its variant is
simpler than building a monopole. It was noticed in practice and simulation
that monopole seems to be sensitive to the design of the ground plane. Besides
the examples presented here, other antenna designs, e.g. circular dipole array
can be easily integrated within the proposed framework.
Conclusion
A general framework of multi-pole was proposed for
antenna array design. Several quadrature array designs using second order multi-poles
were proposed. Trident antennas, a special case of these arrays, were built for
human spine and human posterior cortex imaging, with its field steering
capability demonstrated on phantom at 7 T. The proposed framework can be used
as guidance when designing new antenna arrays.
Acknowledgements
This
research was supported by the Intramural Research Program of the
National Institute of Neurological Disorders and Stroke.References
1. Duan Q, Nair G, Gudino N,
et al. A 7T spine array based on electric dipole transmitters.
Magnetic Resonance
in Medicine. 2015;74(4):1189-1197.
2. Duan Q, Duyn JH, Gudino N,
et al. Characterization of a dielectric phantom for high-field
magnetic resonance imaging applications. Medical
Physics. 2014;41(10):102303.
3. Lakshmanan K, Cloos M,
Lattanzi R, Sodickson D, Novivkov D, Wiggins G. The Circular Dipole.
Joint Annual Meeting
ISMRM-ESMRMB. Milan, Italy: International Society for Magnetic Resonance in
Medicine; 2014:315.