Qi Duan1, Jeff H. Duyn1, 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
7T
spine array based on electric dipole antenna starts to gain attention recently.
Nevertheless, the transmit efficiency of the dipole has a natural decay from
the feeding point, which does not necessarily corresponding to the target
imaging area. In addition, a variety of patient size requires the dipole to be
reconfigured for optimum performance. In this work, we propose a concept of
“segmented dipole” that can be remotely reconfigured for transmit field-of-view
shifting, tuning, and impedance matching characteristics without the need of a
parallel-transmit system. A prototype transmitter was built and the
reconfiguration capability was demonstrated at a 7T scanner.Purpose
Electric
dipole based antenna provides a simpler and more efficient design as RF
transmitters for 7T spine imaging
1. The transmit efficiency for the dipole antenna is
always highest at the center of the antenna and decay as a function of the
distance to the center. In clinical practices (e.g. spinal multiple sclerosis
studies), the region of interests usually do not coincide with the center of
the dipole, led to lower local transmit efficiency and thus higher RF heating
penalties. Since it is practically prohibitive to relocate the patients inside
the scanner, it is desirable if the transmit field-of-view (FOV) can be re-adjusted
remotely in the console room. In addition, patient-specific adjustment of the
tuning and the matching of the transmitter can further increase the transmit
efficiency. In this context, we propose a new concept of “segmented dipole” in
this work, which can be easily reconfigured remotely for each subject. An
example transmitter was built for demonstration purpose with the
reconfiguration capability demonstrated at a 7T scanner.
Methods
The
basic idea of segmented dipole is shown in Figure 1. The continuous dipole is
divided into several segments. A “length control” unit is inserted between each
segment, and an “impedance control” unit is inserted between the balun and the
adjacent segment. A simple implementation of the length control unit contains a
PIN diode in series of the dipole, a parallel trap to improve isolation, and
other supporting components like RF chokes. In this way, each segment can be
easily switched on or off. The impedance control unit contains several parallel
sub-units, each of which contains a capacitor in series with a PIN diode with
corresponding control lines. Depending on the balun design, the impedance
control unit can be integrated with the balun itself. All the control DC lines
can be connected to a control unit in the console room for remote adjustment.
To
demonstrate the feasibility of the proposed segmented dipole design, a
segmented dipole with four length control units as well as four impedance
control units was built, with its diagram shown in Figure 2. Except for the two
segments that connect to the balun, all other segments have same length. Such
setup could provide nine different dipoles with various combinations with
different tunings. Among these combinations, some of them, such as λ0+1+2,
λ0+1+3, and λ0+2+4, have the same resonant frequency but
different center locations. Thus, by choosing different combinations, the
transmit FOV can be shifted without changing the tuning. The impedance change
due to reconfigurations can be further compensated by the impedance control
units (with 16 possible combinations) to further improve transmit efficiency.
MR
experiments were performed on a Siemens Magnetom 7T-830-AS scanner. The
segmented dipole was placed about 2cm above a gel phantom mimicking human
muscle dielectric properties at 7T2. A control box with eight switches was used to
provide the control signal. Gradient-echo images were acquired at the center
sagittal plane that going through the dipole, with following parameters: voxel
size 1.6x1.6x10 mm3, image matrix size 256x112, TE 3.53ms, TR
500ms, Flip angle 50 degrees.
Results and Discussions
The
capability of shifting transmit FOV is clearly demonstrated in Figure 3, using λ0+1+3
configuration (left) and the λ0+2+4 configuration (right). Figure 4
shows images acquired with three different impedance control settings with the
same length control settings, with significant changes in penetration and
sensitivity. In fact, the image intensity dynamic range achievable by the
impedance control was more than six folds.
With
combination of better control signal generator, e.g. FPGA, system with much
finer reconfiguration capability can be implemented. In addition,
three-dimensional (rather than the traditional 2D) field steering can be easily
realized by combining two segmented dipoles and reconfiguring each individual
transmit FOV simultaneously adjusting the phase differences between them.
Similar
functionality may be implemented by separate loops along the longitudinal
direction. However, in comparison to the segmented dipole setup, it would have
lower efficiency1, as well as considerably increased the amount and the
complexity of supporting electronics (e.g. a flexible power divider
simultaneously supporting 2-way and 3-way power distribution), or requiring a
parallel transmit system.
Conclusion
Segmented
dipole framework was proposed for easy remotely reconfiguration of transmit
FOV, tuning, and matching of the dipole transmitter. The feasibility was
demonstrated with a small-scale implementation. The proposed work can
personalize the transmitter and thus improve the transmit efficiency for each
subject.
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.