Myung Kyun Woo1, Chang-Ki Kang2, and Zang-Hee Cho3
1Electrical and Computer Engineering, Seoul National University, Seoul, Korea, Republic of, 2Neuroscience Research Institute, Incheon, Korea, Republic of, 3Seoul National University, Seoul, Korea, Republic of
Synopsis
This
abstract is to propose and evaluate the
Spiral Extended Monopole antenna Array with individual Shield (SEMAS) coil. This coil
was compared with the original Monopole antenna Array (MA) coil and an Spiral Monopole antenna Array coil with no shield (SMA) coil. The SEMAS coil showed
larger flip angle than the MA and SMA
coils in the inferior areas of the brain and relatively uniform flip angles across the brain.Target audience
Radiofrequency (RF) engineers, anyone interested in high field RF coils.
Introduction
A radiative antenna has been proposed to address
more uniform B1+ and B1- patterns
than currently available loop array coils at Ultra High Field (UHF) [1]. When
applied for imaging the whole brain, however, a limited z-directional coverage
of the original Monopole Antenna Array (MA) coil caused degradation in the transmit
and receive performance in the inferior areas of the brain [2].
Fig.
1. Picture of SEMAS coil. The upper
corners of the ground plate were cut to prevent a direct contact of the MRI
bore.
In this work, we explored a new design of the transceiver
monopole antenna coil. We modified monopole antenna array coil to a spiral type
[3]. This coil, which we refer to as an Spiral Extended Monopole antenna Array
with individual Shield (SEMAS) coil, has an increased length of monopole
antennas with shields. To demonstrate the advantage of this newly designed
coil, the performance was compared to the MA coil as well as the Spiral Monopole
antenna Array (SMA) coil [3,4].
Methods
The
photos of new coils are shown in Fig. 1.
Each coil has eight equally spaced monopole antennas, and each antenna is
connected to a coaxial cable via a ground plate at one end. The copper ground on acrylic plate (size of
plate: 36 x 36 cm2) was divided into 21 pieces (size of each piece: 5
x 12 cm2) to reduce eddy current. The divided ground
plates were connected to ceramic capacitors (330 pF). In the original MA coil,
the length of an monopole antenna was adjusted to 20 cm (SMA: 14.1 cm, SEMAS:
20 cm through the z-direction) In the SEMAS coil, copper shields (size of shield: 2 x
28.3 cm2) were placed on both sides of the monopole antenna. The
shields were spaced 1 cm away from the monopole antenna. The distance between
the feeding point of the monopole antenna and the shield was 2 cm.
Fig. 2. (a)
Measured flip angle maps (in degrees) and (b) receive sensitivity maps (in
arbitrary units) in the sagittal, coronal and axial planes. The images are
from mid-sagittal, mid-coronal and a lower axial planes. The number
represents a quantitative measure at an ROI (3 x 3 cm2)
All imaging experiments were performed on a 7T MRI
scanner (Siemens Medical Solutions, Erlangen, Germany). A custom-designed
interface box with an eight-channel power divider was utilized to distribute
the transmit signal to each coil equally. To compare the flip angle
distribution among the three coils, actual flip angle imaging (AFI) pulse
sequence (TR1 / TR2 = 20/100 ms and TE = 3.1 ms, bandwidth = 330 Hz/pixel) was acquired.
To investigate the SNR of each coil, proton density-weighted images (TR = 1000
ms, TE = 2.5 ms,) were obtained for the sagittal, coronal and axial planes. The
reference voltage of MA, SMA and SEMAS for imaging was 240 V.
Results
Fig. 2 shows the measured flip angle maps (Fig. 2a) and the receive sensitivity
maps (Fig. 2b) of the MA, SMA and SEMAS acquired by experiment in sagittal,
coronal and axial view, respectively. All of quantification of specific ROI’s
in the sagittal view is marked in Fig. 2.
The
receive sensitivity (Fig. 2b) in the three coils are no significant differences
through the z-direction. The maximum standard deviation difference of the same
ROIs among the three coils was shown at the occipital lobe. However the measured
flip angle of the SEMAS coil are substantially higher compared to the MA and
the SMA coils. The SEMAS coil shows larger mean flip angles values than the
other two coils (SEMAS: 16˚, MA: 8˚, SMA: 11˚). And the standard
deviation of the measured flip angle was significantly different among three
coils (SEMAS: 9, MA: 25, SMA: 19). A similar observation can be seen in the coronal
and axial plane at measured flip angle maps where the SEMAS coil shows larger flip
angles than the other coils.
Discussion and Conclusion
In this study, we have demonstrated that the
newly designed monopole antenna coil, SEMAS, improves B1+
field uniformity in the whole brain and it efficiently penetrates into the deep
brain when compared with the MA and SMA coils. The improvement was particularly
significant in the inferior part of the brain where the brainstem and the
cerebellum are located. Hence, the new coil may potentially be used for
clinical and scientific applications at UHF (≥
7T) that require a wide spatial coverage including the brainstem and cerebellum
areas.
Acknowledgements
Acknowledgement: This
research was supported by the Brain Research Program through the National
Research Foundation of Korea(NRF) funded by the Ministry of Science, ICT &
Future Planning (NRF-2015M3C7A1031969).References
[1] Raaijmakers et. al. MRM, 66, 5 (2011), [2] SM Hong et. al., MRM,
71, 5 (2014), [3] Alsop et. al., MRM, 40,5 (1998), [4] MK Woo et.al., MRM, doi: 10.1002/mrm.25837