Aidin Ali Haghnejad1, Shaihan J. Malik2, Francesco Padormo2, Cornelis A.T. van den Berg1, Peter R. Luijten1, Dennis W.J. Klomp1, Joseph V. Hajnal 2, and Alexander J.E. Raaijmakers1
1UMC Utrecht, Utrecht, Netherlands, 2King's College London, London, United Kingdom
Synopsis
The
birdcage body coil at 3T has some considerable disadvantages. Most of all it
has very large power requirements. The use of local transmit arrays severely
reduces these power requirements. In this study, we intend to explore the use
of dipole antennas as transceive surface array elements at 3T. Three designs
are investigated after which a strongly meandering dipole antenna is selected.
An array of eight of these element is used for prostate imaging at 3T in a 8ch.
multi-transmit MRI system. Using 8x200W input power, 12 µT is achieved inside the prostate. Relatively
homogeneous T2w images have been acquiredIntroduction
The introduction of the birdcage body coil in 1985[1] has enabled unprecedented B1-field homogeneity. However, at 3T the use of the birdcage body coil has some considerable disadvantages. These include sometimes suboptimal B1+ homogeneity for abdominal imaging and high local SAR levels[2] but most of all: very large power requirements. A phantom study has shown that the use of a local transmit array of loop coils severely reduces these power requirements [3]. In this study, we intend to explore the use of dipole antennas as transceive array elements at 3T.
Methods
Dipole antennas are being used frequently at ultrahigh field
strengths. However, at 3T, the use of dipole antennas requires the addition of
large inductances to the antenna legs to keep them at a reasonable size. We
compared three designs: a segmented dipole antenna where lumped elements
inductors are added between the segments, an antenna where the inductance was
added in the shape of 9 meanders and a similar antenna with 12 (more narrow)
meanders. Elements are evaluated by a
single channel B1+ measurement on a pelvis shaped phantom with
tissue-resembling properties (εr=34, σ=0.4).
AFI B1+ maps have been acquired to compare the performance of each design.
The single element measurements resulted in a clear
advantage for the antenna with 12 meanders . A transceive array of eight of
these dipole antennas has been realized for a 8-channel multi-transmit 3T
system (Philips Healthcare, Best, The Netherlands). In addition, the system was
equipped with an 8-channel Tx/Rx switch box with integrated preamps (MR Coils
BV, Drunen, The Netherlands) and the software was adapted to constantly detune
the present 8-channel TEM body coil. The
elements are driven in the center through a lattice balun that simultaneously
performs impedance matching. Numerical simulations of the array on Virtual
Family model ‘Duke’ [4]. have been performed in Sim4Life (ZMT, Zurich,
Switzerland) to assess the 10g averaged SAR distribution (SAR10g). Combined
with careful calibration and real-time monitoring of the power emitted by the
amplifiers, safe local and global SAR exposure was ensured. One volunteer (31y,
1.82m, 73kg, informed consent) was scanned using 8x200W peak power and T2w TSE
images (TR/TE=2000/90 ms, 0.75x1x3 mm3, 3 slices, TSE-factor: 13) have been
obtained.
Results
and discussion
The in-depth B1+ profiles for the investigated elements are
presented in figure 1. The lumped element design is weaker than the others and was
extremely sensitive to loading variations. The element with 12 meanders
performed the best and also showed the least sensitivity towards loading
variations. This design has been used to realize an eight-element transceive
array (figure 2). Note that although dipole antennas have been presented as
particularly suitable for ultrahigh field strengths[5,6], we now explore their
applicability at 3T mainly because of the relatively homogeneous B1+
field patterns (less steep fall-off) and reduced inter-element coupling. From
the array simulations, the sum-of-magnitude electric field for all antenna
elements has been used to calculate the worst-case SAR distribution as
presented in figure 3. Clearly, the maximum SAR is located at the anterior side
of the thighs where the dipoles end. Using an average power of 1W per channel,
the maximum SAR10g value is 2.2 W/kg. The simulated B1 efficiency for the array
was 10.6 µT
using 8x200 W input power.
Figure 5 shows prostate imaging results for the dipole antenna array at 3T.
Using 8x200W, a B1+ level of 12 µT was achieved inside the
prostate. This corresponds reasonably well to the simulated value and is indeed
much more efficient than the birdcage body coil or the 8-channel TEM body coil
that is integrated in this MRI platform. The current implementation used a
simple transmit-receive operation, limiting reception to only 8 dipoles, which
is less than the state of the art for modern prostate imaging This will be
amended once the array is extended by receive or transceive loop coil elements
underneath the dipoles, similar to Voogt et al [6].
Conclusions
Dipole antennas at 3T can be realized with the addition of
extra inductance in the antenna legs. If the extra inductance is realized as
meanders instead of lumped element inductors, the performance is better and the
antennas are not very sensitive to loading variations. A design consisting of eight
meandering dipole antennas has been realized. Simulations show a worst-case
maximum SAR10g of 2.2 W/kg for 8x1 W accepted input power. In an actual MRI
experiment, the array realizes 12 µT with 8x200W on an average-sized
human subject. T2w prostate images have
been successfully acquired.
Acknowledgements
No acknowledgement found.References
References
[1] C.E.Hayes et al, Journal of Magnetic Resonance 63, 622-628 (1985)
[2] M. Murbach et al, Magn. Reson. Med. 71:839-845 (2014)
[3] C. Leussler, in Proceedings of the ISMRM 23rd Annual Meeting
2015, #1813
[4] R. Lattanzi et al. Magn Reson. Med. 68:286-304 (2012)
[5] Raaijmakers et al. NMR in Biomed. Published online
[6] Voogt et al. in Proceedings of the ISMRM 23rd Annual Meeting
2015, #0631