Isabelle Saniour1, Fraser Robb2, Victor Taracila2, Jana Vincent2, Henning U. Voss1, Michael G. Kaplitt3, J. Levi Chazen1, and Simone Angela Winkler1
1Weill Cornell Medicine, New York, NY, United States, 2MR Engineering, GE Healthcare, Aurora, OH, United States, 3Department of Neurological Surgery, Weill Cornell Medicine, New York, NY, United States
Synopsis
Magnetic
resonance guided focused ultrasound (MRgFUS) is a non-invasive therapeutic
modality for neurodegenerative diseases that allows real-time imaging of the
targeted regions. However, MR image quality is poor and severely limits the technology
due to the use of the body coil for focal targeting. Acoustic
simulations demonstrated an acoustic transparency (signal loss <1%) of the
coil when used for thalamic sonication. In vivo results showed increase of the
SNR over the body coil by a factor of 7.3 and 7.6 in a brain image with and
without the presence of the transducer, respectively.
Introduction
Magnetic Resonance guided Focused
Ultrasound (MRgFUS) is a non-invasive therapeutic modality for
neurodegenerative disorders such as essential tremor and Alzheimer’s Disease
that has achieved dramatic success.1-5 However, the MR image quality is extremely
poor and severely limits the technology due to the use of the body coil for
targeting. This coil is versatile but yields both a very poor signal, and the
dark band in MR images typically seen when used with the water-filled metallic
transducer placed around the human skull.6 Recent
approaches to mitigate this poor image performance issue have included
manipulation of the electrical properties of the water by use of doped water7 or dielectric pads.8 Moreover, different head coil have been designed in
order to achieve better SNR during focused ultrasound (FUS) treatment. Almost
all these methods require costly modification of the INSIGHTEC MRgFUS system,
while having associated drawbacks especially regarding their impacts on the
acoustic beam. A large hindrance to the success of specific coil designs for
MRgFUS has been their acoustic footprint and thus the distortion of ultrasound
signal, which ultimately results in a physical shift, signal loss, and/or
broadening of the focal point. In this work, we present acoustic simulations and
first in vivo MR images with a novel 8-channel head coil design for MRgFUS. The
proposed RF coil array is comprised of ultra-thin wiring mounted on acoustically
transparent fabric.Methods
We used a highly flexible receive
coil architecture inspired by Air™ Coil technology9-12 to build an 8-channel head coil (FUS-Flex) (Figure 1). This coil is very thin (around 1 mm-diameter) and ultra-flexible, which allows for simple usage during an MRgFUS procedure without any costly modification, as it can be placed directly on the surface of the head.
Acoustic footprint: In order to quantify the impact of the coil on the acoustic field, simulations were performed using COMSOL Multiphysics. Figure 2 shows a model of a transducer, water bath, and tissue phantom (radius 150 mm, length 160 mm).13 A coil element was placed at distances of 20 and 80 mm (the latter corresponding to the typical distance of the thalamus) from the focal point as shown in Figure 2b. The transducer is driven at typical low and high frequencies used in FUS treatment, 220 kHz, 650 kHz, and 1 MHz.
In vivo imaging: First in vivo MR images with the FUS-Flex receive coil were acquired on two healthy volunteers (Figure 4) with and without the transducer and were compared with the body coil in receive mode. In a first test, water-filled bags were placed around the head of a volunteer, while the second volunteer was imaged using the INSIGHTEC sealant membrane and the water-filled transducer helmet. A 3D Bravo sequence (TE = 3 ms, TR = 7.4 ms, FA = 12° and pixel bandwidth= 244.1 Hz/px) was used. Results
Acoustic
simulations: The
radial cross-section of the acoustic field magnitude is shown in Figure 3a; results were normalized to the
case without a coil. For all frequencies and at a position of the coil at
80 mm, negligible displacement of the focal point or signal loss was found
compared to the reference simulation without a coil present (Figure 3b). When the coil was located 20 mm
away from the focal point, the focal point shifted by 10 mm and 5 mm
at 650 kHz and 220 kHz, respectively. At 1 MHz and 20 mm,
no visual shift of the focal point was found. Signal
losses at a 20 mm distance were 20%, 5% and 15% for 1 MHz,
650 kHz and 220 kHz, respectively.
In
vivo imaging: Images acquired using the FUS-Flex coil
in Figure
4 depict the position of the thalamus
in a healthy volunteer with high sensitivity and show clear improvement of the
black band. At the location of the thalamus, the SNR gain is 7.3-fold and
7.6-fold compared to the body coil, with and without the MRgFUS transducer
present, respectively. Discussion and conclusions
The acoustic simulations showed
feasibility for the transparency of the coil when it is placed at 80 mm (<1%)
from the focal point. For a closer position of the coil to the focal point, the
signal loss is between 5 and 20% depending on the emitted frequency. However,
most current applications involve deeper regions. Moreover, it should be noted
that the attenuation due to the skull is around 70%14, which is much
higher than the attenuation due the coil or the related electronics.
We showed that the proposed
FUS-Flex coil improves the SNR in MRgFUS procedures in presence of
helmet-shaped water filled (7.3×) at the thalamus region with an acquisition that
is 2 times faster than what can be achieved with the body coil. These results
confirm the potential of our proposed FUS-Flex coil, and even higher SNR gains and
scan times are expected with a higher channel count. Moreover, the proposed
coil is expected to exhibit improved SNR even in conventional, non-MRgFUS,
exams.Acknowledgements
This
work was supported by the National Institutes of Health (NIH K99/R00 4R00EB024341-03) and GE Healthcare.References
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