Shajan Gunamony1,2, Roland Müller3, Paul McElhinney1, Sydney Nicole Williams1, Nicolas Groß-Weege3,4, Nikolaus Weiskopf3,5, Harald E Möller3, and David Feinberg6
1Imaging Centre of Excellence, University of Glasgow, Glasgow, United Kingdom, 2MR CoilTech Limited, Glasgow, United Kingdom, 3Max Planck Institute for Human Cognitive and Brain Sciences, Leipzig, Germany, 4Siemens Healthcare GmbH, Erlangen, Germany, 5Faculty of Physics and Earth Sciences, Felix Bloch Institute for Solid State Physics, Leipzig, Germany, 6Helen Wills Neuroscience Institute, University of California, Berkeley, CA, United States
Synopsis
The NexGen
7T scanner has been designed to reach an unprecedented microscale resolution in
fMRI studies of the cerebral cortex. A radiofrequency coil setup with a high
density receive array is essential to capture the promised benefits. The coil
design, which is already constrained by the limited space on the patient table
inside the head gradient, must be robust, allow routine scanning and offer a
visual field to support fMRI studies. We have developed a compact 16-channel
transmit 96-channel receive head coil for the NexGen 7T scanner. In this
abstract, we present the coil development and preliminary phantom results.
Introduction
High-density ultra-high field receive arrays are expected to
bring significant gains in signal-to-noise-ratio (SNR) and parallel imaging
performance1,2. The NexGen-7T scanner is fitted with a head gradient
insert and consists of an RF architecture with 16-transmit and 128-receive
channels. RF coils for head gradient inserts are constrained by the limited
space in the narrow patient table. However, despite the high channel count, the
coils must support routine use and offer a visual field to support the fMRI studies.
In addition, the transmit and receive arrays must be integrated without
influencing the spatial distribution of the transmit field. We present a
compact 16-channel transmit 96-channel receive head coil custom-built for the
head gradient insert. The coil characterisation and initial phantom
measurements are presented here.Methods
Transmit
array: The transmit array consists of 16-elements arranged in two rows3,4.
Following on from an
earlier work5, the loss mechanisms were investigated and addressed
to create an efficient design. The array was constructed on a fiberglass
tube of 285mm inner diameter and extended 21cm along the z-direction. The outer tube consisted of a slotted double-layered
7µm shield at a distance of 30mm from the coil. The adjacent elements within the row and between the
rows were overlapped and the diagonal elements were inductively decoupled. A
view of the simulation setup (CST Studio
Suite, Dassault
Systems, France) and the transmit array layout is given in figure 1.
Receive
array: The receive array consisted of 96-elements arranged symmetrically in 6
rows. There are 12 elements in the top row, 18 in the second and 24 in the
third row covering from the vertex of the dome to the level of the nose bridge.
The other 42 elements covered the remainder of the helmet surface. The size of
each receive element was about 30mmx45mm. The two eye loops were larger. A
tight fit helmet (175mm along L/R, 215mm along A/P) was chosen to maintain
sample loading on the small receive elements. The helmet was shaped using
anthropometric data and also had a curvature beneath the skull base to provide
a comfortable but tight fit.
The equivalent circuit schematic is as per Ref.3. All circuit
boards were miniaturised and a detailed CAD model was created in Solidworks to
visualise component placement, cable routing and packaging. A picture of the
completed receive array and the final assembly highlighting the visual field
achieved despite the limited space is shown in figure 2.
Test setup:
An elaborate test setup (figure 3) was required to be able to test this
coil in the bench. The test-jigs consisted of: two 8-channel pTx; two
32-channel high-density receive and one 32-channel TIM interfaces.
Tuning, matching, decoupling and preamplifier decoupling of the receive
elements were adjusted while the remaining elements were tuned but decoupled
using the preamplifiers.
Preliminary tests have been conducted on a 7T Terra scanner (Siemens
Healthineers AG, Erlangen, Germany) equipped with 16-transmit channels and
64-received channels. The additional receive channels were actively detuned
through the test-jig by biasing through an external power supply.
VOP6: Two body models
were simulated in three different positions each. Due to the computational
requirements for the 16Tx array, only the worst case from the two models were
chosen and a concatenated VOP was generated using the two datasets, after
applying a 30% overestimation and a manufacturer recommended measurement error
factor. Results
Transmit array: Coupling between
the adjacent elements on each row was less than -16dB and between the two rows was
less than -19dB. The diagonal elements were decoupled by more than -20dB. The active detuning of the transmit array
was less than -30dB. A plot of the
S-parameters characterizing the transmit array with and without the receive
array is shown in figure 3. It is important to note that only the tune and
match of the transmit elements were adjusted after the receive array was
inserted. Clear resonances can be seen for each of the array element despite
the presence of the tightly packed receive array. While most of the coupling behavior
remained unaltered, influence on two pairs of the top row elements were
observed.
Receive array: The decoupling
between the adjacent elements was in the range of -10 to -12dB. The average
preamplifier decoupling of all the 96-receive channels was -21dB and the active
detuning was better than -30dB.
Scanner measurements: Despite
the presence of the 96-channel receive array, the combined and single channel B1+
maps (Figure 4) look as expected and no local influence on the spatial
distribution can be seen. The CP and the CP2+ maps were acquired by setting the
theoretical phase offsets.
The noise correlation maps (figure 5) demonstrate good decoupling. Most
of the nearest coupling coefficients were below 0.3, with only six pairs having
values between 0.5 and 0.55.
A first localiser
image of the 16Tx96Rx setup from the NextGen-7T and a spaghetti squash 3D FLASH
image acquired with 3x5 GRAPPA acceleration with 0.25x0.25x1.5mm resolution are
shown in figure 5. Discussion
Initial
measurements demonstrate SNR gain of more than a factor of two closer to coil
surface. We expect to further characterise the transmit and receive performance
of this coil array in the NexDen-7T scanner. Acknowledgements
1.
Dr Ralph Kimmlingen, Siemens Healthcare
GmbH, Erlangen, Germany, for helping us with the 16Tx interfacing.
2. Dr An Wu, VA Advanced Imaging
Research Center, UCSF, CA, USA for acquiring the 16Tx96Rx images.
References
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