13:30 |
0853.
|
3D-printed RF coils for
solution-state NMR: Towards low-cost, high-throughput arrays
R. Adam Horch1,2 and
John C. Gore1,2
1Department of Radiology & Radiological
Sciences, Vanderbilt University, Nashville, TN, United
States, 2Vanderbilt
University Institute of Imaging Science, Nashville, TN,
United States
3D printing with selective metallization is demonstrated
as a new means to fabricate RF coils for solution-state
NMR. Current capabilities allow construction of mm-scale
solenoids with integral sample chambers for
self-contained NMR probes, and 3D-printed microcoils are
imminent given ongoing advances in technology. The
unique properties of 3D printing enable facile
construction of potentially thousands of coils at low
cost, giving way to large coil arrays for
high-throughput NMR and novel coil geometries.
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13:42 |
0854.
|
Multi-Turn Multi-Gap
Transmission Line Resonators - First Tests at 7 T
Roberta Kriegl1,2, Jean-Christophe Ginefri2,
Marie Poirier-Quinot2, Zhoujian Li2,
Luc Darrasse2, Ewald Moser1,3, and
Elmar Laistler1,3
1Center for Medical Physics and Biomedical
Engineering, Medical University, Vienna, Vienna,
Austria, 2IR4M
(Imagerie par Résonance Magnétique Médicale et Multi-Modalités),
UMR8081 CNRS, Université Paris Sud, Orsay, Essonne,
France, 3MR
Centre of Excellence, Medical University, Vienna,
Vienna, Austria
A novel design scheme for monolithic transmission line
resonators (TLRs) used as NMR surface probes is
presented. The multi-turn multi-gap TLR design provides
an additional degree of freedom for adjusting the TLR
geometry, and therefore enables more accurate
optimization of current distribution, and B1pattern.
It also promotes the use of multi-turn TLR technology
for high-field applications requiring a large FOV, which
has not been possible up to now due to the low
self-resonance frequency of these coils. Here, we
compare three different multi-turn multi-gap TLRs
designed for 1H
imaging at 7 T by 3D electromagnetic simulations and MRI
experiments.
|
13:54 |
0855.
|
Q-spoiling method using
depletion mode Gallium Nitride (GaN) HEMT devices at 1.5T
Jonathan Y Lu1, Kamal Aggarwal1,
Thomas Grafendorfer2, Fraser Robb3,
John M Pauly1, and Greig C Scott1
1Electrical Engineering, Stanford University,
Stanford, CA, United States, 2Advanced
Coils, GEHC Coils, Stanford, CA, United States, 3GE
Healthcare, Aurora, OH, United States
We demonstrate a novel Q-spoiling method using a
depletion mode Gallium Nitride (GaN) HEMT device. This
device, when unbiased, ideally acts as a short and when
biased with a negative gate-to-source voltage acts as an
open switch. Using this device, we constructed a coil
that is Q-spoiled when unpowered and at resonance with
an applied gate to source voltage. Compared with the
conventional Q-spoiling method using a PIN diode, the
new circuit requires less power and yields comparable
SNR coil measurements. In addition, the default
Q-spoiled state allows greater safety benefits, and
easier decoupling with multiple coils.
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14:06 |
0856.
|
On the Contribution of
Electric-Type Current Patterns to UISNR for a Spherical
Geometry at 9.4 T
Andreas Pfrommer1 and
Anke Henning1,2
1Max Planck Institute for Biological
Cybernetics, Tuebingen, Germany, 2Institute
for Biomedical Engineering, UZH and ETH Zurich, Zurich,
Switzerland
Parallel imaging is intrinsically limited by Maxwell’s
equations. A complete set of vector solutions to the
Helmholtz equation consists of both curl-free and
divergence-free fields. In this study we investigated
the contribution of electric-type current patterns to
UISNR for different voxel positions and acceleration
factors in a spherical model at 9.4T. For moderate
acceleration the electric mode increased UISNR by
maximally 55%. For very high acceleration, however,
UISNR was mostly caused by the magnetic mode. The reason
for this might be the much faster growing power loss of
the electric mode with respect to the expansion order.
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14:18 |
0857.
|
3D curved electric dipole
antenna for propagation delay compensation
Gang Chen1,2, Daniel Sodickson1,
and Graham Wiggins1
1Center for Advanced Imaging Innovation and
Research (CAI2R) and Center for Biomedical Imaging,
Department of Radiology, New York University School of
Medicine, New York, NY, United States, 2The
Sackler Institute of Graduate Biomedical Science, New
York University School of Medicine, New York, NY, United
States
For a body-sized phantom at 7 Tesla, the ideal current
patterns for curl-free current modes display V-shaped
distributions due to the need for phase evolution along
the axial direction (z) to account for propagation
delays to or from the central region of interest.
Previous studies have shown that either bending the
electric dipole into a V or shortening a straight dipole
helps to mitigate destructive interference of signal,
and therefore to increase transmit efficiency or SNR, at
the central point of interest. Here we describe a novel
3D curved electric dipole antenna design constructed on
a dielectric substrate to compensate for propagation
delays and increase central B1+ efficiency.
|
14:30 |
0858.
|
New low-order pre-fractal
geometries of high permittivity pads further increase
sensitivity at high magnetic fields
Rita Schmidt1 and
Andrew Webb1
1Radiology, Leiden University Medical Center,
Leiden, Netherlands
In previous work the concept of using high permittivity
materials to increase the strength and homogeneity of
the B1 field has been shown at 3T and 7T. However, it
was also shown that at ultrahigh field instead of a
monotonic sensitivity improvement, high permittivity
pads can also be a source of local signal decreases due
to wavelength effects within the material. In this study
we investigate how the wavelength effects can be
mitigated by using a low order prefractal geometry for
the dielectric pad, which maintains the overall coverage
of the pad, but gives an increase in sensitivity and
homogeneity.
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14:42 |
0859. |
Discovering and working
around effects of unwanted resonant modes in high
permittivity materials placed near RF coils
Gillian G Haemer1,2, Christopher M Collins1,2,
Daniel K Sodickson1,2, and Graham C Wiggins1
1The Center for Advanced Imaging Innovation
and Research, and the Center for Biomedical Imaging,
Department of Radiology, New York University School of
Medicine, New York, NY, United States, 2The
Sackler Institute of Graduate Biomedical Sciences,
Department of Radiology, New York University School of
Medicine, New York, NY, United States
Previous work has shown that high permittivity materials
(HPMs) placed between the coil and the sample can
improve SNR, transmit efficiency, and RF homogeneity.
However dielectric resonances in any HPM placed close to
a transmit/receive coil may create an adverse affect
when tuning and matching RF coils. By visualizing the
dielectric resonant modes and testing various ways to
reduce their effect on the coil we explore one practical
aspect of HPM use.
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14:54 |
0860.
|
Comparison of New Element
Designs For Combined RF-Shim Arrays at 7T
Simone Angela Winkler1, Jason P Stockmann2,
Paul A Warr3, Boris Keil2,
Lawrence L Wald2,4, and Brian K Rutt1
1Dept. of Radiology, Stanford University,
Stanford, CA, United States, 2A.
A. Martinos Center for Biomedical Imaging, Massachusetts
General Hospital, Harvard Medical School, Charlestown,
Massachusetts, United States, 3Department
of Electrical & Electronic Engineering, University of
Bristol, Clifton, United Kingdom, 4Harvard-MIT
Health Sciences and Technology, Massachusetts Institute
of Technology, Cambridge, Massachusetts, United States
Combining RF and B0 shim functions into a single array
is an appealing approach which allows highly flexible
matrix B0 shimming while preserving closely fitting,
high channel count receive array elements. The standard
approach is to add chokes to bypass all loop capacitors
to allow the DC current to flow around the loop, but
this introduces additional loss, heating, RF field
perturbation, bulk and construction complexity. We
report on the analysis (by theory, simulation, and
experiment) of several new combined RF-shim element
designs, with particular focus on SNR performance. We
particularly investigated two new loop designs –
concentric and coaxial types – and compared these to the
standard chokes and RF-only loop types. We conclude that
both new loop types provide viable solutions for RF-shim
loop architectures at 7T.
|
15:06 |
0861.
|
Integrated parallel
reception, excitation, and shimming (iPRES) with split DC
loops for improved B0 shimming
Dean Darnell1, Trong-Kha Truong1,
and Allen Song1
1Brain Imaging and Analysis Center, Duke
University, Durham, North Carolina, United States
It is a challenge to correct small spatial variations in
B0 inhomogeneities with current B0 shimming
implementations due to a lack of shimming spatial
resolution. Building upon the Integrated Parallel
Reception, Excitation and Shimming (iPRES) concept, this
study improves the spatial resolution by increasing the
number of independent magnetic fields available for each
RF coil. Initial experiments show that the additional
magnetic fields introduced for shimming show a notable
improvement in B0 homogeneity root-mean-square error
relative to the original iPRES design.
|
15:18 |
0862. |
ENDOLUMINAL MR RECEIVER
COIL BASED ON ELECTRO-OPTICAL CONVERSION AND ACTIVE OPTICAL
DECOUPLING
Isabelle Saniour1, Anne-Laure Perrier2,
Reina Aydé1, Gwenaël Gaborit2,3,
Lionel Duvillaret3, and Olivier Beuf1
1Université de Lyon, CREATIS, CNRS UMR 5220,
Inserm U1044, INSA-Lyon, Université Lyon 1,
Villeurbanne, France, 2Université
de Savoie, IMEP-LAHC, UMR 5130, Le Bourget-du-Lac,
France, 3KAPTEOS,
Sainte-Hélène-du-Lac, France
The use of metallic coaxial cables in MRI could induce
local high Specific Absorption Rate (SAR). Optical fiber
link could be a promising alternative to coaxial cables
for MRI to ensure patient safety. A novel type of an
endoluminal receiver coil ensuring optical transmission
of NMR signal and optical detuning is designed. Firstly,
the conversion of the NMR electrical signal into an
optical signal is based on Pockels effect and ensured by
an Electro-Optical (EO) waveguide added to the coil
according to the applied electric field. Then, the
decoupling of the coil is done optically using
photodiodes placed on the coil that provide the DC
decoupling current.
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