Joint Annual
Meeting ISMRM-ESMRMB 2014
○
10-16 May 2014
○
Milan, Italy |
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ELECTRONIC
POSTER SESSION ○ MR ENGINEERING |
RF Coils, Waveguides & Dielectrics
Thursday 15 May 2014
Exhibition Hall |
13:30 - 14:30 |
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Computer # |
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4795. |
1 |
High Resolution Double
Resonant 1H/19F
RF Coil for Small Rodent MRI and MRS at 3T
Helmar Waiczies1, Jan Rieger1,
Andreas Graessl2, Andreas Pohlmann2,
Matthias A. Dieringer2,3, and Thoralf
Niendorf2
1MRI.TOOLS GmbH, Berlin, Germany, 2Berlin
Ultrahigh Field Facility (B.U.F.F.), Max Delbrück Center
for Molecular Medicine, Berlin, Germany, 33Working
Group on Cardiovascular Magnetic Resonance, Experimental
and Clinical Research Center (ECRC), Berlin, Germany
A dual-tuned 1H/19F
birdcage coil with high B1+homogeneity
for animal research at a clinical 3T-System has been
constructed. The simulated B1+ fields
and the measured B1+ maps
were found to be in good agreement, including anatomical
coverage, B1+ distribution
and B1+ efficiency.
The acquired ex vivo images showed superb sensitivity
for 19F
MRI as well as high spatial resolution for 1H
MRI. This work demonstrates the feasibility of a double
tuned birdcage coil tailored for 1H/19F
MR in small rodents using a clinical 3T MR system. The
proposed RF coil provides high homogeneity and
sensitivity for very low concentrations of 19F.
This progress may serve to enhance the capabilities of 19F
MR based cell tracking in small rodents and benefits
translational research en route to 19F
MR in large animals or even humans.
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4796. |
2 |
Radiation Damping in a
Detuned Probe by the Bloch-Kirchhoff Equations
James Tropp1
1Engineering, GE Healthcare Technologies,
Fremont, CA, United States
We have calculated the rates of radiation damping as a
function of probe detuning, by numerical solution of the
Bloch-Kirchhoff equations.
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4797. |
3 |
An Active Decoupled HTS
Film Coil for 1.5T MRI
Lian Xue1, Zungang Liu1, Changwu
Hu1, Kuan Zhang1, Erzhen Gao1,
QY Ma1, Nikolaus M Szeverenyi2,
Rebecca Theilmann2, and William Bradley2
1Time Medical Systems, Inc., San Diego, CA,
United States, 2Radiology,
Univ. of California, San Diego, San Diego, CA, United
States
A clinically useful 10 cm diameter high temperature
superconductor (HTS) surface coil was designed,
constructed, and tested for wrist imaging performance on
a 1.5 Tesla scanner. The cryostat was constructed of
fiberglass and had a liquid nitrogen hold time of 5 hrs
and a vacuum hold time of 4 weeks. Comparison of this
coil’s performance with a commercial 10 cm room
temperature copper coil demonstrated a greater than 2
fold improvement in SNR. This receive coil has an active
detuning circuit that can be used in future array coils
designs.
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4798. |
4 |
Helix antennas: approaching
the target from a different angle
Alexander J.E. Raaijmakers1, Abe van der Werf2,
Hugo Kroeze1, Peter R. Luijten1,
Cornelis A.T. van den Berg3, and Dennis W.J.
Klomp1
1Radiology, UMC Utrecht, Utrecht, Utrecht,
Netherlands, 2Machnet
B.V., Roden, Netherlands, 3Radiotherapy,
UMC Utrecht, Utrecht, Netherlands
Helix antennas are a commonly used type of antenna in
communication technology. They emit a circularly
polarized wave with high directivity. For MRI, the helix
antenna has the unique property to transmit or receive
along the longitudinal axis of the scanner. This unique
property enables the coverage of regions that are
otherwise hard to address, particularly at higher field
strengths. For example, the helix antenna can be used to
recover B1 at the apex of the head. For prostate
imaging, the helix antenna can be used to increase
sensitivity by placing the coil between the legs, along
the longitudinal axis.
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4799. |
5 |
Electro-optic RF magnetic
resonance signal based on a Ti:LiNbO3 waveguide
Reina Ayde1, Anne-Laure Perrier1,
Jean Dahdah2, Raphael Sablong1,
Lionel Duvillaret2, Gwenael Gaborit2,3,
and Olivier Beuf1
1University of Lyon 1, CREATIS - CNRS UMR
5220 – INSERM U1044, Villeurbanne, Rhone-Alpes, France, 2Kapteos,
Rhone-Alpes, France, 3University
of Savoie, IMEP-LAHC UMR 5130, Rhone-Alpes, France
The use of metallic coaxial cables in Magnetic Resonance
Imaging 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. Here, the conversion of the Radio-Frequency
magnetic field into an electric signal by electro-optic
effect was demonstrated and characterized. A waveguide
crystal is used together with an endoluminal coil to
demonstrate the ability of such transducer to perform a
deported characterization of Radio-Frequency magnetic
field at 3T. The results show a good agreement with
theoretical values and a minimum magnetic detectable
field of pT order.
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4800. |
6 |
Box Shaped Monopole Antenna
for RF Excitation at 9.4T MRI
Irena Zivkovic1 and
Klaus Scheffler1,2
1High Field MRI, Max Planck Institute for
Biological Cybernetics, Tuebingen, Germany, 2Center
for Integrative Neuroscience, Universuty of Tuebingen,
Tuebingen, Germany
It is a big challenge to produce as homogeneous as
possible B1+ field with single channel antenna in
traveling wave configuration. For that purpose, we
proposed a new and very simple antenna concept. Antenna
is entirely made of copper and without any lumped
elements. By small changes in geometry different RF
excitation patterns can be produced. We presented design
that produced as homogeneous as possible B1+ field in
sagittal, coronal and transversal planes. The second
proposed design produced B1+field pattern in lower brain
and neck region.
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4801. |
7 |
A clinically useful HTS
knee coil for 0.35 T MRI
Zungang Liu1, Changwu Hu1, Erzhen
Gao1, Ronald Tse1, QY Ma1,
Nikolaus M Szeverenyi2, and William G Bradley2
1Time Medical Systems, Inc., Shanghai, China, 2Radiology,
Univ. of California, San Diego, CA, United States
A preliminary HTS volume knee coil was designed to
improve the image quality of a low field MRI system. The
coil is cooled by liquid nitrogen with a very low
nitrogen boil-off rate. Knee images were obtained and
compared to a commercial copper coil.
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4802. |
8 |
A field probe transceiver
system with controllable RF coupling and decoupling
Ying-Hua Chu1, Yi-Cheng Hsu1,
Shang-Yueh Tsai2, and Fa-Hsuan Lin1,3
1Institute of Biomedical Engineering,
National Taiwan University, Taipei, Taiwan, 2Institute
of Applied Physics, National Chengchi University,
Taipei, Taiwan,3Department of Biomedical
Engineering and Computational Science, Aalto University,
Espoo, Finland
We propose a new approach to improve the isolation of
NMR signals originating from the field probe and from
the imaging object without using an independent
transceiver. We use an RF coil (Tx loop) to pick up the
RF energy during RF transmission to the field probe
inside an RF shield. During RF reception, the Tx loop is
detuned such that the NMR signal from the imaging object
will not be picked up by the Tx loop and the field probe
can remain isolated inside the RF shielding. This design
is empirically demonstrated by an one-channel prototype
system.
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4803. |
9 |
Design of a 24-Mesh
Inductive Birdcage for Imaging of the Head at 500 MHz
Joseph Murphy-Boesch1, Qi Duan1,
Steve Dodd1, Natalia Gudino1,
Shumin Wang2, and Jeff Duyn1
1National Institute of Neurological Disorders
and Stroke, National Institutes of Health, Bethesda, MD,
United States, 2Department
of Electrical and Computer Engineering, Auburn
University, Auburn, AL, United States
An inductive birdcage resonator with 24 meshes has been
assembled for imaging of the head in the confined space
of an 11.7T head-only MRI system. To reduce radiative
losses and de-tuning by the head, the resonator was
suspended within its cylindrical shield with no direct
RF connections. Four-port connection to the coil was
effected using inductive couplers with balanced drive to
further reduce E-fields. Bench sensitivity and field
uniformity are similar to a 7T coil. Power testing using
a custom phantom yielded differential temperature
increases that can be used to validate EM simulations.
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4804. |
10 |
Modular and Versatile
Multi-Row Transmit Array based on a Novel Decoupled Coil
Element Design
Riccardo Stara1, Simone A. Winkler2,
Ronald D Watkins2, Alessandra Retico3,
Michela Tosetti4, and Brian K Rutt2
1Dipartimento di Fisica, Università di Pisa,
Pisa, Italy, 2Department
of Radiology, Stanford University, Stanford, CA, United
States, 3Istituto
Nazionale di Fisica Nucleare, Pisa, Italy, 4IRCCS
Stella Maris, Pisa, Italy
B1+ shimming
and parallel transmission can benefit from an increased
number of transmit channels and from 3D segmentation.
However, one of the remaining challenges in RF coil
designs for parallel transmission is the decoupling
between coil elements. We present a novel transmission
line element used in a modular two-row 16-channel
transmit array design. The proposed element employs
cylindrical shielding to provide intrinsic geometric
decoupling, without any additional hardware. The
proposed 16-channel array can be configured for
8-channel single-row and 16-channel two-row mode using
two Butler matrices. Numerical simulations and
preliminary experiments show improved decoupling
performance and B1+/E performance.
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4805. |
11 |
A 16-Channel Transceiver
Array for 7 Tesla Equine Joint MRI
Hai Lu1, Ziyuan Fu2, and Shumin
Wang2
1Auburn University, Auburn, Alabama, United
States, 2Auburn
University, Alabama, United States
Multi-channel transceiver arrays are highly desired for
7 Tesla MRI due to the lack of volume transmitters. We
developed a 16-channel transceiver array for equine
joint MRI at 7T by splitting the single-channel power
input equally into 16 coil elements. The design and
implementation details are discussed. Actual imaging
results further demonstrate the feasibility of the
design.
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4806. |
12 |
A flexible transceiver
array of monolithic transmission line resonators
Roberta Kriegl1,2, Jean-Christophe Ginefri1,
Marie Poirier-Quinot1, Luc Darrasse1,
Ewald Moser2,3, and Elmar Laistler2,3
1Laboratoire d'Imagerie par Résonance
Magnétique Médicale et Multi-Modalités (IR4M),
Université Paris Sud, Orsay, Essonne, France, 2Center
for Medical Physics and Biomedical Engineering, Medical
University of Vienna, Vienna, Vienna, Austria, 3MR
Center of Excellence, Medical University of Vienna,
Vienna, Vienna, Austria
A novel transceiver array composed of monolithic
transmission line resonators, fabricated on flexible
substrate, for MRI at 7 T is presented. Individual array
elements are mutually decoupled via overlapping annexes;
inductive matching and fine-tuning using pick-up loops
in over-coupled mode was implemented. The decoupling and
parallel imaging performance of the array was assessed
in bench and MRI experiments in terms of transmission
S-parameters, noise correlation values and GRAPPA
g-factors, comparing planar and bent array
configuration. It is shown that the developed array may
be form-fitted to non-planar samples without degrading
its performance.
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4807. |
13 |
High Resolution Rodent
Cochlea Imaging on a 3T Clinical Magnet
Joshua D Kaggie1,2, K Craig Goodrich1,
Seong-Eun Kim1, Michael J Beck1,
Dennis L Parker1,2, Robb Merrill1,
Travis A Abele3, Richard Wiggins3,
and J Rock Hadley1
1Utah Center for Advanced Imaging Research,
Radiology, University of Utah, Salt Lake City, UT,
United States, 2Physics,
University of Utah, Salt Lake City, UT, United States, 3Neuroradiology,
University of Utah, Salt Lake City, UT, United States
This work developed a small animal system that could
acquire good in vivo 100μm isotropic resolution images
of a guinea pig cochlea on a 3T clinical MR system. The
system used improved gradients, RF coils, and animal
holder/monitoring equipment when compared to a standard
clinical magnet. FLASH imaging was used to assess the
quality of the system. Gadolinium increased the SNR and
contrast of the cochlea during FLASH imaging. The small
animal system obtained good 100μm isotropic resolution
images of the cochlear chambers in a scan time of only
33 minutes.
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4808. |
14 |
Optimization of 7 T YBCO
Coils for in-vivo and ex-vivo MRI of Small Animals;
Assessment of Achievable SNR Gain
-permission withheld
Jarek Wosik1,2, Kurt H. Bockhorst3,
Krzysztof Nesteruk4, Dhivya Ketharnath1,
Tan I-Chih5, and Ponnada A Narayana3
1Electrical and Computer Engineering,
University of Houston, Houston, Texas, United States, 2Texas
Center for Superconductivity, University of Houston,
Houston, Texas, United States, 3Health
Science Center, University of Texas, Houston, Texas,
United States, 4Polish
Academy of Sciences, Institute of Physics, Warsaw,
Poland, Poland, 5Center
for Molecular Imaging, University of Texas, Houston,
Texas, United States
We report on assessment of achievable SNR gain due to
reduction of thermal noise by cooling receiver coil made
out of copper or superconducting materials. High field
MRI 300 MHz receiver probe with tuning/matching and
decoupling circuitry was used. The coil was fabricated
by patterning double-sided thin superconducting YBCO
film on 0.4 mm thick sapphire substrate and comprises of
two split rings rotated 180 deg. versus each other. Our
main interest in this work is in identification all
losses limiting SNR, such as rf losses from coil, body,
cryostat and tuning/maching/decoupling circuitry and in
discussion on the probe performance optimization.
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4809. |
15 |
An interleaved opposing
monopole transmit-receive array for 7T brain imaging
Gang Chen1, Martijn Cloos1, and
Graham Wiggins1
1The Bernard and Irene Schwartz Center for
Biomedical Imaging, Department of Radiology, New York
University School of Medicine, New York, NY, United
States
At high field, electric dipole antennas are seeing
increasing use. When placed close to a relatively high
dielectric material such as the body the self-resonant
length shortens somewhat, but for 7T head imaging this
still comes out to an inconvenient length of 40 cm or
more. We describe here a modified monopole antenna where
the ground plane is replaced by a strip of conductor.
These are arranged in an 8 element array which allows
alternating monopoles to be driven from opposing ends of
the array, which extends excitation into inferior brain
regions while also providing diverse B1 profiles along
Z.
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4810. |
16 |
31P Birdcage
insert for an 8-channel, multi-transmit, 1H
coil at 7T
Bart L. van de Bank1, Stephan Orzada2,
Miriam W. Lagemaat1, Andreas K. Bitz2,3,
and Tom W.J. Scheenen1,2
1Radiology, Radboud University Medical
Center, Nijmegen, Netherlands, 2Erwin
L. Hahn Institute, University Duisburg-Essen, Essen,
Germany, 3Medical
Physics in radiology, German Cancer Research Center
(DKFZ), Heidelberg, Germany
A dedicated 31P birdcage coil was designed, validated
and constructed as an insert for an 8 channel,
multi-transmit, octagonal shaped, 1H coil to enable
homogeneous excitation and acquisition of 31P compounds
combined with 1H multi-transmit capabilities to asses
metabolic processes in-vivo at 7T.
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4811. |
17 |
Image quality improvement
via phase correction for travelling wave MRI at 3T
Fabian Vazquez1, Oscar Marrufo2,
Sergio E Solis1, and Alfredo O Rodriguez3
1Dep Phys, FC UNAM, Mexico, DF, Mexico, 2Dep
Neuroimage, INNN-MVS, DF, Mexico, Mexico, 3Dep
Elec Ing, UAM Iztapalapa, Mexico, DF, Mexico
Travelling wave magnetic resonance imaging (twMRI)
offers an approach to acquire larger fields-of-view
images at 7T or greater. Images have two main problems:
inhomogeneous acquisition due to the physical
restriction in coaxial waveguide at 7T, and added noise
in parallel-plate waveguide (PPWG) at 3T. We measured
the signal phase added by a PPWG in twMR images at 3T,
using a transmission circular coil and other one for
reception tuned at 128 MHz. Phantom images were acquired
with the PPWG in clinical scanner at 3T. The phase shift
information was used to improve the image quality and
results compared.
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4812. |
18 |
Improved surface coil
performance at any depth in a lossy sphere with a dielectric
disc
Wei Luo1,2, Yang Qing1, and
Christopher M. Collins3
1Radiology, Pennsylvania State University,
Hershey, PA, United States, 2Engineering
Science & Mechanics, Pennsylvania State University,
University Park, PA, United States, 3Radiology,
New York University, New York, NY, United States
A simple hybrid coil-HPM design using a simple loop coil
and a high-permittivity material (HPM) disc was
optimized at 3T using PSO/FDTD method including the
consideration on HPM location, geometry, material
properties, MRI coil location, and coil geometry for the
first time. The coil efficiency of the optimized hybrid
design was better than the one produced by the optimized
single loop coil at any depth in a lossy sphere,
particularly by an average increase of 87% and 22% at
the center and superficial regions, respectively. The
performance of this simple hybrid design encourages us
to expect more improvement with a more sophisticated
design.
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4813. |
19 |
Improving central transmit
efficiency and homogeneity using interleaved shielded
dielectric discs and coil elements in a 4-element
transmit/receive array at 7 T
Manushka V. Vaidya1,2, Christopher M. Collins1,2,
Ryan Brown1, Daniel K. Sodickson1,2,
and Riccardo Lattanzi1,2
1Bernard and Irene Schwartz Center for
Biomedical Imaging, Department of Radiology, New York
University School of Medicine, New York, NY, United
States, 2Sackler
Institute of Graduate Biomedical Sciences, New York
University School of Medicine, New York, NY, United
States
We performed simulations and experiments to evaluate the
benefits of placing shielded dielectric discs between
adjacent coil elements in a 4-element transmit/receive
array surrounding a uniform cylindrical dielectric
phantom at 7 T. Our results showed that array
performance is improved in the presence of
suitably-configured dielectric discs. In particular, the
B1 homogeneity improved by ~27% and the transmit
efficiency and SNR at the center improved by ~5%. The
proposed array design performs better than, and is based
on different physical principles than, conductive
shields placed above or completely surrounding the coil
elements.
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4814. |
20 |
Signal-to-Noise Ratio gain
at 3T using a thin layer of high-permittivity material
inside enclosing receive arrays
Riccardo Lattanzi1,2, Manushka V Vaidya1,2,
Giuseppe Carluccio1, Daniel K Sodickson1,2,
and Christopher M Collins1,2
1The Bernard and Irene Schwartz 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, New
York University School of Medicine, New York, NY, United
States
Cushions of high-permittivity material (HPM) placed
between radiofrequency (RF) coils and the object can
enhance transmit and receive performance. We
investigated in simulation the signal-to-noise ratio (SNR)
gain when covering the inside of a receive array
uniformly surrounding a dielectric sphere with a
continuous 1 cm layer of HPM (εr = 500). The SNR gain
was positive for every voxel when the array had at least
32 coils (average ~ 10%, maximum ~ 30%). Our results
suggest that using a thin encircling layer of HPM could
be a practical method to improve performance of receive
head arrays at 3T.
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4815. |
21 |
Appearant B1+ Asymmetry
in Symmetric Objects at High Fields
Wyger Brink1 and
Andrew Webb1
1Radiology, Leiden University Medical Center,
Leiden, Zuid-Holland, Netherlands
This work investigates, in particular, the origin of the
distinct left-right asymmetry in the B1+ field
typically observed in the head at 7 T.
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4816. |
22 |
Characterization of a
Dielectric Phantom for High-Field MRI Applications
Qi Duan1, Jeff H. Duyn1, Natalia
Gudino1, Jacco A. de Zwart1, Peter
van Gelderen1, Daniel K. Sodickson2,3,
and Ryan Brown2,3
1AMRI, LFMI, National Institute of
Neurological Disorders and Stroke, National Institutes
of Health, Bethesda, Maryland, United States, 2The
Bernard and Irene Schwartz Center for Biomedical
Imaging, Department of Radiology, New York University
School of Medicine, New York, United States, 3NYU
WIRELESS, Polytechnic Institute of New York University,
New York, United States
In order to predict wavelength effects on MRI
performance and tissue heating at high field, a generic
recipe for an inexpensive and nontoxic phantom with
biologically-relevant dielectric properties was
developed. The recipe includes deionized water, NaCl,
sucrose, and benzoic acid. 117 samples were prepared
with a range of NaCl and sucrose concentrations, and
their dielectric properties were measured and fitted to
a three-dimensional polynomial. Nonlinear relationships
between sucrose and NaCl concentrations and measured
dielectric properties were observed, and strong
interactions were found between individual component
concentrations in determining dielectric properties.
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4817. |
23 |
An
Electromagnetic-Simulation based Investigation of the
Dielectric Padding Approach for Head Imaging at 7 T
Andreas Rennings1, Keran Wang1, Le
Chen1, Friedrich Wetterling2, and
Daniel Erni1
1General and Theoretical Electrical
Engineering (ATE), University of Duisburg-Essen,
Duisburg, NRW, Germany, 2Faculty
of Engineering, Trinity College, Dublin University,
Dublin, Ireland
We present a simple model and used it for
electromagnetic simulations to get physical inside to
the dielectric padding approach. Furthermore we
determined the best suited values for the pad
permittivity and the cross-sectional-planes with best
and worst coefficient-of-variation (CoV) for the |B1+|
profile.
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4818. |
24 |
Effects of
high-permittivity materials on absolute RF coil performance
as a function of B0 and
object size
Riccardo Lattanzi1,2, Manushka V Vaidya1,2,
Giuseppe Carluccio1, Daniel K Sodickson1,2,
and Christopher M Collins1,2
1The Bernard and Irene Schwartz 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, New
York University School of Medicine, New York, NY, United
States
Previous work has shown that transmit efficiency and
signal-to-noise ratio (SNR) can be improved by placing
pads of high-permittivity material (HPM) between the
radiofrequency coil and the sample. We employed dyadic
Green’s functions for multi-layered spherical geometries
to calculate the ultimate intrinsic SNR and the SNR of a
32-element loop array surrounding uniform spheres with
different radii. Ultimate performance limits did not
change, but could be approached more closely by the
finite array with HPM added between the coil and the
object. For a head-sized sphere, the SNR advantage was
larger at 1.5T and 3T compared to higher B0 values.
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ELECTRONIC
POSTER SESSION ○ MR ENGINEERING |
MR Engineering
Thursday 15 May 2014
Exhibition Hall |
13:30 - 14:30 |
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Computer # |
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4819.
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25 |
Implementation of low-cost,
instructional tabletop MRI scanners
Clarissa Z Cooley1,2, Jason P Stockmann3,4,
Cris LaPierre2,4, Thomas Witzel2,
Feng Jia5, Maxim Zaitsev5, Pascal
Stang6,7, Greig Scott7, Yang
Wenhui8, Wang Zheng8, and Lawrence
L Wald2,9
1Electrical Engineering, Massachusetts
Institute of Technology, Cambridge, MA, United States, 2Athinoula
A. Martinos Center for Biomedical Imaging, Department of
Radiology, Massachusetts General Hospital, Charlestown,
MA, United States, 3Athinoula
A. Martinos Center for Biomedical Imaging, Department of
Radiology, Massachusetts General Hospital, Charlestown,
Massachusetts, United States, 4Department
of Physics, Harvard University, Cambridge, MA, United
States, 5Department
of Radiology – Medical Physics, University Medical
Centre Freiburg, Freiburg, Baden-Württemberg, Germany, 6Procyon
Engineering, San Jose, CA, United States, 7Electrical
Engineering, Stanford University, Stanford, CA, United
States, 8Department
of Electromagnetic Detection and Imaging Technology,
Institute of Electrical Engineering, Chinese Academy of
Sciences, Beijing, China, 9Harvard
Medical School, Boston, MA, United States
A low-cost, open-interface classroom MRI scanner is
demonstrated. The scanner was used in an undergraduate
lab course to interactively teach the concepts of free
induction decay, flip angle measurement, B0 shimming,
gradient echo, spin echo, 1D projection, and 2D as well
as 3D MR imaging. An open library of GUIs, pulse
sequences, and reconstruction codes is being developed
in MATLAB to help build a user base.
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4820. |
26 |
New cardiac and breathing
monitoring tool in MRI.
André Guillou1,2, Gregory Petitmangin2,
Roger Abächerli3, Laurent Bonnemains1,
and Jacques Felblinger1
1Inserm U947 (IADI), Nancy, Lorraine, France, 2Schiller,
Wissembourg, Alsace, France, 3Schiller,
Baar, Zoug, Switzerland
As the ECG in MRI is disturbed by MR gradient swithings,
hall sensors are used as input for gradient artifact
reduction tools (as adaptive filtering), to provide
clean ECG trace. Placed in the MR bore, this sensor was
found to give additional information about respiration
and heart pulse. We explored the possibility to use
these data for patient monitoring during cardiac MRI.
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4821.
|
27 |
Design of multi-channel
switching system for matrix coils
Huijun Yu1, Frank Huethe2,
Sebastian Littin1, Feng Jia1,
Jürgen Hennig1, and Maxim Zaitsev1
1Dept. of Radiology, Medical Physics,
University Medical Center Freiburg, Freiburg, Germany, 2Dept.
of Clinical Neurology and Neurophysiology, University of
Freiburg, Germany
We present a hardware design of multi-channel switches
for a dedicated matrix gradient coil. The switching
system is used to control the combination of the matrix
coil elements. The system consists of a controller and a
number of analog switches. The analog switches are
designed to be placed in the immediate vicinity of the
matrix coil elements inside the magnet bore. A timer
circuit in combination with a current source charges the
bootstrap capacitor periodically and generates the power
supply for the floating driver output circuit. The
realized setup for switching high currents switched
correctly following the coil setting code. Due to its
modular design, the number of channels can be customized
in future systems by choosing the appropriate number of
analog switches.
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4822. |
28 |
Toward 10.5T MRI
J. Thomas Vaughan1, Lance DelaBarre1,
Jinfeng Tian1, Sungmin Sohn1,
Devashshish Shrivastava1, Gregor Adriany1,
and Kamil Ugurbil1
1CMRR - Dept. of Radiology, University of
Minnesota, Minneapolis, MN, United States
To safely and successfully image the whole human at
10.5T, new RF methods and technologies must be
developed. This abstract outlines and shows results for
the first steps toward 10.5T MRI.
|
4823. |
29 |
Magnetic Carrier for
Hyperpolarized 13C
Sample Transfer from DNP Polarizer to MR Scanner
Hong Shang1, Timothy Skloss2,
Cornelius vonMorze1, Lucas Carvajal1,
Mark Van Criekinge1, Peder E.Z. Larson1,
Ralph Hurd3, and Daniel B. Vigneron1
1Radiology and Biomedical Imaging, UCSF, San
Francisco, California, United States, 2GE
Healthcare, Wisconsin, United States, 3GE
Healthcare, California, United States
A specialized magnetic carrier was constructed to supply
a suitable magnetic field(> 50 G) to preserve the
polarization during hyperpolarized sample transfer,
especially for hyperpolarized C-13 urea. It improved the
SNR measured in the MR scanner by 2 fold for C-13 urea
in our experimental tests.
|
4824. |
30 |
Eulerian Video
Magnification for Heart Pulse Measurements in MRI Scanners
Nicolai Spicher1,2, Christopher Brumann1,
Markus Kukuk1, Mark E. Ladd2,3,
and Stefan Maderwald2
1University of Applied Sciences and Arts
Dortmund, Dortmund, Germany, 2Erwin
L. Hahn Institute for Magnetic Resonance Imaging,
University Duisburg-Essen, Essen, Germany, 3Division
of Medical Physics in Radiology, German Cancer Research
Center Heidelberg, Germany
The Eulerian Video Magnification approach is used in
this work for color amplification of video data to offer
an alternative to the conventional contact-based
hardware for peripheral pulse triggering or monitoring
units in MR scanners; the triggering is obtained by
contactless video analysis. Two different test
scenarios, one inside the scanner room of a 7T scanner
and one inside the scanner bore during MR measurements
at 3T, are shown. The results of the algorithm bear good
resemblance with the measured pulse oximeter logs. The
validation of real-time feasibility remains to be done.
|
4825. |
31 |
A platform independent
infrastructure for real-time MRS/MRI data streaming,
processing and storage
Brian J. Soher1
1Radiology, Duke University Medical Center,
Durham, NC, United States
The dynamic flow of MR data from scanners to external
computers during data acquisition is complicated by the
hierarchical study/series organization of data
acquisition and processing and by the variety of
hardware, software and network infrastructures inherent
to MR platforms. These and other issues slow application
prototyping. We introduce a platform/OS independent
software package, called RTView, that simplifies dynamic
data transfer through the use of the Python programming
language and standard network communication protocols
known as XML-RPC. We demonstrate the use of the RTView
platform for streaming real-time multinuclear 31P MR
spectroscopy data off a 3T Siemens Trio.
|
4826. |
32 |
advanced heart tissue
phantom as a reference for MRI sequence evaluation
Michael Werner Eder1 and
Volker Rasche2
1University Hospital Ulm, Ulm, BW, Germany, 2University
Hospital Ulm, BW, Germany
For evaluating dynamic cardiac MR imaging sequences a
advanced heart simulator has been built. The phantom
uses a polyvinyl alcohol (PVA) based tissue model and is
able to simulate heart beat and breathing motion. The
device is specially designed to fit into a clinical
environment. No modifications of the MRI system are
required that could cause the loss of approval. As the
phantom feeds trigger signals directly over the
physiology board all evaluated sequences can be
transferred directly to clinical examination without the
need of sequence reprogramming. Its design allows the
use of cardiac anterior and posterior dedicated receiver
coils.
|
4827. |
33 |
Virtual Phantom MRI: a
novel quantitation method. Temporal stability and spatial
linearity validation.
Giulio Gambarota1,2, Pierre-Antoine Eliat3,
Johanne Bezy-Wendling1,2, and Hervé
Saint-Jalmes1,2
1Université de Rennes 1, LTSI, Rennes,
F-35000, France, 2INSERM,
UMR 1099, Rennes, F-35000, France, 3PRISM
- Biosit CNRS UMS 3480, INSERM UMS 018, Rennes, F-35000,
France
The field of MRI is rapidly moving towards more
quantitative approaches. In this context, virtual
phantoms that would provide a reference signal could be
useful for quantification purposes in MRI. The aim of
the present study was i) to implement a dedicated
experimental set-up to generate MR images of virtual
phantoms ii) to test its temporal stability and signal
linearity. This approach is here referred to as Virtual
Phantom (ViP) MRI. MR images of virtual phantoms were
generated using a stand-alone, independent unit. Thus,
ViP MRI can be performed on MR scanners from different
vendors.
|
4828. |
34 |
Touch NMR: An NMR data
processing application for mobile device
Qiyue Li1, Zhiwei Chen1, Zhiping
Yan2, and Zhong Chen1
1Department of Electronic Science, Xiamen
University, Xiamen, Fujian, China, 2Chenggong
Hospital Affiliated to Xiamen University, Xiamen,
Fujian, China
Mobile devices are playing a more and more important
role in daily life. However, there was no useful
application on mobile devices to help NMR researchers
handle their data. To meet the needs, a free iPad
application, Touch NMR, designed for basic NMR data
processing is introduced. The software system can
process FID data of Agilent, Bruker and JEOL formats. It
can accomplish basic NMR data operations: FFT,
manual/automatic phase correction, automatic baseline
correction, referencing, peak picking, integration and
so on. Besides 1D data, DEPT spectra edit, T1/T2
fitting, and 2D spectrum with projections in the two
dimensions can also be accomplished in Touch NMR. In
addition, the application takes full advantage of
multi-touch technology and gives users a better
experience.
|
4829. |
35 |
Hybrid inverse/FDTD
computational electromagnetic methodology and its potential
application in MR RF field design
Sherman Xuegang Xin1,2 and
Christopher Michael Collins1
1Bernard and Irene Schwartz Center for
Biomedical Imaging, New York University School of
Medicine, New York, NY, United States, 2Biomedical
Engineering, Southern Medical University, Guangzhou,
Guangdong, China
The inverse method in computational electromagnetic
calculation has its particular advantage, that is, the
source electromagnetic field can be specially designed
from the targeted field, which can be designed exactly.
However, it is difficult to directly use inverse method
for the human body in the high-field MR environment,
where the complicated coil-tissue interaction must be
considered. A new methodology, i.e. hybrid inverse/FDTD
method, which has not been reported previously to the
best of the authors’ knowledge, was proposed here for
goal-oriented RF source field design loaded with human
body at high-field MRI.
|
4830. |
36 |
Automation system based on
piezoelectric motor for tuning and matching miniature
monolithic NMR coils
Zhoujian Li1, Georges Willoquet1,
Marie Poirier-Quinot1, Luc Darrasse1,
and Jean-christophe Ginefri1
1Imagerie par Résonance Magnétique Médicale
et Multi-Modalités (IR4M), UMR8081 CNRS, Univ. Paris
Sud, Orsay, France
An automation system based on a piezoelectric motor that
offers high resolution displacement is developed to
automatically tune and match miniature monolithic coils
used in MR microscopy. Tuning is done by approaching a
dielectric slice to shift down the resonant frequency
and matching is achieved by inductive coupling to a
pick-up loop. The piezo-motor is driven by a dedicated
board, which communicates with control software for
automation. The resolution achieved by the developed
system allows automatic matching and tuning with respect
to specified matching level and target frequency with
configurable tolerance.
|
4831. |
37 |
Integral Equations Based
Modeling Approach to Dielectric Shimming
Wyger Brink1 and
Andrew Webb1
1Radiology, Leiden University Medical Center,
Leiden, Zuid-Holland, Netherlands
This work presents a numerical approach using an
integral equations method to model the effect of a
dielectric shim in the RF field. By including body
loading effects explicitely into the Green's function,
the problem complexity is reduced to the interactions
within the dielectric shim.
|
4832. |
38 |
Evaluation of electric
fields induced in the patient during body rotations in the
static magnetic field of a MRI-LINAC system
Adnan Trakic1, Limei Liu1, Hector
Sanchez Lopez1, Luca Zilberti2,
Feng Liu1, Ewald Weber1, and
Stuart Crozier1
1The School of Information Technology and
Electrical Engineering, The University of Queensland,
Brisbane, QLD, Australia, 2Divisione
Elettromagnetismo, Istituto Nazionale di Ricerca
Metrologica, Torino, Italy
This novel study evaluates the induced electric field
and current densities due to the rotation of the patient
in a static magnetic field produced by the split
superconducting magnet of a realistic MRI-Linear
Particle Accelerator (LINAC) system. It was found that
rotating the patient in the radial orientation relative
to the magnet gap with periods larger than about 15.3
seconds would not exceed the ICNIRP exposure limits.
This new research provides useful insights into the safe
use of the MRI-LINAC technology and optimal orientations
of the patient during image-guided treatment.
|
4833. |
39 |
A quiet, fast,
high-resolution desktop MRI capable of imaging solids
Aleksandar Nacev1, Edward Anashkin1,
Juan Pablo Rigla Perez2, Jose Maria Benlloch
Baviera2, Mario Urdaneta1, Azeem
Sarwar1, Pavel Stepanov1, Irving
Weinberg1, and Stanley Thomas Fricke3
1Weinberg Medical Physics, Bethesda, MD,
United States, 2Institute
for Instrumentation in Molecular Imaging (I3M),
Valencia, Spain, 3Children's
National Medical Center, Washington, DC, United States
An inexpensive MRI device that can image solid
structures with short T2 times was developed by adding
gradient coils, pulse sequences, and a GUI to a 0.34T
commercial spectrometer. Gradient coils were created by
hand winding or additive manufacturing. The 3D-printed
coils produced a homogenous gradient and minimized
acoustic noise. The GUI was created so that custom pulse
sequences could be programmed, data gathered, and images
reconstructed. Custom pulse sequences were encoded in C
including: gradient echo pulse sequence; spin echo pulse
sequences; and three dimensional volume acquisitions.
Images were obtained under one second with 50 micron
resolution.
|
4834. |
40 |
Metamaterial cell for B1+
field manipulation at 9.4T MRI
Irena Zivkovic1 and
Klaus Scheffler1,2
1High Field MRI, Max Planck Institute for
Biological Cybernetics, Tuebingen, Germany, 2Center
for Integrative Neuroscience, University of Tuebingen,
Tuebingen, Germany
Many techniques have been developed to improve magnitude
and homogeneity of B1+ field at high field MRI. In order
to manipulate B1+ field, we have designed one cell
metamaterial (MM) plate. When proposed material was
placed between RF transmit coil and phantom, B1+
magnitude and homogeneity significantly improved.
Measured results show over 100% increase of B1+
magnitude in specific area in the case when box monopole
antenna was used as a transmitter. When small loop
antenna was used as a transmitter, there was zero B1+
field without MM plate and significant B1+ when MM plate
was inserted.
|
4835. |
41 |
Rotating sample acquisition
in ultra-low-field MRI
Yi-Cheng Hsu1, Koos C. J. Zevenhoven2,
Ying-Hua Chu1, Juhani Dabek2,
Risto J. Ilmoniemi2, and Fa-Hsuan Lin1,2
1National Taiwan University, Taipei, Taiwan, 2Department
of Biomedical Engineering and Computa of Biomedical
Engineering and Computational Science, Aalto University,
Finland
We propose the rotating sample acquisition (RSA) to
achieve efficient ultra-low-field MRI (ULF-MRI).
Specifically, the sample rotates in the instrument and
we measure ULF-MRI signals without any phase encoding.
The concomitant field artifacts can be minimized because
only frequency encoding is used. Using empirical data,
we demonstrate that RSA is more efficient than
conventional Fourier encoding when only three SQUID
sensors are used. The RSA method holds promise for a
portable imaging system using no phase encoding
gradients and few NMR signal detectors.
|
4836. |
42 |
MPI meets MRI: A first MPI/MRI
hybrid scanner
Patrick Vogel1,2, Steffen Lother1,2,
Martin A. Rückert1, Walter H. Kullmann3,
Peter M. Jakob1,2, Florian Fidler2,
and Volker C. Behr1
1Experimental Physics 5 (Biophysics),
University of Würzburg, Würzburg, Bayern, Germany, 2Research
Center for Magnetic Resonance Bavaria e.V., MRB,
Würzburg, Bayern, Germany, 3Institute
of Medical Engineering, University of Applied Sciences
Würzburg-Schweinfurt, Schweinfurt, Bayern, Germany
This abstract describes the first setup of a bimodal
Magnetic-Particle-Imaging/Magnetic-Resonance-Imaging
tomograph and shows the first results.
|
4837. |
43 |
Evaluation of a Ultra High
Dielectric Constant (uHDC) Package for Enhanced Cervical
Spine Imaging
Christopher Sica1, Sebastian Rupprecht1,
Wei Luo2, Jeff Vesek3, Raffi Sahul4,
Seongtae Kwon4, Michael Lanagan2,
Dan Nguyen3, and Qing Yang1
1Radiology, Penn State College of Medicine,
Hershey, Pennsylvania, United States, 2Engineering
Science and Mechanics, Penn State University,
Pennsylvania, United States, 3Radiology,
Hershey Medical Center, Hershey, Pennsylvania, United
States, 4TRS
Technologies, State College, Pennsylvania, United States
Previously, we explored the use of dielectric pads
containing water and barium titanate beads to enhance
imaging of the cervical spine. One drawback to that
approach was the volume of dielectric required for
enhancement. In this work, we quantify the performance
of a ultra high dielectric constant (uHDC) package
containing monolithic blocks of relative permittivity
~800. This package is reduced in volume relative to our
previous configuration. SNR gains of 20 – 40% were
observed on discs C1 – C4. Gains of about 10% were found
on C5, and a slight loss on C6. Average reduction of
system power was 64.18%.
|
4838. |
44 |
Automatic selection of
anterior floating coil array based on lipid layer signal
analysis
Bing Wu1, Qingyu Dai1, Xuelian Lu1,
and Jiabin Yao1
1GE healthcare, Beijing, Beijing
Municipality, China
A rapid and robust method for determining the location
of floating anterior coil array is proposed, hence
allowing automatic selection of the proper coil element
in real time scan. In vivo experiments have been
proposed for verification. This method may be combined
with standard system scout scan and adds little or no
additional scan time.
|
4839. |
45 |
Catheter-mounted expandable
loop (CAMEL) balloon RF coil for high-resolution
intracardiac MR imaging
Nelly A. Volland1,2, J. Rock Hadley1,2,
Eugene G. Kholmovski1,2, Nassir F. Marrouche2,
and Dennis L. Parker1,2
1Utah Center for Advanced Imaging Research,
University of Utah, Salt Lake City, Utah, United States, 2Comprehensive
Arrhythmia Research & Management Center, University of
Utah, Salt Lake City, Utah, United States
Purpose: A catheter-mounted expandable loop (CAMEL)
balloon RF coil for cardiac applications was developed
and evaluated. Methods: The coil inductive flexible loop
was sandwiched between two balloons to protect the coil
from fluids. The inner balloon was inflated with saline
to expand the coil and reduce the susceptibility
mismatch between the inner balloon volume and phantom
solution. Results and conclusion: A balloon CAMEL coil
prototype was successfully constructed. MR images were
acquired at 3T in a saline phantom. The SNR with in the
coil sensitive volume was over 20 times the SNR of the
external coils currently commercially available.
|
4840. |
46 |
Faster imaging for MEG-MRI
Angelo Galante1, Allegra Conti2,
Cinzia De Luca2, Vittorio Pizzella3,
Gian Luca Romani3, Raffaele Sinibaldi2,
Marcello Alecci4, Piero Sebastiani5,
Antonello Sotgiu5, and Stefania Della Penna3
1MESVA, Department of Life, Health &
Environmental Sciences, L'Aquila University, L'Aquila,
AQ, Italy, 2Department
of Neuroscience and Imaging, University of Chieti, CH,
Italy, 3Institute
of Advanced Biomedical Technologies, University of
Chieti, CH, Italy, 4MESVA,
Department of Life, Health & Environmental Sciences,
L'Aquila University, AQ, Italy, 5ITA
S.r.l., AQ, Italy
Results from a new hybrid MEG-MRI system, working at
8.9mT without prepolariztion pulses, are presented. When
scaled to a full size system, suitable for human
imaging, they give indications that this approach allows
faster imaging and better spatial resolution if compared
to other existing devices based on SQUID parallel
imaging in the kHz range and prepolarization pulses.
|
4841. |
47 |
A novel MR-guided
radiotherapy system: simulation and experimental validation
Teo Stanescu1,2, Jason Marle3,
Tony Tadic1, Jeff Winter4, Michael
Sweitzer3, and David Jaffray1,2
1Radiation Physics, Princess Margaret Cancer
Centre, University Health Network, Toronto, Ontario,
Canada, 2Radiation
Oncology, University of Toronto, Toronto, Ontario,
Canada, 3Varian
Medical Systems, Palo Alto, CA, United States, 4IMRIS,
Minnetonka, MN, United States
Numerical simulations and experiments were performed to
quantify the magnetic field decoupling between
sub-components (i.e. linear accelerator gantry, patient
couch assembly and 1.5T MR) for an MR-guided linac
system.
|
4842. |
48 |
Role of Birdcage Volume
Resonators for High-Resolution Wrist Imaging at High and
Ultra-High Fields
Yusuf A Bhagat1, Po-Hsiang Lai1,
Xu Zhu1, Insoo Kim1, and Zhouyue
Pi1
1Emerging Technology Lab, Samsung R&D
Institute America, Richardson, Texas, United States
This educational review draws attention to birdcage
volume resonators as a simple alternative to
phased-array receive coils for high-resolution
microstructural imaging of the human wrist. The value of
quadrature volume coils for transmit-receive (Tx-Rx)
applications is better realized at ultra-high fields ( 7T)
due to lack of body Tx coils. Here, by virtue of
examples, we discuss the design of birdcage resonators
for wrist imaging at 3T and 7T. Further, we highlight
their utility for specific absorption rate-compliance,
patient setup for improved tolerance and a rapid
spin-echo based technique for high-quality imaging of
trabecular (spongy) bone microstructure.
|
|
|
|
ELECTRONIC
POSTER SESSION ○ MR ENGINEERING |
Magnets, Gradients & Shimming
Thursday 15 May 2014
Exhibition Hall |
14:30 - 15:30 |
|
|
|
Computer # |
|
4843. |
25 |
The effect of anchoring of
MR scanners to prevent earthquake hazards – an analysis of
the damages to the 602 MR scanners in Great East Japan
Earthquake
Sachiko Yamaguchi-Sekino1, Yoshio Machida2,
Toshio Tsuchihashi3, Haruo Isoda4,
Takeshi Noguchi5, and Toshiharu Nakai6
1National Insitiute of Occupational Safety
and Health, Japan, Kawasaki, Kanagawa, Japan, 2Tohoku
University, Graduate School of Medicine, Miyagi, Japan,3Department
of Radiology, Nippon Medical School Hospital, Tokyo,
Japan, 4Nagoya
University, Graduate School of Medicine, Aichi, Japan, 5National
Institute for Material Science, Ibaraki, Japan, 6NeuroImaging
& Informatics, National Center for Geriatrics and
Gerontology, Aichi, Japan
In order to evaluate the potential risk to MR scanners
and consider patient safety under large earthquakes, we
have performed a survey study to investigate damages in
MR scanners caused by Great East Japan Earthquake. It
was confirmed that the extent of damage was
significantly different between seismic scale (SS) 5 and
SS over 6. Logistic regression analysis suggested that
anchoring for MR facilities reduced the occurrence of
quake-induced damages in MR scanners. And significant
decrease in machine damages was observed in the group of
base isolation structure for medical facilities compared
with earthquake-proof structures.
|
4844. |
26 |
A whole body conduction
cooled MRI magnet design for ultra-high field strength of 7T
Michael Martens1, Tanvir Baig1,
Zhen Yao1, Charles Poole1, Robert
Deissler1, Robert Brown1, David
Doll2, and Michael Tomsic2
1Department of Physics, Case Western Reserve
University, Cleveland, Ohio, United States, 2Hyper
Tech Research Inc., Columbus, Ohio, United States
A 7T conduction-cooled MRI whole-body magnet design
using Nb3Sn superconductor is found for a current
density of 179.95 A/mm2, a maximum peak field on a
bundle of 11.59T, and operating at 8K. The high current
density on wire allowed by the larger peak field helps
to reduce the superconductor volume in comparison with
high field NbTi magnet designs. Although the present
manufacturing cost of Nb3Sn is higher than NbTi, the
wire volume reduction and the 99% decrease in liquid
helium usage may make Nb3Sn conduction cooled magnets a
viable alternative for ultra-high field magnet systems.
|
4845. |
27 |
Sequencial Abnormal Events
in High-Temperature Superconducting MRI Magnet
Shin-ichi Urayama1, Yasuyuki Terao2,
Osamu Ozaki2, Hitoshi Kitaguchi3,
Shinya Kawashima2, Takashi Hase2,
Ken-ichi Sato4, and Hidenao Fukuyama1
1Human Brain Research Center, Kyoto
University, Kyoto, Kyoto, Japan, 2Kobe
Steel, Ltd., Kobe, Japan, 3National
Institute for Materials Science, Ibaraki, Japan, 4Sumitomo
Electric Industries, Ltd., Osaka, Japan
Because of recent deficit of liquid helium, helium-free
MRI magnets with high temperature superconducting (HTS)
materials have been expected as one of the solutions. We
have developed a 3T HTS-MRI system for human brain
research with Bi-2223 tapes and showed its feasibilities
at 1.5T. However, in spite that we succeeded energizing
to 3T three times, sequencial abnormal events were
happened for longer than ten minutes during the
ramp-down at the third trial to 3T. Here, we show these
unique events specific to HTS magnets.
|
4846. |
28 |
Experimental Investigations
on Gradient Coil Induced Magnet Heating in MRI System
Longzhi Jiang1, Yihe Hua2, Liya Ma3,
Sung Moon1, Jun Li2, Kishore
Mogatadakala1, and Tim Havens1
1Global MRI, GE Healthcare, Florence, SC,
United States, 2GE
Global Research, Shanghai, China, 3GE
Healthcare, Beijing, China
The dynamic coupling between gradient coil and magnet
has generated image quality issues at low frequencies
and limited operational duty cycle at medium and high
frequencies due to induced magnet Joule heating. With
the combined demand for high patient through-put and
high performance gradient coils in high field MRI
systems, numerous researchers have attempted to develop
both improved simulation capability and experimental
apparatus to understand the Joule heating induced helium
boil-off. However, to the authors’ best knowledge, the
effects of dynamic coupling induced Joule heating is not
yet fully understood. In this study, a novel
experimental apparatus was devised to understand
gradient coil induced magnet heating under different
gradient coil mounting conditions. The apparatus
included a whole body magnet with hermetically sealed
cooling system having very limited helium volume and a
gradient coil with minimum interaction. This paper
demonstrates consistent correlation between the full
mechanical-electro-magnetic coupling model and the
experimental results. Furthermore, 100% operational duty
cycle has been achieved for clinical protocols.
|
4847. |
29 |
Integrated Image
Reconstruction and Gradient Nonlinearity Correction
Joshua D. Trzasko1, Shengzhen Tao1,
Yunhong Shu1, Armando Manduca1,
and Matt A. Bernstein1
1Mayo Clinic, Rochester, MN, United States
The gradient fields used for spatial encoding in
clinical MRI are never truly linear over the imaging
FOV. As standard MRI signal models presume gradient
linearity, reconstructed images exhibit geometric
distortion unless gradient deviations are properly
accounted for. Geometric distortion is typically
corrected via image-domain interpolation. Although this
approach is straightforward, it does not account for the
effects of finite sampling, undersampling, or noise, and
may degrade spatial resolution. In this work, we propose
a correction strategy that accounts for gradient
nonlinearity during – rather than after – k-space to
image reconstruction, and lessens the tradeoff between
geometric accuracy and spatial resolution.
|
4848. |
30 |
Accurate Measurement of MRI
Gradient Characteristics
Gerald B Matson1,2 and
Hui Liu1
1Center for Imaging of Neurodegenerative
Diseases, Department of Veterans Affairs, San Francisco,
California, United States, 2Pharmaceutical
Chemistry, University of California, San Francisco, San
Francisco, California, United States
The imperfect fidelity of MRI gradient systems results
in altered k-space trajectories, which can result in
image degradation. Under the assumption that the
gradient system is linear and time invariant, accurate
measurement of the MRI gradient impulse response
function (GIRF) can be used to predict the actual output
gradient waveform as opposed to the requested waveform.
In this study we demonstrate a simple sample and coil
arrangement can be used to obtain GIRFs of high
precision that can accurately predict gradient output
waveforms. This capability could potentially be used to
predict actual k-space trajectories for improved
fidelity of image reconstruction.
|
4849. |
31 |
Integrated RF/Shim Coil
Array for Parallel Reception and Localized B0 Shimming
in the Human Brain at 3T
Trong-Kha Truong1, Dean Darnell1,
and Allen W Song1
1Brain Imaging and Analysis Center, Duke
University, Durham, NC, United States
Multi-coil shimming with localized shim coils can
effectively shim high-order B0 inhomogeneities,
but requires an additional shim coil array outside or
inside the RF coil, which compromises the shimming
performance and/or SNR. To address these limitations, we
recently proposed a new concept that enables parallel RF
excitation/reception and B0/B1 shimming
with a single coil array, thus maximizing both the SNR
and shimming performance, and demonstrated its
feasibility in phantom experiments. Here, we further
validate it in vivo by demonstrating its ability to
perform parallel reception and localized B0 shimming
in the human brain at 3T, specifically for distortion
correction in DTI.
|
4850. |
32 |
Which is the impact of the
coil track width and frequency over a split gradient coil
performance?
Fangfang Tang1, Hector Sanchez Lopez1,
Fabio Freschi2, Feng Liu1, Yu Li1,
and Stuart Crozier1
1School of Information Technology and
Electrical Engineering, The University of Queensland,
Brisbane, Queensland, Australia, 2Politecnico
di Torino Corso Duca Degli Abruzzi, Department of
Energy, Torino, Italy
In order to study the influence on gradient coils of
different track widths and frequencies, 30 split and
shielded, whole-body x-gradient coils were designed. The
track width was set from 1mm to 30mm with an increment
of 1mm. The 30 designed split x-gradient coils were
analyzed to study the interaction between the coils and
the metallic surroundings, which took into account the
skin and proximity effects. This study provides very
valuable information which will guide coil engineers to
choose the optimal wire track on regards the MRI coil
applications.
|
4851. |
33 |
Design, Construction and
Initial Evaluation of a Folded Insertable Head Gradient Coil
Trevor Paul Wade1,2, Andrew Alejski1,
Janos Bartha1, Dina Tsarapkina1,
R. Scott Hinks3, Graeme C. McKinnon3,
Brian K. Rutt4, and Charles A. McKenzie2
1Robarts Research Institute, The University
of Western Ontario, London, Ontario, Canada, 2Medical
Biophysics, The University of Western Ontario, London,
Ontario, Canada, 3GE
Healthcare, Waukesha, WI, United States, 4Radiology,
Stanford University, Stanford, CA, United States
A symmetric, folded gradient, was designed for human
brain imaging, with a target gradient strength of 80
mT/m and slew rate of 2900 mT/m/s. This design should
limit forces and torques leading to a quieter coil with
better eddy-current performance. The ultra-short design
allows for human brain imaging without the need for
shoulder cut-outs. The insertable coil was built using
litz wire for transverse axes and hollow copper for Z to
facilitate cooling. It was successfully interfaced with
a clinical scanner and its electrical and imaging
performance was characterised.
|
4852. |
34 |
A Traveling-Wave Approach
to Acoustic Noise Reduction in MR Gradient Coils
Simone Angela Winkler1, Andrew Alejski2,
Trevor Wade2, Charles McKenzie2,
and Brian K Rutt1
1Dept of Radiology, Stanford University,
Stanford, California, United States, 2Robarts
Research Institute, The University of Western Ontario,
London, Ontario, Canada
We present a new wave-based framework for understanding
acoustic noise in MR gradient coils, and propose two new
concepts for acoustic noise reduction. Results of this
wave-based coupled structural-acoustic modeling, as well
as experimental measurements, demonstrate that the
addition of an impedance matching “horn” and an
absorbing end cap both act to decrease acoustic noise
inside the gradient coil. Simulation results show mean
sound pressure level reductions of 2 dB for horn and end
cap, and 3 dB for both used in combination. Experimental
results show mean SPL reductions of 4 dB for horn and 9
dB for end cap.
|
4853. |
35 |
Fast Shimming strategy
using intermediate space conversion
Hongpyo Lee1, Sung-Min Gho1,
Eunhae Joe1, Joonsung Lee2,3, and
Dong-Hyun Kim1
1Electrical and Electronic Engineering,
Yonsei University, Sin-chon dong, Seoul, Korea, 2Nanomedical
Research Center, Yonsei University, Sin-chon dong,
Seoul, Korea, 3SIRIC,
Yonsei University, Sin-chon dong, Seoul, Korea
In this abstract, we introduce an in vivo volumetric
shim strategy which can be performed in a very short
time using an intermediate space conversion idea. Linear
shimming and high-order shimming approaches are
presented.
|
4854. |
36 |
Balancing a 500 mm central
gap split gradient coil for a hybrid MRI-linac scanner.
Hector Sanchez-Lopez1, Fangfang Tang1,
and Stuart Crozier1
1School of Information Technology &
electrical Engineering, The University of Queensland,
Brisbane, QLD, Australia
This study aims to present a robust guideline to design
a 500 mm transversal and 620 mm axial gap split
x-gradient coil to be installed in a hybrid Linac-MRI
scanner. The target torque (force) was varied from 0 to
15 Nm (15N) while the changes on slew rate, achieved net
torque (force), peak current density, average power loss
in the coil and cryostat and stored magnetic energy were
observed. We found a nearly zero torque (force) coil
capable to produce more than 200 T/m/s, and 33 µT/mA.
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4855. |
37 |
A Robust guideline to
design a split gradient coil for a hybrid Linac-MRI scanner
Hector Sanchez-Lopez1, Fangfang Tang1,
and Stuart Crozier1
1School of Information Technology &
electrical Engineering, The University of Queensland,
Brisbane, QLD, Australia
This study aims to present a robust guideline to design
a 500 mm transversal and 620 mm axial gap split
x-gradient coil to be installed in a hybrid Linac-MRI
scanner. The methodology is divided in two parts:
selection of the optimal shielding strategy (this work)
and torque/force balancing. Four shielding approaches
are studied in order to determine the most suitable for
torque balancing and high coil performance. We found
that coils designed using the minimizations of the
magnetic energy in the whole system are the most
suitable for torque/force balancing, optimal
pre-emphasis, high slew rate and lower power loss.
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4856. |
38 |
Designing biplanar gradient
coils with minimum power dissipation for NMR microscopy
Peter T. While1, Markus V. Meissner1,
and Jan G. Korvink1,2
1Department of Microsystems Engineering
(IMTEK), Laboratory for Simulation, University of
Freiburg, Freiburg im Breisgau, Baden-Württemberg,
Germany,2Freiburg Institute for Advanced
Studies (FRIAS), University of Freiburg, Freiburg im
Breisgau, Baden-Württemberg, Germany
High-resolution NMR microscopy demands strong gradient
fields. Power dissipation in micro-gradient coils is a
primary concern and must be controlled carefully to
avoid over-heating the system or the sample and to
maximize the duty cycle. In this work, a recently
reported method for designing minimum power gradient
coils that accounts for the subsequent means of
fabrication is applied to the design of a 3-axis
biplanar micro-gradient system. A survey of results is
presented, comparing coils designed for x-, y- and
z-gradients, using both the standard and the new
approach, and contrasting the merits of building using
tracks or wires.
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4858. |
40 |
Temperature simulations for
the inverse boundary element gradient coil design method
Michael Stephen Poole1, Clemente Cobos
Sanchez2, and N Jon Shah1,3
1INM-4, Forschungszentrum Jülich, Jülich,
Germany, 2Ingeniería
en Automática, Electrónica, Arquitectura y Redes de
Computadores, Universidad de Cádiz, Cadiz, Spain, 3Department
of Neurology, RWTH Aachen, Aachen, Germany
In this work we describe a method by which the
temperature of gradient coils, designed with arbitrary
geometry using the inverse boundary element method, can
be simulated. The method requires tuning of the thermal
parameters of the coil and its support. This simulation
method should aid the coil design process by allowing
the thermal performance of multiple coil designs to be
estimated without construction.
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4859. |
41 |
Realization of a
synergistic passive and active shimming system to optimize B0 field
homogeneity in micro MR imaging
Rahul Dewal1, Zhipeng Cao2,
Sebastian Rupprecht3, and Qing X. Yang1,3
1Bioengineering, Penn State College of
Medicine, Hershey, PA, United States, 2Institute
of Imaging Science, Vanderbilt University, Nashville,
TN, United States, 3Radiology,
Penn State College of Medicine, Hershey, PA, United
States
The B0 field
inhomogeneity artifacts near the air-tissue interfaces
in animal and human brains at high field are difficult
to remove with standard active shim coils as the
associated gradients are high-order and highly
localized. Several passive and localized active shimming
methods have been proposed to deal with this problem but
have high calibration or hardware requirements. Here, a
synergistic shimming system that simultaneously
optimizes the linear active shim coil settings and
passive shim element configuration is demonstrated via
application to an in
vivo mouse
brain. This synergistic shimming approach is expected to
be extensible to high-field human MRI systems.
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4860. |
42 |
Toward Gradient Systems
with Really Identical Gradient Coils
Gerrit Schultz1, Feng Jia1, and
Maxim Zaitsev1
1Dept. of Radiology - Medical Physics,
University Medical Center Freiburg, Freiburg, Germany
Cylindrical gradient coils are typically designed on
three different layers having different radii. As a
consequence, the x- and y- gradients or, in case a magic
angle gradient system is constructed, all three gradient
coils may be designed to be similar, but they are not
identical. Identical designs are desirable to further
reduce the differences of the coil properties such as
switching speed or maximum gradient strength. MR
acquisitions would potentially profit from such an
approach, and, with identical designs, also the
optimization and fabrication of gradient systems may be
facilitated. In this abstract, gradient system designs
are proposed that consist of such identical gradient
coils.
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4861. |
43 |
Experimental validation of
modal gradient coil design methodologies
Elliot Charles Smith1, Hector Sanchez Lopez1,
Michael Poole2, and Stuart Crozier1
1ITEE, The University of Queensland,
Brisbane, Queensland, Australia, 2Institute
of Neuroscience and Medicine, Jülich, Jülich, Germany
In this work we validated the feasibility of design and
analysis of a coil which excites only certain eigenmodes
in a surrounding structure. The work validated previous
theoretical results.
|
4862. |
44 |
Fast Method for Parametric
System Identification of Gradient Systems
Yu-Chun Chang1,2, Martin Eschelbach1,
Nikolai Avdievitch1, Klaus Scheffler1,
and Anke Henning1,3
1Max Planck Institute of Biological
Cybernetics, Tuebingen, Baden-Wuerttemburg, Germany, 2Graduate
School of Neural & Behavioural Sciences, University of
Tuebingen, Tuebingen, Baden-Wuerttemburg, Germany, 3Institute
for Biomedical Engineering, University and ETH Zurich,
Switzerland
A method for characterising a gradient system is
introduced. This is a parametric method and thus the
system has an analytic form. It is fast and requires
only one measurement in each gradient direction and can
thus be completed in minutes. It can also be extended to
characterise the shim system. Monitoring the B0 field is
done using a 16 channel field camera. The predicted
model is compared to measured data.
|
4863. |
45 |
Measurement and Correction
of Gradient Nonlinearity by Spherical Harmonic Fitting using
the ADNI Phantom
Shengzhen Tao1, Joshua D. Trzasko1,
Jeffrey L. Gunter1, Seung-Kyun Lee2,
Ek T. Tan2, Yunhong Shu1, Kaely B.
Thostenson1, and Matt A. Bernstein1
1Mayo Clinic, Rochester, MN, United States, 2GE
Global Research, Niskayuna, NY, United States
Standard strategies to correct image distortion due to
gradient non-linearity are based on a parameterization
of the gradient field. The correction coefficients are
predetermined and the same set of coefficients is
applied to all systems in the field. In this work, we
develop a simple method to measure and fit the gradient
correction on a per-system basis using the Alzheimer’s
Disease Neuroimaging Initiative phantom. A 3D spherical
harmonic approximation of the distortion is determined
and used for correction. The proposed method does not
require detailed knowledge of gradient system and can be
used in a variety of settings.
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4864. |
46 |
Phantom Results with a
Matrix Shim Coil
Derek A. Seeber1, Kevin Koch2, and
Dirk Beque3
1GE Healthcare, Florence, SC, United States, 2Applied
Science Lab, Milwaukee, WI, United States, 3GE
Reseach, Munich, Germany
A 27 cm diameter phantom was placed inside a 3T system
consisting of a gradient coil with a 24 channel matrix
shim array in a 6x4 array and was used to shim the
phantom. The phantom studies demonstrate a 3 times
reduction in frequency spread as compared with gradient
only shimming across the entire phantom. Slice by slice
shimming is shown to further reduce the frequency spread
by an additional factor of 2 over a global shim. The low
induced gradient voltages in the shim coils and fast
switching times demonstrate a potential for dynamic
shimming in the future.
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4865. |
47 |
Automatic Gradient Delay
Correction Using Center-Acquisition-at-Partial-Ramp Imaging
(CAPRI)
Anna-Katinka Bracher1, Erich Hell2,
Johannes Ulrici2, and Volker Rasche1
1Internal Medicine II, University Hospital of
Ulm, Ulm, BW, Germany, 2Sirona
Dental Systems, HE, Germany
Center-Out imaging sequences like UTE are very sensitive
to trajectory imprecision in waveform and to k-space
shift due to system delays. In this article an automatic
delay correction method is introduced to determinate the
delays by direct measurement of the echo peak shift.
Therefore a conventional UTE imaging sequence is
combined with an additional pre-phasing gradient to
shift k-space center along the rising slope of the
readout gradient. Furthermore the signal acquisition is
started in front of k-space origin to acquire a partial
echo for echo peak detection.
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