Traditional Posters
: Engineering
|
Click on
to view the
abstract pdf and click on
to view the pdf of the poster viewable in the poster hall.
|
RF Circuits & Systems
Wednesday May 11th
Exhibition Hall |
13:30 - 15:30 |
1849. |
Improving UHF
Transmit Efficiency with Voltage Baluns
Debra Strick Rivera1, Carsten
Koegler1, and Robert Turner1
1Neurophysics, Max Planck
Institute for Human Cognitive and Brain
Sciences, Leipzig, Germany
Cable radiation reduces effective transmit
power. Radiated power increases with the
fourth power of frequency, and can therefore
be detrimental to UHF transmit arrays.
Baluns can improve voltage balance across
transmit coils, and thereby reduce cable
radiation. Amplitude balance, phase balance,
and common-mode rejection ratio were
introduced as simple quantitative methods.
Wide-band and narrow-band 180° baluns were
analyzed. Performance of narrow-band baluns
was dramatically improved through amplitude
and phase matching measurements. Transmit
efficiency was characterized in the scanner
from flip-angle maps. The addition of 180°
baluns improved transmit power efficiency
between 10% (on average) and over 50% at 7T.
|
1850. |
High-Efficiency RF Power-Amplifier Module for
Magnetic-Resonance Imaging
Frederick H. Raab1, Martin C.
Poppe2, and Daniel P. Myer3
1Green Mountain Radio Research
Company, Colchester, VT, United States, 2Poppe
Associates, 3Communication
Power Corporation
This amplifier system is based upon the Kahn
EER (envelope-elimination-and-restoration)
technique. The amplifier system incorporates
class-E RF-power amplifiers, class-S
modulators, and a digital signal processor.
The DSP includes capability for generating
stored signals as well as digitizing and
amplifying low-level analog RF inputs. The
module incorporates four RF-power amplifiers
and can produce up to 750 W with an overall
efficiency of 70 percent. It has a bandwidth
of 250 kHz and an envelope rise time of 1
s, and can be configured for operation
between 10 and 128 MHz.
|
1851. |
RF Coil
Element Mounted Power Amplifiers
John T Vaughan1, and Daniel Myer2
1University of Minnesota,
Minneapolis, MN, United States, 2CPC
RF power amplifiers can be mounted on the
coil, in the magnet for improved efficiency
and lower cost.
|
1852. |
Silicon
Carbide MRI Transmitters
Oliver Heid1, and Timothy Hughes1
1Corporate Research, Siemens AG,
Erlangen, Bavaria, Germany
Silicon Carbide JFETs promise to
revolutionize RF power generation up to UHF
frequencies. The main advantages are
extremely high efficiency, power density and
the absence of RF load matching
requirements. We report on the design and
testing of a 11kW prototype RF transmitter
module.
|
1853. |
High Q
Reactive Network for Automatic Impedance
Matching
Barbara L Beck1,2, Sien Wu3,
Walker J Turner3, Rizwan
Bashirullah3, and Thomas H Mareci2,4
1McKnight Brain Institute,
University of Florida, Gainesville, FL,
United States, 2National
High Magnetic Field Laboratory, Tallahassee,
FL, United States, 3Electrical
and Computer Engineering, University of
Florida, 4Biochemistry
and Molecular Biology, University of Florida
MR coil-impedance matching for in vivo
animal studies in high field, small
diameter, horizontal bore magnets is a time
consuming and challenging procedure due to
limited space and large frequency shifts
from sample loading. We developed a High-Q
input circuit attached to an automatic
impedance matching system that optimizes,
within seconds, the tuning and matching of a
single-frequency coil. The procedure can be
performed with the animal in the magnet,
negating the need for laborious manual
tuning, while at the same time, reducing the
stress on the animal. Comparison to a coil
with discrete components demonstrates
equivalent SNR.
|
1854. |
Time Domain
Modeling of MR Linear Balanced Duplexers
Switched with Low Magnetic Moment PIN Diodes
Robert H Caverly1, William E
Doherty2, and Ronald Watkins3
1ECE, Villanova University,
Villanova, PA, United States, 2Microsemi-Lowell, 3Radiology,
Stanford University
The time domain simulation techniques
outlined in the abstract will help MR
engineers to optimize the parameters of TR
switching and to help improve minimum echo
time. The work will help MR engineers pick
the appropriate PIN diode for their TR
switching applicaiton.
|
1855. |
Tunable
Adjustable Inductive Decoupling (TAID) Board
Victor Taracila1, Aleksey Zemskov1,
Miguel A Navarro1, Vijayanand
Alagappan1, and Fraser Robb1
1GE Healthcare, Aurora, Ohio,
United States
One of the subsets of inductive decoupling
is the so-called transformer decoupling,
which in fact represents a remote inductive
decoupling. It is used when overlapping
between elements is not desired due to
possible sensitivity overlap that affects
the g-factor in accelerated imaging. The
traditional transformer used in MRI coils is
built out of inter-woven or adjacent
inductors sharing a common axis. One of the
disadvantages of this type of transformer is
the difficulty of adjustment of the
coupling, dimensions and possible inductive
coupling to other inductors in the MRI
system. In this work we propose a
transformer based on “RF Invisible”
inductors shape with adjustable inductive
coupling strength and no self-inductance,
which is very handy for MRI coil design and
applications.
|
1856. |
Noise Power
Reduction Strategy by Matching Receiver
Bandwidth to the Coil Sensitivity Profile of the
Phased Array Coil
Sergei Obruchkov1, William
O'Reilly2, and Arsen Hajian3
1University of Waterloo,
Waterloo, ON, Canada, 2Tornado
Medical Systems, Toronto, ON, Canada, 3Systems
Design Engineering, University of Waterloo,
Waterloo, ON, Canada
Digital receiver technology is relatively a
new comer to the field of MRI and it offers
great opportunity for customization and
research. The purpose of our work was to
show how developments in digital
communication technology may be used to used
as MR receiver chains such that each receive
channel is optimized to acquire data from an
individual coil in the phased array. The
findings showed that by decreasing receiver
bandwidth and digital filtering it is
possible to reduce noise power, thus by
matching receiver channel to individual coil
signal from phased array coils could be
optimized.
|
1857. |
Radio
Frequency Front-End Circuitry for an Implantable
Multiple Frequency Coil
Walker J. Turner1, Barbara L.
Beck2, Sien Wu1,
Thomas H. Mareci3, and Rizwan
Bashirullah1
1Electrical and Computer
Engineering, University of Florida,
Gainesville, FL, United States, 2McKnight
Brain Institute, University of Florida, 3Biochemistry
and Molecular Biology, University of Florida
This RF front-end circuitry is designed for
clock and data extraction from wirelessly
transmitted RF pulses for use in controlling
the resonance of an implantable receiver
coil with a digitally controlled capacitor
array intended for monitoring an implanted
artificial pancreas. The fabricated chip
measures 650um by 450um and demonstrates the
capability of data/clock recovery. The
design is compatible with current NMR
console technology and can be further
integrated for in vivo operation.
|
1858. |
Common-mode
differential-mode (CMDM) method for quadrature
transmit/receive surface coil for ultrahigh
field MRI
Ye Li1, Yong Pang1,
and Xiaoliang Zhang1,2
1Department of Radiology and
Biomedical Imaging, Univerisity of
California San Francisco, San Francisco,
California, United States, 2UCSF/UC
Berkeley Joint Graduate Group in
Bioengineering, San Francisco, California,
United States
We propose a CMDM design of quadrature
transmit/receive surface coil at 7T. A
prototype coil was fabricated. Bench test
and MR phantom experiments were carried out
to evaluate the coil performance. Our
results show that the common-mode and
differential-mode are decoupled sufficiently
at 300MHz range due to the intrinsic
decoupling of the two modes. SNR improvement
is achieved in the whole region of interest.
The CMDM coil is feasible for parellel
imaging. The proposed method is an
efficient, robust and simple approach to
increase the SNR of surface coils as well as
surface coil elements in array coils.
|
1859. |
Vertical Loop
Decoupling Method for Gapped Phased-Array Coils
Yoshihisa Soutome1, Yosuke Otake1,
and Yoshitaka Bito1
1Central Research Laboratory,
Hitachi Ltd., Kokubunji, Tokyo, Japan
We have developed a new decoupling method
using a vertical loop for gapped
phased-array coils. The vertical loop is
placed between nearest-neighbor coils, and
by changing the value of the capacitor in
the vertical loop, decoupling can be easily
achieved. We also fabricated a 3.0T 2-ch
loop array with vertical loop and
demonstrated its decoupling performance. The
coupling S12 measured between the two coils
was −28 dB. Phantom images showed no
significant coupling between the coils.
These results indicate that the proposed
method can effectively decouple between the
nearest-neighbor coils in gapped
phased-array coils.
|
1860. |
Capacitor/Inductor Decoupling and Its New
Application to Microstrip Array
Bing Wu1, and Xiaoliang Zhang2,3
1Coil Engineering, GE Healthcare,
Wauehsha, WI, United States, 2Radiology
and Biomedical Imaging, UCSF, 3UCSF/UC
Berkeley Joint Graduate Group in
Bioengineering, San Francisco, CA, United
States
Transformer or capacitor is often required
to electromagnetically decouple the gapped
loops, non-adjacent loops, or microstrip
resonators in RF coil arrays when
conventional coil overlapping is not
applicable. In this abstract, we analyze the
general L/C decoupling circuits and suggest
the use of inductor for decoupling at high
fields. Based on the circuit analysis, a new
inductive decoupling method is proposed for
designing microstrip arrays at high magnetic
fields.
|
1861. |
Optimised LNAs
for 3 T, 7 T and 9.4 T
Andreas Peter1, and Jan G.
Korvink1,2
1Department of Microsystems
Engineering - IMTEK, University of Freiburg,
Freiburg, Germany, 2Freiburg
Institute of Advanced Studies (FRIAS),
University of Freiburg, Freiburg, Germany
We present the design and optimisation of a
novel single and dual-stage low-Z LNAs for 3
T, 7 T and 9.4 T. Cascaded two-port networks
represent the small-signal behaviour of the
LNA. Matlab is used to optimise the
component values to fulfil the desired
matching conditions at the input and the
output of the LNA together with a minimal
noise figure, a maximum gain and
unconditional stability. A gain of 38 dB
together with a noise-figure of 0.3 dB was
achieved at 7 T.
|
1862. |
Miniaturized
two-stage preamplifiers for receive-array coils
at 400 MHz
Elmar Fischer1, Andreas Peter2,
Daniel Sonner3, Hermann Massler3,
Jan G Korvink2,4, Jürgen Hennig1,
and Maxim Zaitsev1
1Radiology, University Medical
Center Freiburg, Freiburg, Germany, 2Microsystems
Engineering – IMTEK, University of Freiburg,
Freiburg, Germany, 3Hochfrequenz-Bauelemente
und -Schaltungen, Fraunhofer IAF, Freiburg,
Germany, 4Freiburg
Institute of Advanced Studies (FRIAS),
University of Freiburg, Freiburg, Germany
This work is on the implementation of
miniaturized two-stage preamplifiers for 9.4
T (400 MHz), intended to be used for each
coil, respectively, in multi-parallel
receive array coils. Amplifier performance
has been tested successfully with signals of
up to eight coils of a receive array with
eight preamplifiers in parallel. Amplifier
performance could be verified for magnetic
fields up to 9.4 T.
|
1863. |
Scalability
and channel independency of the digital
broadband dStream architecture
Cecilia Possanzini1, Phil van
Liere1, Hans Roeven1,
Jan den Boef1, Charlie Saylor2,
Jan van Eggermond1, Paul Harvey1,
and Elisabeth Moore1
1Philips Healthcare, Best,
Netherlands, 2Invivo
Corp., Gainsville, Florida, United States
This work describes a scalable digital
broadband receive system architecture which
no longer limits the number of receive
channels that can be connected and provides
a consistent signal fidelity independent of
the number of channels. In this study, we
show that in this architecture increasing
the ‘channel count’ of the system is simply
achieved by placing additional coils on the
patient support, without modifying anything
on installed receive chain of the system as
for traditional analog architecture.
|
1864. |
Comparison of
Three Preamplifier Technologies: Variation of
Input Impedance and Noise Figure With B0 Field
Strength
Russell Lagore1, Brodi Roberts1,
B. Gino Fallone1,2, and Nicola De
Zanche1,2
1Dept. of Oncology, University of
Alberta, Edmonton, Alberta, Canada, 2Dept.
of Medical Physics, Cross Cancer Institute,
Edmonton, Alberta, Canada
Three preamplifier technologies are compared
at various B0 field
strengths, highlighting sensitivity to
changes in noise figure and input impedance.
|
1865. |
Optical
Transmission System for High Field Systems
Taner Demir1, Lance DeLaBarre2,
Burak Akin1, Gregor Adriany2,
Kamil Ugurbil2, and Ergin Atalar1
1National Magnetic Resonance
Research Center (UMRAM), Bilkent University,
Ankara, Ankara, Turkey, 2Center
for Magnetic Resonance Research, University
of Minnesota, Minneapolis, Minnesota, United
States
In this work, we introduce an optical
transmission system for a 3T and a 7T
system. The transmission system reduces the
interconnection problems between large
number of coil elements and the scanner and
possibly enhances RF safety. The system
transmits the analog MRI and detuning
signals optically. In order to demonstrate
the performance of the system, phantom and
human experiments are performed.
|
1866. |
Reducing
Element Coupling in Array Coils Using Off-Tuned
Elements
Boris Keil1, Veneta Tountcheva1,
Christina Triantafyllou1,2, and
Lawrence L Wald1,3
1A. A. Martinos Center for
Biomedical Imaging, Department of Radiology,
Massachusetts General Hospital, Harvard
Medical School, Charlestown, MA, United
States, 2McGovern
Institute for Brain Research, MIT,
Cambridge, MA, United States, 3Harvard-MIT
Division of Health Sciences and Technology,
Cambridge, MA, United States
An intentionally mistuned approach was
tested as a simple additional decoupling
method for array coils. To address this
issue, we exploit a phenomena associated
with preamplifier decoupling, which allows
array coil element to be tuned off-resonance
from the Larmor frequency without
significant degradation of SNR. This
approach can potentially facilitate
decoupling in arrays with high element
coupling, especially in flexible arrays
where geometric decoupling from overlap or
shared impedances is not feasible for all
positions of the flexing former.
|
1867. |
A 32-Channel
Parallel Exciter/Amplifier Transmit System for
7T Imaging
Lou Poulo1, Robert Haefner1,
Bernd Stoeckel2, Cem Murat Deniz3,
Leeor Alon3, Daniel K Sodickson3,
and Yudong Zhu3
1Analogic Corporation, Peabody,
MA, United States, 2Siemens
Medical Solutions USA Inc, New York, NY,
United States, 3Center
for Biomedical Imaging, Department of
Radiology, NYU School of Medicine, New York,
NY, United States
The development and initial testing of a
complete 7T, 32-channel RF transmit system
is described. This RF subsystem, consisting
of a new RF sequencer/controller,
independent waveform generation, and power
amplifiers, is designed to be an add-on
expansion to an existing 7T imager. The new
RF capability will enable research into the
tradeoffs in the various questions/tradeoffs
relating to the number of available
channels. The system is modular in 8-channel
increments, and the architecture allows
relatively straightforward integration into
most scanners
|
1868. |
8-Channel
Parallel Transmit and Receive System for 3 Tesla
Wolfgang Loew1, Randy Giaquinto1,
Laura Sacolick2, William Allyn
Grissom2, and Mika Vogel2
1Cincinnati Children's Hospital
Medical Center, Cincinnati, Ohio, United
States, 2GE
Global Research Europe, Germany
To increase homogeneity of the transmit
field at 3 Tesla an 8-channel transceiver
system implementation is presented. Shorter
distance to the imaging object reduces the
amount of power needed for a desired B1 field
in the object. The system consists of an
8-channel head T/R-coil, 8 modified GE
T/R-switches, and 8 high power bias tees.
Imaging experiments were performed in-vivo
with this setup and B1 magnitude
and phase maps were acquired.
|
|
|
Traditional Posters
: Engineering
|
Click on
to view the
abstract pdf and click on
to view the pdf of the poster viewable in the poster hall.
|
Novel Coils & Arrays
Thursday May 12th
Exhibition Hall |
13:30 - 15:30 |
1869. |
A 7 T receive array for in
vitro studies of human brain tissue
Andreas Peter1, Matthias Kladeck2,
Oliver Speck2, and Jan G. Korvink1,3
1Department of Microsystems Engineering -
IMTEK, University of Freiburg, Freiburg, Germany, 2Biomedical
Magnetic Resonance, Otto-von-Guericke University,
Magdeburg, Germany, 3Freiburg
Institute of Advanced Studies (FRIAS), University of
Freiburg, Freiburg, Germany
We present a 19-channel, 2D coil array for large in
vitro studies of human brain tissue, such as whole brain
slices at 7 T. The sample is to be placed in a separate
container horizontally between two of these arrays. The
channels are amplified and decoupled from their
neighbours by home-made low impedance low noise
amplifiers. All adjacent elements show an isolation of >
26 dB, the circuit Q of an uloaded single element is on
average 100.
|
1870. |
A New Intravascular
Loopless Monopole Antenna (ILMA) for MR Imaging
Hong Yang Yuan1, Xing Lv1, Rui
Zhang1, Xue Dong Yang2, Xiao Ying
Wang2,3, Xiao Hai Ma4, Zhao Qi
Zhang4, Jue Zhang1,3, and Jing
Fang1,3
1College of Engineering, Peking University,
Beijing, China, People's Republic of, 2Dept.
of Radiology, Peking University First Hospital, Beijing,
China, People's Republic of, 3Academy
for Advanced Interdisciplinary Studies, Peking
University, Beijing, China, People's Republic of, 4Dept.
of Radiology, Beijing Anzhen Hospital, Beijing, China,
People's Republic of
Although intravascular MR probe has been proposed for
many years, the rigid and bulky guide-wire presents
major challenges when the intravascular detectors are
applied into small vessels. In this study, to overcome
these inherent limitations and improve the longitudinal
coverage, a novel long intravascular loopless monopole
antenna (ILMA) design with a thin non-shielded flexible
guide-wire is presented. In vitro and in vivo test were
carried out to assess the feasibility of the ILMA.
Results show that the proposed design has the advantage
of providing high SNR, high spatial resolution, and
greater longitudinal coverage in this preliminary study.
|
1871. |
HTS volume coil enhanced
SNR in Wideband mice whole body screening
In-Tsang Lin1,2, Edzer L. Wu2,3,
Hong -Chang Yang4, and Jyh-Horng Chen1,2
1Graduate Institute of Biomedical Electronics
and Bioinformatics, National Taiwan University, Taipei,
106, Taiwan, 2Interdisciplinary
MRI/MRS Lab, Department of Electrical Engineering,
National Taiwan Univeristy, Taipei, 106, Taiwan, 3Department
of Biomedical Engineering, National Taiwan University,
Taipei, 106, Taiwan, 4Department
of Physics, National Taiwan University, Taipei 106,
Taiwan
With a nearly 2-fold SNR increase using the world¡¯s
first high temperature superconducting (HTS) animal
volume coil, the W=3 accelerated Wideband
high-resolution mice whole body scan serves as an
example of good balance between image quality and
temporal/spatial resolution. The experiment was
conducted with copper and Bi2Sr2Ca2Cu3Ox (Bi-2223)
volume coils to show the difference.
|
1872. |
High-Temperature
Superconducting RF surface coil Platform for In-vivo brain
structural differences
In-Tsang Lin1,2, Bing-Hsuan Lei2,3,
Hong -Chang Yang4, and Jyh-Horng Chen1,2
1Graduate Institute of Biomedical Electronics
and Bioinformatics, National Taiwan University, Taipei,
106, Taiwan, 2Interdisciplinary
MRI/MRS Lab, Department of Electrical Engineering,
National Taiwan University, Taipei, 106, Taiwan, 3Department
of Electrical Engineering, National Taiwan University,
Taipei, 106, Taiwan, Taipei, 106, Taiwan, 4Department
of Physics, National Taiwan University, Taipei 106,
Taiwan
MRI provides useful method for revealing brain
structure. Neuroanatomical differences between strains
have been studied at the histologic level. However, the
scanning time in 3 T MRI needs more than one hour to
obtain the enough resolution to reveal neuroanatomical
differences between strains. High-temperature
superconducting (HTS) radio-frequency (RF) coil has been
proposed as a promising tool in the investigation of the
tissue microscopy with high resolution due to its
low-resistance characteristic for the MR probe design.
Our method to reduce the scanning time is using a 40 mm
in diameter Bi2Sr2Ca2Cu3Ox (Bi-2223) HTS RF surface
coil. In the present study, we succeed to apply HTS RF
surface coil to evaluate the brain structural
differences between C57BL/6J and 129S1/SvImJ mouse.
|
1873. |
A 13 channel 3 Tesla
Shoulder Coil on a Domed Conformable Former
Graham Charles Wiggins1, Bei Zhang1,
Christian Glaser1, Bernd Stoeckel2,
Michael P Recht1, and Daniel Sodickson1
1Radiology, NYU Medical Center, New York, NY,
United States, 2Siemens
Medical Solutions, New York, NY, United States
Musculoskeletal imaging depends on anatomically-specific
RF coils, which provide better performance than general
purpose body arrays. The shoulder is poorly served by
commonly available commercial coil designs, which
typically consist of a rigid concave former that does
not wrap substantially around the shoulder joint. We
present a 13 element shoulder array on a flexible domed
former which wraps around the shoulder and conforms to a
variety of body types. We demonstrate SNR gains 2-fold
or better in deep tissue such as the labrum and
capsular-ligamentous structures. This has the potential
to impact the clinical MRI-based assessment of shoulder
instability.
|
1874. |
MULTILAYER MICRO COIL
PHASED ARRAY FOR MRI
Oliver Georg Gruschke1, Lars Clad1,
Vlad Badilita1, Kai Kratt1,
Mohammad Mohammadzadeh2, Nicoleta Baxan2,
Dominik von Elverfeld2, Andreas Peter1,
Jürgen Hennig2, Ulrike Wallrabe1,
and Jan G. Korvink1,3
1Microsystems Engineering – IMTEK, University
of Freiburg, Freiburg, Germany, 2Dept.
of Radiology Medical Physics, University Medical Center,
Freiburg, Germany, 3Freiburg
Institute of Advanced Studies (FRIAS), University of
Freiburg, Freiburg, Germany
Receive-only micro phased coil array for cell and thin
film materials research.
|
1875. |
A Printed Loop Element
with Integrated Capacitors and Co-Planar Shield for 7 Tesla
Mary Preston McDougall1,2, Steven M Wright1,2,
Joseph Rispoli1, Mario Carillo2,
Ivan Dimitrov3, Sergey Cheshkov3,
and Craig Malloy3
1Biomedical Engineering, Texas A&M
University, College Station, TX, United States, 2Electrical
Engineering, Texas A&M University, College Station, TX,
United States, 3University
of Texas Southwestern Medical Center, Dallas, TX, United
States
Shields for RF surface coils have been investigated
since the earliest days of MRI. Some authors have stated
that RF shields are essential for 7T surface coils over
10 cm in diameter, and others have successfully built
smaller loops as array elements without using shields,
consistent with this guideline. This abstract examines
the effectiveness of a co-planar shield at 7T. The
co-planar configuration, combined with coils using the
capacitance of dual-sided PC boards to replace
segmenting capacitors, enables simple, printed coils.
This may be useful in constructing array coils,
particularly when compared to coils with full
ground-plane shields.
|
1876. |
High Performance
Nanomaterial Coil for Carotid Imaging
Raju Viswanathan1, Bradley Goldstein2,
Gabor Mizsei3, and Sushmitha Rajakutty2
1Tursiop Technologies, LLC, Cleveland, OH,
United States, 2Tursiop
Technologies, LLC, 3Tursiopp
Technologies, LLC
A high performance RF coil based on a structured
nanomaterial is described for high field imaging in a
carotid application.
|
1877. |
Design and
Characterization of A Set Of MRI Histology RF Coils
Dedicated to Standardized Slide Sections
Dung Minh Hoang1, Chao Zhang1,
Mesha Shamsie1, Latifa Fakri-Bouchet2,
and Youssef Zaim Wadghiri1
1Radiology, NYU School of Medicine, New York,
NY, United States, 2CREATIS,
Lyon 1 University - Claude Bernard, Lyon, France
A set of three histological coils were designed and
tested to accommodate standard off-the-shelf cover-slips
commonly used for tissue examination under a microscope
with sizes enabling the imaging of any mouse organ. The
gain in sensitivity was achieved through the
optimization of the filling factor by tightly fitting
the cover-slip while maintaining a homogeneous rf B1
field coverage within the FOV of the tissue section of
interest. Several mouse organs were examined spanning
from the olfactory bulb to the liver, one of the largest
organ while testing the sensitivity limits achievable at
7-Tesla. Our results show that sensitivy achieved can
enable MRI section as low as 10-um thickness when
immersed in 5mM doped buffer acquired during eight
hours.
|
1878. |
Counter Rotating Currents
Cryogenic Surface Coils
Jarek Wosik1,2, Andrzej Jesmanowicz3,
Lian Xue4, Leiming Xie1, and Flora
Suk-Yin Ip1
1Electrical and Computer Engineering,
University of Houston, Houston, Texas, United States, 2Texas
Center for Superconductivity, Houston, TX, United
States, 3Biophysics,
Medical College of Wisconsin, Milwaukee, WI, United
States, 4Time
Medical, Metuchen, NJ, United States
In this work we have developed a simple method of
estimation of a potential SNR gain, which can be
obtained for a given coil and body configuration. Four
and six laboratory bench Qs measurements had to be
carried out to allow for SNR gain calculations of 77 K
Cu and Cu/HTS coils, respectively. It was tested on a 3
T whole-body GE scanner using planar
counter-rotating-currents (CRC) and twin-horseshoe (HS)
coils (receive only) integrated with a G-10 liquid
nitrogen cryostat. Cryogenic performance comparison of
the CRC and HS coils were carried out using a 3.0 T GE
whole-body scanner.
|
1879. |
Remote detection by MRI at
3T using a waveguide
Fabian Vazquez1, Rodrigo Martin1,
Sergio E Solis2, and Alfredo O Rodriguez1
1UAM Iztapalapa, DF, Mexico, Mexico, 2Laboratorio
de Neurofisiologia Integrativa, Instituto Nacional de
Psiquiatria Ramon de la Fuente, DF, Mexico, Mexico
The generation of magnetic resonance images with
waveguides has been successfully demonstrated at 7 Tesla
for whole-body systems. We have previously shown that
the waveguide approach can also be used with magnetic
field intensities lower than 7T and whole-body systems
using a parallel-plate waveguide. The aim of this paper
is to investigate the variation of the image intensity
as a function of the separation between a coil and a
phantom using a parallel-plate waveguide for MRI at 3T.
In this work, a waveguide composed of only tow parallel
plates was used and phantom images were acquired at
different separations.
|
1880. |
Simple quadrature volume
antenna transformed from loop
Hideta Habara1, Yoshitaka Bito1,
Hisaaki Ochi1, Yoshihisa Soutome1,
Yukio Kaneko1, Masayoshi Dohata1,2,
Hiroyuki Takeuchi2, and Tetsuhiko Takahashi2
1Central Research Lab., Hitachi Ltd.,
Kokubunji, Tokyo, Japan, 2Hitachi
Medical Corporation, Kashiwa, Chiba, Japan
Quadrature-driven cylindrical volume antennas, such as
birdcage or TEM antennas, are indispensable hardware for
commercial MRI scanners. However, they consist of many
parts, making them complex to build. We introduce a
simple quadrature volume antenna having only five parts
by transforming a one-loop antenna. If a loop on a
cylindrical surface is folded 2N times and the number of
current nodes in the loop is 2(N-1), a uniform B1+ field
is created in the center of the cylinder. A prototype of
a 3T head antenna was made, and a phantom image was
obtained.
|
1881. |
A method for increasing
electrical length of microstrip waveguides
Rock Hadley1, Dennis Parker1, and
Glen Morrell1
1Radiology - UCAIR, University of Utah, Salt
Lake City, Utah, United States
A method for increasing the electrical length of
non-resonant microstrip waveguides is presented. This
method uses lumped element distributed capacitance
evenly distributed along the length of a microstrip
transmission line to effectively increase the phase
shift down the length of the line. This work presents an
analysis of the field properties of a single microstrip
line that uses this technique to increase the electrical
length of the line. This work is a step towards the
development of linear phase volume coils that could be
used at 3T frequencies.
|
|
|
Traditional Posters
: Engineering
|
Click on
to view the
abstract pdf and click on
to view the pdf of the poster viewable in the poster hall.
|
Array Coil Applications
Monday May 9th
Exhibition Hall |
14:00 - 16:00 |
1882. |
Study on a 3T Head
Coil: Channel Reduction from 32 to 24
Bing Wu1, Haidong Peng1, Dan
Xu1, and Liang Xuan1
1GE Healthcare, Waukesha, WI, United
States
Through the study on a commercial 32ch coil, we find
that the channel number can be reduced from 32 to 24
without degrading its SNR and parallel imaging
performance. Reduced losses from coil components,
reduced cost and increased stability are then
expected.
|
1883. |
Simulating Array SNR
and effective Noise Figure in dependance of Noise
Coupling
Christian Findeklee1, Randy Duensing2,
and Arne Reykowski2
1Philips Research Laboratories, Hamburg,
Hamburg, Germany, 2Invivo,
United States
The effect of element coupling in receive arrays has
been investigated for a long time. With new insights
into noise coupling and array noise matching, we now
can quantify this SNR reduction. Optimized matching
is able to avoid SNR reduction for a target
location; however, it may still yield significant
SNR-loss in other areas. In our experiments, we
demonstrate how inductive decoupling can increase
the area of high SNR.
|
1884. |
4D flow-sensitive MRI
of the thoracic aorta using 12- and 32-channel coils
Aurelien F Stalder1, Zhi Yuan Dong1,
Yang Qi1, Jelena Bock2, Jürgen
Hennig2, Michael Markl2, and
Kun Cheng Li1
1Dept. of Radiology, Xuanwu Hospital of
Capital Medical University, Beijing, China, People's
Republic of, 2Dept.
of Radiology - Medical Physics, University Hospital
Freiburg, Germany
4D flow-sensitive MRI was performed in the thoracic
aorta of 11 healthy volunteers at 3T using 12- and
32-channel coils and parallel imaging (GRAPPA) with
accelerations R=2 and R=3. SNR, velocity divergence
and streamlines length quantification as well as
semi-quantitative image grading was performed to
assess data quality. R=3 allowed to save 19.5±5%
measurement time compared to R=2 (14.2±2.4 min). 12
channels with R=2 and 32 channels with R=3 produced
data with significantly higher quality compared to
12 channels and R=3. There was no significant
difference between 12 channels with R=2 and 32
channels with R=3 but for the depiction of
supra-aortic branches where the 32-channel coil was
superior.
|
1885. |
Development of a
Receiver Coil Array for 2D Accelerated Imaging of the
Complete Neurovascular System
Petrice Marie Mostardi1, Eric G Stinson1,
Thomas C Hulshizer1, Phillip J Rossman1,
and Stephen J Riederer1
1MR Research Laboratory, Mayo Clinic,
Rochester, MN, United States
Currently there is no coil that allows for 2D
acceleration over the entire head and neck. The
purpose of this work was to develop a multi-element
receiver coil array that has high SNR and the
capability for high (R =4-8) 2D SENSE acceleration
from the head through the upper torso. The coil
design consists of a newly developed neck/torso
array which is used in combination with the clinical
8HRBRAIN coil. The neck/torso array was designed as
an eight element linear array wrapped around the
neck with three circular elements on each side of
the neck and two longer rectangular elements on the
anterior neck and chester. In phantom and in vivo
studies this coil shows higher SNR and lower g
factors than clinically available coils throughout
the desired FOV.
|
1886. |
The potentialities of
implantable micro-coil for detection of brain’s proton
metabolites by NMR micro-spectroscopy
Aziz Kadjo1, Ludovic Martin-Durupty1,
Raymond Cespuglio2, Danielle
Graveron-Demilly1, and Latifa
Fakri-Bouchet1
1University of Lyon, Lyon1,Laboratoire
CREATIS-LRMN, UMR CNRS 5220, INSERM U 630, INSA de
Lyon, Villerbanne, France, 2University
of Lyon, Lyon1, Laboratoire «Radicaux
libres/substrats énergie et physiopatho cérébrale,
Lyon cedex 08, France
Considering the need to explore a limited sample
volume (microlitre), the feasibility to use a new
micro-coil concept is proposed. Simulations of B1
field distribution correlated to MR imaging,
demonstrates the potential of micro-coil in terms of
sensitivity, (Vactive~2 µl), SNR and limits of
detection (LOD). Estimated LOD from MR-observable
brain metabolite spectra are compared to those
obtained using a commercial surface-coil. A gain
factor about 2 is obtained. The micro-coil
advantage, in spite of its small sensitive volume,
to detect a small concentration is demonstrated.
This result opens the way to new spatially resolved
explorations on animal model.
|
1887. |
Experimental
Verification of SNR and Parallel Imaging Improvements
Using Complete Coil Arrays
Adam Maunder1, Tyler Charlton1,
B. Gino Fallone1,2, and Nicola De Zanche1,2
1Dept. of Oncology, University of
Alberta, Edmonton, Alberta, Canada, 2Dept.
of Medical Physics, Cross Cancer Institute,
Edmonton, Alberta, Canada
Complete arrays capture all three components of the
RF magnetic field using additional loops placed
orthogonally to the standard surface coils. This
experimental study at 3T confirms improvements in
SNR and parallel imaging performance predicted by
theory, and demonstrates an effective method to
increase channel density three-fold without
decreasing coil size.
|
1888. |
Comprehensive
Neurovascular Evaluation Using an Automatic Optimal SNR-based
Channel Combination from a 62 Element Coil Array at 3T
Amol Pednekar1, Claudio Arena2,
Greg Wilson3, Cecilia Possanzini4,
Charles Saylor2, and Raja Muthupillai2
1Philips Healthcare, Houston, Texas,
United States, 2Diagnostic
and Interventional Radiology, St. Luke's Episcopal
Hospital, Houston, Texas, United States, 3Philips
Healthcare, Cleveland, United States, 4Philips
Healthcare, Best, Netherlands
The study summarises the experience with a 62
element neurovascular array. (a) It is feasible to
obtain a high resolution 3D-ToF images of the entire
neuro-vascular tree from the aortic arch to the
intra-cranial vessels ( < 8 min), as well as
targeted high-resolution carotid vessel wall imaging
( < 7 min) using a 62 element coil array without
operator intervention; (b) Automated selection of
coil elements using SNR contribution to the region
of interest performed just as well as manual
selection of dedicated coil elements.
|
|
|
Traditional Posters
: Engineering
|
Click on
to view the
abstract pdf and click on
to view the pdf of the poster viewable in the poster hall.
|
Non-Proton Coils & Hardware
Tuesday May 10th
Exhibition Hall |
13:30 - 15:30 |
1889. |
Proton traps for
multi-nuclear RF coils: design analysis and practical
implementation for 13C MRS in humans at 7T
Martin Meyerspeer1,2, Rolf Gruetter1,3,
and Arthur W Magill1,4
1LIFMET, Ecole Polytechnique Fédérale de
Lausanne, Lausanne, Switzerland, 2MR
Centre of Excellence and ZMPBMT, Medical University
of Vienna, Vienna, Austria, 3Radiology,
University of Geneva and Lausanne, Switzerland,
Switzerland, 4Radiology,
University of Lausanne, Lausanne, Switzerland
Trapped coil designs allow the operation of
lower-frequency coils in the presence of a proton
coil. Adding a second capacitor to a trap in the
non-proton RF coil allows control over the trap
reactance at the low and high frequency (here 13C
and 1H) and the frequency of the trap mode. We
demonstrate the interdependence of the parameters
controlled and show analytical and numerical
solutions to fulfill the design constraints. Our
experiments show that, using the simulations, it
possible to construct an effective second order trap
for 13C at 7T.
|
1890. |
RF Field Optimization
of 4T Double-Tuned Surface TEM Resonators for 1H/23Na
MRI
Assunta Vitacolonna1, Sandro Romanzetti2,
Joerg Felder2, Nadim Jon Shah2,3,
Antonello Sotgiu4, and Marcello Alecci1
1Scienze della Salute, University of
L'Aquila, L'Aquila, Italy, 2Inst.
of Neuroscience and Medicine, Research Centre,
Jülich, Germany, 3Faculty
of Medicine, Department of Neurology, RWTH Aachen
University, Aachen, Germany, 4ITA
srl, L'Aquila, Italy
Sodium MRI/MRS benefits of improved SNR obtainable
at high fields (3-12 T). Surface TEM resonators are
especially designed for high-field applications. In
recent works a novel double-tuned (DT) surface TEM
resonator, made by three microstrip elements and
suitable for sodium and proton MRI at 4T was
described. Here, we report workbench and 4T MRI data
showing the optimization of the RF field
distribution of the 23Na channel by a proper
selection of the relative distance between the
external microstrips, while maintaining the 1H field
distribution.
|
1891. |
In Vivo Quantification
of Renal Sodium Concentration with a Dual RF Resonator
System
Raffi Kalayciyan1, Friedrich Wetterling1,
Sabine Neudecker2, and Lothar R. Schad1
1Computer Assisted Clinical Medicine,
Heidelberg University, Mannheim, Germany, 2Medical
Research Center, Heidelberg University, Mannheim,
Germany
The quantification of local Tissue Sodium
Concentration (TSC) can serve as a diagnostic
measure for renal diseases, because TSC is strongly
linked to the corticomedullary function regulating
the vascular ion concentrations. In this work, for
the TSC quantification the required homogeneous B1
is achieved by a dual RF resonator system composed
of a newly-developed low noise preamplifier
receive-only coil without the need to tune and
match, that was used in conjunction with a
commercial transmit birdcage volume resonator. The
TSC quantification in the rat kidney was illustrated
through TSC maps using 3D-UTE sequence.
|
1892. |
Double tunable TxRx 1H/ 19F
Helmholtz pair for MR imaging and spectroscopy at 11.7T
Mark Jacobus van Uden1, Yi Sun1,
and Arend Heerschap1
1Department of Radiology (667), Radboud
University Nijmegen Medical Centre, Nijmegen,
Netherlands
Within tissue engineering the restore, replacement
or regeneration of defective tissues and their
function by biological substitutes is monitored. To
monitor this process contrast agents that contain
fluorine atoms are used. Defects that are inflicted
on a rat hind leg are imaged on 1H and 19F. An
overlay of these image provides a good insight in
the healing process. We present a Helmholtz pair
that has a good coverage and good SNR to image rat
hind leg. The Helmholtz pair is combined using a
Wilkinson lumped element divider/ splitter.
|
1893. |
Zig-zag 13C
surface coil at 7T for high-sensitivity subcutaneous
lipid MRS
Ivan Emilov Dimitrov1,2, Craig R Malloy3,4,
and Andrew G Webb5
1Philips Medical Systems, Cleveland, OH,
United States, 2Advanced
Imaging Reseach Center (AIRC), UT Southwestern,
Dallas, TX, United States, 3Advanced
Imaging Research Center (AIRC), UT Southwestern,
Dallas, TX, United States, 4VA
North Texas Health Care System, Dallas, TX, United
States, 5Radiology,
Leiden University Medical Center, Leiden,
Netherlands
The metabolic implications of lipid accumulation may
depend on the composition of the fat itself.
Analytical high-resolution studies of 13C
have shown the ability of MRS to distinguish a
variety of fat components. Here we report on a
high-sensitivity 13C
surface coil with tailored penetration designed to
specifically obtain high-resolution human in
vivo carbon
spectra of subcutaneous fat at 7T. The coil uses a
zig-zag pattern with 5 mm distance between the
opposing-current segments and shows the desired
penetration depth of a few millimeters. In
vivo coupled
spectra show high sensitivity, and good decoupling
is observed in phantoms.
|
1894. |
Dual-Tuned 1H/13C
Orthogonal Double Solenoid Volume Coil for Simultaneous
Acquisition in Small Animals in Vivo
Laura Claire Bell1, Eric T Peterson1,
Jeremy W Gordon1, Sean B Fain1,
and Krishna N Kurpad1
1Medical Physics, University of
Wisconsin-Madison, Madison, Wisconsin, United States
Development of radio frequency dual-tuned coils is
important for spectral shimming and correct
functional/anatomical registration. We present a
dual-tuned 1H/13C Orthogonal Double Solenoid (ODS)
volume coil for pre-clinical applications. This
design can be placed coaxially within the bore of
horizontal small animal scanner, upholds the 1H SNR
at high fields and the sensitivity of 13C, and its
versatile design has the potential to image other
nuclides of choice. Preliminary results from
simultaneous acquisition of a rat in vivo
demonstrate feasibility of the coil design.
|
1895. |
A 1H-31P Array Coil
for Human Brain Spectroscopy at 3 T
Wolfgang Driesel1, Andre Pampel1,
Christian Labadie2, Toralf Mildner3,
and Harald E. Möller4
1Max Planck Institute for Human Cognitive
and Brain Sciences, Leipzig, Saxony, Germany, 2Max
Planck Institute for Human Cognitive and Brain
Sciences, 3Max
Planck Institute for Human Cognitive and Brain
Sciences, Germany, 4Max
Planck Institute for Human Cognitive and Brain
Sciences, Leipzig, Germany
In this work, the concept of a stacked combination
of loop coils and microstrip transmission-line (MTL)
elements was adopted to build a helmet-shaped,
dual-tuned array coil for human brain 31P
spectroscopy and 1H decoupling and imaging at 3 T.
The 1H channel is based on a pure MTL design with
four spokes. On each spoke, a loop coil was added to
permit 31P transmission/reception (Tx/Rx). Initial
results from investigations of the performance for
31P MRSI including phantom studies are presented.
|
1896. |
A 7T Halo Loop
Resonator for Registration of 31P MRSI
Thomas Michael Barbara1, Manoj Sammi1,
John Grinstead2, and William D Rooney1
1AIRC, Oregon Health and Sciences
University, Portland, Oregon, United States, 2Siemens
Healthcare, Portland, Oregon
An axially oriented loop resonator is used to obtain 1H
co-registration images for 31P
spectroscopic imaging at 7T using a 12 leg 31P
birdcage coil. The 8 cm diameter loop provides
extended coverage from crown to brain stem with low
coupling to the 31P
volume coil. This approach provides a useful
alternative to the careful subject positioning
required with two coils or the construction of a
double tuned resonator.
|
1897. |
One coil to light them
all: Broadband body coil for multi-frequency imaging
using a coaxial waveguide
Stefan Alt1, Marco Müller1,
Armin Michael Nagel1, Florian Meise1,
Reiner Umathum1, and Michael Bock1
1Medical Physics in Radiology, German
Cancer Research Center (DKFZ), Heidelberg, Germany
The native wave propagation mode of a coaxial
waveguide (TEM) has no cut-off frequency, which
offers the opportunity of broadband operation for
mulit-nuclei studies. We acquired proton (1H)
and sodium (23Na) images at four
different Larmor frequencies from 63 to 297MHz using
the same coaxial waveguide setup for both spin
excitation and signal reception.
|
1898. |
Developement of
multi-tranceiver dual-tuned knee coil at 3T
Junghwan Kim1, Chanhong Moon1,
Bumwoo Park1, Alessandro Furlan1,
Anthony Defranco2, Tiejun Zhao3,
and Kyongtae Ty Bae1
1Department of Radiology, University of
Pittsburgh, Pittsburgh, PA, United States, 2MR
research center, University of Pittsburgh,
Pittsburgh, PA, United States, 3MR
Research Support, Siemens Healthcare, Pittsburgh,
PA, United States
We have developed a multi-transceiver dual-tuned
knee coil at 3T which provides high SNR and imaging
depth for sodium and co-register of both proton and
sodium imaging in a single session. The coil allowed
us to acquire in vivo knee cartilage with high SNR
in a clinically acceptable time (~30 minutes total
session). Further studies on B1-phase shimming are
essential to produce a homogenous B1 field and to
test the accuracy and reliability of sodium
concentration measurement in knee cartilage.
|
1899. |
A 1H-31P Array Coil
for Human Brain Spectroscopy at 3T
Wolfgang Driesel1, André Pampel1,
Christian Labadie1, Toralf Mildner1,
Harald E Moeller1, and Harald E Moeller1
1Max Planck Institute for Human Cognitive
and Brain Sciences, Leipzig, Germany
Previously, a modular approach has been suggested
for designing large arrays. It is based on a stacked
combination of loop coils and microstrip
transmission-line (MTL) elements, which are
intrinsically orthogonal. In this work, this concept
was adopted to build a helmet-shaped, dual-tuned
array coil for human brain 31P spectroscopy and 1H
decoupling and imaging at 3 T. The 1H channel is
based on a pure MTL design with four spokes. On each
spoke, a loop coil was added to permit 31P
transmission/reception (Tx/Rx). Initial results from
investigations of the performance for 31P MRSI
including phantom studies are presented.
|
1900. |
A 7-Tesla Transmit
with 15-Channel Receive-Only Array Knee Coil for Sodium
Imaging
Matthew Finnerty1, Xiaoyu Yang1,
Tsinghua Zheng1, Jeremiah Heilman1,
Nicholas Castrilla1, Joseph Herczak1,
Hiroyuki Fujita1,2, Graham C Wiggins3,
Ryan Brown3, Guillaume Madelin3,
Gregory Chang3, Ravinder R Regatte3,
Michael Recht3, Siegfried Trattnig4,
Vladimir Juras4, Wolfgang Renz5,
Franz Schmitt5, Bernd Stoeckel6,
Andreas Potthast5, and Karsten Wicklow5
1Quality Electrodynamics, Mayfield
Village, Ohio, United States, 2Departments
of Physics and Radiology, Case Western Reserve
University, Cleveland, Ohio, United States, 3Department
of Radiology, NYU Langone Medical Center, New York,
New York, United States, 4Department
of Radiology, Medical University of Vienna, Vienna,
Austria, 5Siemens
Healthcare, Erlangen, Germany,6Siemens
Medical Solutions USA, Inc., Malvern, Pennsylvania,
United States
The higher SNR found at 7T allows for more
diagnostic applications for nuclei other than
hydrogen. In particular, sodium imaging has been
found to be useful in characterizing cartilage
degeneration in the joints, with the focus primarily
on the knee. In an effort to design RF coil hardware
optimized for these x-nuclei applications, a 12-rung
birdcage transmitter and 15-channel receive-only
array coil has been developed for sodium imaging of
the knee.
|
1901. |
1H/ 19F
large coverage homogeneous transmit coil with dedicated
multi-element receive coils.
Mark Jacobus van Uden1, Fernando Bonetto1,2,
E.G.W. ter Voert1, Stephan Orzada3,
IJM de Vries2, Hanneke van Laarhoven4,
and Arend Heerschap1
1Department of Radiology (667), Radboud
University Nijmegen Medical Centre, Nijmegen,
Netherlands, 2Department
of Tumor Immunology, Radboud University Nijmegen
Medical Centre, Nijmegen, Netherlands, 3Erwin
L. Hahn Institute for Magnetic Resonance Imaging,
Essen, Germany, 4Department
of Medical Oncology, Radboud University Nijmegen
Medical Centre, Nijmegen, Netherlands
Homogeneous excitation and reception provides a much
better base for in vivo absolute quantification of
cells and drugs levels with respect to inhomogeneous
signal distribution. In this work we present a
Helmholtz pair that is capable of generating a
homogeneous transmit field at both 1H and 19F at 3T.
To obtain signals with high SNR and optimal coverage
over the liver and lymph nodes two dedicated
multiple element receive coils were developed.
|
|
|
Traditional Posters
: Engineering
|
Click on
to view the
abstract pdf and click on
to view the pdf of the poster viewable in the poster hall.
|
Traveling Waves in MRI
Wednesday May 11th
Exhibition Hall |
13:30 - 15:30 |
1902. |
Safety evaluation of a
multiple-channel travelling-wave system at 7T
Jan Paska1, David O Brunner2,
Juerg Froehlich1, and Klaas P Pruessmann2
1Laboratory for Electromagnetic Fields and
Microwave Electronics, ETH Zurich, Zurich, Zurich,
Switzerland, 2Institute
for Biomedical Engineering, University and ETH Zurich,
Zurich, Switzerland
The travelling wave concept was recently extended to
multiple channels showing promising results in phantoms.
For in vivo imaging a reliable SAR evaluation is
necessary considering all uncertainties particular to
this RF system. Methods were developed to calculate an
input power limit, such that the local SAR limits are
not exceeded, in any case of operation and within the
uncertainties given.
|
1903. |
Traveling Wave Mode
Transformation in a Waveguide with High Dielectric Medium
for Ultra High Field MRI
Alexey Tonyushkin1,2, and Andrew J. M.
Kiruluta1,2
1Radiology, Massachusetts General Hospital,
Harvard Medical School, Boston, MA, United States, 2Physics
Dept., Harvard University, Cambridge, MA, United States
Existing ultra-high field MR scanners allow propagation
of TE and TM modes in high permittivity dielectrics, but
the actual B1 field inside the dielectric can be hard to
predict. Here, we present the analysis of B1-field map
of traveling waves inside a cylindrical waveguide with a
dielectric insert and explain features of B1 field by
mode transformation to higher order ones. In practice,
the modes diversity depends on the tissue efficient
diameter, relative permittivity, conductivity, and the
Larmor frequency. A more complicated case of
heterogeneous axial symmetric dielectric can be also
analyzed using effective permittivity and mode
transformation approach.
|
1904. |
MR experiment validation
of parallel traveling-wave with quadrature patch antenna
transceiver array
Yong Pang1, Daniel Vigneron1,2,
and Xiaoliang Zhang1,2
1Radiology & Biomedical Imaging, University
of California San Francisco, San Francisco, CA, United
States, 2UCSF/UC
Berkeley Joint Graduate Group in Bioengineering, San
Francisco & Berkeley, CA, United States
Recently, studies on parallel accelerated imaging with
traveling-wave have been reported. In this work, the
method of implementing parallel traveling-wave using
single-feed quadrature patch antenna transceiver array
was investigated and validated using MR experiments on a
7T whole body MR scanner. A two-element patch antenna
array was built, and a human head phantom was positioned
85 cm away from the patch antenna array in experiment.
Excellent parallel imaging performance in both axial and
sagittal planes at acceleration factor of 2 was
demonstrated with both SENSE and GRAPPA accelerated
imaging.
|
1905. |
Multi-Pass Travelling Wave
Volume Coil
Reiner Umathum1, and Michael Bock1
1German Cancer Research Center, Heidelberg,
B.W., Germany
Despite the existence of the TEM resonator and some
travelling wave excitation methods most 7T body imaging
is performed with local TX/RX arrays. A novel volume
coil concept for high and ultra high field MRI body
systems is presented with simulation results which does
not utilize a resonating structure but excites a large
volume with a multi-pass travelling wave in a very
simple way.
|
1906. |
Travelling wave coil with
limited SAR
Marco Mueller1, Stefan Alt1,
Reiner Umathum1, Wolfhard Semmler1,
and Michael Bock1
1Medical Physics in Radiology, German Cancer
Research Center (DKFZ), Heidelberg, Germany
Travelling wave MRI exposes the human body to high
levels of SAR. Recently, a targeted travelling wave
approach using an interrupted coaxial wave¬guide was
presented. We present hardware measurements about the
opportunity of SAR restriction by using a travelling
wave coaxial coil with variable imagion regions. Signal
and flip angle distributions were calculated and
evaluated for different sizes of the variabel imaging
regions. The measurements show a good RF restriction to
the respective imaging region.
|
1907. |
Experimental Verification
of Numerical EM Field Simulations for Ultra-High Field
Travelling Wave MRI
Daniel Brenner1, Frank Geschewski1,
Joerg Felder1, Kaveh Vahedipour1,
and Nadim Jon Shah1,2
1Institute of Neurosciene and Medicine - 4,
Forschungszentrum Juelich, Juelich, Germany, 2Department
of Neurology, Faculty of Medicine, JARA, RWTH Aachen
University, Aachen, Germany
This work provides validation of Finite-Integral-Method
(FIM) electromagnetic field simulations of a patch
antenna for travelling wave excitation using
experimental data measured in a 9.4T human MRI scanner.
Quantification of the excitation field was performed
with the Actual Flip angle Imaging (AFI) sequence. Good
quantitative agreement is illustrated between simulation
and experimental data.
|
1908. |
Numerical study of the
waveguide magnetic field via the principal mode for MRI at 3
T
Fabian Vazquez1, Rodrigo Martin1,
David Flores1, Sergio Solis2, and
Alfredo O Rodriguez1
1UAM Iztapalapa, DF, Mexico, Mexico, 2Laboratorio
de Neurofisiologia Integrativa, Instituto Nacional de
Psiquiatria Ramon de la Fuente, DF, Mexico, Mexico
Waveguides have been successfully used to generate
magnetic resonance images at 7 Tesla for whole-body
systems. We have shown that the waveguide approach can
be used at 3T and whole-body systems. A parallel-plate
waveguide was used to numerically simulate the
fundamental mode (TM0) describing uniform magnetic
fields tangent to the copper plates. The TM0 mode can
propagate at any frequency and there are no variations
of the fields inside the waveguide. Numerical
simulations of the magnetic field generated by a
parallel plate waveguide were computed at 3T via the
propagation of the principal mode and results compared
with experimental data.
|
1909. |
new travelling wave coil
concepts
Marco Mueller1, Reiner Umathum1,
Stefan Alt1, Wolfhard Semmler1,
and Michael Bock1
1Medical Physics in Radiology, German Cancer
Research Center (DKFZ), Heidelberg, Germany
Travelling wave MRI can be used to attenuate the
standing wave prob¬lem of volume resonators at high
magnetic field strengths, We present two designs of
travelling wave stripline coils, which excite the RF
field in the imaging region. These travelling wave coils
limit the RF field to the region of interest, create a
good homogeneous B1+ field distribution and reduce the
global SAR. The coils can be realized as local TX/RX
coils and also as an overall body coil. B1+ and SAR
field distribution are shown and evaluated with a
phantom and an anatomical human model.
|
1910. |
Improvement of Travelling
Wave Excitation for Whole Body 7T MRI with an Extended
Gradient Coil RF-shield of 1.58 m Length
Tim Herrmann1, Johannes Mallow1,
Kyoung Nam Kim1, Johannes Bernarding1,
and Joerg Stadler2
1Department of Biometry and Medical
Informatics, OvG University Magdeburg, Magdeburg,
Saxony-Anhalt, Germany, 2Leibniz-Institute
for Neurobiology, Magdeburg, Saxony-Anhalt, Germany
Whole body MRI at 7T is still a big challenge on the
route to clinical use. This study shows how the
travelling wave concept can be optimized to work as an
efficient body-coil replacement. By simulating the
RF-system including the complete 7T whole body scanner
it was possible to consider all the important parameters
of the experiment. Directional characteristics, distance
to the object, and the excitation parameters of the
constructed patch antenna were optimized. Tx-only as
well as Tx-Rx scenarios were performed. Furthermore, a
comparison shows that the travelling wave (TW) concept
can keep up with conventional RF methods.
|
|