Electronic Posters
: Engineering
|
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Safety: Implants & Devices
Monday May 9th
Exhibition Hall |
14:00 - 16:00 |
Computer 66 |
14:00 |
3763. |
RF Safety
Assessment of a Generic Deep Brain Stimulator
during 1.5T MRI Exposure
Eugenia Cabot1, Tom Lloyd2,
Andreas Christ1, Gregg Stenzel2,
Wolfgang Kainz3, Steve Wedan2,
and Niels Kuster1,4
1IT'IS Foundation, Zurich,
Switzerland, 2Imricor
Medical Systems, United States, 3FDA,
Rockville, United States, 4Swiss
Federal Institute of Technology (ETHZ),
Zurich, Switzerland
A methodology for RF safety assessment of
implants based on a 4 tier approach was
evaluated for 1.5T scanners using a generic
model of a deep brain stimulator. A
combination of numerical (FDTD simulations)
and experimental techniques was used. The
different tiers were followed to assess the
energy deposition and the temperature
increase at the tip of the implant in a
human head model. Each consecutive tier
yields a less conservative result, but
requires greater computational effort to
demonstrate safety. Results showed that Tier
4 is technically feasible but too
computationally demanding. An enhanced Tier
3 is then suggested.
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14:30 |
3764. |
Radio-Frequency Heating at Deep Brain
Stimulation Lead Electrodes due to Imaging with
Head Coils in 3 T and 7T
Devashish Shrivastava1, Jingeng
Tian1, Aviva Abosch1,
and John T Vaughan1
1University of Minnesota,
Minneapolis, MN, United States
Radio-frequency (RF) heating was measured
using fluoroptic probes at the deep brain
stimulation (DBS) lead electrodes and 5 mm
away from the distal lead tip due to head
imaging with a transcieve head coil in 3
tesla (T) and 7T at the whole head average
SAR of 3 W/kg. The effect of the loop
orientation of the extra-cranial portion of
the lead on the RF heating was studied.
Clinically harmful RF heating may be
produced in both fields with head coils. The
RF heating was a function of the
extra-cranial lead placement and head coil.
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15:00 |
3765. |
Measurements
of RF Heating During 3.0T MRI of a Pig Implanted
with DBS
Krzysztof R Gorny1, Stephan J
Goerss2, Michael F Presti3,
Sun Chul Hwang4, Dong-Pyo Jang4,
Inyong Kim4, Kendall H Lee5,
and Matt A Bernstein1
1Radiology, Mayo Clinic,
Rochester, MN, United States, 2Neurosurgery,
Mayo Clinic, Rochester, MN, United States, 3Neurology,
Mayo Clinic, Rochester, MN, United States,4Neurologic
Surgery, Mayo Clinic, Rochester, MN, United
States, 5Neurologic
Surgery, Mayo Clinic, Rochester, MN
We use fluoroptic thermometry to measure
local heating near DBS electrodes implanted
in pig's brain during 3.0T MRI. For IR SPGR
and resting state fMRI sequences temperature
changes of less then 0.3° were observed.
These data could be valuable in assessment
of safety during 3.0T MRI of patients with
implanted DBS systems.
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15:30 |
3766. |
Fast
T1-Thermometry of the RF Induced Heating of
Conductive Wires
Daniel Gensler1, Florian Fidler1,
Marcus Warmuth2, Theresa Reiter2,
Peter Nordbeck2, Oliver Ritter2,
Mark E Ladd3, Harald H Quick4,
Peter M Jakob1, and Wolfgang R
Bauer2
1Forschungszentrum
Magnet-Resonanz-Bavaria e.V., Wuerzburg,
Bavaria, Germany, 2Medizinische
Klinik und Poliklinik I,
Universitätsklinikum Würzburg, Wuerzburg,
Bavaria, Germany, 3Erwin
L. Hahn Institut für Magnetresonanz,
Universität Duisburg-Essen, 4Institut
für Medizinische Physik,
Friedrich-Alexander-Universität
Erlangen-Nürnberg
The number of MRI examinations in patients
with medical implants is highly increasing,
raising several safety issues. Major
intention of the current work is to develop
a fast T1-based method, which allows
controlled heating of an implant while
simultaneously quantifying the spatial
temperature distribution during MRI. For
this purpose an inversion recovery sequence
was implemented where the heating is caused
by additional RF pulses. The presented
T1-based thermometry method allows spatial
and temporal quantification of dynamic
RF-induced heating near a conducting medical
implant. Hence it is possible to precisely
analyze the spatial temperature distribution
of an implant using a single measurement
even in inhomogeneous surroundings.
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Tuesday May 10th
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13:30 - 15:30 |
Computer 66 |
13:30 |
3767. |
An MR
Thermometry-GBHTM ‘Hybrid’ Model to Determine
Radiofrequency Heating near Implanted Leads in
High Field Imaging
Devashish Shrivastava1, Ute
Goerke1, Shalom Michaeli1,
Jingeng Tian1, Aviva Abosch1,
and John T Vaughan1
1University of Minnesota,
Minneapolis, MN, United States
A proton resonance frequency (PRF) shift
based MR thermometry method and the newly
developed generic bioheat transfer model
(GBHTM) were used together as an ‘hybrid’
model to determine radiofrequency (RF)
heating near a deep brain stimulation (DBS)
lead electrodes in 3T. The PRF shift method
was used to image temperatures outside the
susceptibility artifact region of the DBS
lead after an SAR intensive spin echo
sequence. The imaged temperatures were used
as inputs to the GBHTM to determine RF
heating in the artifact region near the
lead. The ‘hybrid’ model predicted accurate
peak temperatures at the DBS electrodes.
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14:00 |
3768. |
Resonant Traps
as a Safety Measure: Influence of Inaccurate
Tuning
Falk Uhlemann1, Peter Mazurkewitz1,
and Oliver Lips1
1Philips Research Laboratories,
Hamburg, Germany
Guidewires or cabling inside catheters can
cause severe heating during MRI. The
associated common mode currents can be
reduced by resonant traps. We investigate if
safety issues can arise from inaccurately
tuned traps (due to e.g. tolerances,
movement, surrounding tissue). Tip heating
of wires inside the MR is analyzed depending
on their length and trap tuning. Results
show that the effect of inaccurate tuning or
inadvertent detuning has to be considered,
since the safety can easily be deteriorated.
Slight detuning can result in configurations
where the trap even increases the tip
heating of the wire.
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14:30 |
3769. |
Influence of
Electrical Connections on Catheter Heating
Oliver Lips1, Bernd David1,
Sascha Krueger1, Kai-Michael
Luedeke1, and Steffen Weiss1
1Philips Research Laboratories,
Hamburg, Germany
The dependence of catheter heating on the
electrical connections is investigated. RF
simulations and corresponding measurements
analyze the effect of different impedances
at various positions along the connections.
Additionally, tip heating for several,
realistic active tracking set-ups is
measured employing catheters equipped with
standard cables as well as
transformer-cables. Using standard wires
resonant heating was observed in several
connecting conditions. Transformer cables do
not show a relevant tip heating in any
configuration. Thus, it is advisable to
prevent RF heating inside the catheter in
order to avoid any negative influence from
the electrical connections.
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15:00 |
3770. |
Assessment of
RF induced heating of coronary stents in 7T MRI
Davide Santoro1, Julia Marie Vogt2,
Wolfgang Renz3, Johanna
Gellermann4, Frank Seifert5,
Valeriy Tkachenko4, Jeannette
Schulz-Menger4, and Thoralf
Niendorf1,4
1Berlin Ultra-High Field Facility
(BUFF), Max Delbrück Center for Molecular
Medicine (MDC), Berlin, Germany, 2Department
of Physics, Humboldt University Berlin,
Berlin, Germany, 3Siemens
Healthcare, Erlangen, Germany, 4Experimental
and Clinical Research Center (ECRC), Charité
Campus Berlin Buch, 5Physikalisch-Technische
Bundesanstalt (PTB)
The advantage of ultrahigh field MRI holds
the promise to enhance, spatial and/or
temporal resolution in MRI. Such
improvements would benefit an ever growing
set of indications for cardiovascular MR.
However, intracoronary stents used for
treatment of coronary artery disease are
currently considered to be
contra-indications for CMR at 7.0 T. The
presence of a metallic implants in
combination with RF wave lengths and RF
power deposition used at 7.0 T may induce
local heating which might cause myocardial
tissue damage, influence coagulation or
endothelial function. For all these reasons
it is essential to carefully assess RF
induced heating in coronary stents commonly
used in percutaneous coronary intervention.
This work examines RF induced heating of
coronary stents in agarose phantoms using
electromagnetic field simulations, fiber
optic temperature measurements and MR
thermometry at 7.0 T.
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Wednesday May 11th
|
13:30 - 15:30 |
Computer 66 |
13:30 |
3771. |
Detection and
Countermeasures for RF Unsafe Conditions for
MR-conditional Devices
Ingmar Graesslin1, Steffen Weiss1,
Emna Hassani1, Kai Nehrke1,
Peter Vernickel1, and Sascha
Krueger1
1Philips Research Laboratories,
Hamburg, Germany
Aging population causes an increasing demand
for MR-examinations in patients wearing
implants, which usually is a
contra-indication for an MR examination.
Previous work proposed to cancel planned
scans if a reverse-polarization pre-scan
detected a device or as soon as unsafe
situations were detected by pick-up-coils.
This work has the objective to detect unsafe
RF coupling events to a device during an MR
measurement and to change the
scan-parameters of the parallel TX-system
rather than terminating the scan. The aim is
to re-establish a safe situation while
trying to maintain image quality. The
proposed approach was evaluated in phantom
as well as volunteer studies.
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14:00 |
3772. |
Reduction of
RF Heating of Metallic Devices by Using a
Two-Channel Transmit Array System : Application
to Arbitrary Lead Geometries
Yigitcan Eryaman1, Burak Akin1,
Cagdas Oto2, Oktay Algin3,
and Ergin Atalar1
1National Magnetic Resonance
Research Center (UMRAM), Bilkent University,
Ankara, Turkey, 2Veterinary
Medicine,Department of Anatomy, Ankara
University, Ankara, Turkey, 3Department
of Radiology, Ataturk Training and Research
Hospital, Ankara, Turkey
In this work, it is shown that the RF
heating at the tip of metallic leads can be
reduced by using a two-channel transmit
array system. A zero electric field plane is
steered inside the body by controlling the
currents at two ports of the birdcage coil.
As the field is steered, the RF current
artifact near the lead tip is monitored and
the excitation pattern which minimizes the
current artifact is found. Phantom and
animal experiments are performed with copper
wires and DBS leads in order to demonstrate
the reduction in tip temperature.
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14:30 |
3773. |
Comparison of
RF Heating in Cables equipped with different
Types of Current Limitations
Steffen Weiss1, Bernd David1,
Oliver Lips1, Jan Hendrik
Wuelbern1, and Sascha Krueger1
1Philips Research Laboratories,
Hamburg, Germany
Various methods have been used to limit
MR-induced RF currents and associated RF
heating in wired interventional devices,
including resistors, resonant RF chokes,
transformers, and mechanical switches as
current-limiting elements. Here, RF heating
for six such transmission lines was
evaluated at the tip and along the full
length of the line using fiber-optic probes
and an infrared camera simultaneously. While
all methods effectively suppressed tip
heating, heating at the current limiting
elements was largest for resonant chokes and
lowest for transformers and switches. The IR
imaging method is suitable to quickly and
globally identify sources of ohmic heating.
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15:00 |
3774. |
MR Safety
Assessment of Potential RF Heating from Cranial
Fixation Plates at 7 Tesla
Oliver Kraff1,2, Karsten H Wrede1,3,
Stephan Orzada1,2, Philipp
Dammann1,3, Mark E Ladd1,2,
and Andreas K Bitz1,2
1Erwin L. Hahn Institute for MRI,
University Duisburg-Essen, Essen, Germany, 2Department
of Diagnostic and Interventional Radiology
and Neuroradiology, University Hospital
Essen, Essen, Germany, 3Clinic
for Neurosurgery, University Hospital Essen,
Essen, Germany
Examination of patients with implants has
become relevant at research facilities with
ultra-high field strength systems. In this
study we focus on miniplate implants used
for refixation of the bone flap after
craniotomy. Since typical temperature
measurements performed with fiber-optic
probes to assess potential heating yield
only point-wise information, a much more
detailed assessment of MRI-related heating
due to interactions of the RF field with the
implants was performed. The test protocol
included full wave simulations on different
numerical models as well as external
measurements of the H and E field and SAR
distribution using a 7T head coil.
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Thursday May 12th
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13:30 - 15:30 |
Computer 66 |
13:30 |
3775. |
A novel
phantom design to reduce thermal losses during
radio frequency (RF) induced heating testing
according to ASTM F2182-09 standard
Christian Koch1,2, Gregor
Schaefers1, and Waldemar Zylka2
1MR:comp GmbH, MR Safety Testing
Laboratory, Buschgrundstraße 33, 45894
Gelsenkirchen, North Rhine-Westphalia,
Germany, 2Deptartment
of Physical Engineering, Medical Physics
Laboratory, University of Applied Sciences
Gelsenkirchen, Neidenburger Str. 43, 45877
Gelsenkirchen, North Rhine-Westphalia,
Germany
A new phantom design is proposed to improve
the accuracy of calorimetrically determined
whole phantom specific absorption rate (SAR)
for RF heating measurements. Emphasis has
been laid on reducing the thermal error
caused by heat capacity of the phantom’s
material. To assess this calorimetrical
accuracy, numerical calculations of
temperature distribution and averaged
temperature rise have been carried out for
two different phantom models. It is
demonstrated that the thermal inaccuracy due
to phantom body material can be reduced
significantly, i.e. below the resolution of
the temperature measurement device.
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14:00 |
3776. |
MR thermometry
using a paramagnetic lanthanide complex for
evaluation of RF safety
Shalmali Dharmadhikari1,2, and
Navin Bansal1,2
1Purdue University, West
Lafayette, Indiana, United States, 2Indiana
Univeristy, Indianapolis, Indiana, United
States
Determination of RF-induced heating during
MRI is important for safety evaluation of
RF-devices, pulse sequences and implants.
Calorimetric assessment of specific
absorption rate (SAR) requires accurate
measurement of small temperature changes
produced during MRI. MR thermometry with
TmDOTP5- enables temperate measurement with
high temperature and spatial resolution.
Since the temperature changes during MRI
occur due to heat deposition as well as
dissipation, a model considering the effect
of heat loss, for computation of SAR has
been proposed. Application and development
of MR thermometry technique with TmDOTP5- to
image SAR has been successfully
demonstrated.
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14:30 |
3777. |
TEM cell for
calibration of an electro-optic E-field sensor
in a clinical scanner
Frank Seifert1, Tobias Klepsch1,
Tomasz David Lindel1, Werner
Hoffmann1, and Bernd Ittermann1
1Physikalisch-Technische
Bundesanstalt, Braunschweig und Berlin,
Germany
EM field simulations of RF coils and coil
arrays are basic tools for predicting SAR in
the human body. Besides B1(+) measurements,
complementary E-field measurements using MR
compatible E-field sensors are inevitable
for an experimental validation of such
simulations using the MR scanner itself.
However, the significance of such
measurements is limited by the quality of
the sensor’s calibration. We present a MR
compatible transverse electromagnetic cell
(TEM cell) used as calibrating device for a
time-domain electro-optic E-field sensor via
B1(+) measurements. Since in a TEM cell the
E-Field is exactly related to the B1(+)
field by E = 376.73 Ohm*2*B1(+)/µ0 the
calibration procedure is based on MR
techniques only.
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15:00 |
3778. |
Optical Dipole
Probes for Quantitative Electric Field
Measurements up to 7T
Jens Groebner1, Reiner Umathum1,
Stefan Hoffmann1, Moritz
Cornelius Berger1, Michael Bock1,
Florian Martin Meise1, Wolfhard
Semmler1, and Jaane Rauschenberg1
1Medical Physics in Radiology,
German Cancer Research Center (DKFZ),
Heidelberg, Germany
Up to now, E-field probes have been
presented for relative SAR estimation. In
this work, an optical dipole-controller
system was developed, to measure absolute
E-field values. The dipole probe was
calibrated in a custom built Crawford TEM
cell to assure the accuracy of the measured
E-field values. The new probe can determine
E-fields between 65 and 643.5 V/m, which
could be demonstrated of a known 7 T head
coil.
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Electronic
Posters : Engineering
|
Click on
to view the abstract pdf and click on
to view the video presentation. |
Gradient & Shim Coil Design
Monday May 9th
Exhibition Hall |
14:00 - 16:00 |
Computer 67 |
14:00 |
3779. |
A Finite-Difference based
Method for the Design of Gradient Coils in MRI
Ling Xia1, Minhua Zhu1, Guofa Shou1,
Feng Liu2, and Stuart Crozier2
1Department of Biomedical Engineering,
Zhejiang University, Hangzhou, China, People's Republic
of, 2School
of Information Technology & Electrical Engineering,
University of Queensland, Brisbane, Australia
This paper presents a finite difference (FD) based
method for the design of gradient coils in MRI. The
design method firstly uses the FD approximation to
describe the current density of the coil space and then
employs the stream function method to extract the coil
pattern. During the numerical implementation, a linear
equation has been constructed and solved using a
regularization scheme. This abstract briefly describes
the algorithm details through X-gradient coil design
examples. The proposed gradient coil design scheme can
be integrated into a finite-difference based EM
framework, which can handle multi-physics including RF
and gradient fields presented in the MR engineering.
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14:30 |
3780. |
A novel coil design method
for manufacturable configurations at optimal performance
Feng Jia1, Zhenyu Liu2, and Jan G
Korvink1,3
1Freiburg Institute of Advanced Studies
(FRIAS), University of Freiburg, Freiburg, Germany, 2Changchun
Institute of Optics, Fine Mechanics and Physics (CIOMP),
Chinese Academy of Sciences, Changchun, China, People's
Republic of, 3Department
of Microsystems Engineering (IMTEK), University of
Freiburg, Freiburg, Germany
Based on an alternative differentiable objective
function which is related with the maximum of current
density, an iterative optimization method is proposed to
design a biplanar micro-coil in this abstract. The main
goal of this method is to increase the minimal distance
between adjacent conductors of the coil. The planar
surface can be discretized using a high-order triangular
mesh. The magnetic field is calculated using the
Biot-Savart law where the surface current density is
expressed using a stream function and the surface
integration is implemented using surface numerical
integration based on the shape functions of the finite
element.
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15:00 |
3781. |
Behaviour of Gradient
Coils Designed With Varying Degrees of Minimised Maximum
Current Density
Michael Stephen Poole1, Peter While2,
Hector Sanchez Lopez1, Larry Forbes2,
and Stuart Crozier1
1ITEE, University of Queensland, Brisbane,
QLD, Australia, 2Mathematics,
University of Tasmania, Hobart, Tasmania, Australia
A new method to design gradient and shim coils was
recently presented that spreads out close wires. This
has the effect of being able to increase the coils
efficiency when limited by minimum wire size. Also, it
can be used to reduce the peak temperature in a coil.
Here we investigate the behaviour of such coils on the
interval between standard minimum power and the new
minimax current density coils. Performance properties
and heating experiments and simulations were performed
and the results analysed.
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15:30 |
3782. |
Suppressing local hot
spots in RF coils and shields due to gradient eddy currents
Zhen Yao1, Aaron Shojinaga1, Yong
Wu1, Timothy Eagan2, Shmaryu
Shvartsman2, Thomas Chmielewski2,
and Robert Brown1
1Department of Physics, Case Western Reserve
University, Cleveland, OH, United States, 2ViewRay
Inc., Oakwood Village, OH, United States
A design goal for MRI is to limit the eddy currents
generated on the RF coils and shields due to the
gradient coils and in particular to suppress the
associated eddy current heating. It is important, for
example, to avoid hot spots in the proximity of the
patient as well as in the vicinity of soldering joints.
We simulate the generation of eddy current and
corresponding heat distributions resulting from gradient
magnetic flux, and make successful comparisons to
experimental measurements. Specific patterns of cuts for
reducing troublesome heating locations are studied.
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Tuesday May 10th
|
13:30 - 15:30 |
Computer 67 |
13:30 |
3783. |
Magnetic Particle Imaging:
Linear Gradient Array for Imaging with a Traveling Wave
Peter Klauer1,2, Martin Andreas Rückert1,2,
Patrick Vogel1,2, Walter H. Kullmann1,
Peter M. Jakob2,3, and Volker Christian Behr2
1Electrical Engineering, University of
Applied Sciences Würzburg-Schweinfurt, Schweinfurt,
Germany, 2Department
of Experimental Physics 5 (Biophysics), University of
Würzburg, Würzburg, Germany, 3Research
Center for Magnetic Resonance Bavaria e.V (MRB),
University of Würzburg, Würzburg, Germany
This work presents a new gradient design for magnetic
particle imaging that will allow performing dynamic
imaging in a linear sampling scheme rather than a
Lissajous trajectory by generating a traveling wave.
Aside from the simplified trajectory, this approach
provides the possibility of increasing the field of view
arbitrarily in one dimension without increasing the
sampling time.
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14:00 |
3784. |
A Hybrid Field-harmonics
Approach for Passive Shimming Design in MRI
Feng Liu1, Jianfeng Zhu2, Ran
Zhang3, Ling Xia2, and Stuart
Crozier1
1School of Information Technology and
Electrical Engineering, University of Queensland,
Brisbane, Queensland, Australia, 2Department
of Biomedical Engineering, Zhejiang University,
Hangzhou, Zhejiang, China, People's Republic of, 3School
of Electrical Engineering, Shandong University, Jinan,
Shandong, China, People's Republic of
This paper presents a new passive shimming (PS) design
scheme for the correction of static magnetic field
inhomogeneities in MRI systems. The PS procedure usually
employs field-based (a) or harmonics-based (b) methods
to find an optimum iron piece configuration to improve
the field uniformity in the imaging region. For the PS
technique (a), the peak-to-peak field inhomogeneity is
minimized and the harmonic components are inherently
unconstrained; in the technique (b), selected unwanted
harmonics are minimized and the overall field uniformity
is consequently reduced. The approach (a) usually
provides good field homogeneity but lacks flexibility in
managing all terms of spherical harmonic field
expansion; the approach (b) is capable of controlling
targeted low-order harmonic terms but can have
difficulty in producing optimal overall field
homogeneity and in controlling high-order harmonics. The
proposed algorithm attempts to combine the strengths of
these two methods for a better PS solution. During the
PS implementation, an explicit expression of the system
matrix with both field and harmonics sensitivities is
generated, and then an optimization procedure is
performed for the determination of shim piece
thicknesses and locations. An experimental study showed
that the hybrid method provided good quality, flexible
solutions for controlling individual harmonics
impurities and also overall field uniformity.
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14:30 |
3785. |
Construction and
optimization of local 3rd order passive shim system for
human brain imaging at 4T MRI
Mohan Lal Jayatilake1,2, Judd Storrs1,3,
Jeff Osterhage1, and Jing-Huei Lee1,4
1Center for Imaging Research, University of
Cincinnati, Cincinnati, OH, United States, 2Department
of Physics, University of Cincinnati, Cincinnati, OH,
United States,3Department of Psychiatry and
Behavioural Neuroscience, University of Cincinnati,
Cincinnati, OH, United States, 4School
of Energy, Environmental, Biological, and Medical
Engineering, University of Cincinnati, Cincinnati, OH,
United States
Magnetic susceptibility variation can lead to B0 field
inhomogeneity and cause artifacts including signal
dropout and image distortions. We introduce a method
that the addition of the third order passive shim system
along with the first and second active shimming
significantly improves the homogeneity of the static
magnetic field within the human brain.
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15:00 |
3786. |
Optimization of
computational speed for BE method of coil design
Chad Tyler Harris1, William B Handler1,
and Blaine A Chronik1
1Physics and Astronomy, University of Western
Ontario, London, Ontario, Canada
The Boundary Element (BE) method is proving to be an
extremely powerful and versatile tool in the
electromagnetic design of gradient, shim, and shielding
coils. We have been strongly motivated by its many
strengths to optimize the computational implementation
of the math since its first use. We have found that a
significant decrease in computation time is achievable
relatively easily. In this study, we describe the most
important steps in the optimization of this algorithm,
and show that it is able to produce detailed wire
patterns in a matter of seconds.
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Wednesday May 11th
|
13:30 - 15:30 |
Computer 67 |
13:30 |
3787. |
Synergistic active and
passive shimming to optimize B0 field
homogeneity in micro MR imaging
Rahul Dewal1, Zhipeng Cao1,
Christopher Sica2, Christopher Collins2,
and Qing Yang1,2
1Bioengineering, The Pennsylvania State
University, Hershey, PA, United States, 2Radiology,
The Pennsylvania State University, Hershey, PA, United
States
Passive shimming can be used to correct for the static B0 field
inhomogeneities caused by air-tissue boundaries in the
sinus cavities and ear canals. By placing pieces of shim
material with high susceptibility values into the magnet
at precise locations, the magnetic field can be
perturbed such that higher-order inhomogeneities are
corrected. This method uses a numerical optimization
algorithm in conjunction with a Fourier transform-based
fast magnetic field calculation method to determine the
optimal configuration of shim materials for an agar gel
phantom. Optimized active shims are calculated alongside
passive shim optimization to form a synergistic shimming
approach.
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14:00 |
3788. |
Fast Eddy Current
Simulation in Thick Split Cylinders of Finite Length Induced
by Coils of Arbitrary Geometry
Hector Sanchez-Lopez1, Michael Poole1,
Limei Liu1, and Stuart Crozier1
1School of Information Technology &
electrical Engineering, The University of Queensland,
Brisbane, QLD, Australia
In this paper we presented a new and fast eddy current
simulation method. The approach is valid for currents
induced in thick and split cylinders of finite length
induced by coils of arbitrary geometry. The method
divides thick conducting axially split/continues
cylinders into thin layers (thinner than the skin depth)
and expresses the current density on each as a
normalized Fourier series. The coupling between each
mode with every other is modeled with an inductive
network method calculated in Fourier space. In this way,
the eddy currents induced in realistic cryostat surfaces
by coils of arbitrary geometry can be simulated.
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14:30 |
3789. |
Reducing Short Term
Gradient Heating by Usage of Adapted Encoding Schemes
Paul Freitag1
1Bruker BioSpin MRI GmbH, Ettlingen, Germany
Classic Cartesian phase encoding schemes cause high
short temporal power dissipation in the gradient system
in the K-space edges. Optimizing the phase encoding
scheme allows to achieve an approximately constant
averaged power dissipation. Applying this to fast 3D
imaging sequences, a smaller field of view or shorter
repetition times can be selected without damaging the
gradient system. The proposed optimization algorithm can
easily be integrated into routine sequences allowing
performance gains of up to 20% regarding minimum
repetition time.
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15:00 |
3790. |
Design of Gradient and
Shim Coils for a Head-Only, Vertical, HTS MRI System
Michael Stephen Poole1, Hector Sanchez Lopez1,
Stuart Crozier1, Iwao Nakajima2,
and Shin-ichi Urayama3
1ITEE, University of Queensland, Brisbane,
QLD, Australia, 2Takashima
Seisakusho Co., Ltd., Tokyo, Japan, 3Human
Brain Research Center, Kyoto University Graduate School
of Medicine, Kyoto, Japan
Gradient and shim coils were designed for a
high-temperature superconductor magnet system.
Particular attention was paid to minimisation of the
eddy currents generated in the cryostat of the
experimental magnet. The constrained space and
requirement for wide wire spacing in the design dictated
the use of minimax current density technique which more
than doubled the efficiency of the transverse gradient
coils.
|
Thursday May 12th
|
13:30 - 15:30 |
Computer 67 |
13:30 |
3791. |
Simple minimum energy
method for calculating shielding coils on arbitrary
geometries
Dustin W Haw1, Chad T Harris1,
William Bradfield Handler1, and Blaine A
Chronik1
1Physics and Astronomy, University of Western
Ontario, London, Ontario, Canada
A simple method for calculating shielding coils on
arbitrary geometries is presented. This new method not a
time-consuming iterative method. It is a direct
calculation of an energy minimizing total current
density.
|
14:00 |
3792. |
A design method for
asymmetric gradient coils with reduced hot spot temperatures
Peter T. While1, Larry K. Forbes1,
and Stuart Crozier2
1School of Mathematics and Physics,
University of Tasmania, Hobart, TAS, Australia, 2ITEE,
University of Queensland, Brisbane, QLD, Australia
Gradient heating and coil hot spots can result in system
failure or image distortion. A previously reported
method is extended to the design of asymmetric gradient
coils with improved temperature distributions and
reduced hot spot temperatures. The method combines an
optimisation constraint derived from a spatial
temperature distribution model with a relaxed fixed
point iteration routine. In comparison to minimum power
coils, the new coil windings are more spread out with
lower maximum temperatures, at little or no cost to coil
performance. For the design of coils with different
thermal material properties, considerably different
winding pattern solutions are obtained.
|
14:30 |
3793. |
Bi-planar shim coil
designed by Stream Function method improves B0 homogeneity
along Z-axis
Daiki Tamada1, Yasuhiko Terada1,
and Katsumi Kose1
1Institute of applied physics, University of
Tsukuba, Tsukuba, Ibaraki, Japan
A new method using stream function was proposed to
correct inhomogeneity of the magnetic field with
single-channel shim coils. The inhomogeneity achieved by
the stream function method was comparable to that
achieved by the target field method. Moreover, the
inhomogeneity along z-axis was also corrected, which
could not be done by the target field method. The method
presented here provides large three dimensional
homogeneity without multi-channel shim coils, which
leads to the enlargement of available space for samples.
|
15:00 |
3794. |
Design of compact planar
GC for high field open MRI using the computational tool
DUCAS
Mitsushi Abe1, Yukinobu Imamura1,
and Hiroyuki Takeuchi2
1Energy and Environmental Syustems Lab.,
Hitachi, Ltd., Hitachi, Ibaraki, Japan, 2Hitachi
Medical Corp., Kashiwa, Chiba, Japan
Design of a compact planar GC for high field open MRI
using the computational tool DUCAS was done. The DUCAS
can treat arbitral sheet currents and was applied on the
GC design. The designed GC is a ASGC. It has umbrella
shaped shield coil and plane main coil with direct
connection between them. These two characteristics made
the GC size compact and the leakage field weak. Then we
conclude this ASGC can be used as planar ASGC for
high-field open MRI.
|
|
|
Electronic
Posters
: Engineering
|
Click on
to view the abstract pdf and click on
to view the video presentation. |
MR+: Multimodality Systems & Methods
Monday May 9th
Exhibition Hall |
14:00 - 16:00 |
Computer 68 |
14:00 |
3795. |
On the Effects of
Magnetic Fields up to 9.4T on PET Image Resolution and
Quality Measured with an MR-BrainPET
Nadim Jon Shah1,2, Hidehiro Iida3,
Christoph Weirich1, Lutz Tellmann1,
Joachim Kaffanke1, Liliana Caldeira4,
Elena Rota Kops1, Stefan Spellerberg5,
and Hans Herzog1
1Institute of Neuroscience and Medicine -
4, Research Centre Jülich, Jülich, Germany, 2Department
of Neurology, Faculty of Medicine, JARA, RWTH Aachen
University, Aachen, Germany, 3Department
of Investigative Radiology, National Cardiovascular
Center Research Institute, Osaka, 4Instituto
de Biofísica e Engenharia Biomédica, Faculdade de
Ciências da Universidade de Lisboa, Lisboa, Spain, 5Institute
of Neuroscience and Medicine - 5, Research Centre
Jülich, Jülich, Germany
In a hybrid MR-PET system, the magnetic field is
expected to reduce the positron range in the x-y
plane. The positron range of 18F and 120I was
investigated from zero up to 9.4T in a 9.4T human
whole-body scanner equipped with a BrainPET insert.
The positron range (and thus resolution) of 18F is
not affected much by the magnetic field. For the
more energetic emitter, I120, there is a significant
improvement in resolution at 9.4T.
|
14:30 |
3796. |
Systematic
Investigation and Correction of MR Influences on
Simultaneous PET Measurements
Christoph Weirich1, Daniel Brenner1,
Lutz Tellmann1, Hans Herzog1,
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
The combination of MRI (Magnetic Resonance Imaging)
and PET (Positron Emission Tomography) offers the
prospect of improved diagnostics, therapeutic
monitoring and preclinical research. Recent studies
showed an influence of MR measurements on
simultaneous PET acquisitions resulting in drop of
the measured count rate. This study aims at a
systematic investigation and first steps towards a
correction of this phenomenon. The overall measured
PET count rate is sensitive to the action of MR
gradients with each gradient direction exhibiting a
different sensitivity.
|
15:00 |
3797. |
Hybrid MR-PET -
Simultaneous FET-PET and Chemical Shift Imaging
N. Jon Shah1,2, Irene Neuner1,2,
Joachim B. Kaffanke1, Christian Filss1,
Gabriele Stoffels1, Hans Herzog1,
and Karl-Josef Langen1
1Institute of Neuroscience and Medicine
4, Forschungszentrum Juelich, Juelich, Germany, 2Department
of Neurology, Faculty of Medicine, JARA, RWTH Aachen
University, 52074 Aachen, Germany
PET imaging is well established for the diagnosis of
brain tumours. It is a valuable tool in the
differential diagnosis of pathologies detected by
MRI. Its metabolic specificity delivers valuable
information about the malignancy and the extent of
tumour tissue. Metabolic information from PET can be
cross-validated and/or extended by MR spectroscopy.
In heterogeneous brain tumours the ratio of
Myo-Inositol to NAA in different parts may help to
distinguish between brain tumour, oedema and scar
tissue.
|
15:30 |
3798. |
Reproducibility of
MRI-DUTE-based attenuation correction maps in brain
tumor patients
Grace Sooyeon Kim1, Daniel Burje Chonde1,
Thomas Benner1, Michael Hamm2,
Alma Gregory Sorensen1, and Ciprian
Catana1
1A.A. Martinos Center for Biomedical
Imaging, Charlestown, MA, United States, 2Siemens
Healthcare, Charlestown, MA, United States
Bone/air segmentation is a significant challenge in
developing the MRI-based attenuation correction (AC)
method. We determined good reproducibility of a
dual-echo ultra-short echo time (DUTE)
sequence-based AC method used in ten brain tumor
patients over four time points (relative SD between
2.17 to 13.40%). We found that the DUTE-based method
yielded a 85.30% average agreement with respect to
the silver-standard segmented CT-based µ map. The
greatest challenges with this method involve
segmentation of the full thickness of the skull and
distinguishing air from tissue in difficult sinus
regions. Further development of the DUTE-based AC
method is under way.
|
Tuesday May 10th
|
13:30 - 15:30 |
Computer 68 |
13:30 |
3799. |
PET-MR-US in drug
delivery
Yu Liu1, Brett Z Fite1,
Charles F Caskey1, Chun-Yen Lai1,
Dustin E Kruse1, Jai Woong Seo1,
Benoit Larrat2, Erik Dumont3,
and Katherine W Ferrara1
1Biomedical Engineering, UC Davis, Davis,
CA, United States, 2Laboratoire
Ondes et Acoustique, ESPCI, Paris, France, 3Image
Guided Therapy, Pessac, France
Synopsis: There is intense research in the area of
ultrasound-enhanced drug delivery, including
enhanced accumulation of particles resulting from
tumor insonation with a temperature elevation of
~5ºC. High field MRI (7T) has advantages in
monitoring such treatments in that the region of
treatment and temperature can be controlled; since
T2* scales with field strength, temperature
estimation is efficient and sensitive at high field.
We have integrated a real-time high-field MR-guided
focused ultrasound system (Image Guided Therapy,
France) in studies of mild hyperthermia and apply
this technology to improve local drug delivery by
coupling PET, MRI and ultrasound (US).
|
14:00 |
3800. |
Simultaneous PET/MRI:
Evaluation of electromagnetic interactions and in
vivo imaging
in 9.4 T MRI
Sri-Harsha Maramraju1,2, S-David Smith2,
Sean Stoll2, Daniela Schulz2,
Sergio Rescia2, Sachin Junnarkar2,
Martin Purschke2, Bosky Ravindranath1,2,
Paul Vaska1,2, Craig Woody2,
and David Schlyer1,2
1SUNY Stony Brook University, Stony
Brook, New York, United States, 2Brookhaven
National Laboratory, Upton, New York, United States
The electromagnetic interactions between the PET and
MRI systems were evaluated by assessing the MR image
quality and evaluating the PET performance. Results
from the MRS and EPI data show no signs of
interference on the MR images during PET acquisition
and the PET data were quantitative. Studies were
carried out using radiolabeled iron oxide
nanoparticles in mice to study the dynamics and
biodistribution of nanoparticles in vivo. These
studies help to understand the toxicological effects
and biological fate of these nanoparticles in vivo.
|
14:30 |
3801. |
RF coil design for
simultaneous PET/MR
Peter Herrick1, Richard Ansorge1,
Rob Hawkes2, Steve Sawiak2,
Joe Stevick1, and Adrian Carpenter2
1Cavendish Laboratory, University of
Cambridge, Cambridge, Cambridgeshire, United
Kingdom, 2Wolfson
Brain Imaging Centre, Addenbrooke's Hospital,
University of Cambridge, Cambridge, Cambridgeshire,
United Kingdom
An engineering challenge of simultaneous PET/MR is
to minimize and quantify the effect of RF coil
hardware on PET signal intensity. This RF hardware
is usually invisible in MRI, thus proposed
segmentation methods for MR-based attenuation
correction are not suitable. We have used Monte
Carlo simulations of gamma-ray interactions to
demonstrate the impact of structural components and
coil positions on PET images. This shows that the
adverse effects of using conventional RF coils can
be dramatic, resulting in 25% loss of PET signal
intensity and 0.5mm loss in spatial resolution.
Quantitative measurements of uptake values are
crucial for PET diagnosis.
|
15:00 |
3802. |
Rapid Re-shimming for
Rotated Views in MR-SPECT Imaging
Mark Jason Hamamura1, Seunghoon Ha1,
Werner W Roeck1, and Orhan Nalcioglu1,2
1Tu & Yuen Center for Functional
Onco-Imaging, University of California, Irvine, CA,
United States, 2Department
of Cogno-Mechatronics Engineering, Pusan National
University, Pusan, Republic of Korea
In a combined MRI and SPECT system (MR-SPECT),
metallic components of the SPECT hardware distort
the B0 field
for MR imaging. Rotation of the SPECT hardware for
tomographic imaging thus alters the B0 field
and requires re-shimming. To perform rapid
re-shimming, pre-determined field maps were utilized
to calculate the optimum currents to apply to the
shim channels. These calculations do not require any
additional MRI acquisitions, allowing for
re-shimming immediately after any rotation.
|
Wednesday May 11th
|
13:30 - 15:30 |
Computer 68 |
13:30 |
3803. |
Towards reliable
calibrated transducers for MR-guided focused ultrasound
Tobias Klepsch1, Julian Haller1,
Klaus-Vitold Jenderka1, Werner Hoffmann1,
Bernd Ittermann1, and Frank Seifert1
1Physikalisch-Technische Bundesanstalt,
Braunschweig und Berlin, Germany
High Intensity Focused Ultrasound (HIFU) guided by
MR thermometry is a promising tumor therapy in
organs such as liver, uterus and prostate. Although
the technique is already clinical routine the
calibrated measurement of high intensity ultrasound
fields still needs closer examination. We present an
approach towards finding a traceable calibration for
MR guided focused ultrasound (MRgFUS) using a
reference heating element. Furthermore we examined
the focal zone of a commercial MR compatible
transducer with MR thermometry at 3 tesla. This was
done either for a fixed position or during
translational movement of the transducer.
|
14:00 |
3804. |
Characterization of a
MRI-RF Hyperthermia Dual-Function Coil Element Design
Xing Yang1, Jing Wu2, Xu Chu1,
Thomas K Foo3, and Desmond Teck Beng Yeo3
1Power Conversion Circuits Lab, GE Global
Research, Shanghai, China, People's Republic of, 2Electrical
and Computer Engineering, Northeastern University,
Boston, MA, United States, 3Imaging
Technologies, GE Global Research, Niskayuna, NY,
United States
During an RF hyperthermia procedure, careful
monitoring of tissue temperature is required in the
tumor and healthy tissue. The ability to perform
targeted heating and monitor temperature with the
same multi-channel coil allows for faster
acquisition via parallel imaging, and potentially
higher SNR due to the smaller elements placed closer
to the body. In this study, a MRI-RF hyperthermia
dual-function coil element design is proposed, and
its working principle is presented along with
numerically computed characterization data of the
trade-offs involved when the key design parameters
are varied. These parameters include antenna
dimension, adjacent coil overlap area, inter-element
coupling, and antenna phase shifts.
|
14:30 |
3805. |
A UNILATERAL RF COIL
FOR MR-SCINTIMAMMOGRAPHY
Seunghoon Ha1, Mark Jason Hamamura1,
Werner W. Roeck1, and Orhan Nalcioglu1
1University of California Irvine, Irvine,
California, United States
Synopsis: Many studies have indicated that
preoperative MRI is useful in local staging for
surgical planning, especially for patients with
lobular cancer. However, the low specificity of MRI,
despite its high sensitivity, may lead to many
unnecessary biopsies or over-treatment.
Scintimammography (SMM) can be a tool to supplement
MRI for improving the diagnostic specificity in
breast cancer imaging. In this study, a unilateral
breast array coil and CZT detector module
specialized for MR-SMM is introduced. The variation
of RF coil performance due to assembly with a CZT
detector module is discussed with results from
simulation and experiment.
|
15:00 |
3806. |
Simultaneous, Dynamic
SPECT-MRI Demonstrated in Three Small-Animal Prototypes
James W Hugg1, Benjamin M W. Tsui2,
Orhan Nalcioglu3, Dirk Meier4,
Mark J. Hamamura3, Douglas J. Wagenaar1,
and Bradley E. Patt1
1Gamma Medica, Northridge, CA, United
States, 2Johns
Hopkins University, Baltimore, MD, United States, 3University
of California, Irvine, CA, United States, 4Gamma
Medica, Oslo, Norway
We have built and tested three SPECT prototypes that
can be inserted into small-animal or whole-body MRI
systems for simultaneous, dynamic imaging of mice
and rats. We have measured and characterized the
Hall Effect due to the Lorentz force in the
MR-compatible CZT gamma photon detectors. Otherwise,
the MR and SPECT systems do not significantly affect
each other. We have demonstrated simultaneous,
dynamic SPECT-MR imaging in mice. We are developing
MR attenuation and scatter corrections and MR priors
for quantitative SPECT reconstruction. Imaging a
SPECT agent can provide a molecular imaging contrast
for MR images at pico- to nano-molar sensitivities.
|
Thursday May 12th
|
13:30 - 15:30 |
Computer 68 |
13:30 |
3807. |
Radiation induced RF
coil degradation in hybrid MRI-accelerator systems
Sjoerd Crijns1, Bas Raaymakers1,
Jan Kok1, Kimmy Smit1, Jan Van
Ooijen2, and Jan Lagendijk1
1Radiotherapy, UMC Utrecht, Utrecht,
Netherlands, 2Philips
Medical Systems, Best, Netherlands
The radiation damage to an RF receiver coil as a
function of accumulated dose in a hybrid
MRI-accelerator is characterized. We conclude that
damage per treated patient is small and that any
problems with standard receiver coils are not to be
expected.
|
14:00 |
3808. |
A MULTI ELEMENT RF
COIL AND GAMMA RAY RADIATION SHIELDING ASSEMBLY FOR
MRSPECT SYSTEM
Seunghoon Ha1, Mark Jason Hamamura1,
Werner W. Roeck1, and Orhan Nalcioglu1
1University of California Irvine, Irvine,
California, United States
In medical imaging, single-photon emission computed
tomography (SPECT) can provide specific functional
information while magnetic resonance imaging (MRI)
can provide high-spatial resolution anatomical
information as well as complementary functional
information. However, some of the major problems
facing MRSPECT systems include the degradation of
the signal to noise ratio (SNR) and distortion of
the MR image. In this study, we present a new RF
coil design to retain the tremendous potential of
MRSPECT to provide high sensitivity and specificity
while minimizing the interference between the MRI
and SPECT systems. This new RF coil, described in
the study for small animal imaging, could be used
with multiple ã-ray radiation shields to prevent MR
image distortion and degradation of the SNR.
Experimental results demonstrating the advantages of
the new assembly are presented.
|
14:30 |
3809. |
Real-time target
displacement prediction using Dynamic MRI for
radiotherapy
Nilesh N Mistry1, Jiachen Zhuo2,
Kathleen Malinowski1,3, Rao Gullapalli2,
and Warren D D'Souza1
1Radiation Oncology, University of
Maryland School of Medicine, Baltimore, MD, United
States, 2Radiology,
University of Maryland School of Medicine,
Baltimore, MD, United States, 3Fischell
Department of Bioengineering, University of
Maryland, A. James Clark School of Engineering,
College Park, MD, United States
Advanced radiation therapy delivery techniques have
the potential to deliver the required doses to the
tumor while minimizing the dose to healthy normal
tissue. However, these advancements require highly
conformal dose delivery and without effective motion
management techniques such therapies can be
sub-optimal. In this work we explore the feasibility
of using cine-MRI images acquired in conjunction
with the real-time external surrogates to assist in
the development of a robust model for real-time
tumor displacement prediction.
|
15:00 |
3810. |
Ultra-low-field MRI
system for hybrid MEG-MRI
Panu Tapani Vesanen1, Juha Hassel2,
Jari S Penttilä3, Jaakko Oskari Nieminen1,
Juhani Dabek1, Koos Zevenhoven1,
Juho Luomahaara2, Sarianna Alanko1,
Nadia Catallo4, Fa-Hsuan Lin5,
Juha Simola6, Antti Ahonen6,
and Risto J Ilmoniemi1
1Dept. of Biomedical Engineering and
Computational Science, Aalto University, Espoo,
Finland, 2VTT
Technical Research Centre of Finland, Espoo,
Finland, 3Aivon
Oy, Espoo, Finland, 4Dept.
of Health Sciences, University of L’Aquila, Italy, 5Institute
of Biomedical Engineering, National Taiwan
University, Taiwan, 6Elekta
Oy, Helsinki, Finland
In ultra-low-field MRI (ULF MRI), spins precess in
microtesla magnetic fields, and the signal is
measured by superconducting quantum interference
devices (SQUIDs). Low fields offer several
advantages compared to conventional MRI such as
narrow line-widths, enhanced T1 contrast, imaging of
objects in the presence of metal, and a possibility
for simultaneous magnetoencephalography (MEG)
measurement. In this work, we describe the current
state of our multichannel ULF-MRI system. We present
phantom images and discuss technical solutions for
coil design in a magnetically shielded environment.
|
|
|
Electronic
Posters
: Engineering
|
Click on
to view the abstract pdf and click on
to view the video presentation. |
Coils & Arrays for UHF MRI
Monday May 9th
Exhibition Hall |
14:00 - 16:00 |
Computer 69 |
14:00 |
3811. |
Remote Tuning and
Matching an 8-Channel Transceive Array at 7T
Carl Snyder1, Christopher Rogers2,
Lance DelaBarre1, Mattew Robson2,
and J. Thomas Vaughan1
1University of Minnesota, Minneapolis,
MN, United States, 2Oxford
University, Oxford, Oxfordshire, United Kingdom
Here an 8-channel transceive array was remotely
tuned and matched using piezoelectric actuators;
this process, can be automated by monitoring and
reducing the standing wave ratio on the transmission
line leading to the coil.
|
14:30 |
3812. |
An Improved
Constellation Coil
Arslan Amjad1
1GE Healthcare, Waukesha, WI, United
States
Parallel transmit multi-port volume coils are
becoming important due to increased field strengths
in order to improve B1+ homogeneity and to minimize
Specific Absorption Rate (SAR). Y. Zhu introduced a
design for a parallel transmit volume coil,
“constellation coil” that does not require tuning
and is scalable to various field strengths. In this
work, we have introduced a modified constellation
coil that improves the B1+ homogeneity of Zhu’s
design, and makes the B1+ profile similar to the
birdcage structure.
|
15:00 |
3813. |
A Full-Wavelength
Dipole RF Coil Element for 7 T MRI with Maximized
Longitudinal FOV and Two-Peak SAR Distribution
Andreas Rennings1, A. Litinsky1,
P. Schneider1, S. Orzada2, and
S. Otto3
1General and Theoretical Electrical
Engineering (ATE), Faculty of Engineering,
University of Duisburg-Essen, 47048 Duisburg,
Germany, 2Erwin
L. Hahn Institute for Magnetic Resonance Imaging,
University of Duisburg-Essen, 45141 Essen, Germany, 3High-Frequency
Engineering (HFT), Faculty of Engineering,
University of Duisburg-Essen, 47048 Duisburg,
Germany
A novel RF coil element for 7 T is proposed. It is
based on a recently published symmetrically fed
dipole element with meander termination for better
decoupling. The novel full-wavelength dipole offers
two distinct improvements – an RF field of view that
is maximized due to the longer extent and a lowered
peak SAR-10g due to a more appropriate two-peak
electric field distribution.
|
15:30 |
3814. |
Novel 24 Element
Multi-Transmit Volume Coil for High Field MRI
Can Akgun1, Hyoungsuk Yoo2,
Lance DelaBarre1, Carl J Snyder1,
Gregor Adriany1, Pierre-Francois Van de
Moortele1, Anand Gopinath3,
Kamil Ugurbil1, and John Thomas Vaughan1
1Center for Magnetic Resonance Imaging,
University of MInnesota, Minneapolis, MN, United
States, 2Department
of Biomedical Engineering, School of Electrical
Engineering, University of Ulsan, Ulsan, Korea,
Republic of, 3Department
of Electrical and Computer Engineering, University
of Minnesota, Minneapolis, MN, United States
At vert high field strengths multi-element RF
transmit coils have been shown to benefit
applications such as RF shimming and parallel
transmission. In this work we present a 24 element
TEM volume coil strategy that is as RF efficient as
a traditional TEM volume coil. Simulation studies
are performed at 7 T.
|
Tuesday May 10th
|
13:30 - 15:30 |
Computer 69 |
13:30 |
3815. |
Stepped Impedance
Resonators for High Field MRI
Can Akgun1, Lance DelaBarre1,
Hyoungsuk Yoo2, Carl J Snyder1,
Anand Gopinath3, Kamil Ugurbil1,
and John Thomas Vaughan1
1Center for Magnetic Resonance Imaging,
University of MInnesota, Minneapolis, MN, United
States, 2Department
of Biomedical Engineering, School of Electrical
Engineering, University of Ulsan, Ulsan, Korea,
Republic of, 3Department
of Electrical and Computer Engineering, University
of Minnesota, Minneapolis, MN, United States
Since its inception in high field MRI volume coils,
there have been very few modifications of the
traditional microstrip transmission line for optimal
performance. In this study, two different microstrip
designs with varying impedance lines referred to as
stepped impedance resonators (SIRs) are presented. A
3-section SIR can be designed to produce a peak B1+
in the center, while a 7-section SIR can be designed
to limit SAR effects when compared to the
traditional microstrip resonator. Imaging and
simulation results for 8 element volume coils with
these designs are obtained at 7T for the human head.
|
14:00 |
3816. |
Clinical neuroimaging
using high dielectric materials at 7T
Wouter M Teeuwisse1, Nadine B Smith1,
and Andrew G Webb1
1Radiology, Leiden University Medical
Center, Leiden, Netherlands
High dielectric materials based on calcium titanate
suspensions in deuterated media can significantly
improve clinically relevant scans at 7 Tesla with
essentially zero background signal. Increases in the
transmit field of up to 100% are measured in the
cerebellum and temporal lobes. T1-weighted, FLAIR
and especially T2-weighted scans show increased
signal-to-noise and tissue contrast with thin
dielectric pads surrounding the head.
|
14:30 |
3817. |
Abdominal Imaging at
7T with a 32-channel Body Array Coil - Initial Results
Jochen Leupold1, Florian Meise2,
Matt Finnerty3, Tsinghua Zheng3,
Jürgen Hennig1, and Michael Bock2
1Dept. of Radiology, Medical Physics,
University Medical Center, Freiburg, Germany, 2Abt.
Medizinische Physik in der Radiologie, Deutsches
Krebsforschungszentrum, Heidelberg, Germany, 3Quality
Electrodynamics (QED), Mayfield Village, OH, United
States
Application of ultrahighfield-MR (UHF-MR) at 7T on
humans is currently mainly limited to the brain due
to the expected strong inhomogeneity of the B1-field
in the body and abdomen. We present first results of
a 7T transmit/receive body coil array, which has
been designed as an array of multiple small coil
elements with the goal to minimize coil induced
B1-inhomogeneities.
|
15:00 |
3818. |
30 channel unilateral
breast coil for ultra high resolution MRI at 7T
Ingmar Jacob Voogt1, Bart L van de Bank1,
Peter R Luijten1, Dennis W Klomp1,
Michel Italiaander1, and Rudy Roon1
1Radiology, UMC Utrecht, Utrecht,
Utrecht, Netherlands
The specificity in dynamic contrast enhanced MRI in
breast cancer may be increased by enabling the
simultaneous detection of high morphological
details. Therefore the high sensitivity of 7T is
used to obtain sufficient SNR in the high spatial
resolution that needs to be obtained within the time
frame of contrast enhancement time curves. Therefore
a 30 channel dedicated unilateral breast coil was
designed for 7T that enables high acceleration while
maintaining SNR.
|
Wednesday May 11th
|
13:30 - 15:30 |
Computer 69 |
13:30 |
3819. |
A 7-Tesla High Density
Tx/Rx Mammography Coil
Tsinghua Zheng1, Xiaoyu Yang1,
Matthew Finnerty1, Jeremiah Heilman1,
Joseph Herczak1, Hiroyuki Fujita1,2,
Graham Wiggins3, Ryan Brown3,
and Bernd Stoeckel4
1Quality Electrodynamics, LLC, Mayfield
Village, Ohio, United States, 2Physics,
Case Western Reserve University, Cleveland, Ohio,
United States, 3Radiology,
NYU Langone Medical Center, New York, New York,
United States, 46Siemens
Medical Solutions USA, Inc, Malvern, Pennsylvania,
United States
We have constructed a7T transmit-and-16-channel
receive array breast coil for Siemens Magnetom 7T
scanner. Comparison of in vivo volunteer images with
a commercially available 4 channel breast array coil
at 3T showed significant advantage of the 7T breast
array coil with its ultra high spatial resolution,
which is critical to the early breast cancer
detection.
|
14:00 |
3820. |
A Prototype Head Coil
for 11.7T using the Inductive Birdcage Geometry
Joseph Murphy-Boesch1, Stephen Dodd1,
Peter van Gelderen1, Alan Koretsky1,
and Josef H. Duyn1
1LFMI/NINDS, National Institutes of
Health, Bethesda, MD, United States
A shielded inductive resonator configured as a
backward-wave transmission structure has been
designed for use as a transmit/receive head coil at
11.7 Tesla. Transmission line analysis and a
four-element distributed impedance model have been
used to optimize the design for high-frequency. A
prototype coil constructed with these methods
displays a homogeneous mode in excess of 500 MHz.
The coil frequencies are in good agreement with the
model, and an axial field plot of the unloaded coil
shows good field uniformity at mid-elevation.
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14:30 |
3821. |
A Flexible Microstrip
Transceiver Coil for Imaging Flexed Human Knee Joints at
7 Tesla
Karupppasamy Subburaj1, Yong Pang1,
Serena Scott1, Bagrat Amirbekian1,
Richard B Souza1,2, Sharmila Majumdar1,
and Xiaoliang Zhang1
1Department of Radiology and Biomedical
Imaging, University of California San Francisco, San
Francisco, California, United States, 2Department
of Physical Therapy and Rehabilitation Science,
University of California San Francisco, San
Francisco, California
Traditional cylindrical knee coils designs present
difficulties when imaging flexed knee joints in
kinematic studies. We present a novel flexible TR
coil based on microstrip transmission lines for
in-vivo MR imaging of flexed human knee joints at
7T. This single channel coil was designed to have
wing shaped symmetrical loops on a partially
foldable teflon substrate to take advantage of 2nd
harmonic resonance and a large coverage volume. The
coil has a good Q factor ratio and the resonant
frequency can be tuned to a broad range in order to
adapt to various knee sizes.
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15:00 |
3822. |
Radio-Frequency
Heating in Swine with an 8 Channel, 7 T (296 MHz) Head
Coil
Devashish Shrivastava1, Jeramy Kulesa1,
Jinfeng Tian1, Gregor Adriany1,
Lance DelaBarre1, and J T Vaughan1
1CMRR, University of Minnesota,
Minneapolis, MN, United States
Radio-frequency (RF) heating was fluoroptically
measured in the scalp; 5 mm, 10 mm, 15 mm, 20 mm,
and 25 mm in the brain; and rectum in three
anesthetized swine due to a continuous wave power
deposition with a 7T head coil at the average whole
head SAR of 2.94 W/kg. The RF heating was simulated
using the new, theoretical generic bioheat transfer
model (GBHTM) and the empirical Pennes’ bioheat
transfer equation (BHTE). The average temperature
change in the brain was 2.1 0C after 3 hours of the
power deposition. The GBHTM simulated RF heating
more accurately than the Pennes’ BHTE.
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Thursday May 12th
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13:30 - 15:30 |
Computer 69 |
13:30 |
3823. |
A Loop Coil Design
Based on the Broadside-Coupled Split Ring Resonator at
7T
Marcos Alonso Lopez Terrones1, Gunthard
Lykowsky2, Jose Miguel Algarín1,
Manuel J. Freire1, Maria Castillo
Velazquez-Ahumada1, Peter M. Jakob2,3,
and Ricardo Marques1
1Electronics and Electromagnetism,
University of Seville, Seville, Andalucia, Spain, 2Research
Center Magnetice Resonance Bavaria, Würzburg,
Bavaria, Germany,3Experimental Physics 5,
University of Würzburg, Würzburg, Bavaria, Germany
In the design of coils, it is required a uniform
current distribution in the loop to generate a
homogeneous magnetic field. In the broad-side
coupled split ring resonator (BC-SRR) design, the
sum of the currents flowing in the two rings is
constant so that the field produced is homogeneous.
A BC-SRR and two conventional loops were simulated
and built at 7T. In the design of loops with
distributed capacitance, it is not necessary to
split the ring in several gaps. The total current
flowing in the two loops of the BC-SRR design is
constant independently of the number of gaps
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14:00 |
3824. |
A radiofrequency coil
configuration for imaging the human vertebral column at
7 Tesla
Maartje E Vossen1, Wouter M Teeuwisse1,
Monique Reijnierse1, Nadine B Smith1,
Chris M Collins2, and Andrew G Webb1
1Radiology, Leiden University Medical
Center, Leiden, Netherlands, 2Radiology,
Hershey Medical College
A quadrature transmit, eight-channel receive array
RF coil configuration was designed for the
acquisition of images of the entire human spinal
column at 7 Tesla. RF transmission through the
anterior part of the body was shown using
electromagnetic simulations to be more efficient in
terms of B1+ to SAR ratio than through the posterior
side. Using this coil geometry, high resolution
images from healthy volunteers could be acquired in
clinically acceptable imaging times.
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14:30 |
3825. |
A 15-Channel receive
array and 16 channel detunable transmit coil for human
brain imaging at 9.4T
G Shajan1, Jens Hoffmann1, and
Rolf Pohmann1
1Magnetic Resonance Center, Max Planck
Institute for Biological Cybernetics, Tuebingen,
Baden Wuttenberg, Germany
Even more than at 7 T, constructive and destructive
interferences cause strong inhomogeneities of the B1
field produced by a volume coil, causing shading
over large parts of the image. In this study at
9.4T, we present initial results from a 16-channel
actively detunable transmit array combined with a 15
element receive only array. In addition to the high
sensitivity offered by the receive array, transmit
field inhomogeneities can be significantly reduced
by RF shimming methods for whole brain coverage at
9.4T.
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15:00 |
3826. |
Electrically
auto-tuned RF coil design
Sung-Min Sohn1, Anand Gopinath1,
and J. Thomas Vaughan1,2
1Electrical and Computer Engineering,
University of Minnesota, Minneapolis, Minnesota,
United States, 2Center
for Magnetic Resonance Research, University of
Minnesota, Minneapolis, Minnesota, United States
RF coil based on microstip transmission lines, the
TEM coil, has been widely used for high-field MRI
and has narrow bandwidth due to its high quality
factor (Q). Although high Signal-to-Noise Ratio (SNR)
of MR coils is obtained from this property it has a
critical drawback, human body (loading) effect that
causes the resonance frequency and Q of RF coil to
change when different human bodies are loaded. This
work proposes an adaptive impedance matching
technique to avoid mismatch of the RF loaded coils
at the Larmor frequency and alternative manual
tuning that needs a several minutes and remains a
major obstacle to the use of TEM coils in
ultra-high-fields MRI systems.
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