Joint Annual
Meeting ISMRM-ESMRMB 2014
○
10-16 May 2014
○
Milan, Italy |
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TRADITIONAL
POSTER SESSION ○ MR ENGINEERING; MR SAFETY: SAFETY & BIOEFFECTS;
ULTRA-HIGH FIELD |
MR Engineering: RF & Other
Monday 12 May 2014
Traditional Poster Hall |
16:30 - 18:30 |
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1276. |
A Wireless Digital
Capacitor Module for Tuning Receive Coil Arrays
Arne Reykowski1 and
Randy Duensing1
1Invivo Corporation, Gainesville, Florida,
United States
This paper presents a novel approach for tuning RX coil
arrays using wireless digital programmable capacitors.
This hardware is intended for research to improve coil
tuning strategies and improve combined SNR beyond the
currently accepted limits. The ability to change tune
settings in the absence of a cable connection or the
need to touch the hardware should greatly improve the
accuracy of repeated SNR measurements.
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1277. |
Optical power transmission
can help to build receive coils without coaxial cables
Jens Höfflin1, Elmar Fischer2,
Oliver Gruschke1, Jürgen Hennig2,
and Jan G Korvink1,3
1Lab of Simulation - Department of
Microsystems Engineering, University of Freiburg - IMTEK,
Freiburg, Germany, 2Medical
Physics - Department of Radiology, University Medical
Center Freiburg, Freiburg, Germany, 3Freiburg
Institute for Advanced Studies - FRIAS, University of
Freiburg, Freiburg, Germany
We present the use of optical power transmission as a
possibility to power electronic components like an LNA
inside the magnet without needing to use copper cables.
The use of switching DC-to-DC converters inside high
magnetic fields is evaluated, and SNR measurements are
presented to compare the performance of different
receive coil setups.
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1278. |
23Na Magnetic
Resonance Spectroscopic Imaging (MRSI) on a High-Density
3d-cell culture on chip (3D-KITChip)
Andreas Neubauer1, Michaela Ruttorf1,
Raffi Kalaycian1, Jan Sachs1,
Cordula Nies2, Stefan Giselbrecht2,
Eric Gottwald2, and Lothar Schad1
1Computer Assisted Clinical Medicine, Medical
Faculty Mannheim, Heidelberg University, Mannheim,
Baden-Wuertemberg, Germany, 2Institute
for Biological Interfaces-1, Karlsruhe Institute of
Technology, Eggenstein-Leopoldshafen, Baden-Wuertemberg,
Germany
In this study we present a setup capable to monitor
changes in ionic concentration gradients in
vitro. The main parts of the setup are a three
dimensional cell
culture, a completely MR-compatible bioreactor and a 23Na
surface coil. In a pilot study we performd a 23Na
CSI experiment to show that we are able to resolve a non
varying reference compartment from a compartment with
varying physiological parameters.
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1279. |
Harnessing Embedded Linux
and Python for Stand-Alone MRI Applications
Pascal P Stang1,2 and
Greig Scott2
1Procyon Engineering, San Jose, CA, United
States, 2Electrical
Engineering, Stanford University, Stanford, CA, United
States
Advances in RF electronics, high-speed data converters,
and multi-core processors have long fueled high-end MRI
techniques such as parallel imaging and real-time
scanning, yet these same technology advances can also be
leveraged to benefit small-scale MR. We present a
compact stand-alone MRI console powered by embedded
Linux and programmed in Python to investigate the
potential of such a platform to deliver modern
performance and versatility for NMR/MRI applications
constrained in size, power, cost, or user interface.
Potential applications include desktop scanners,
chemical spectroscopy and relaxometery, RF ablation
control, and interventional device safety monitoring.
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1280. |
Web-interactive sharing of
medical images and processing algorithms: the WISDM
framework
Jeremy F Magland1 and
Felix W Wehrli1
1Department of Radiology, University of
Pennsylvania, Philadelphia, PA, United States
WISDM is an open source software allowing web
browser-based sharing of medical imaging data stored on
any internet-connected computer. Users may interactively
browse raw, intermediate, and resulting image arrays. In
addition, processing algorithms written in a variety of
scripting languages (MATLAB/Octave, C/C++, and Python)
may be browsed on-line, and even edited and executed by
authorized users. The framework has been used within the
authors' institution to manage imaging data and
processing pipelines for two imaging laboratories and
allows multiple researchers to process and interact with
a common pool of data from any operating system without
downloading datasets or installing software.
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1281. |
BirdcageBuilder Mobile: New
Functionality and Portability for a Standard MR Engineering
Tool
Giuseppe Carluccio1, Chih-Liang Chin2,
and Christopher Michael Collins1
1Bernard and Irene Schwartz Center for
Biomedical Imaging, New York University School of
Medicine, New York, New York, United States, 2Merck
Sharp & Dohme, Singapore, Singapore
Birdcage coils are the most commonly used-volume coils
in MRI for their ability to provide homogeneous
circularly polarized fields inside their volume with a
quadrature channel excitation. One of the most used
tools by RF coils designers is BirdcageBuilder, a
software which provides the values of the capacitors
needed to make the coil able to resonate. In this work
we extend the functionality and portability of the
software by designing a version which can run on common
mobile devices for easy access anywhere coils are
constructed, and provide all resonant frequencies of the
coil as designed.
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1282. |
Actively shielded bias
magnetic field tuning coil for optically pumped atomic
magnetometer toward direct MR signal detection in ultra-low
field MRI
Takenori Oida1, Masahiro Tsuchida1,
and Tetsuo Kobayashi1
1Department of Electrical Engineering,
Graduate School of Engineering, Kyoto University, Kyoto,
Kyoto, Japan
Recently, optically pumped atomic magnetometers (OPAMs)
have been developed and allow us easily to measure
extremely small magnetic fields. An ultra-low field
(ULF) MRI system with an OPAM has been attracted
attentions in recent years. In this study, we proposed
an actively shielded bias magnetic field tuning coil
toward direct detection of MR signals with an OPAM.
Results of magnetic field distribution analyses
demonstrated that the active shield could reduce the
magnetic distortion caused by the bias tuning coil and
the actively shielded bias magnetic field tuning coil
was feasible to detect MR signals directly with an OPAM.
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1283. |
Very low field imaging of
laser-polarized noble gases
Yuan Zheng1, Gordon D Cates2, John
P Mugler2, William A. Tobias2, and
G Wilson Miller2
1University of Virginia, Charlottesville, VA,
United States, 2University
of Virginia, VA, United States
We built an inexpensive low field MRI system and
implemented a novel design of transverse gradient coils.
We presented images of hyper-polarized He-3 and Xe-129
phantoms. Our system can also be expanded for small
animal and even human lung imaging.
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1284. |
Phase Coherent
Multi-Channel Synthesizer of Transmit Pulses at Larmor
Frequencies up to 512 MHz
Andrzej Jesmanowicz1
1Biophysics, Medical College of Wisconsin,
Milwaukee, Wisconsin, United States
The method of multi-channel RF pulse creation is
presented here by the use of a set of independent
wave-form synthesizers. They can operate directrly at
Larmor frequency as high as 512 MHz. Up to 16 channels
with absolute phase coherency can supply pulses to
transmit amplifiers of scanners operating at magnetic
fields up to 12 Tesla.
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1285. |
Comparison of analog and
digital transceiver systems for magnetic resonance imaging
Seitaro Hashimoto1, Katsumi Kose1,
and Tomoyuki Haishi2
1University of Tsukuba, Tsukuba, Ibaraki,
Japan, 2MRTechnology
Inc., Tsukuba, Ibaraki, Japan
Analog and digital transceivers for MRI systems were
critically evaluated under identical experimental
conditions. The MRI experiments were performed using a
4.74-Tesla vertical-bore superconducting magnet and a
high-sensitivity gradient coil probe. 3D spin-echo
images of a kumquat were acquired with and without using
a gain-stepping scan technique to extend the dynamic
range of the receiver systems. The acquired MR images
clearly demonstrated that nearly identical image quality
was obtained for both transceiver systems, but DC and
ghosting artifacts were obtained for the analog
transceiver. We therefore concluded that digital
transceivers have several advantages over the analog
transceivers.
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1286. |
A Generalized Concept for
Preamplifier Decoupling
Enrico Pannicke1,2, Roland Müller2,
Oliver Speck3, Ralf Vick1, and
Harald E. Möller2
1Institute for Medical Engineering,
Otto-von-Guericke-University Magdeburg, Magdeburg,
Saxony-Anhalt, Germany, 2Max
Planck Institute for Human Cognitive and Brain Sciences,
Leipzig, Saxony, Germany, 3Biomedical
Magnetic Resonance, Otto-von-Guericke-University
Magdeburg, Saxony-Anhalt, Germany
Preamplifier decoupling is a valuable technique in the
development of multi-channel receiver array coils.
Although well established, there is currently no simple
rule available to design a proper network with desired
properties. A suitable equation can be derived utilizing
the concept of impedance transformations. With this
concept, the robustness of the coil against varying
loading conditions of the coil was investigated as a
further property of the circuit.
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1287. |
Near-Magnet Power Amplifier
with built-in Coil Current Sensing
Klaus Solbach1, Ashraf Abuelhaija1,
and Samaneh Shooshtary1
1RF Technology, University Duisburg-Essen,
Duisburg, Germany
A new concept of a near-magnet PA is presented which
operates without circulator/isolator but closely
cooperates with the coil to allow control of the coil
current. The concept features a voltage probe at the PA
output and a tuned transmission line connecting the
coil. The probe voltage is proportional to the coil
current which allows control of the coil current under
mismatch and mutual coupling from other coils in an pTx
array without extra pick-up loop. The function is
demonstrated by an experimental set-up creating a wide
range of load impedance by varying the coil distance to
a phantom.
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1288. |
Stability Test of
Near-Magnet Power Amplifier
Kabir Hasanzadeh1, Klaus Solbach1,
and Samaneh Shooshtary1
1RF Engineering, University Duisburg-Essen,
Duisburg, NRW, Germany
In this work a method to test the Stability of
Near-Magnet Power Amplifier (DUT) is explained and the
test results are presented. The method includes a bench
stability test which employs an electronic circuit
designed to realize reflection coefficients with
variable magnitude and phase, which is implemented using
the concept of the laod-pull. The mutual effect between
the antennas around the coil have also been tested to
confirm the stability of the DUT in such situations.
Results show that although the DUT is stable for all the
situations, but the output power is depended on the
variation of the load.
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1289. |
Sensing of Birdcage Rung
Currents for Detection of Anomalous Loading
Christopher Ellenor1, Pascal Stang1,2,
John Pauly1, and Greig Scott1
1Electrical Engineering, Stanford University,
Stanford, CA, United States, 2Procyon
Engineering, San Jose, CA, United States
A birdcage coil is fitted with optically coupled current
sensors on each of its rungs. This tool gives new, rapid
and realtime information about the spatial distribution
of current in the coil under different loading
conditions. The detection of anomalous loading
conditions may be indicative of certain RF safety
hazards such as resonant wire coupling or strong
coupling to tissue through the bore wall, leading to
burns. Phantom experiments are conducted and distortion
of the rung current pattern due to anomalous loading is
observed.
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1290. |
Modeling PIN Diode
Temperature Rise in High Induced Current MR Receive Coils
Robert Caverly1, Ronald Watkins2,
and William E Doherty3
1Villanova University, Villanova, PA, United
States, 2Department
of Radiology, Stanford University, Stanford, CA, United
States, 3Microsemi,
Lowell, MA, United States
A new electrothermal SPICE-based model that predicts
both electrical and thermal behavior of PIN diodes used
in high field, high power MR imaging is described. The
model accurately predicts the temperature rise in
blocking applications and is fully compatible with
industry-standard simulators such as SPICE as well as it
variants. Knowledge of the temperature rise in PIN
protection diodes is important because failure rates of
these devices dramatically increase if temperatures
exceed approximately 150 oC, with a potential loss of
patient and equipment protection
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1291. |
14T Dual-tuned RF Probes
for 13C/1H MRI Using Common-Mode Differential-Mode (CMDM)
Method
Hong Shang1, Xiaoliang Zhang1,2,
Yiran Chen1, Subramaniam Sukumar1,
Peder Larson1, Daniel B Vigneron1,2,
and Duan Xu1,2
1Radiology and Biomedical Imaging, University
of California San Francisco, San Francisco, CA, United
States, 2UC
Berkeley/UCSF Joint Bioengineering Program, San
Francisco, CA, United States
Double-tuned radiofrequency (RF) coils are critical for
multinuclear MR applications, with advantage of image
co-registration of proton anatomic images and
multinuclear metabolic images, and B0 shimming using
proton channel for low natural abundance heteronuclear
MRSI. In this work, a 14T double-tuned surface coil was
built based on the CMDM method, which has been proposed
for designing double-tuned RF coils with better
decoupling between channels and was demonstrated to
provide excellent performance and easy implementation at
7T. Bench tests and phantom imaging were performed and
demonstrated excellent decoupling between the two
channels, efficient impedance match, and independent
tuning.
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1292. |
Independent active
decoupling circuit for RX coil on MR systems without active
decoupling capabilities (0.2T) or with connecting issues
(3T).
Thomas Feuillet1,2, Herve Saint-Jalmes3,4,
Marie-Jose Seurin2, Michele Zani5,
Alejandro Bordelois6, and Olivier Beuf1
1Université de Lyon, CREATIS ; CNRS UMR 5220
; INSERM U1044 ; INSA-Lyon ; Université Lyon 1,
Villeurbanne, France, 2SARL
Cirma, Marcy l'Etoile, France, 3LTSI
; INSERM U1099, Université Rennes 1, Rennes, France, 4CRLCC,
Centre Eugene Marquis, Rennes, France, 5Agilent
Technologies, Oxford, United Kingdom, 6CBM,
Universidad de Oriente, Santiago, Cuba
Some MR systems do not provide an active decoupling bias
signal to RX coil and use only passive and/or
geometrical decoupling. An external circuit which
independently generates an active decoupling signal for
RX coils for any MR system was developed. The circuit
was tested on a 0.2T system with no active decoupling,
and at 3T to demonstrate its interest when an additional
dedicated RX coil is designed and its connection is
unknown or third part coil is not allowed. Results were
considered at both fields and were comparable to
reference decoupling methods, in terms of delays, SNR
and B1 uniformity.
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1293. |
Design of Flanged RF Shield
for Mitigation of RF and Gradient Coil Interactions
Muhammad Hassan Chishti1, Jean-Baptiste
Mathieu1, Joseph E Piel1, Desmond
T.B. Yeo1, Christopher J Hardy1,
Dominic Graziani1, and Seung-Kyun Lee1
1GE Global Research Center, Niskayuna, New
York, United States
Radio-frequency (RF) shields mitigate undesired
interactions between gradient coils and RF transmit
coils. RF losses in gradient windings can lower the Q of
the RF coil and result in increased power requirements.
In this work, we present full-wave electromagnetic
modeling and analysis of an end-flanged shield for use
with an asymmetric head gradient coil. Differences in B1
maps with and without the flanged shield indicate that
flanged shield is effective in ameliorating RF field
leakage to the gradient coils. Bench measurements also
show that Q of the RF coil improved from 50 (without
flanged shield) to 185 (with flanged shield).
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1294. |
Regional Faraday shielding
for improved dynamic hyperpolarized 13C
MRI
Cornelius von Morze1, Galen D Reed1,
Hong Shang1, Hsin-Yu Chen1, Lucas
Carvajal1, James Tropp2, Daniel B
Vigneron1, and Peder EZ Larson1
1Dept. of Radiology & Biomedical Imaging,
UCSF, San Francisco, CA, United States, 2GE
Healthcare, Fremont, CA, United States
We investigated the use of regional Faraday shielding to
help prevent loss of hyperpolarized 13C
magnetization due to premature excitation during tracer
delivery and recirculation about a primary region of
interest. The value of this approach was demonstrated in
simulations and hyperpolarized phantom experiments.
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1295. |
Cross-Validation of
Magnetic Resonance Elastography by Continuous Acoustic
Vibration and Ultrasound Elastography by Acoustic Radiation
Force Impulse: a Phantom Study
Mikio Suga1,2, Riwa Kishimoto2,
Atsuhisa Koyama1, Tetsuya Wakayama3,
Takayuki Obata2, and Hiroshi Tsuji2
1Chiba University, Chiba, Chiba, Japan, 2National
Institute of Radiological Sciences, Chiba, Chiba, Japan, 3GE
Healthcare Japan, Tokyo, Japan
For noninvasive evaluation of biomedical tissue
elasticity, magnetic resonance elastography (MRE) and
ultrasound elastography (USE) using acoustic radiation
force impulse (ARFI) have become common for use in
clinical practice. However, USE-ARFI has not yet been
compared with MRE. In this study, the quantitativity of
MRE and USE-ARFI (VTTQ) measurement was evaluated by
polyacrylamide phantoms. There was strong correlation
between MRE and rheometer, and VTTQ and rheometer. VTTQ
with 4 MHz convex probe showed higher standard
deviation, and VTTQ and MRE showed different depth
dependency. Therefore, we should consider of the
properties of each method.
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1296. |
Construction and Use of a
Micro Resolution Phantom for Small Bore MRI
Samuel Barnes1, Naomi Santa Maria1,
and Russell Jacobs1
1Biology, Caltech, Pasadena, CA, United
States
Despite their usefulness in quality assurance of high
resolution small bore systems, resolution phantoms with
feature sizes of 100um are not commercially available.
This works describes the design, manufacture, and use of
resolution phantoms with features in the 100um to 500um
range. These can be easily designed using CAD software
and manufactured using laser drilling techniques. This
provides a custom cost effective solution for labs to
perform testing on new or existing sequences.
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1297. |
A resistive heating system
for homeothermic maintenance in small animals.
Stuart Gilchrist1, Philip D Allen1,
John S Beech1, Veerle Kersemans1,
Paul Kinchesh1, Boris Vojnovic1,
and Sean C Smart1
1Gray Institute for Radiation Oncology and
Biology, Department of Oncology, University of Oxford,
Oxford, United Kingdom
Anaesthesia is usually required for the immobilisation
of animals for imaging. This induces a heat loss that
must be artificially offset. It is commonplace for warm
fluids (piped liquids or circulating air) to be used to
provide this heat but these systems require significant
space in which to circulate. We demonstrate a resistive
heating system that creates no discernible artefacts in
MR images or spectroscopy, and which requires no
additional space as it embedded within the animal
support cradle.
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1298. |
Development of an MRI
method for awake mouse imaging using soft immobilization and
a fast MR acquisition procedure
Shunsuke Kusanagi1, Kazunari Kimura1,
Makoto Hirakane1, Shigeto Iwamoto1,
Rikita Araki2, Sosuke Yoshinaga1,
and Hiroaki Terasawa1
1Faculty of Life Sciences, Kumamoto
University, Kumamoto, Japan, 2Bruker
Biospin K.K., Yokohama, Kanagawa, Japan
Mouse MRI studies facilitate the elucidation of the
pathogenic mechanisms underlying various diseases and
the appropriate medical treatments, due to the
remarkable advances in mouse genetic technology. It is
difficult to acquire accurate MR images when an imaging
target moves in the scanner, and thus treatment with
anesthesia and fixing apparatuses are usually required.
However, the brain activation profiles were reportedly
affected by anesthesia. To exclude the unfavorable
anesthetic effects, we successfully developed an
easy-to-operate method for awake mouse brain imaging,
which uses softer immobilization with clothes for mice
and a fast MR acquisition procedure, without surgery and
training.
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1299. |
Noncontact physiological
measurements using video recording inside an MRI scanner
Shang-Yi Yang1, Hsaio-Hui Huang1,
Chi-Wei Liang1, Shang-Yueh Tsai2,
and Teng-Yi Huang1
1National Taiwan University of Science and
Technology, Taipei, Taiwan, Taiwan, 2The
Graduate Institute of Applied Physics, National Chengchi
University, Taipei, Taiwan, Taiwan
This study attempts to use video recording as a tool for
physiology monitoring in an MRI scanner. During a
cardiac cycle, facial skin blood perfusion changes alter
optical path of ambient light emitted to the subject¡¦s
face. Using a conventional digital camera to capture the
changes of the reflected light and using ICA analysis to
remove other sources in light, we identify that this
method is feasible in a low-light MRI bore. This method
is an optic-based technique which avoids the problem
associated with switching gradient system.
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1300. |
MR-compatible normobaric
gas mixer for hypercapnic vasoreactivity studies on humans
L. Lamalle1,2, J.-B. Menut3, S.
Vergès4, J. M. Warnking5,6, and A.
Krainik7,8
1Inserm — US 17, Grenoble, France, 2Université
Grenoble Alpes — UMS IRMaGe, Grenoble, France, 3SMTEC,
Sport & Medical Technologies S.A., Nyon, Switzerland, 4Université
Grenoble Alpes — Laboratoire HP2, Grenoble, France, 5Inserm
— U836 (Équipe 5), Grenoble, France, 6Université
Grenoble Alpes — Grenoble Institut des Neurosciences,
Grenoble, France, 7Université
Grenoble Alpes — Faculté de Médecine, Grenoble, France, 8CHU
de Grenoble — Unité IRM, Grenoble, France
A normobaric gas mixer was developed to allow MR-based
hypercapnic vasoreactivity studies on humans. It
operates safely close to the magnet and can be remotely
computer controlled. Hypercapnic episodes with FiCO2 less
than 10 % can be programmed to chain in succession for
prescribed numbers of MR scanner trigger events. Device
performance is demonstrated in a cerebral BOLD
block-designed fMRI experiment.
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1301. |
3D printing of MRI
compatible components: Why every MRI research group should
have a low-budget 3D printer
Karl-Heinz Herrmann1, Clemens Gärtner1,
Martin Krämer1, Daniel Güllmar1,
and Jürgen R. Reichenbach1
1Medical Physics Group, Institute of
Diagnostic and Interventional Radiology I, Jena
University Hospital - Friedrich Schiller University
Jena, Jena, Germany
The capabilities of a current low budget 3D printer was
evaluated by designing and building a mouse head
fixation custom fitted to a dedicated recieve coil.
While the low budget 3D printing technology has not yet
outgrown some inherent problems like warping due to
thermal stresses, it was possible to build a fully
functional multipart mouse head fixation. The printing
material Polylactic Acid (PLA) is fully MRI compatible
as even its susceptibility is close to biological
tissue. We therefore consider a low budget 3D printer a
quite useful assessory for MRI labs.
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1302. |
Evaluation of an MR
compatible head fixation device using a custom-made 3D
printed frame in combination with a thermoplastic head mask
Daniel Güllmar1, Karl-Heinz Herrmann1,
Clemens Gärtner1,2, Nico Banz3,
Thomas G Wendt3, and Jürgen R Reichenbach1
1Medical Physics Group, Institute of
Diagnostic and Interventional Radiology I, Jena
University Hospital - Friedrich Schiller University
Jena, Jena, Germany, 2Medical
Engeneering and Biotechnology, University of Applied
Sciences, Jena, Germany, 3Department
of Radiotheraphy and Radiooncology, Jena University
Hospital - Friedrich Schiller University Jena, Jena,
Germany
Head fixation using a custom-made frame in combination
with a thermoplastic head mask was evaluated in terms of
repositioning accuracy as well as degree of
immobilization. In back-to-back scans regular fixation
using clamps performed equally well compared to mask
fixation. Repositioning accuracy using mask fixation was
found to be very high (< 0.2mm, < 0.2°). Under heavy
motion the degree of immobilization did not exceed 1.5
mm in translation and 1.5° in rotation. The approach can
be used to acquire MR scans which require minimal head
motion during very long scan times (e.g. DTI, fMRI,
Perfusion, high-res anatomy scans).
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1303. |
An MRI Compatible Surface
Scanner
Oline V. Olesen1,2, Jakob Wilm1,3,
Andre van der Kouwe2, Rasmus R. Jensen1,
Rasmus Larsen1, and Lawrence L. Wald2
1DTU Compute, Technical University of
Denmark, Lyngby, Denmark, 2Athinoula.
A. Martinos Center for Biomedical Imaging, Dept. of
Radiology, Massachusetts General Hospital,
Massachusetts, United States, 3Department
of Clinical Physiology, Nuclear Medicine & PET,
Rigshospitalet, University of Copenhagen, Denmark
We present the hardware design of an optical surface
scanner for in-bore applications. It is the first remote
structured light scanner that transmits projected
patterns onto the subject and captures their images
through optical fiber bundles. MPRAGE and EPI images of
a phantom were acquired with simultaneous surface
scanning. The system design was shown to be MRI
compatible and functional on the Siemens mMR Biograph.
This technology could be used for monitoring and
markerless tracking of surfaces e.g. real-time motion
correction feedback without the use of MR navigators or
optical markers.
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1304. |
Imaging in a Rotating
Frame: MRI without B0 Gradients
Steven M Wright1, Brian J Bass1,
and John C Bosshard1
1Electrical and Computer Engineering, Texas
A&M University, College Station, TX, United States
Spatial encoding with reduced reliance on Bo gradients
has always been an interest for specialized
applications. Some investigators have demonstrated
entirely replacing gradient encoding in one direction
and rotating a receiver coil at very high rates to
create a virtual array for RF spatial encoding. Here we
demonstrate early results from a novel planar imaging
technique for MR imaging that uses no gradients at all,
performing all spatial encoding by a combination of RF
encoding and rotating the object. The specific interest
here is the development of a simple, low-cost imaging
system that is robust to magnetic field homogeneity.
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TRADITIONAL
POSTER SESSION ○ MR ENGINEERING; MR SAFETY: SAFETY & BIOEFFECTS;
ULTRA-HIGH FIELD |
Array Coils & Systems
Monday 12 May 2014
Traditional Poster Hall |
16:30 - 18:30 |
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|
1305. |
Four Channel Transceiver
Array for Functional Magnetic Resonance Spectroscopy in the
Human Visual Cortex at 9.4 T
Andreas Pfrommer1, Nikolai Avdievich1,
and Anke Henning1,2
1Dept. of High-Field Magnetic Resonance, Max
Planck Institute for Biological Cybernetics, Tübingen,
Baden-Württemberg, Germany, 2Institute
for Biomedical Engineering, University and ETH Zürich,
Zürich, Switzerland
RF coils for functional magnetic resonance spectroscopy
at ultra-high field strength must be designed with high
SNR, high transmit efficiency and optimized to guarantee
SAR safety. With numerical EM simulations we compared
two possible 4 channel RF coil setups for the
application in the human visual cortex. It turned out
that overlapping loop elements can provide 12.5 % more
B1+ /√SAR(10g) than without overlap for this particular
case. Based on the simulation we have constructed a
tight fit 4-channel transceiver head phased array. We
could reach a B1+ of 63 µT in a 12.4x12.4 mm² sized
voxel in the visual cortex region in a human
head-and-shoulder phantom.
|
1306. |
Evaluation of ICE and
capacitive decoupling methods using in 8-channel loop array
coils at 7T
Xinqiang Yan1,2, Xiaoliang Zhang3,4,
Chuangxin Ma2, Long Wei2, and Rong
Xue1
1State Key Laboratory of Brain and Cognitive
Science, Beijing MRI Center for Brain Research,
Insititute of Biophysics, Chinese Academy of Sciences,
Beijing, Beijing, China,2Key Laboratory of
Nuclear Analysis Techniques, Institute of High Energy
Physics, Chinese Academy of Sciences, Beijing, Beijing,
China, 3Department
of Radiology and Biomedical Imaging, University of
California San Francisco, San Francisco, California,
United States, 4UCSF/UC
Berkeley Joint Graduate Group in Bioengineering, San
Francisco, California, United States
In this study, two eight-channel transmit/receive
volume-type loop array coils were built for human head
imaging at 7T by using the ICE decoupling method and
capacitive decoupling method, respectively. We have
conducted research on comparison between these arrays in
terms of S-parameter matrix, SNR and parallel imaging
capability. Compared with the capacitively decoupled
array, the ICE-decoupled array has better isolation
between adjacent coil elements, higher SNR at periphery
area and better parallel imaging capability.
Additionally, ICE decoupling method is more robust that
decoupling loops do not need to be retuned for different
loads.
|
1307. |
High SNR bilateral breast
MRI with a dual transmit, 26-channel receive RF coil with
simultaneous 31P
CSI at 7 tesla
Tijl A. van der Velden1, Michel Italiaander2,
Wybe J.M. van der Kemp1, Alexander Schmitz1,
Kenneth Gilhuijs1, Peter Luijten1,
Vincent O Boer1, and Dennis W.J. Klomp1
1Radiology, University Medical Center
Utrecht, Utrecht, Utrecht, Netherlands, 2MR
Coils, Drunen, Netherlands
Synopsis: Strong T1-weighted, high resolution dynamic
contrast enhance MR images are key in the detection of
breast cancer. Combined with phospholipid detection
using 31P Chemical Shift Imaging (CSI), the earlier
alterations in metabolism can be obtained using a novel
decoupling loop a bilateral breast coil was designed for
uncompromised 1H and 31P MR(S)I at 7 tesla enabling
increased spatial and temporal resolution with the 26 1H
receiver channels integrated in the coil. We demonstrate
high spatial and temporal resolution imaging and 31P CSI
in patients with breast cancer.
|
1308. |
Comparison of three
different microstrip transmit elements for use in
multichannel Tx/Rx body coils at 7 Tesla
Stephan Orzada1, Klaus Solbach2,
Mark E. Ladd1,3, and Andreas K. Bitz1,3
1Erwin L. Hahn Institute for MRI, Essen,
Germany, 2Institute
of Microwave and RF Technology, University of
Duisburg-Essen, Duisburg, Germany, 3Medical
Physics in Radiology, German Cancer Research Center (DKFZ),
Heidelberg, Germany
In this study three different elements are compared
regarding their suitability for large-diameter,
multi-element body coils at 7T: the centrally-fed
microstrip line2 (MSL), the centrally-fed microstrip
line with meanders3, and a new design where the meanders
of the aforementioned element are loaded with a
dielectric to eliminate the end capacitors. Comparison
is done through simulations and phantom experiments on
the single elements. The element with dielectrically
loaded meanders shows a more focused sensitivity then
the MSL or the meander element terminated with
capacitors, which might be beneficial for parallel
transmit and parallel reception.
|
1309. |
Optimization of B1 field
homogeneity along the longitudinal direction for 7T MTL
resonators by using a multi-row design
Xinqiang Yan1,2, Xiaoliang Zhang3,4,
Chuangxin Ma2, Long Wei2, and Rong
Xue1
1State Key Laboratory of Brain and Cognitive
Science, Beijing MRI Center for Brain Research,
Insititute of Biophysics, Chinese Academy of Sciences,
Beijing, Beijing, China,2Key Laboratory of
Nuclear Analysis Techniques, Institute of High Energy
Physics, Chinese Academy of Sciences, Beijing, Beijing,
China, 3Department
of Radiology and Biomedical Imaging, University of
California San Francisco, San Francisco, California,
United States, 4UCSF/UC
Berkeley Joint Graduate Group in Bioengineering, San
Francisco, California, United States
In this work, we used a double-row microstrip
transmission line (MTL) array by varying the termination
capacitance distribution to generate more homogeneous
B1+ field along longitudinal direction. The coupling
between elements of adjacent rows was reduced by using
the induced current compensation decoupling method.
Full-wave electromagnetic modeling was used to study and
compare the performances of the new design and the
conventional MTL resonator. The B1+ homogeneity
improvement along longitudinal direction was obvious and
this new design has also paved the way for similar
designs for human imaging.
|
1310. |
A hybrid
dielectric/birdcage double tuned volume resonator for high
field MRI
Sebastian Arnold Aussenhofer1, Paul de Bruin1,
and Andrew Webb1
1Radiology, C.J. Gorter Center for High Field
MRI LUMC, Leiden, Select, Netherlands
This work describes a new principle to build double
tuned volume resonators for high field human imaging by
combining a dielectric HEM mode resonator with a
birdcage coil. The dielectric resonator acts as the
proton transceiver (298 MHz at 7T); the birdcage acts as
the sodium transceiver (79 MHz at 7T). By inserting the
birdcage into the dielectric coil a double tuned volume
coil can be constructed if each of the birdcages rungs
is proton frequency trapped. The homogenous B1 fields of
the two resonators are preserved in the joint setup. A
resonator was constructed to acquire high resolution
proton and sodium images of the human wrist.
|
1311. |
An 8 channel Transceiver
phased array coil combined with a Surgical Robot for an MR
assisted Robotic surgery.
Seunghoon Ha1, Haoqin Zhu1, and
Labros Petropoulos1
1Research and Development, IMRIS Inc,
Minneapolis, MN, United States
To fully utilize Robotic assisted surgery in MR, it is
imperative that the RF coil design should be fully
integrated with a Head Fixation Device. The combination
of the RF coil, HFD, and Robotic surgery introduces
clinical requirements and needs that cannot be satisfied
with the design of a traditional RF coil that is
targeted for diagnostic MR Imaging. In this study, we
propose an new eight channel transceiver array coil that
is seamlessly integrated with an MR safe HFD and an MR
safe Robot by minimizing peak and average SAR, inside
the surgical field containing the RF field outside the
robot and optimizing image quality and SNR using EM
simulation results and verifying the results with
measurements on a prototype coil.
|
1312. |
Comparison of RF Resonators
Using Microstrip for Human Head at 3T
Hyeok-Woo Son1, Young-Ki Cho1, and
Hyoungsuk Yoo2
1Kyungpook National University, Daegu, Korea, 2University
of Ulsan, Ulsan, Korea
16-channel head coils using a variety of RF resonators
were tested on study participants at 3 Tesla, and the
penetrated RF magnetic fields were compared amongst four
different RF resonators in a spherical phantom. we
proposed using a 16-channel coil with a SIR with four
arms, and we compared it to other RF resonators based on
microstrip transmission lines. The 16-channel coil
provided better B1+ fields and can be effectively
controlled for parallel imaging in 3 Tesla MRI systems.
16-channel head coils using the SIR with four arms for
parallel imaging could be used in hospitals for higher
quality imaging.
|
1313. |
A novel design approach for
planar local transmit/receive antennas in 3T spine imaging
Johanna Schöpfer1, Klaus Huber1,
Stephan Biber2, Sebastian Martius1,
and Helmut Greim2
1Corporate Technology, Siemens AG, Erlangen,
Germany, 2Healthcare
Sector, Siemens AG, Erlangen, Germany
The human spine is one of the most frequently imaged
body parts in clinical MRI. The imaging performance can
be restrained by SAR restriction, B1+-inhomogeneities or
insufficient B1+-peak values. In the following an
optimized local transmit antenna structure for spine
imaging is presented which offers reduced SAR values,
improved B1+-inhomogeneity and reduced power
requirements in comparison to examination with the body
coil antenna. Following EM-simulations, the antenna
structure was manufactured and successfully integrated,
showing significant potential for future work in 3T MRI
imaging with local transmit coils.
|
1314. |
Design and Implementation
of Flexible Printed Receive Coils Arrays
Joseph Russell Corea1, Anita Flynn1,
Galen Reed1,2, Peter Shin2, Greig
Scott3, Ana Claudia Arias1, and
Michael Lustig1
1Electrical Engineering and Computer
Sciences, University of California, Berkeley, Berkeley,
California, United States, 2Radiology
and Biomedical Imaging, University of California, San
Francisco, San Francisco, California, United States, 3Electrical
Engineering, Stanford, Stanford, California, United
States
Creating receive coil arrays using ultra-high quality
components is the standard method of fabrication for
arrays today. However, concessions can be made trading
off excess quality factor for a more conformable device
using screen printed materials. This is possible because
in clinical scanners, the system is body noise dominated
so lowering the quality factor of the coil does not
necessarily lower the signal-to-noise ratio of the
image. Here we discuss the implications of using printed
materials for creating receive coil arrays and include a
demonstration of a 4-channel fully printed prototype on
different areas of a volunteer.
|
1315. |
A 64-Channel Cardiac
Receive-Only Phased Array Coil for Cardiac Imaging at 3T
Mark Schuppert1, Boris Keil2,
Bastien Guerin2, Stefan Fischer1,
Robert Rehner3, Lawrence L. Wald2,4,
and Laura M. Schreiber1
1Section of Medical Physics, Department of
Radiology, University Medical Center of the Johannes
Gutenberg University, Mainz, Germany, 2A.A.
Martinos Center for Biomedical Imaging, Department of
Radiology, Massachusetts General Hospital, Charlestown,
MA, United States, 3Siemens
AG, Healthcare Sector, Erlangen, Germany, 4Harvard
Medical School, Boston, MA, United States
A 64-channel cardiac receive-only phased array prototype
coil was built. We show its use for accelerated imaging
(tGRAPPA, acceleration factors R = 3, 5, 7, and 8) in
comparison to a 38-channel commercial coil setup (Body
18/Spine 32 Tim coils). Compared to the commercial coil
setup, the achieved center SNR with the 64-channel coil
was 6% less using optimally combined complex data in
phantom measurements. Nonetheless, at R = 7 mean noise
amplification in phantom measurements was 50% less with
the new coil. In vivo image quality was superior with
the 64-channel cardiac phased array coil at R=5 and R=7.
|
1316. |
Non-resonance 16-element
transceiver array for human head imaging at 7T
Yong Pang1 and
Xiaoliang Zhang1,2
1Radiology and Biomedical Imaging, University
of California San Francisco, San Francisco, CA, United
States, 2UC
Berkeley/UCSF Joint Bioengineering Program, CA, United
States
Decoupling issue is a challenging problem in transceiver
array designs at high fields. The Non-resonance RF
method (NORM) using traveling wave provides a promising
way to alleviate this problem and also has
multi-frequency excitation and reception capability. In
this work, a 16-element transceiver NORM array for 7T
human head imaging is modeled and simulated using FDTD
method. The unmatched decoupling and excellent g-factors
were achieved, indicating the feasibility of parallel
imaging using the proposed NORM array. The same NORM
array is able to perform multinuclear excitation and
detection, such as C13 and P31, which is verified by
FDTD simulation.
|
1317. |
A Double-Row Transmit Array
with Broadband Sheath-Wave Damping for 7T Human Head Imaging
Roland Müller1, Andreas Schäfer1,
Debra S. Rivera1, Robert Turner1,
and Harald E. Möller1
1Max Planck Institute for Human Cognitive and
Brain Sciences, Leipzig, Germany
Goal of the project was to design an eight-element,
double-row, transmit RF array coil for imaging of human
heads at 7T. Both rows should be tuned independently
using the reflected power minimization approach. At high
fields, the common mode problem is presenting a source
of loss as well as a potential safety issue. This was
addressed by a PCB based 3D coil structure. The
combination of balanced feeding, balanced feed lines and
resistor-bypassed line shield gaps was sufficient to
eliminate sheath waves and hand effects. No conventional
traps were required. A good longitudinal coverage of B1+
field can be shown.
|
1318. |
Effects of Co-Planar
Element Shielding on Array Performance at 7T
Samantha By1, Joseph V. Rispoli1,
Ivan Dimitrov2,3, Sergey Cheshkov2,4,
Craig Malloy2,4, Steven M. Wright1,5,
and Mary Preston McDougall1,5
1Biomedical Engineering, Texas A&M
University, College Station, TX, United States, 2Advanced
Imaging Research Center, University of Texas
Southwestern Medical Center, Dallas, TX, United States, 3Philips
Medical Systems, Cleveland, OH, United States, 4Radiology,
University of Texas Southwestern Medical Center, Dallas,
TX, United States,5Electrical and Computer
Engineering, Texas A&M University, College Station, TX,
United States
At higher field strengths, shielding of RF coils to
mitigate radiation losses becomes increasingly
necessary. In an array configuration, however, shielding
individual elements can be complex, particularly when
the elements are overlapped for geometric decoupling.
This work presents the benefits of a co-planar shielding
configuration of the elements of an overlapped array at
7T. Compared to the unshielded array, the shielded array
provided a 39% improvement in mean SNR throughout the
entire phantom, an average decrease in mean g-factors
for all three views of 8.9%, and a lower power setting
required to produce a 90 degree tip angle.
|
1319. |
Replacing Individual Baluns
with Quarter Wavelength Baluns in Multi-Channel Arrays
Thomas Grafendorfer1, Greig Scott2,
Paul Calderon3, Fraser Robb4, John
Pauly2, and Shreyas Vasanawala5
1Advanced Coils, GEHC Coils, Stanford, CA,
United States, 2Electrical
Engineering, Stanford University, CA, United States, 3Engineering
consultant, Stanford Radiology, CA, United States, 4Advanced
Coils, GEHC Coils, OH, United States, 5Radiology,
Stanford University, CA, United States
Baluns and cable traps are widely used in coil arrays to
prevent common mode currents on cables and feeding lines
that can severely impact coil performance. But this
approach is often done in a trial and error fashion;
arbitrarily moving and adding Baluns until the coil
somehow works. Here we show a more controlled approach,
where ground loops formed by cables are purposely set to
hold certain resonance frequencies. In that case
individual Baluns can be replaced with quarter
wavelength Baluns, which is noting else than shorting
individual cable shields together at the right location.
|
1320. |
Four Element Endorectal
Array Coil for Improved Sensitivity in Human Prostate
Imaging
Ronald D Watkins1 and
Kim Butts Pauly1
1Radiology, Stanford University, Stanford,
CA, United States
We have designed, built, and tested a miniature four
element linear surface coil array for high resolution
imaging of human prostate. The prototype coil has
demonstrated a factor of 2 increase in SNR near the
array, over a single coil equal to the size of the
array. In addition it is possible to perform parallel
imaging with this array.
|
1321. |
Design of a 96-Channel
Bilateral Prone Breast Array for High Performance Parallel
MRI
Mike J Smith1 and
Scott B King1
1National Research Council of Canada,
Winnipeg, Manitoba, Canada
We investigate SNR and parallel imaging limits of prone
positioned MR breast imaging by evaluating different
96-Channel receive array coils. We show that the
96-Channel array has SNR and g-factor capabilities that
allow 3x faster breast MRI than currently available with
16-Channel coils.
|
1322. |
An eight-channel
transmit/receive phased-array head coil with an ICE
decoupling method at 7T
Xinqiang Yan1,2, Xiaoliang Zhang3,4,
Chuangxin Ma2, Long Wei2, and Rong
Xue1
1State Key Laboratory of Brain and Cognitive
Science, Beijing MRI Center for Brain Research,
Insititute of Biophysics, Chinese Academy of Sciences,
Beijing, Beijing, China,2Key Laboratory of
Nuclear Analysis Techniques, Institute of High Energy
Physics, Chinese Academy of Sciences, Beijing, Beijing,
China, 3Department
of Radiology and Biomedical Imaging, University of
California San Francisco, San Francisco, California,
United States, 4UCSF/UC
Berkeley Joint Graduate Group in Bioengineering, San
Francisco, California, United States
In this work, an eight-channel transmit/receive loop
array with induced current elimination (ICE) decoupling
method was built and investigated to demonstrate its
feasibility and robustness for human head imaging at 7T.
This array has been validated through bench tests and
in-vivo human head MR imaging experiments. Isolation
between the adjacent loop elements is better than -25dB
by employing this new design. The ICE-decoupled array
also shows excellent parallel imaging capability that
the average g-factor of human head in the sagittal plane
was as low as 1.14 when acceleration factor achieves 4.
|
1323. |
An 8-Channel Integrated
Balun Phased Array (IBPA) for Small Anatomical Features
Wolfgang Loew1, Randy O. Giaquinto1,
Brynne Williams1, J. Matthew Lanier1,
Christopher Ireland1, Ronald Pratt1,
and Charles Dumoulin1
1Imaging Research Center, Cincinnati
Children's Hospital Medical Center, Cincinnati, Ohio,
United States
A 3 Tesla 8-channel receive phased array for small
anatomical features is presented in this abstract. The
array uses a novel coil design integrating a balun into
each coil element. Coupling and matching was assessed
through network analysis. High-resolution imaging
experiments were performed on a phantom and human
fingers confirming high image quality and proof of
concept.
|
1324. |
Prototype 8-Channel
Parallel Transmit Body Array in a Clinical 3T System
Wei Luo1,2, Christopher T. Sica1,
YeunChul Ryu3, Yang Qing1, and
Christopher M. Collins4
1Radiology, Pennsylvania State University,
Hershey, PA, United States, 2Engineering
Science & Mechanics, Pennsylvania State University,
University Park, PA, United States,3Samsung,
Korea, 4Radiology,
New York University, New York, NY, United States
A prototype of an eight-channel transmit array which can
be inserted into a commercial 3T system above the
patient bed and used with commercial receive-only arrays
was designed and implemented based on our previous
studies. This design benefits from the signal-to-noise
ratio offered by the commercial receive-only array and
restricts the geometry and placement of the array
elements. Here, we report progress on this prototype,
including its implementation, preliminary shimming
result on phantom, and its very first in vivo images.
|
1325. |
An Optimized 8-Channel
Helmet Array for Head Imaging at 6.5 mT
Cristen D LaPierre1,2, Lawrence L Wald1,3,
and Matthew S Rosen1,2
1Department of Radiology, A.A. Martinos
Center for Biomedical Imaging, Charlestown, MA, United
States, 2Department
of Physics, Harvard University, Cambridge, MA, United
States, 3Harvard-MIT
Division of Health Science and Technology, Cambridge,
MA, United States
A low-field imager offers a potentially transportable
and rapidly deployable human imaging system without many
of the system requirements of typical scanners. The aim
of this study was to construct an 8-channel receive-only
helmet array for imaging the human brain. The helmet was
3D printed. Coils consisted of 4x12 cm and 4x14 cm
loops, each with 30 turns of 24 AWG copper wire.
Geometric decoupling between nearest neighbors was at
least -30 db while next nearest neighbors was -6 dB.
Future work will compare parallel imaging to incoherent
random undersampling and SENSE.
|
1326. |
Performance comparison of a
form fitted coil array vs. a quadrature birdcage coil for 31P
MRS studies in the human calf at 7T
Sigrun Goluch1,2, Andre Kuehne1,2,
Ewald Moser1,2, and Elmar Laistler1,2
1MR Center of Excellence, Medical University
of Vienna, Vienna, Vienna, Austria, 2Center
for Medical Physics and Biomedical Engineering, Medical
University of Vienna, Vienna, Austria
This work compares the performance of a 3 channel
transceive 31P
surface coil with a comparable sized 16-leg birdcage for
the application in 31P
localized spectroscopy experiments in the human calf at
7T with 3D electromagnetic simulation. B1+ as
well as SNR calculation for a comprehensive
investigation is presented for both designs, showing
higher B1+ and
SNR in the regions of interest for the surface coil,
while as expected the birdcage exhibits better
homogeneity. Since the ROIs are small voxels the
advantage of better homogeneity is of minor importance
compared to high sensitivity in terms of B1+ and
SNR.
|
1327. |
Inverse RF Array Head Coil
Design for MRI-LINAC System
Yimeng Wang1, Yu Li1, Feng Liu1,
Ewald Weber1, Hector Sanchez Lopez1,
and Stuart Crozier1
1School of ITEE, University of Queensland,
Brisbane, Queensland, Australia
This paper focuses on the theoretical inverse design of
cylindrical head RF phased array coils applied in the
Magnetic Resonance Imaging Linear accelerator
(MRI-Linac) system. A MRI-Linac system is the
combination of cancer detection and real time, image
guided radiotherapy. In this work, a RF phased-array
coils with gaps are designed. Those gaps provide easy
access for the accelerator without any disturbance, and
multiple receiver coils can realize the fast imaging
requirements. The simulation results show that
homogeneous magnetic field within a given region of
interest (ROI) can theoretically be achieved by the new
designed coil.
|
1328. |
Spatial Normalization Can
Morph RF Coils into Geometries Optimized for fcMRI Studies
in Specific Brain Regions
Iain P Bruce1, L Tugan Muftuler2,3,
and Daniel B Rowe1,2
1Mathematics, Statistics and Computer
Science, Marquette University, Milwaukee, WI, United
States, 2Biophysics,
Medical College of Wisconsin, WI, United States, 3Center
of Imaging Research, Medical College of Wisconsin, WI,
United States
Many degenerative brain disorders are commonly
associated with specific regions of the brain that are
often off-center and can reside within aliased regions
prior to a SENSE reconstruction. While a conventional
array of rectangular coils may generate the most uniform
magnetic field sensitivities throughout the brain, the
human brain is not symmetric, and such sensitivities may
not be optimal for fcMRI studies in all regions. This
study proposes an approach of using spatial
normalization together with an iterated conditional
modes algorithm to morph an array of rectangular coils
into a geometry that is more optimal for a specific ROI.
|
1329. |
Numerical analysis of a
four channel array with intrinsically dual tuned single
element antennas providing a congener resonant behavior for
combined 23Na/1H
MRI at 7T
Jan Taro Svejda1, Daniel Erni1,
and Andreas Rennings1
1General and Theoretical Electrical
Engineering (ATE), University of Duisburg-Essen,
Duisburg, NRW, Germany
An intrinsically dual tuned single element antenna
providing a congener resonance behavior is utilized
within a four channel setup for combined 23Na and 1H MRI
at 7T. The antenna is based on the composite
right-/left-handed transmission line technique with
short circuited line terminations. The array shows a
homogeneous B1-field distribution for both resonances
while the specific absorption rate is evenly distributed
along the antennas.
|
1330. |
Static shim optimization of
7T dual row arrays
Mikhail Kozlov1, Nicolas Boulant2,
and Robert Turner1
1Max Planck Institute for Human Cognitive and
Brain Sciences, Leipzig, Saxony, Germany, 2CEA,
DSV, I2BM, NeuroSpin, UNIRS, Saclay, France
|
1331. |
Cartesian Feedback
Configuration with Direct RF Signal Injection for Power
Amplifier Linearization at 1.5T MRI
Jonathan Y Lu1, Pascal P. Stang1,
John M. Pauly1, Marta G. Zanchi2,
and Greig C. Scott1
1Dept of Electrical Engineering, Stanford
University, Stanford, CA, United States, 2School
of Medicine, Stanford University, Stanford, CA, United
States
We demonstrate a modified version of Cartesian feedback,
an RF power amplifier linearization technique, for use
at 1.5T. In this feedback configuration, the MRI RF
signal is directly injected at a point in the feedback
loop that allows us to eliminate the initial
down-converter needed to convert the MRI signal to
baseband or intermediate frequency. Amplifier
linearization is important especially in multichannel
transmit where unpredictable coil loading conditions can
affect amplifiers in the stage before, while this
particular arrangement allows appreciable components
savings and simplification in architecture when multiple
coils are used.
|
1332. |
B1+ distortion by residual
currents in decoupled Receive arrays
Ed B Boskamp1 and
David M Goldhaber1
1Engineering, GE Healthcare, Waukesha, WI,
United States
Whole body RF transmit coil B1+ uniformity distortion
due to residual currents in receive arrays is being
studied. Complex arrays may be decoupled from B fields
at first glance, but currents can still be induced in
the copper traces by E fields and by B fields in loops
that are not apparent but do exist due to parasitics.
Proper placement of the blocking networks is crucial to
minimize currents in the array and thus B1+ distortion.
|
1333. |
Simultaneous Deep-local
Hyperthermia and 1.5T MR Imaging – an Experimental Systems
Interactions Study
Matthew Tarasek1, Tomas Drizdal2,
Ruben Pellicer2, Wouter Numan2,
Paolo Togni2, Gyula Kotek2, Gerard
van Rhoon2, Maarten Paulides2, and
Desmond Yeo1
1MRI, GE global research, Niskayuna, NY,
United States, 2Erasmus
Medical Center, Netherlands
The MRlabcollar was designed as a magnetic resonance
(MR)-compatible array for simulation guided conformal
radiofrequency (RF) hyperthermia treatment of head and
neck (H&N) tumors. Here we present a comprehensive
characterization of interactions between the MRI scanner
and MRlabcollar to analyse MR image quality, especially
with simultaneous operation of both RF sub-systems. We
characterize image SNR, the relative B1+ uniformity, B0
distortion due to placement of the array, and
phase-difference MR thermometry (MRT) maps acquired
during RF transmit from the array. Results show that
concurrent heating and imaging is feasible with no
significant adverse effects on image quality.
|
1334. |
Analysis of Gain and Noise
Relationship in RF Feedback Power Amplifier Linearization
for Use at 1.5T MRI
Jonathan Y Lu1, Pascal P. Stang1,
John M. Pauly1, Marta G. Zanchi2,
and Greig C. Scott1
1Dept of Electrical Engineering, Stanford
University, Stanford, CA, United States, 2School
of Medicine, Stanford University, Stanford, CA, United
States
We analyze the possibility of improving noise in an RF
Cartesian feedback system, a power amplifier
linearization technique, for use at 1.5T MRI. This
involves reducing the amount of attenuation in the
feedback path without changing the open loop gain of the
system and would entail essentially moving the RF input
location in our feedback loop. While gain was reduced,
we observed a reduction in noise for the same output
voltage. This suggests that by driving a closed loop
system with reduced gain at higher input power, we could
achieve a linear output with reduced noise.
|
1335. |
Investigating interactions
between a TMS system and a novel MR device for concurrent
TMS/fMRI experiments
Lucia Isabel Navarro de Lara1,2, Christian
Windischberger1,2, Jürgen Sieg1,2,
Ewald Moser1,2, Elmar Laistler1,2,
and Andre Kuehne1,2
1Center for Medical Physics and Biomedical
Engineering, Medical University of Vienna, Vienna,
Vienna, Austria, 2MR
Center of Excellence, Medical University of Vienna,
Vienna, Vienna, Austria
A dedicated 7-channel MR coil was built for concurrent
TMS/fMRI Studies. The developed hardware can be placed
under the TMS due to the ultra-slim design in the
middle, ensuring efficient TMS stimulation and
performing a very high SNR at a target depth up to 6 cm.
With these satisfactory results, it had to be shown that
the functionality of neither the novel MR head coil or
the TMS system when working in combination was affected.
The possible interactions of the dedicated MR coil on
the TMS device and vice versa were the focus of this
work.
|
1336. |
A method to calculate the
noise factor of the receive coil matching network
Xueming Cao1, Elmar Fischer1, Jan
G Korvink2, Jürgen Hennig1, and
Maxim Zaitsev1
1Department of Radiology, University Medical
Center Freiburg, Freiburg, Germany, 2Institute
of Microsystem Technology, Freiburg, Germany
In ordinary MRI experiments using local receive coil,
major noise sources in signal reception are the sample
and the preamplifier. However, as the sizes of
individual coil elements becomes smaller, noise
contribution from the coil matching network needs to be
taken into account. Here, we present a method to
calculate the noise factor of coil matching network.
Approximations are also developed to allow the
estimation of a coil matching network noise factor on
the RF bench. Based on the calculations, a method to
reduce the coil matching network noise factor is
presented.
|
1337. |
New matching networks for
coil and preamplifier
Xueming Cao1, Maxim Zaitsev1,
Jürgen Hennig1, Jan G Korvink2,
and Elmar Fischer1
1Department of Radiology, University Medical
Center Freiburg, Freiburg, Germany, 2Institute
of Microsystem Technology, Freiburg, Germany
Based on the assumption that the sample and preamplifier
are the dominant noise sources for MRI, the coil loop is
matched to 50 Ohm through a coil matching network and
the preamplifier is noise matched to 50 Ohm too, through
another matching network. However, with receiving coils
in an array becoming increasingly smaller, the noise
contributed from their matching networks cannot be
neglected. Here we present two methods to simplify the
coil and preamplifier matching networks, therefore their
noise contribution is reduced
|
1338. |
Automatic matching of
transmit arrays with optically controlled capacitors
Giorgos Katsikatsos1 and
Klaas Paul Pruessmann1
1Institute for Biomedical Engineering, ETH
Zurich, Zurich, Zurich, Switzerland
A closed-loop controlled matching for Tx-arrays for a 7T
scanner has been implemented as an autonomous system to
react to load changes in various stages of an MR
experiment. Building blocks of the system are the
L-matching networks, built from custom low-loss
capacitors actuated by piezoelectric motors, controlled
by an external computer. The feedback is provided by a
network analyzer which triggers the re-matching
procedure. The matching algorithm is based on previous
knowledge about the matching circuit connected to the
array and uses common objective functions to detect the
best matching settings for arbitrary loads.
|
1339. |
A Fully Integrated
Automatic Tune and Match System for an 8-Channel
Transmit/Receive Cardiac TEM Array at 7T: Initial Results in
a Phantom and Volunteers
Graeme A Keith1, Christopher T Rodgers1,
Aaron T Hess1, Carl J Snyder2, J
Thomas Vaughan2, and Matthew D Robson1
1Oxford Centre for Clinical Magnetic
Resonance Research, University Of Oxford, Oxford,
Oxfordshire, United Kingdom, 2Center
for Magnetic Resonance Research, University of
Minnesota, Minneapolis, Minnesota, United States
Results in both a saline phantom and in humans are
presented for an auto-tune system using piezoelectric
actuators and MATLAB control. The system was implemented
on an 8-channel pTx cardiac TEM array for use at 7T. A
rigorous performance evaluation algorithm was run on the
phantom and found that in the majority of cases the S11 was
significantly improved by the system. The system was
then employed on human subjects, and it was found that
it could successfully tune on a person in a maximum of 6
minutes. The system is now in routine use in our lab.
|
1340. |
Single Configuration of
Coil and High-Permittivity Material Improves Performance for
a Wide Range of Subjects
Christopher M. Collins1 and
Qing X. Yang2
1Bernard and Irene Schwartz Center for
Biomedical Imaging, Department of Radiology, New York
University School of Medicine, New York, NY, United
States, 2Radiology,
The Pennsylvania State University, PA, United States
Using numerical simulations, we explore the potential of
a single high-permittivity receive head coil former to
improve performance of a large encircling transmit array
at 7T for six different human subjects with a wide range
in size and morphology. This is important to demonstrate
the possibility of incorporating HPMs into arrays for
high-throughput, high performance MRI. The ability to
perform RF shimming with the large volume array was not
adversely affected by the presence of the
high-dielectric former in any of the subjects and the
former greatly improved efficiency and homogeneity of
the transmit array for all subjects.
|
1341. |
Improvement of parallel
imaging using high permittivity material (HPM) -
demonstration with liver imaging at 3T
Zhipeng Cao1, Wei Luo2, Sebastian
Rupprecht3, Christopher Sica3,
Michael Lanagan2, Christopher M. Collins4,
and Qing X. Yang3
1Institute of Imaging Science, Vanderbilt
University, Nashville, TN, United States, 2Engineering
Science and Mechanics, Penn State University, University
Park, PA, United States, 3Radiology,
Penn State University, Hershey, PA, United States, 4Radiology,
New York University, New York, NY, United States
Experimental demonstration of using HPM to improve
parallel imaging on liver imaging at 3T. The HPM
resulted in smaller g-factor loss and more SNR
preservation with high data undersampling factors.
|
1342. |
Approaching Ultimate SNR:
Comparison of Composite and Surface Coil Arrays
Adam Maunder1, Mojgan Daneshmand1,
Pedram Mousavi1, B. Gino Fallone2,
and Nicola De Zanche2
1Electrical and Computer Engineering,
University of Alberta, Edmonton, Alberta, Canada, 2Oncology,
University of Alberta, Edmonton, Alberta, Canada
It has been shown that at high MRI frequencies current
patterns other than those provided by surface coils are
required to approach the ultimate SNR. SNR improvements
in realistic arrays become limited due to noise from
coils and matching networks in large arrays. Arrays of
three orthogonal coils are naturally decoupled, provide
complementary sensitivities and allow the use of larger,
body loss dominated, coils. Simulations of large 18-,
36- and 54-element arrays composed of composite and
surface coils are compared in terms of SNR and parallel
imaging performance. Noise contributions from the coil,
matching networks and preamplifiers are included for a
realistic comparison.
|
1343. |
Active optical-based
decoupling circuit for receiver endoluminal coil
Reina Ayde1, Raphael Sablong1,
Gwenael Gaborit2,3, Lionel Duvillaret3,
Anne-Laure Perrier1, and Olivier Beuf1
1CREATIS - CNRS UMR 5220 – INSERM U1044,
University of Lyon 1, Villeurbanne, Rhone-Alpes, France, 2IMEP-LAHC
UMR 5130, University of Savoie, Rhone-Alpes, France,3Kapteos,
Rhone-Alpes, France
The use of metallic coaxial cables in MRI could induce
local high Specific Absorption Rate. Optical fiber link
could be an alternative to coaxial cables to ensure
patient safety. In order to assure a complete optical
endoluminal receiver coil, an optical system for
decoupling the receiver coil was made. The MRI for a
phantom of ionized water was taken with three
endoluminal coils with different decoupling system:
classical, optical and without decoupling system. The
SNR and the uniformity of signal distribution were
studied and compared. The results show that the
decoupling system works perfectly and does not induce
field inhomogeneity.
|
|
|
|
TRADITIONAL
POSTER SESSION ○ MR ENGINEERING; MR SAFETY: SAFETY & BIOEFFECTS;
ULTRA-HIGH FIELD |
Non-Array RF Coils, Dielectrics & Waves
Monday 12 May 2014
Traditional Poster Hall |
16:30 - 18:30 |
|
|
1344. |
A susceptibility matched
endorectal coil design suited for the MRS examination of the
rectal wall
Jean-Marie Verret1,2, Frank Pilleul3,4,
Cécile Rabrait2, and Olivier Beuf1
1Université de Lyon; CREATIS; CNRS UMR 5220;
Inserm U1044; INSA-Lyon; Université Lyon 1,
Villeurbanne, France, 2General
Electric Healthcare, Buc, France, 3Hospices
Civils de Lyon; Département d’imagerie digestive; CHU
Edouard Herriot, France, 4Centre
Léon Bérard - Centre de Lutte contre le Cancer, France
A susceptibility matched endorectal coil was tested and
compared against a classical endorectal coil design. For
different phantom angulations, it enabled a significant
decrease (~30%) of the FWHM of spectra acquired on in
vitro NMR tubes. These promising results and the
restricted FWHM observed suggest the interest of this
new coil for the acquisition of in vivo spectra
especially for the characterization of the colorectal
cancer.
|
1345. |
Endoluminal MRI coils for
mice rectal wall assessment
Hugo Dorez1, Raphaël Sablong1,
Laurence Canaple2, Sophie Gaillard1,
Driffa Moussata3, and Olivier Beuf1
1Université de Lyon, CREATIS CNRS UMR 5220 –
INSERM U1044 – INSA Lyon 1, Villeurbanne, Rhône-Alpes,
France, 2Institut
de Génomique Fonctionnelle de Lyon, Université de Lyon
1, UMR 5242 CNRS, Ecole Normale Supérieure de Lyon,
Lyon, Rhône-Alpes, France, 3Service
hépato-gastroentérologie, Hospice Civil Lyon Sud,
Pierre-Bénite, Rhône-Alpes, France
The purpose of this project research is to assess mice
rectum wall using MRI combined with endomicroscopy and
conventional endoscopy. Endoluminal MRI coils with
active decoupling circuit were developed and
characterized on phantoms. Then, in-vivo examination was
finally done on mice (c57 black6j). Endoluminal coils
improve significantly the local SNR compared to body
mice volume birdcage coil. Rectal wall layers are better
visualized due to improved spatial resolution achieve
with SNR gain. This study shows the feasibility to use
small endoluminal coils for mice rectal wall assessment
and opens perspectives to better understand rectal
pathologies.
|
1346. |
Double-Resonant 13C/1H
Coil System for {1H} 13C
in vivo NMR Spectroscopy on a 7-T Whole-Body MR Tomograph
Tanja Platt1, Andreas Korzowski1,
Reiner Umathum1, and Peter Bachert1
1Medical Physics in Radiology, German Cancer
Research Center, Heidelberg, Baden-Württemberg, Germany
13C NMR spectroscopy enables a noninvasive
quantification of various metabolites in vivo (without
or with an enrichment of 13C)
and takes advantage of high B0 and
of 1H-decoupling.
The aim of this study was to design, implement and test
a surface coil system for in vivo 1H-decoupled 13C
NMR spectroscopy on an experimental 7-T whole-body MR
tomograph. The use of a transmission line resonator
concept with special frequency selective filter circuits
ensures sufficient electromagnetic decoupling for both
frequencies (13C, 1H).
The resulting coil system allows among other
applications the acquisition of high resolution 1H-decoupled 13C
NMR spectra in vivo.
|
1347. |
A variable diameter
resonator for high field proton and sodium musculoskeletal
MRI
Sebastian Arnold Aussenhofer1, Paul de Bruin1,
and Andrew Webb1
1Radiology Leiden University Medical Center,
C.J. Gorter Center for High Field MRI, Leiden,
South-Holland, Netherlands
A variable-diameter birdcage resonator has been
constructed for sodium imaging of the knee at 7 Tesla
(78.85 MHz) in order to optimize sensitivity for
different patient sizes. Anatomical proton data are
acquired using two microstrip lines (tuned to 298 MHz)
mounted on the inside of the shield of the variable
diameter birdcage. The diameter of the birdcage can be
varied between 13.5 and 18 cm. Co-registered proton and
sodium images have been acquired from three volunteers
ranging from a large male subject to a small female one.
|
1348. |
Novel RF-coil assembly to
simultaneously investigate fMRI and electrophysiology in
non-human primates in a large bore vertical magnet
Jozien Goense1,2, Michael Beyerlein2,
Jens Hoffmann2, Gunamony Shajan2,
Thomas Steudel2, Klaus Scheffler2,3,
Nikos Logothetis2,4, and Hellmut Merkle5
1University of Glasgow, Glasgow, United
Kingdom, 2Max-Planck
Institute for Biological Cybernetics, Tuebingen,
Germany, 3University
of Tuebingen, United Kingdom, 4University
of Manchester, United Kingdom, 5National
Institutes of health, MD, United States
RF-coil design for combined electrophysiology and fMRI
in non-human primates is challenging because any coil
design needs to be sufficiently open to allow for
electrode access to the brain. Patch antennas allow for
a more open design, but since our bore is too small for
a 300 MHz traveling wave, we developed an open
quadrature transmit coil/antenna placed in-situ. The
transmit coil/antenna is capable of producing a
sufficiently homogenous B1 field. This device can be
used alone in transceiver mode or in combination with
dedicated receive arrays which allow for maximum
flexibility while maintaining a very high SNR.
|
1349. |
A Circularly-Polarized Dual
Litz RF Coil for High-Throughput Eight Whole Mouse Head
Samples
Dung Minh Hoang1, Evelyn B Voura1,
and Youssef Zaim Wadghiri1
1Radiology, NYU - School of Medicine, New
York, New York, United States
In this work, we aimed to increase the throughput of ex
vivo samples during overnight unattended sessions by
designing a coil and setup accommodating up to eight
whole mouse heads. Using our single channel MRI
installation equipped with a gradient insert with a
60-mm diameter spherical volume (DSV), we considered a
design based on the use of commonly accessible off-the
shelf supplies and ease of sample preparation. Among the
various structures examined, a dual litz structure
electrically-fed through the mid-point of the rung
proved to be the most electrically balanced and
homogeneous coil throughout the length of the rung.
|
1350. |
A target-field design of
open multi-purpose coil for musculoskeletal MR imaging at 3T
Rui Zhang1, Qunzhi Chen2, Hongyang
Yuan3, Wenchao Cai4, Kai Zhao4,
Jue Zhang1,2, Xiaoying Wang2,4,
and Jing Fang1,2
1College of Enigneering, Peking University,
Beijing, Beijing, China, 2Academy
for Advanced Interdisciplinary Studies, Peking
University, Beijing, Beijing, China, 3Department
of Radiology, The University of North Carolina at Chapel
Hill, Chapel Hill, North Carolina, United States, 4Department
of Radiology, Peking University First Hospita, Beijing,
Beijing, China
MRI plays an important role in diagnosing the diseases
of musculoskeletal tissues at different body parts. In
this study, based on the target-field method, we
proposed a kind of open multi-purpose RF coil with
three-plane structure for musculoskeletal MR imaging
with satisfied homogeneity and high SNR. The design can
meet the need of various body parts and provide large
joint movement region for dynamic evaluation. The
imaging results have demonstrated the effectiveness and
advantage of this proposed design. In the near future,
it is believed that the coil can be applied for
real-time imaging of joint movement under dynamic
situations.
|
1351. |
Ladder-design volume coil
with good uniformity and signal to noise for hyperpolarised 13C
investigations of animals on a 3T clinical system
Deborah K. Hill1,2, Craig Cummings1,
Jessica K. R. Boult1, Matthew R. Orton1,
Yuen-Li Chung1, Thomas R. Eykyn1,3,
Martin O. Leach1, David J. Collins1,
and Rafal Panek1
1CR-UK and EPSRC Cancer Imaging Centre, The
Institute of Cancer Research and Royal Marsden NHS
Trust, Sutton, Surrey, United Kingdom, 2Department
of Circulation and Medical Imaging, NTNU, Trondheim,
Sør-Trøndelag, Norway, 3St
Thomas Hospital, Kings College London, London, United
Kingdom
Signal enhancement by Dynamic Nuclear Polarisation of 13C
makes it possible to conduct real-time measurements of
low concentration metabolites in
vivo. Implementation of preclinical work on clinical
systems for DNP studies is attractive, but severely
limited by surface coils when moving from subcutaneous
to orthotopic and genetically modified models. We
describe and characterise a custom-made 13C
volume ladder-design coil; the coil shows superior SNR
and B1 homogeneity
in both phantom studies and in
vivo in
mice when compared to a typical surface coil.
|
1352. |
Design of a detachable rat
head coil for MRI-guided stereotaxic interventions
Jijun Han1, Fulang Qi1, and
Bensheng Qiu1
1Department of Electronic Science and
Technology, University of Science and Technology of
China, Hefei, Anhui, China
A detachable head coil with an aperture for MRI-guided
stereotaxic rat brain surgery was proposed in this
study. The distribution of B1 field was evaluated with
numerical calculation. The design of the detachable RF
head coil is capable of not only producing the
homogenous B1 field, but also providing a free operation
path for interventional instruments, which will enable
MRI-guided stereotaxic neurosurgery of the rat in vivo.
|
1353. |
Current limited
superconducting RF coils
Christopher Stumpf1, Tobias Frank1,
Markus Vester2, Sebastian Martius3,
Robert Rehner2, Rainer Engelbrecht1,
and Lorenz-Peter Schmidt1
1Institute of Microwaves and Photonics,
University of Erlangen-Nuremberg, Erlangen, Bavaria,
Germany, 2Healthcare
Sector, Siemens AG, Erlangen, Bavaria, Germany,3Corporate
Technology, Siemens AG, Erlangen, Bavaria, Germany
Superconducting self-resonant RF coils can be used in
MRI as receive coils to raise the image SNR. Those coils
distort the TX magnetic field if they are not detuned. A
new method is presented to passively detune
self-resonant HTS coils without Q-factor reduction by
inserting a taper into the coil structure. Measurements
of RF current in the loop at varying absorbed powers
show that the current is limited to a maximum value. By
reducing the trace width of the taper the maximum
current value is reduced and the distortion of the TX
field due to induction is decreased.
|
1354. |
A large volume HEM
dielectric resonator for musculoskeletal applications at
ultra high field
Sebastian Arnold Aussenhofer1 and
Andrew Webb1
1Radiology Leiden University Medical Center,
C.J. Gorter Center for High Field MRI, Leiden,
South-Holland, Netherlands
A water-based dielectric resonator operating in the
quadrature HEM mode has been designed and constructed
for imaging the human knee at 7 Tesla. The continuous
current distribution throughout the resonator results in
an extremely simple design of a water-filled annulus
connected to the scanner through two impedance matching
networks. High resolution images of the knee at
sub-millimeter resolution have been acquired in less
than 4 minutes using this resonator.
|
1355. |
RF Field Enhancement at
0.5T to 1.5T with Ultra High Dielectric Constant Material (uHDC)
Christopher Sica1, Sebastian Rupprecht1,
Wei Luo2, Raffi Sahul3, Seongtae
Kwon3, Michael Lanagan2, and Qing
Yang1,4
1Radiology, Penn State College of Medicine,
Hershey, Pennsylvania, United States, 2Engineering
Science and Mechanics, Penn State University,
Pennsylvania, United States,3TRS
Technologies, State College, Pennsylvania, United
States, 4Neurosurgery,
Penn State College of Medicine, Hershey, Pennsylvania,
United States
Previous studies have established the benefits offered
by dielectric materials at 3T and 7T, including reduced
B1+ inhomogeneity and SAR, and increased transmit
efficiency and SNR. We explored the application of
dielectrics to field strengths of 1.5T and below.
Utilizing simulation, the effects of ultra high
dielectric constant material (up to εr = 28000) were
examined with a block of uHDC material within a phantom
at 0.5T, 1T, 1.5T, and 3T. We demonstrated a 2 to 3-fold
enhancement in B1 at all field strengths studied, and
that lower fields require higher permittivity for
enhancement. Experimental results are presented at 1.5
and 3T utilizing available uHDC materials.
|
1356. |
Single and Multiple Coaxial
Inputs to Excite a Cylindrical Waveguide for Traveling Wave
MRI at 21.1 T
Jose A Muniz1,2, Smriti Sagaram1,3,
Jens T Rosenberg1,2, and Samuel Colles Grant1,2
1National High Magnetic Field Laboratory, The
Florida State University, Tallahassee, FL, United
States, 2Chemical
& Biomedical Engineering, The Florida State University,
Tallahassee, FL, United States, 3Electrical
& Computer Engineering, The Florida State University,
Tallahassee, FL, United States
In traveling wave MRI, propagating RF fields are excited
through an antenna located at a distance to a given
sample such that excitation and detection in MRI can be
induced in the far field [1-3]. In this project,
traveling wave MRI at ultra-high field is implemented
using a concentric waveguide composed of a dielectric
filled inner cylinder and an outer copper cylinder with
dimensions similar to the magnet bore of a vertical 21.1
T ultra-wide bore magnet. Uniquely, this waveguide is
excited by coaxial inputs at single and multiple points.
|
1357. |
SNR Enhancement by Free
Local Resonators for Traveling Wave MRI
Xiaoliang Zhang1,2, Yong Pang1,
and Daniel B Vigneron1,2
1Radiology and Biomedical Imaging, University
of California San Francisco, San Francisco, CA, United
States, 2UC
Berkeley/UCSF Joint Bioengineering Program, San
Francisco, CA, United States
One of drawbacks of traveling wave MRI is its relatively
low signal-to-noise ratio (SNR) due to the use of far
fields in excitation and reception. In this work, we
present and investigate a method based on free local
resonator to improve MR SNR in traveling wave MR. In
vivo imaging in rats performed using the proposed free
local resonator method at 7T shows a significantly SNR
gain over the traditional traveling wave MR.
|
1358. |
Accurate and fast
longitudinal RF magnetic field profiling for 7T
traveling-wave MRI systems
Thorsten Liebig1, Jan Taro Svejda1,
Hongyi Yang1, Andreas Rennings1,
Juerg Froehlich2, and Daniel Erni1
1General and Theoretical Electrical
Engineering (ATE), University of Duisburg-Essen,
Duisburg, NRW, Germany, 2Laboratory
for Electromagnetic Fields and Microwave Electronics (IFH),
ETH Zurich, Zurich, ZH, Switzerland
We propose an adaptive, fast and accurate scheme for
tailoring the RF magnetic field along the bore of a 7T
traveling-wave MRI system. The setting consists of a
periodic arrangement of quadrature fed resonant CRLH
metamaterial ring antennas that are perfectly apt to
excite, mold, and dump the propagating TE11 mode within
the cylindrical bore. We have achieved narrow field
profiles for larynx illumination while tackling the
inverse problem using efficient electromagnetic
simulations in conjunction with a direct (weighted)
least-squares solution. This localized traveling-wave
approach has the potential to act as a non-resonant head
coils supporting uniform high-resolution brain imaging.
|
|
|
|
TRADITIONAL
POSTER SESSION ○ MR ENGINEERING; MR SAFETY: SAFETY & BIOEFFECTS;
ULTRA-HIGH FIELD |
RF Modelling & Safety
Monday 12 May 2014
Traditional Poster Hall |
16:30 - 18:30 |
|
|
1359. |
Flip Angle Inhomogeneity
Constrained pTx Pulse Design for Minimum Peak Local SAR
Mihir Pendse1, Simone Winkler2,
and Brian Rutt2
1Department of Electrical Engineering,
Stanford University, Stanford, CA, United States, 2Department
of Radiology, Stanford University, CA, United States
This work introduces a new minimum SAR spokes-based pTx
pulse design algorithm using a spokes trajectory that
achieves a desired flip angle inhomogeneity (FAI)
threshold while minimizing peak local SAR. Several
realistic scan situations are modeled including the use
of slightly inaccurate E-field maps for SAR matrix
computation to represent patient/body model mismatch and
enforcing a constraint on computation time for the
optimization. Simulated L-curves show that for four
different cases our proposed method achieves equal or
lower SAR at low values of FAI compared to prior
approaches for SAR-constrained pTx pulse design.
|
1360. |
Transmit field fitting at
9.4 T using analytical solutions to Maxwell's equations
Michael Stephen Poole1, Desmond H Y Tse1,
Arthur W Magill1, and N Jon Shah1,2
1INM-4, Forschungszentrum Jülich, Jülich,
Germany, 2Department
of Neurology, RWTH Aachen University, Aachen, Germany
Transmit B1+ fields need to be accurately acquired for
B1+ shimming, kt-points homogenisation, spokes slice
selection and parallel RF pulse design. We investigated
the application of forcing relative B1+ maps to obey
Maxwell's equations in order to provide properly scaled
B1+ maps. The method was applied to B1+ maps acquired at
400 MHz in phantom and in vivo and compared to AFI-weighted
B1+ and DREAM maps. Furthermore predicted CP mode and kt-points
excitations were compared and found to be in good
agreement in phantom. The in vivo maps compare
qualitatively well with DREAM but conductivity is poorly
predicted.
|
1361. |
A Numerical Study Comparing
Adult Body, Head and Knee Coils for Paediatric MRI
Gemma R Cook1, Martin J Graves1,
Owen J Arthurs2, Fraser J Robb3,
and David J Lomas1
1Radiology, University of Cambridge,
Cambridge, United Kingdom, 2Great
Ormond Street Hospital, London, United Kingdom, 3GE
Healthcare Coils, Aurora, OH, United States
Limited availability of dedicated paediatric coils means
MRI is typically performed using a transmit/receive coil
(considered to be more SAR and SNR advantageous). This
study uses a FEM-compatible model of a two month infant
inside birdcage coils of typical body, head and knee
coil sizes. Transmit and receive fields were calculated
and the Specific Absorption Rate (normalised to 4W/kg)
was calculated for 1cm³ cubes. SAR maps determined the
heat source for further temperature change simulations
and maximal SAR and temperature change positions were
compared to determine the advantages of each coil.
|
1362. |
Illustration of the Impact
of Tuning Configuration on 7T RF Coil Simulations
Joseph V Rispoli1, Steven M Wright1,2,
and Mary Preston McDougall1,2
1Biomedical Engineering, Texas A & M
University, College Station, TX, United States, 2Electrical
& Computer Engineering, Texas A & M University, College
Station, TX, United States
This work illustrates the ramifications of two different
approaches to tuning and exciting coils in a high-field
simulation environment: 1) forcing an ideal resonant
condition versus 2) specifying actual implemented lumped
element component values. This abstract uses the example
of a loop coil at 7T to demonstrate that results using
the second approach exhibit a more uniform current
distribution, more homogeneous |B1+|,
and 29% lower maximum 10-g average SAR. These results
illustrate that power/safety considerations of coils at
7T benefit from a simulation approach including
implemented component values rather than forcing ideal
resonance as typically simulated at lower field
strengths.
|
1363. |
Skin effect estimation
accuracy in FDTD coil simulations
Andre Kuehne1,2, Helmar Waiczies3,
Ewald Moser1,2, and Elmar Laistler1,2
1Center for Medical Physics and Biomedical
Engineering, Medical University of Vienna, Vienna,
Vienna, Austria, 2MR
Center of Excellence, Medical University of Vienna,
Vienna, Vienna, Austria, 3MRI.Tools
GmbH, Berlin, Germany
|
1364. |
Influence of Deep-Region RF
Hyperthermia System on B1+ Field of 1.5T MR Scanner: a
Simulation Study
Tomas Drizdal1, Matthew R. Tarasek2,
Ruben Pellicer1, Muhammad H. Chishti2,
Wouter C. M. Numan1, Gyula Kotek1,
Desmond T. B. Yeo2, and Margarethus M.
Paulides1
1Erasmus MC, Rotterdam, Netherlands, 2GE
Global Research, Niskayuna, NY, United States
Modeling of radio frequency hyperthermia system and 1.5T
MR scanner.
|
1365. |
Magnetic Force Estimation
around MRI Magnets
Zhenyu Zhang1 and
Timothy J. Havens1
1MR Science & Technology, GE Healthcare,
Florence, South Carolina, United States
Magnetic forces around MRIs have long been a major
concern for operator and patient safety. Due to the
difficulty to calculate exact forces, the consensus of
the industry is to provide a quantity which represents a
good estimation of magnetic forces. This quantity has
been included in IEC 60601-2-33. However, the
mathematical definition of this quantity has been
discussed recently where two suggestions are presented.
In this paper, we make an effort to clarify the
situation by demonstrating a very simple derivation for
one expression and proving that the other expression
does not hold in general.
|
1366. |
Improved method and
technique for monitoring SAR in transmit coils and arrays
Carl J. Snyder1, Seunghoon Ha1,
Haoqin Zhu1, and Labros Petropoulos1
1IMRIS, Minnetonka, Minnesota, United States
With the advent of multi-channel transmitters,
ultra-high field imaging and power-intensive techniques
like Transmit SENSE, the need for real time power
monitoring is becoming an important need. Recent studies
have shown that current methods, (monitoring the forward
and reflected power at the output of the amplifier) is
insufficient as coupling and mismatched coils can change
e-field and possibly SAR in transmit arrays. We are
proposing a three-point method, monitoring the forward,
reflected on the coax and, monitoring the field at the
coil.
|
1367. |
Variation in thermal maps
during RF heating due to variation in electrical
conductivity in TEM coil at 298 MHz
Muhammad Hassan Chishti1, Matthew R. Tarasek1,
Margarethus M. Paulides2, and Desmond Teck
Beng Yeo1
1GE Global Research Center, Niskayuna, New
York, United States, 2Erasmus
Medical Center, Rotterdam, Netherlands
Synopsis: The uncertainty of electrical conductivity (σ)
values used in electromagnetic (EM) simulations may lead
to incorrect assessment of SAR and risks for tissue
ablation in patients during MR imaging at ultra-high
fields and in RF thermotherapy applications. In this
work, we investigate the errors in predicted
temperatures due to incorrect assignment of values to σ
caused by (i) variations in reported values in the
literature, and (ii) temperature-induced variations of
σ. Results from our full-wave EM (298 MHz) and thermal
simulations show that the uncertainties in σ may induce
temperature prediction errors by up to 5.3 ºC.
|
1368. |
Assessment of miniaturized
RF traps for RF heating reduction and reception coil
sensitivity profile restoration
Jean-Marie Verret1,2, Frank Pilleul3,4,
Cécile Rabrait2, and Olivier Beuf1
1Université de Lyon; CREATIS; CNRS UMR 5220;
Inserm U1044; INSA-Lyon; Université Lyon 1,
Villeurbanne, France, 2Clinical
Science Development Group, General Electric Healthcare,
Buc, France, 3Hospices
Civils de Lyon; Département d’imagerie digestive; CHU
Edouard Herriot, France, 4Centre
Léon Bérard - Centre de Lutte contre le Cancer, France
To reduce RF-induced heating, standard passive RF traps
are known to be efficient. Novel miniaturized RF traps
are as efficient as standard ones for this purpose.
Furthermore, it is demonstrated that RF traps enable a
restoration of the signal intensity pattern of the coil.
It is thus possible to perform a MR endoscopy of deeper
regions of the bowel (after left colonic flexure for
instance) since the coaxial cable incorporating
miniaturized RF traps now may be inserted through the
rectum with limited discomfort for the patient.
|
1369. |
EMF exposure and
temperature increase of anatomical pregnant women models
within a 3T RF shimmed birdcage.
Manuel Murbach1, Esra Neufeld1,
Fraser JL Robb2, and Niels Kuster1,3
1ITIS Foundation, Zurich, Switzerland, 2GE
Healthcare, Aurora, OH, United States, 3Swiss
Federal Institute of Technology (ETH), Zurich,
Switzerland
Our study investigates the effect of RF shimming at 3T
on EMF exposure and subsequent temperature increases in
pregnant women of different gestational periods. The
effect of relative I-Q phases and amplitudes is
investigated in terms of B1+ uniformity (CV(B1+)) and
local SAR enhancements. For selected worst-case
scenarios, thermal simulations − including local
thermoregulation − estimate the potential temperature
increase in the mother, amniotic fluid, and fetus.
Preliminary results indicate a relatively low thermal
load for the fetus (< 38°C) when considering local
thermoregulation of the mother in the normal operating
mode.
|
1370. |
A system for calibrated
measurements of RF electromagnetic fields inside a clinical
MR scanner
Gerd Weidemann1, Isabela Frese1,
Frank Seifert1, Antonino Mario Cassara'1,
Werner Hoffmann1, and Bernd Ittermann1
1Physikalisch-Technische Bundesanstalt (PTB),
Berlin, Germany
For accurate and complete SAR assessment of an RF coil
all E and B field components are required. A system for
the calibration of fiber optic time-domain E1 and
B1 field
sensors using an MR compatible TEM cell and the MR
scanner itself was developed. The complex field
amplitudes of E1, B 1+ and
B1 were
reliably measured in an ASTM body phantom equipped with
provisions for internal and external field sensors.
Utilizing the body coil of a clinical 3 T scanner, the
measurements are used to evaluate the accuracy of EMF
simulations.
|
1371. |
Transmitted Power from a
Tx/Rx Birdcage Coil to Nearby Conductors in Air and in Gel
Zoltan Nagy1,2, Aaron Oliver-Taylor3,
Andre Kuehne4,5, and Nikolaus Weiskopf1
1Wellcome Trust Centre for Neuroimaging,
University College London, London, United Kingdom, 2Laboratory
for Social and Neural Systems Research, University of
Zürich, Zürich, Switzerland, 3Institute
for Women's Health, University College London, United
Kingdom, 4Center
for Medical Physics and Biomedical Engineering, Medical
University of Vienna, Austria, 5MR
Center of Excellence, Medical University of Vienna,
Austria
Tx/Rx birdcage head coils are often considered safe for
patients with abdominal implants but whether such
practice is indeed safe has not been tested
systematically. We used radio frequency B/E field probes
to investigate the transmitted power through air and
conductive gel by a Tx/Rx coil in a 3T scanner. We could
detect significant levels of both fields at distances up
to 50 cm from the Tx/Rx coil. These findings were
confirmed with simulations. Preliminary heating results
around straight and looped wires did not result in
significant temperature elevation but this may be due to
the insensitivity of the “implants”.
|
1372. |
Determination of in-vivo
temperature rise and gradient induced voltage during MRI of
cut sacral neuromodulation leads
John Nyenhuis1 and
John Welter2
1Electrical and Computer Engineering, Purdue
University, West Lafayette, Indiana, United States, 2Neuromodulation,
Medtronic, Minneapolis, Minnesota, United States
In-vitro tests and numerical simulations were made to
determine the in-vivo temperature rise and during MRI of
cut Neuromodulation leads (Medtronic 3889 and 3093)
which were retained in-vivo after being used for
treatment of urinary incontinence in women. The overall
method follows the procedure described in ISO-IEC 10974.
For retained lead length of 7-cm, maximum temperature
rise for whole body SAR of 2 W/kg was 2.4 C at 1.5T and
3.7 C at 3T. Rises at the cut exceeded those at the
electrode. These rises yield in-vivo temperature that is
less than the maximum safe value for neurological
tissues.
|
1373. |
The Feasibility of Combined
Magnetic Resonance Thermometry and Multiphysics Simulation
to Evaluate RF Induced Heating of Metallic Devices
David C. Gross1,2, Yu Ding2,
Sergei Yushanov3, Jeff Crompton3,
Alan Leewood4, and Orlando P. Simonetti5,6
1Biomedical Engineering, The Ohio State
University, Columbus, Ohio, United States, 2Dorothy
M. Davis Heart and Lung Research Institute, The Ohio
State University, Columbus, Ohio, United States, 3AltaSim
Technologies, LLC, Columbus, Ohio, United States, 4MED
Institute, Inc., West Lafayette, Indiana, United States, 5Cardiovascular
Medicine, The Ohio State University, Columbus, Ohio,
United States, 6Radiology,
The Ohio State University, Columbus, Ohio, United States
RF induced heating is an important safety concern as the
number of patients implanted with medical devices
increases and the use of 3T MRI becomes more prevalent.
We hypothesize that the combination of Magnetic
Resonance Thermometry (MRT) and multiphysics simulation
would provide a more accurate assessment of MR safety
than current in vitro test methods, and could ultimately
be used to evaluate RF induced heating of devices in
vivo. The purpose of this work is to evaluate the
feasibility of this approach by comparing temperature
probe measurements with MRT and multiphysics simulation
of RF induced heating near a metallic device.
|
1374. |
EM and thermal validation
of a numerical elliptical birdcage at 3T in the presence of
a long conductive wire
Mélina Bouldi1 and
Jan M. Warnking1,2
1Grenoble Institut des Neurosciences - UJF,
Grenoble, Rhônes Alpes, France, 2Inserm
U836, Grenoble, Rhônes Alpes, France
Understanding the risk of overheating in the presence of
implants requires a rigorous simulation of experimental
conditions. We have built a model of the whole body
transmit coil in the Philips Achieva TX® system. The
validity of that model was verified by comparing
electromagnetic and thermal simulations to phantom
experiments for an ASTM phantom alone and in presence of
a long copper wire. RF fields are in good agreement.
Local temperature variations show similar dynamics and
amplitudes. Realistic temperature simulations, as
opposed to SAR simulations, provide a metric directly
comparable to experimental results and thus facilitate
validation.
|
1375. |
OSSARTE: an Open-Source
software for SAR and Temperature Estimation
Giuseppe Carluccio1, Josh Vega1,
Christian Gonzalez-Capizzi2, David Greydanus1,
and Christopher Michael Collins1
1Bernard and Irene Schwartz Center for
Biomedical Imaging, New York University School of
Medicine, New York, New York, United States, 2Oratory
Prep School, Summit, New Jersey, United States
To ensure safe use of MRI it is desirable to estimate
and limit the Specific energy Absorption Rate (SAR)
averaged over the whole body, whole head, and the
maximum SAR averaged over any 1 or 10g region in the
body. Safety guidelines by the IEC recommend limits on
the maximum values of both SAR and temperature. In this
work, we present a useful open source software which
includes tools to locally average SAR and to compute
temperature increase with different methods, letting the
user choose whether to prioritize accuracy or
computation speed.
|
1376. |
MR Safety of
Magneto-inductive Receivers
Richard Syms1, Khoonsake Segkhoonthod1,
and Ian Young1
1EEE Dept., Imperial College London, London,
Middlesex, United Kingdom
Radio frequency heating may be induced when linear
conductors are inserted in the body during MRI, due to
electrical excitation of surface wave resonances. The
effect occurs even when inserted lengths are short, due
to the high RF dielectric constant of tissue. We have
developed receivers for internal imaging using
magneto-inductive waveguides, a form of
transformer-segmented waveguide that can be realized in
thin film form and mounted on a catheter. This paper
presents accurate EM simulation using AWR Microwave
Office designed to confirm RF safety. The results
highlight the effect of heatshrink material on surface
wave resonances and parasitic capacitances.
|
1377. |
Online SAR measurement
error in high resolution slice accelerated 2D EPI
An T. Vu1, Edward Auerbach1, Kamil
Ugurbil1, and Essa Yacoub1
1University of Minnesota, CMRR, Minneapolis,
MN, United States
Slice accelerated or multiband (MB) 2D EPI has recently
enabled fast, high resolution, whole brain imaging.
However, as MB factors, resolution, and brain coverage
increase so do the temporal frequency modulations of the
MB RF pulses. Such rapidly modulated RF pulses can
result in SAR overestimation during online SAR
monitoring resulting in prematurely aborted scans even
when pre-calculated SAR levels are below (60-70%) the
FDA limit. We show that recent methods for minimizing
peak power can also reduce SAR measurement errors with
little or no cost in TR or image quality – allowing MB
acceleration gains to be more fully realized.
|
1378. |
Accurate EM modelling of a
not-fully accessible RF body coil at 3T for quantitative SAR
investigations
Antonino Mario Cassara'1, Gerd Weidemann1,
Frank Seifert1, and Bernd Ittermann1
1Physikalisch-Technische Bundesanstalt (PTB),
Berlin, Germany
Accurate electromagnetic modelling of RF transmit coils
for MRI, e.g. for quantitative SAR assessments, can be
difficult when not all coil details are directly
accessible to the modelers. This is typically the case
for commercial coils and most notably for the body coil
of a clinical scanner. The present work illustrates the
steps for the creation of an accurate model of a
commercial 3 T body coil. Information provided by the
manufacturer is merged with in-situ RF measurements on
accessible ports and results from numerical simulations.
The accuracy of this modeling is quantified comparing
simulated and measured B1+ field maps in a extensive
phantom study.
|
1379. |
Eigen matrix approach in
coupled-circuit numerical simulation of eddy currents in MRI
systems
Md. Shahadat Hossain Akram1, Yasuhiko Terada1,
Keiichiro Ishi1, and Katsumi Kose1
1Institute of Applied Physics, University of
Tsukuba, Tsukuba, Ibaraki, Japan
In coupled-circuit simulation of eddy currents, system
of differential equations is solved to get eddy currents
transient responses in different domains at different
locations. It is desirable to improve computational
efficiency whenever possible. Implementing Eigen matrix
techniques to solve this system of equations removes
singularity problems totally and reduces calculation
time to a large level. We have implemented this approach
to analyze eddy currents for both open and large
closed-bore MRI systems. We have also conducted FID
measurement of eddy fields by NMR probe to verify our
approach. We have found good agreement between
simulation and experiment.
|
1380. |
Comprehensive analysis of
parallel transmission local SAR errors introduced by an
assumed uniform density distribution
Andre Kuehne1,2, Sigrun Goluch1,2,
Ewald Moser1,2, and Elmar Laistler1,2
1Center for Medical Physics and Biomedical
Engineering, Medical University of Vienna, Vienna,
Vienna, Austria, 2MR
Center of Excellence, Medical University of Vienna,
Vienna, Vienna, Austria
In this work, the validity of the commonly made
assumption of an isotropic tissue density (1000 kg/m³)
for SAR calculations is investigated. SAR matrix
Eigenvalues- and vectors of an 8-channel head array for
7T MRI are compared and a statistical analysis
performed. It is found, that the simplified SAR
distribution leads to an overestimation of local SAR by
11-12% on average.
|
1381. |
Coil Evaluation Metrics
Jinfeng Tian1, Lance Delabarre2,
and J. Thomas Vaughan2
1CMRR - Dept. of Rad., U. of Minnesota,
Minneapolis, Minnesota, United States, 2CMRR
- Dept. of Rad., U. of Minnesota, Minnesota, United
States
Several differing coil arrays at 3T and 7T were
simulated and evaluated for B1+ efficiency relative to
net input power, global SAR and local SAR to demonstrate
the importance of normalizing efficiency in terms of
both input power and SAR. Large volume efficiency
metrics are better for coils that have variation in the
z-axis.
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|
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|
TRADITIONAL
POSTER SESSION ○ MR ENGINEERING; MR SAFETY: SAFETY & BIOEFFECTS;
ULTRA-HIGH FIELD |
Gradients, Shims, Magnets & Field Monitoring
Monday 12 May 2014
Traditional Poster Hall |
16:30 - 18:30 |
|
|
1382. |
A new magnet design for
field cycling OMRI
Constantin Job1, Jean-Philippe Galons1,
and Diego Martin1
1Medical Imaging, University of Arizona,
Tucson, Arizona, United States
A custom-built low-inductance solenoid magnet enables
the cycling of the magnetic field strength in the range
from 0 to 4700 Gauss in less than 10 msec
|
1383. |
A finite-difference model
for the analysis of Acoustic Noise generated by Gradient
Coil switching
Liyi Kang1, Zhifeng Chen1, Zhiqian
Ye1, Feng Liu2, and Ling Xia1
1Department of Biomedical Engineering,
Zhejiang University, Hangzhou, Zhejiang, China, 2School
of Information Technology and Electrical Engineering,
The University of Queensland, Brisbane, Queensland,
Australia
In this work, a force-vibration-noise model has been
developed for the analysis of gradient switching induced
acoustic noise in MRI. The acoustic model is based on
the finite difference method, and it can quantitatively
evaluate the acoustic noise produced by typical gradient
switching procedure. With the Tikhonov regularization
based optimization technique, new gradient coils are
designed; compared with conventional coils, the new
gradient coils offer excellent magnetic field linearity
and the sound pressure level is decreased by about 10%.
|
1384. |
generalized measure to
assess gradient coil performance
Feng Jia1, Gerrit Schultz1, Anna
Masako Welz1, Frederik Testud1,
Hans Weber1, Sebastian Littin1,
Huijun Yu1, Jürgen Hennig1, and
Maxim Zaitsev1
1Department of Radiology, Medical Physics,
University Medical Center Freiburg, Freiburg,
Baden-Württemberg, Germany
We present a general performance measure to assess all
the gradient coils from the perspective of different
purposes. A matrix coil is used to demonstrate this
general performance measure.
|
1385. |
Multi physics modeling of
eddy current vibration damping in MRI systems
Kishore Venkata Mogatadakala1, Ming Yao1,
Sampath Telikicherla Kandala1, Longzhi Jiang1,
and Timothy Havens1
1Magnet and Gradient engineering, GE Health
care, Florence, SC, United States
Vibration induced eddy currents generate magnetic field
disturbance in MRI systems and degrade image quality
(IQ). In this work, a multi-physics based finite element
approach is presented to simulate mechanical vibration
and eddy currents. Both simulation and test results
indicate that the induced eddy currents play a
significant role in attenuating the vibration response
and corresponding field disturbance. In order to
demonstrate the applicability of the developed technique
to a complicated mechanical resonance mode, simulation
was performed on a locally deforming hollow cylinder and
the results are presented with and without
electromagnetic damping.
|
1386. |
Measuring the Spatial
Magnetic Field Gradients within a Scanner Bore
Karlene M Fraser1,2, Elizabeth Morris3,
Jonathan Ashmore4, Stephen Wastling2,
Ruth O'Gorman4,5, and Gareth Barker2
1Neuroimaging, Maudsley Hospital, London,
United Kingdom, 2Centre
for Neuroimaging Sciences, King's College London,
London, United Kingdom, 3Medical
Engineering and Physics, King's College Hospital,
London, United Kingdom, 4Neuroradiology,
King's College Hospital, London, United Kingdom, 5Centre
for MR Research, University Children's Hospital, Zurich,
Switzerland
Manufacturers of medical implants and devices classify
some as MR conditional, and specify maximum spatial
magnetic field gradient (MFG) restrictions in G/cm or
T/m. Measurements of the MF within the bores of a 1.5T
and 3.0T HD.x, and two 3.0T MR750 MR scanners were
obtained using a THM1176 Hall probe. Maximum spatial MFG
calculated for the 1.5T and each 3.0T scanner was
respectively over 400 G/cm and 700 G/cm, and
approximately 1.5 and 2 times less that reported by the
scanner manufacturer. Had the manufacturer’s
measurements been restricted to the patient accessible
area, our measurements may have been more comparable.
|
1387. |
Faster Feedback Field
Control using Shim Pre-Emphasis
Yolanda Duerst1, Bertram J Wilm1,
Signe J Vannesjo1, Benjamin E Dietrich1,
Simon Gross1, David O Brunner1,
Thomas Schmid1, and Klaas P Pruessmann1
1ETH Zurich, Zurich, ZH, Switzerland
Real-time field feedback as implemented previously
assumed instantaneous and uncoupled shim responses. The
violation of this assumption by the real system leads to
distortions in the feedback loop. The current work shows
the implementation of self-term pre-emphasis for
decreasing the shim response time and cross-term
pre-emphasis in order to decouple the individual
channels. This allows for a faster response to changes
in the target field pattern and enables faster and more
stable field feedback.
|
1388. |
Couple Electromagnetic and
Neuronal Dynamics Simulation of Gradient Coil Switching
Induced Nerve Stimulation
Ioannis Vogiatzis Oikonomidis1,2, Esra
Neufeld1, Johanna Wolf1, Deepika
Sharma1,3, Yngve Hamnerius2, and
Niels Kuster1,3
1IT'IS Foundation, Zurich, Switzerland, 2Signals
and Systems, Chalmers University of Technology,
Gothenburg, Sweden, 3Information
Technology and Electrical Engineering, Swiss Federal
Institute of Technology, Zurich, Switzerland
Nerve stimulation by rapidly switching gradient coils is
a safety concern in MR. An EM and thermal simulation
platform has been coupled with a neuronal dynamics
modeling code, to investigate such interactions in
realistic anatomical models. A locally temperature
dependent variant of the SENN model, commonly employed
for safety threshold assessment, has been developed.
Modeling of sciatic nerve stimulation by gradient coil
switching, considering the impact of RF birdcage coil
induced heating, showed that the model anisotropy, the
field variation along the nerve and local temperature
have a relevant impact that can be studied using the
coupled EM-neuron simulation platform.
|
1389. |
Improved magnetically
induced torque measurement for MRI safety testing
Fred Tam1, Peter Geng2, and Simon
J Graham1,3
1Physical Sciences, Sunnybrook Research
Institute, Toronto, Ontario, Canada, 2Department
of Mechanical and Mechatronics Engineering, University
of Waterloo, Waterloo, Ontario, Canada, 3Department
of Medical Biophysics, University of Toronto, Toronto,
Ontario, Canada
Torque measurements for MRI safety testing are often
qualitative, despite ASTM standard F2213-06 which
prescribes a quantitative measurement method and
apparatus. To facilitate quantitative measurement,
practical improvements were made to this apparatus,
including a calibration procedure for its torsion
springs. The resulting apparatus has increased capacity
and simplified construction, and its accuracy has been
characterized. Calibration data reveal nonlinear
behaviour, warning against naive use of the simple
formula in F2213-06. Example usage of the apparatus
shows a prototype tablet device for fMRI passes F2213-06
criteria.
|
1390. |
k-t-Calibration improves
continuous field monitoring for image reconstruction
Benjamin E. Dietrich1, Bertram J. Wilm1,
David O. Brunner1, Yolanda Duerst1,
Christoph Barmet1,2, and Klaas P. Pruessmann1
1Institut for Biomedical Engineering,
University and ETH Zurich, Zurich, Zurich, Switzerland, 2Skope
Magnetic Resonance Technologies, Zurich, Switzerland
By means of NMR probe based magnetic field monitoring,
the spatio-temporal magnetic field evolution and hence
k-space trajectory can be observed and used to improve
image reconstruction. Continuous field monitoring based
on time interleaved acquisition of sets of fast relaxing
probes enables sequence independent monitoring over
arbitrary durations without limitations on k-space
range, but suffered so far under accumulated errors in
the calculated trajectories due to violations of the
assumption that the probes behave like point sources.
The presented k-space and time domain calibration method
addresses these problems and enables continuous
monitoring for image reconstruction.
|
1391. |
Mapping and correcting
respiration-induced field changes in the brain using
fluorine field probes
Mads Andersen1,2, Kristoffer Madsen1,
Lars Hanson1,2, Vincent Boer3,
Tijl van der Velden3, Dennis Klomp3,
Joep Wezel4, Matthias van Osch4,
and Maarten Versluis4
1Danish Research Centre for Magnetic
Resonance, Copenhagen University Hospital Hvidovre,
Copenhagen, Denmark, 2Biomedical
Engineering Group, DTU Elektro, Technical University of
Denmark, Kgs. Lyngby, Denmark, 3Department
of Radiology, University Medical Center Utrecht,
Utrecht, Netherlands, 4C.J.
Gorter center, Department of Radiology, Leiden
University Medical Center, Leiden, Netherlands
Breathing induced dynamic B0 field perturbations in the
head degrade image and spectral quality. It has recently
been proposed to continuously stabilize the magnetic
field by real-time updating of the shim fields, based on
synchronous field measurements with external probes. A
thorough analysis of how accurate such field
measurements outside the head can reflect the spatially
varying dynamic fields inside the head is currently
lacking. We present such an analysis and see that 14
external field probes reflect the field in the head
sufficiently well so it can be significantly stabilized.
|
1392. |
Design Methods for Magnetic
Resonance Based Field Monitoring Devices
Wieland A. Worthoff1, Stefan Schwan1,
Arthur W. Magill1, Michael S. Poole1,
and N. Jon Shah1,2
1INM - 4, Research Centre Jülich GmbH, Jülich,
Germany, 2Department
of Neurology, RWTH Aachen University, Aachen, Germany
Developing MR based field probes requires careful
design, because a distorted local magnetic field within
the sample droplet can lead to a significant reduction
in signal fidelity. By simulating the local field
variations due to the susceptibility of the field probe
itself, we demonstrate a novel approach to acquiring
appropriate design parameters in order to optimise the
performance of new probe prototypes. We compare our
numerical results with experimental data in order to
verify and explore the capabilities of the simulation.
|
1393. |
Hybrid Digital Phase-Locked
Loop and Moving Average Filtering Improves SNR in Spatio-Temporal
Field Monitoring
Yu-Chun Chang1,2, Martin Eschelbach1,
Klaus Scheffler1, and Anke Henning1,3
1Max Planck Institute of Biological
Cybernetics, Tuebingen, Baden-Wuerttemburg, Germany, 2Graduate
School of Neural & Behavioural Sciences, University of
Tuebingen, Tuebingen, Baden-Wuerttemburg, Germany, 3Institute
for Biomedical Engineering, University and ETH Zurich,
Switzerland
Recent spatio-temporal B0 field monitoring methods
utilise an array of NMR probes to measure the dynamics
of the B0 field. The B0 field is usually characterised
by spherical harmonic coefficients which are obtained
from the phase signals (or phase coefficients) of the
probe FIDs. A hybrid method is presented that uses a
moving average filter in conjunction with a digital
phase locked-loop filter to improve the SNR of the phase
signals measured by the NMR probes. This method takes
advantage of the FID SNR to reduce the phase jitter in
the phase signal. It is also easy to implement for
real-time applications.
|
1394. |
Noise Reduction of Impulse
Response Function of the Encoding Fields Calculation
Frederik Testud1, Johanna S. Vannesjö2,
Christoph Barmet2,3, Klaas P. Pruessmann2,
Jürgen Hennig1, and Maxim Zaitsev1
1Medical Physics, Department of Radiology,
University Medical Center, Freiburg, Germany, 2Institute
for Biomedical Engineering, University and ETH Zürich,
Zürich, Switzerland, 3Skope
Magnetic Resonance Technologies, Zürich, Switzerland
The Impulse Response function of the scanners’ Encoding
Fields (IREFs) allows improving the scanners’
preemphasis or the image reconstruction by predicting
the encoding trajectory. The impulse response function
was assessed by mean of magnetic field monitoring where
the field evolution of triangular-shaped waveforms were
used as inputs. The IREFs need to be low-pass filtered
to reduce high-frequency noise. We propose to achieve
this by obtaining the field probes’ phase derivative
using the Savitzky-Golay filter and to use the discrete
test waveform for IREF calculation. The repetition
number can be potentially reduced by the proposed
improvements in the impulse response calculation.
|
1395. |
3D-printed geometric
distortion correction phantom for MRI
David W Holdsworth1,2, Matthew G Teeter1,2,
Jaques S Milner2, Steven I Pollmann2,
and Maria Drangova2,3
1Department of Surgery, Western University,
London, Ontario, Canada, 2Robarts
Research Institute, London, Ontario, Canada, 3Department
of Medical Biophysics, Western University, London,
Ontario, Canada
Accurate correction of geometric distortion is
increasingly important for MRI applications in
image-guided intervention. Advances in 3D printing have
made it possible to fabricate structures with
three-dimensional features that facilitate automated
analysis of geometric distortions. We describe the
fabrication of a plastic structure comprised of 4.5 mm
beads, supported by 1.5 mm struts at 13 mm nominal
spacing, which is immersed in a tissue-mimicking liquid.
Automated analysis produces a point cloud of fiducial
locations and a vector map of distortion. MRI imaging at
3T demonstrates the ability to determine average local
distortions of ±0.53 mm, over a 500 ml volume.
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|
TRADITIONAL
POSTER SESSION ○ MR ENGINEERING; MR SAFETY: SAFETY & BIOEFFECTS;
ULTRA-HIGH FIELD |
PET-MRI Engineering & Methods
Monday 12 May 2014
Traditional Poster Hall |
16:30 - 18:30 |
|
|
1396. |
Validation of a PET-derived
Respiratory Signal by Comparison with an MRI Pencil-Beam
Navigator Signal in Simultaneous PET/MR
Richard Manber1, David Atkinson1,
Anna Barnes2, Brian Hutton1, Celia
O'Meara2, Sebastien Ourselin1,
Simon Arridge1, and Kris Thielemans1
1University College London, London, United
Kingdom, 2University
College London Hospital, London, United Kingdom
Respiratory gating in PET imaging is common practice to
correct for motion. It has previously been shown that a
respiratory signal can be extracted from PET list-mode
data using Principal Component Analysis (PCA). We
demonstrate the validity of this signal by showing a
strong correlation with the ‘gold-standard’ MRI
navigator signal, simultaneously acquired on 9 patients
with a range of PET tracers, and by showing comparable
PET gating results based on the PET and MRI derived
respiratory signals respectively. Finally we show
improvements in image sharpness of ‘motion corrected’
images, formed by warping and combining gates.
|
1397. |
Probabilistic Atlas-Based
Generation of Continuous-Valued Attenuation Correction Maps
for Hybrid MR-PET Imaging
Kevin T. Chen1,2, David Izquierdo-Garcia2,
Clare Poynton2, Daniel B. Chonde2,3,
and Ciprian Catana2
1Health Sciences and Technology,
Massachusetts Institute of Technology, Cambridge, MA,
United States, 2A.
A. Martinos Center for Biomedical Imaging, Massachusetts
General Hospital, Harvard Medical School, Charlestown,
MA, United States, 3Biophysics,
Harvard University, Boston, MA, United States
We have implemented a method of generating
continuous-valued attenuation coefficient maps for PET
data correction in hybrid MR-PET scanners. This method
combines atlas coregistration along with a trained
classifier to provide information about subject local
anatomy.
|
1398. |
Improvement and Evaluation
in PET Performance of 16-Channel Receive Anterior Array
Coils for 3T Simultaneous PET/MR Scanner
Yun-Jeong Stickle1, Jianhua Yu2,
Tae-Young Yang1, Sahil Bhatia1,
and Dmitriy V Londarskiy1
1GE Healthcare, Aurora, OH, United States, 2GE
Healthcare, Waukesha, WI, United States
The purpose of this study was to develop and evaluate
the novel coil designs with new materials adopted to
reduce the coil impact on PET image quality. We
developed a new plastic-free 3T 16-channel flexible
anterior array (AA) RF coil with V0 flammability rating
and biocompatibility (PET/MR prototype AA2) for torso
and cardiac imaging and validated the PET performances
for a GE conventional AA coil and two improved PET/MR
prototype coils. The results show a 48% and a 79%
average sensitivity loss improvement on PET/MR prototype
AA1 coil and PET/MR prototype AA2 coil, respectively,
from GE conventional AA coil.
|
1399. |
Whole Body RF Coil Design
for a Simultaneous PET-MR System
Saikat Saha1
1GE Healthcare, GE, Waukesha, WI, United
States
In conventional whole body RF transmit coils, various RF
components such as diodes, capacitors, inductors, cables
etc. are placed throughout the coil for optimal MR
performance. If such components are placed in the FOV of
the PET detector in a simultaneous PET/MR system, they
will scatter some of the PET signals (511keV
annihilation photons), affecting image quality. To
address this problem we have created a “zero PET
attenuation” whole body transmit/receive coil with
minimal use of high density RF components. We present
design and performance for the resulting body coil as
implemented in our 3.0T simultaneous PET/MR system.
|
1400. |
A Low PET Attenuation
Transmit-Receive Head Coil for Simultaneous PET and MR
Spectroscopy
Gillian Haemer1,2, David Faul3,
Thomas Koesters1,4, Kimberly Jackson1,
Oded Gonen1, and Graham Wiggins1
1The Bernard and Irene Schwartz Center for
Biomedical Imaging, Department of Radiology, New York
University School of Medicine, New York, NY, United
States, 2The
Sackler Institute for Graduate Biomedical Sciences, New
York University School of Medicine, New York, NY, United
States, 3Siemens
Medical Solutions, New York, NY, United States,4Center
for Advanced Imaging Innovation and Research, Department
of Radiology, New York University School of Medicine,
New York, NY, United States
In order to allow for simultaneous PET and MR
Spectroscopic imaging (MRSI) on a PET/MR Hybrid system,
RF coil designs must be MR efficient, transmit-receive
capable, and provide low PET attenuation. We present a
birdcage coil design based on these requirements, which
provides sufficient efficiency for MRSI, while creating
minimal attenuation. We compare the MR efficiency of
this coil to an MR Instruments TEM coil, and the PET
attenuation to the attenuation-minimized receive-only
head coil provided with the PET/MR system, and find that
this design provides comparable MR efficiency and
superior attenuation minimization.
|
1401. |
Combining MRI with PET for
partial volume correction improves image-derived input
functions in mice
Eleanor Evans1, David Izquierdo Garcia2,
Guido Buonincontri1, Carmen Methner3,
Rob C Hawkes1, Thomas Kreig3, T.
Adrian Carpenter1, and Stephen J Sawiak1,4
1Wolfson Brain Imaging Centre, University of
Cambridge, Cambridge, United Kingdom, 2Athinoula
A. Martinos Centre for Biomedical Imaging, Harvard
University, Massachusetts, United States, 3Department
of Medicine, University of Cambridge, Cambridge, United
Kingdom, 4Behavioural
and Clinical Neurosciences Institute, University of
Cambridge, Cambridge, United Kingdom
Kinetic modelling in Positron Emission Tomography (PET)
allows metabolic measures to be obtained, but requires
the tracer arterial input function (AIF). Blood sampling
to acquire the AIF is prohibitive in mice due to low
blood volumes. Image-derived AIFs are therefore
preferred, although their extraction from blood vessels
is hampered by low spatial resolution (~1.5-2mm). We
found that using an AIF extraction method which employed
partial volume correction (PVC) in the mouse heart was
crucial for deriving accurate AIFs and gave best results
when ROIs were based on MRI data rather than PET data.
|
1402. |
Evaluation of MR
Compatibility of a SiPM-based PET scanner for simultaneous
PET/MR studies operating at animal 7-T MR scanner
Guen Bae Ko1, Daehong Kim2, Hyun
Suk Yoon1, Min Sun Lee1, In Chan
Song3, and Jae Sung Lee1
1Department of Nuclear Medicine, Seoul
National University, Seoul, Korea, 2Molecular
Imaging and Therapy Branch, National Cancer Center,
Goyang, Gyeonggi, Korea,3Department of
Radiology, Seoul National University, Seoul, Korea
Here, we¡¯d like to report relevant influences of novel
SiPM-based PET scanner on MR images at ultra-high
magnetic field. Several MR image including FSE, SE, GRE,
3D SPGR, and EPI were evaluated with a 7-T MRI scanner
and 35-mm-inner-diameter mouse body transceiver coil.
The experimental results show that the PET insert unit
affects only minor effect on MR images that can be
ensured for preclinical evaluation. It was also proved
that to perform multi-functional study of PET and
functional MRI using our PET insert unit is possible.
|
1403. |
Bayesian segmentation of
dual-echo UTE images for PET/MR attenuation correction
Gaspar Delso1, Michael Carl1,
Florian Wiesinger2, Martin Hüllner3,
and Patrick Veit-Haibach3
1Global MR Applications & Workflow, GE
Healthcare, Waukesha, WI, United States, 2GE
Global Research, Munich, Germany, 3University
Hospital, Zurich, Switzerland
MR-based attenuation correction is a critical component
of integrated PET/MR scanners. This is generally
achieved by segmenting MR images into a set of tissue
classes with known attenuation properties (e.g. bone,
fat, soft tissue, lung, air). Ultra-short echo time
(UTE) sequences capable of imaging tissues with short
T2* times (<1 ms) have been proposed in the past as a
means to locate bone tissue1-4. In this study, we used
tri-modality PET/CT+MR data from oncology patients to
develop an improved classification algorithm for the
localization of bone tissue in the head and neck area.
|
1404. |
Integrated PET/MR: Phantom
Studies Towards Radiotracer Dose Reduction
Mark Oehmigen1, Susanne Ziegler1,
Björn W. Jakoby2,3, and Harald H. Quick1
1Institute of Medical Physics, University of
Erlangen-Nuremberg, Erlangen, Germany, 2Siemens
Healthcare Sector, Erlangen, Germany, 3University
of Surrey, Guildford, Surrey, United Kingdom
In integrated PET/MR hybrid imaging data acquisition
times per bed position are comparatively longer than in
PET/CT imaging. Increasing PET data acquisition times
may allow decreasing the injected radiotracer dose while
maintaining image quality. All measurements were
performed on an integrated PET/MR whole-body hybrid
system using the NEMA image quality phantom. PET images
were acquired with doubled time but halved activity. The
images acquired at different tracer activity levels and
acquisition times show no visible difference in quality
and only small quantitative measurable changes. Longer
PET acquisition time in PET/MR enable the reduction of
the administered PET tracer activity.
|
1405. |
Wireless MR active marker
based PET motion correction in simultaneous brain MR-PET
Chuan Huang1, Jerome L Ackerman2,
Yoann Petibon1, Marc D Normandin1,
Georges El Fakhri1, and Jinsong Ouyang1
1Center for Advanced Medical Imaging
Sciences, Massachusetts General Hospital, Harvard
Medical School, Boston, MA, United States, 2Athinoula
A. Martinos Center for Biomedical Imaging, Massachusetts
General Hospital, Harvard Medical School, Boston, MA,
United States
Recently, wireless active markers have been used in head
motion tracking/correction in brain MRI due to its
improved patient safety, ease-of-use and simpler
manufacturing. Head motion is even more a problem in
brain PET since dynamic brain PET can last more than an
hour. Furthermore, anesthesia is often used to keep
animals still during brain PET acquisitions, but many
studies showed that anesthesia can also perturb the
neurological process under study. Simultaneous MR-PET is
a novel hybrid modality generated substantial interest
in recent years. Complementary information of the brain
from PET and MR can be simultaneously obtained. This new
modality also opens the possibility to use MR active
marker derived motion information for PET motion
correction. In this work, we demonstrate in phantom and
non-human primate studies the use of wireless active
markers to track head motion and incorporating the
measure motion information in the list-mode PET
reconstruction to obtain PET images without motion
artifacts in simultaneous MR-PET.
|
1406. |
Quantitative evaluation of
the short-lived eddy currents in shield boxes of the novel
MRI head coil integrated with PET detectors
Mikio Suga1,2, Takayuki Obata2,
Kodai Shimizu1, Fumihiko Nishikido2,
Atsushi Tachibana2, Hideto Kuribayashi3,
Iwao Nakajima4, Yoshihiko Kawabata4,
and Taiga Yamaya2
1Chiba University, Chiba, Chiba, Japan, 2National
Institute of Radiological Sciences, Chiba, Chiba, Japan, 3Siemens
Japan K. K., Tokyo, Japan, 4Takashima
Seisakusho Co., Ltd., Tokyo, Japan
We are developing a new PET/MRI system in which PET
detectors are closely located at the MR head coil. To
reduce electromagnetic interaction between PET detectors
and MRI coil, the PET detectors are covered with
conductive shield boxes. In this study, we
quantitatively evaluated the secondary magnetic field
induced by short-lived eddy currents in shield boxes and
the effect of slits in shield boxes. The results showed
that the secondary magnetic field induced by the shield
boxes without slits was not negligible for EPI. We can
observe the eddy current reduction effect by making a
slit in a shield box.
|
1407. |
An MR-PET phantom for
studies of the male pelvis
Philipp Mann1, Armin Runz2, Martin
Schaefer3, and Peter Bachert1
1Department of Medical Physics in Radiology,
German Cancer Research Center, Heidelberg, Germany, 2Department
of Medical Physics in Radiation Oncology, German Cancer
Research Center, Heidelberg, Germany, 3Department
of Radiopharmaceutical Chemistry, German Cancer Research
Center, Heidelberg, Germany
An MR-PET phantom for evaluation of studies of the male
pelvis was designed. Hollow components mimicking thigh
bone, bladder, and prostate were built using 3D printing
technique. Experimental tests were performed with 68Ga-PET, 1H-MRI,
and 1H
spectroscopic imaging.
|
1408. |
Direct evaluation of MR-derived
attenuation correction maps for PET/MR of the mouse
myocardium
Eleanor Evans1, Guido Buonincontri1,
Rob C Hawkes1, Richard E Ansorge2,
T. Adrian Carpenter1, and Stephen J Sawiak1,3
1Wolfson Brain Imaging Centre, University of
Cambridge, Cambridge, United Kingdom, 2Department
of Physics, University of Cambridge, Cambridge, United
Kingdom,3Behavioural and Clinical
Neurosciences Institute, University of Cambridge,
Cambridge, United Kingdom
Attenuation correction (AC) must be applied to provide
quantitative measurements of Positron Emission
Tomography (PET) tracer activity concentrations. The
gold standard AC method involves passing a transmission
source around the subject and surrounding scanner
equipment. Due to the limited space in PET/MR scanners,
MR-derived AC (MRAC) must be used instead. This is
problematic as MR signals are not directly related to
the amount of gamma radiation absorbed. By comparing to
gold standard transmission scans, we found a single
tissue region MRAC segmentation approach, derived from
whole body MRI, provided accurate myocardial SUV values
in mice.
|
1409. |
Influence of patient motion
in bone tissue maps obtained with ultra-short echo time MR
Patrick Veit-Haibach1, Michael Carl2,
Mehdi Khalighi2, Florian Wiesinger3,
Konstantinos Zeimpekis1, and Gaspar Delso2
1University Hospital, Zurich, Switzerland, 2Global
MR Applications & Workflow, GE Healthcare, WI, United
States, 3GE
Global Research, Munich, Germany
Accurate mapping of the attenuation properties of
patient tissue is instrumental for quantitative positron
emission tomography (PET). In hybrid PET/MR scanners,
this can be achieved using dedicated MR images to
identify tissue classes of known attenuation (e.g. fat,
lung, air). For the particular case of bone tissue,
standard sequences are not adequate due to the fast T2*
relaxation time. Ultra-short echo time (UTE) sequences
have been reported to provide adequate bone tissue
identification for the purposes of PET attenuation
correction. These sequences do, however, require
acquisition times in the order of 2 to 5 minutes to
cover a typical PET station. Such long acquisition times
increase the probability of patient movement occurring
during the acquisition. In this study, we analyze the
artifacts introduced by patient motion on the bone maps
obtained with UTE.
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TRADITIONAL
POSTER SESSION ○ MR ENGINEERING; MR SAFETY: SAFETY & BIOEFFECTS;
ULTRA-HIGH FIELD |
Applications of Ultra-High Fields
Monday 12 May 2014
Traditional Poster Hall |
16:30 - 18:30 |
|
|
1410. |
Accelerated multiplexed-EPI
with PSF-based distortion correction at 9.4T
Seong Dae Yun1 and
N. Jon Shah1,2
1INM - 4, Research Centre Jülich GmbH, Jülich,
Germany, 2Department
of Neurology, RWTH Aachen University, Aachen, Germany
The relatively high imaging speed of EPI has led to its
widespread use in dynamic MRI studies. The performance
of the EPI can be improved by combining it with in-plane
acceleration techniques such as multi-shot, parallel MRI
and EPI with Keyhole (EPIK). For even faster volumetric
acquisition in EPI, the multiplexed-EPI (M-EPI) method
has also been presented (Feinberg et al.). This study i)
verifies the use of the in-plane acceleration techniques
on the M-EPI at 9.4T and ii) quantitatively assesses the
performance of each imaging method. Lastly, the robust
removal of geometric distortions is demonstrated with
the PSF-based correction method.
|
1411. |
High-Resolution MR
Angiography at 7T: Detection of Perforating Arteries of the
Anterior Communicating and Distal Middle Cerebral Arteries
Taisuke Harada1, Yuiko Sato2,
Takamasa Nanba2, Takahiro Kouji2,
Takaaki Beppu2, Tsuyoshi Matsuda3,
Hiroyuki Kabasawa3, Fumio Yamashita1,
Ikuko Uwano1, Kohsuke Kudo4,
Kuniaki Ogasawara2, and Makoto Sasaki1
1Ultra-High Field MRI, Iwate Medical
University, Morioka, Iwate, Japan, 2Neurosurgery,
Iwate Medical University, Morioka, Iwate, Japan, 3Global
Applied Science Laboratory, GE Healthcare, Hino, Tokyo,
Japan, 4Diagnostic
and Interventional Radiology, Hokkaido University
Hospital, Sapporo, Hokkaido, Japan
Minute perforating arteries such as the hypothalamic
branch of the subcallosal artery and the long insular
artery, which can cause severe neurological
complications when injured during surgery, have not been
visualized using imaging modalities including magnetic
resonance angiography (MRA) at 3 Tesla or below. We
revealed that high-resolution MRA at 7T, particularly
with a magnetization transfer contrast pulse, can
readily visualize these arteries and their relationship
with surrounding structures. This technique may
contribute to avoiding complications of surgery on
aneurysms at the anterior communicating artery and
tumors in the insulo-opercular regions.
|
1412. |
Clinical Application of 7T
MRI for Deep Brain Stimulation (DBS) Surgery and
Postoperative Programming
Yuval Duchin1, Guillermo Sapiro2,
Shai Chazin1, Kenneth Baker3, Jon
McIver4, Jerrold Vitek3, and Noam
Harel1,5
1Radiology / CMRR, University of Minnesota,
Minneapolis, Minnesota, United States, 2Electrical
and Computer Engineering, Duke University, Durham, North
Carolina, United States, 3Neurology,
University of Minnesota, Minneapolis, Minnesota, United
States, 4Neurosurgery,
Regions Hospital, St. Paul, Minnesota, United States, 5Neurosurgery,
University of Minnesota, Minneapolis, Minnesota, United
States
Deep brain stimulation (DBS) surgery has emerged as a
powerful neuromodulation clinical therapy. Current
standard clinical imaging protocols do not have
sufficient resolution and/or SNR to delineate brain
structures relevant to DBS surgery. Structural images
acquired at 7T exhibit rich informational content with
potential utility for clinical applications. Here we
utilized 7T images to create patient-specific anatomical
models to enhance pre-surgical DBS targeting as well as
post-surgical visualization of the DBS lead position and
orientation, including its four individual contacts.
These new visualization capabilities will enhance and
improve DBS outcomes.
|
1413. |
Imaging the human brainstem
at 7 Tesla using multi-modal echo-planar imaging
Florian Beissner1, Jonathan R. Polimeni1,
Marta Bianciardi1, Ville Renvall1,2,
Cornelius Eichner1,3, Vitaly Napadow1,
and Lawrence L. Wald1,4
1Athinoula A. Martinos Center for Biomedical
Imaging, Charlestown, MA, United States, 2Brain
and Mind Laboratory, Aalto University, Finland, 3Max
Planck Institute for Human Cognitive and Brain Sciences,
Leipzig, Germany, 4Harvard-MIT
Division of Health Sciences and Technology,
Massachusetts Institute of Technology, Cambridge, MA,
United States
The human brainstem is a notoriously difficult structure
to study with MRI. Here, we present an entirely EPI-based
approach that allows for the acquisition of T2*-weighted
functional, T1-weighted structural as well as
diffusion-weighted images at a resolution of 1.2 mm
isotropic. Due to matched voxel size and distortion,
BOLD and DTI images can be normalized to MNI space
applying transformation parameters estimated from the
T1-weighted EPI image, minimizing coregistration errors.
Using masked independent component analysis we were able
to detect brainstem nuclei at the single-subject level
and to depict their functional connectivity to the rest
of the brain.
|
1414. |
GRE reference scan for
robust reconstruction of high resolution slice and in-plane
accelerated 2D GE EPI at 7T
An T. Vu1, Steen Moeller1, Edward
Auerbach1, Kamil Ugurbil1, and
Essa Yacoub1
1University of Minnesota, CMRR, Minneapolis,
MN, United States
High temporal, high spatial resolution 2D EPI requires
acceleration along both the in-plane phase encode (e.g.
GRAPPA) and slice directions (e.g. multiband, MB). For
such acquisitions, image quality is particularly
sensitive to motion during segmented multi-shot
reference scans, which is lengthened by a factor of MB.
We propose the GRE flash for in-plane unaliasing of high
resolution slice accelerated 2D EPI. With this
technique, motion during reference scan related
artifacts and reconstruction noise are significantly
reduces especially at higher spatial resolutions
(<1.25mm isotropic). For 0.9mm data, we found SNR to
improve by 40% over conventional segmented EPI reference
scans.
|
1415. |
Comparison between
Single-Shot Diffusion Weighted Methodologies at 3 and 7
Tesla on Brain Volunteers
Eddy Solomon1, Noam Ben-Eliezer2,
Daniel K. Sodickson2, and Lucio Frydman1
1Chemical Physics, Weizmann Institute of
Science, Rehovot, Israel, 2Bernard
and Irene Schwartz Center for Biomedical Imaging,
Radiology, New York University School of Medicine, New
York, NY, United States
The potential of a recently proposed single-shot
methodology, SPatio-temporal ENcoding (SPEN), was
explored towards brain diffusion imaging on a 7T
whole-body scanner. To better evaluate this imaging
performance, studies were repeated at 3T, and done in
parallel with diffusion-weighted SE-EPI scans. In both
axial and coronal scans, SPEN evidenced a higher
robustness to overcome the B0-inhomogeneities that arise
particularly at 7T and also at 3T. The diffusion
measurements of the brain showed fair agreement between
both acquisitions methods, even despite the slight
differences evidenced between the 3T and 7T ADC maps.
|
1416. |
Clinical relevance of EPI
distortion correction in presurgical fMRI at 7T
Barbara Dymerska1, Florian Fischmeister1,2,
Alexander Geissler1,2, Eva Matt1,2,
Siegfried Trattnig1, Roland Beisteiner1,2,
and Simon Robinson1
1Departement of Biomedical Imaging and
Image-guided Therapy, Medical University of Vienna,
Vienna, Vienna, Austria, 2Department
of Neurology, Medical University of Vienna, Vienna,
Vienna, Austria
FMRI is increasingly being applied in presurgical
planning. Although ultra-high field provides higher tSNR
it also induces stronger geometric distortions. We
investigate the clinical relevance of distortion
correction using B0 field maps. Analysis of eight
patients performing hand and chin tasks at 7T revealed
that neglecting geometric distortions could lead to the
misidentification of the central sulcus. Moreover, the
distance between the pathology and activation could be
wrongly estimated, which could affect decisions about
resection margins. It is therefore important to correct
for distortions in patient fMRI data to ensure that
reliable clinical decisions are made.
|
1417. |
Feedback field control in
3D T2* imaging at 7T
Yolanda Duerst1, Michael Wyss1,
Bertram J Wilm1, Benjamin E Dietrich1,
Simon Gross1, David O Brunner1,
Thomas Schmid1, and Klaas P Pruessmann1
1ETH Zurich, Zurich, ZH, Switzerland
Field changes due to respiratory motion disturb
T2*-weighted imaging not only in 2D acquisition but also
in 3D. Due to the inherent averaging of 3D scans,
artifacts were not as pronounced as in 2D in the upper
parts of the brain but manifested as a general blurring
of the image. However, 3D T2*-weighted scans showed
strong ringing artifacts around cavities as well as
intensity modulations in the cerebellum. By using
real-time field feedback breathing induced
spatiotemporal field changes could be corrected and the
observed artifacts were strongly reduced.
|
1418. |
Effect of embedding media
on post-mortem MRI of formalin-fixed brain tissue at 7.0 T
Petr Dusek1,2, Vince Istvan Madai3,
Matthias Dieringer4,5, Fabian Hezel4,
Thoralf Niendorf4,5, Jan Sobesky3,5,
Radoslav Matej6, and Jens Wuerfel1,7
1Institute of Neuroradiology, University
Medicine Goettingen, Goettingen, Germany, 2Department
of Neurology and Center of Clinical Neuroscience,
Charles University in Prague, 1st Faculty of Medicine
and General University Hospital in Prague, Praha, Czech
Republic, 3Department
of Neurology and Center for Stroke Research Berlin
(CSB), Charité-Universitaetsmedizin, Berlin, Germany, 4Berlin
Ultrahigh Field Facility (B.U.F.F.), Max-Delbrueck
Center for Molecular Medicine, Berlin, Germany, 5Experimental
and Clinical Research Center (ECRC),
Charité-Universitaetsmedizin and Max Delbrueck Center
for Molecular Medicine (MDC), Berlin, Germany, 6Department
of Pathology and Molecular Medicine, Thomayer Teaching
Hospital, Praha, Czech Republic, 7NeuroCure
Clinical Research Center, Charité-Universitaetsmedizin,
Berlin, Germany
It is well known that formalin fixation of post-mortem
material affects its contrast mechanism and MR
characteristics. It is however not clear how these
parameters and image quality are affected by the medium
in which is the post-mortem material embedded during
scanning. Our goal was to compare different embedding
media (deuterium oxide (D2O), formalin, low-melting
temperature agarose and phosphate-buffered-saline) for
post-mortem MRI and ascertain which gives the best
signal-to-noise ratio and contrast results. Also, we
wanted to find out whether embedding medium has
influence on signal intensity of formalin fixed brain
slices. We employed T2 mapping, T1 mapping, T2* mapping,
MP-RAGE and TIRM sequences. The results for all
embedding media are shown.
|
1419. |
Two-voxel Hadamard encoded
semi-LASER spectroscopy for in
vivo MRS at
ultra-high field
Adam Berrington1, Peter Jezzard1,
Stuart Clare1, and Uzay Emir1
1FMRIB Centre, University of Oxford, Oxford,
Oxfordshire, United Kingdom
Large chemical shift displacement errors in MRS at
ultra-high field can limit SNR and lead to spurious
J-evolution across the VOI. Multi-voxel approaches are
particularly susceptible to poor localisation, resulting
in signal bleed between voxels. By incorporating two-voxel
Hadamard encoding with a semi-LASER localisation
sequence at 7T, we show that both CSD and inter-voxel
bleeding can be minimised. Demonstrating this method in
vivo on 4 volunteers, we are able to obtain highly
resolved spectra with efficient water suppression
simultaneously from both voxels. Metabolites such as
GABA, Glu, Lac and Ins can be reliably determined with
the method.
|
1420. |
Laminar features of
cortical natural sound processing in humans
Michelle Moerel1, Federico De Martino2,
An T Vu1, Valentin G Kemper2,
Kamil Ugurbil1, Elia Formisano2,
and Essa Yacoub1
1Department of Radiology, Center for Magnetic
Resonance Research, University of Minnesota,
Minneapolis, Minnesota, United States, 2Faculty
of Psychology and Neuroscience, Maastricht University,
Maastricht, Netherlands
We present preliminary data showing the feasibility of
examining frequency preference based on natural sounds
across cortical depths. The use of natural sounds will
enable the exploration of laminar tuning to features
beyond frequency, such as temporal and spectral
modulations.
|
1421. |
Brain Imaging with 7T vs.
9.4T: A direct Comparison of MR parameters and SNR
Rolf Pohmann1 and
Klaus Scheffler1,2
1Magnetic Resonance Center, Max Planck
Institute for Biological Cybernetics, Tübingen, Germany, 2Department
of Bioimaging, University of Tübingen, Germany
Increasing the magnetic field strength beyond 7 T is
expected to result in an increase of SNR, but this may
be limited by the more unfavorable relaxation times, the
B1inhomogeneity and the more difficult coil
design. Here, SNR and MR parameters are compared for
field strengths of 3 T, 7 T and 9.4 T. After correction
for flip angle variations, a strong gain in SNR of
almost a factor of two is found when going from 7 T to
9.4 T, but increasing inhomogeous B1-fields
and shorter T2* demand
for improved imaging techniques.
|
1422. |
Imaging oculomotor
subsystems in the cerebellum at 7 Tesla
Melissa A Batson1,2, Natalia Petridou3,
Dennis WJ Klomp3, Maarten A Frens2,
and Sebastian FW Neggers1
1Brain Center Rudolf Magnus, UMC Utrecht,
Utrecht, Netherlands, 2Neuroscience,
Erasmus Medical Center, Rotterdam, Zuid Holland,
Netherlands, 3Imaging
Division, UMC Utrecht, Utrecht, Netherlands
Using an innovative combination of high-density
multi-unit surface coils, dual transmission, ROI
shimming and 3D parallel imaging at 7T it is possible to
clearly image the deep and complex structures and
functions of the cerebellum during various motor tasks,
including oculomotor tasks requiring eye tracking.
Results demonstrate superior functional localisation
within both oculomotor vermis and, when a cognitive
component is present, in both CrusI and CrusII. In
addition, BOLD signal strengths vary with the magnitude
of difficulty of the task for both motor and cognitive
components in a manner consistent with the changes in
firing patterns observed in animal cerebellum.
|
1423. |
The optimization of B1
insensitive T1 weighted MP2RAGE sequence at high field.
Wanyong Shin1, Sehong Oh1, Tobias
Kober2,3, and Mark J Lowe1
1Radiology, Cleveland Clinic, Cleveland,
Ohio, United States, 2Advanced
Clinical Imaging Technology, Siemens Healthcare IM BM
PI, Lausanne, Switzerland, 3CIBM-AIT,
École Polytechnique Fédérale de Lausanne, Lausanne,
Switzerland
Large spatial B1 inhomogeneities are observed at
ultra-high magnetic field (=7T), which creates
non-uniform signal intensity across an image volume.
While MP2RAGE has shown the potential to minimize B1
variation, a long TR (>8s) is necessary to generate the
high signal to noise ratio and contrast to noise ratio
by providing the large dynamic contrast range. In this
study, we optimize fast MP2RAGE parameters to generate
T1 weighted contrast at 7T with 10% of image
non-uniformity in brain tissues. A healthy subject was
scanned with the optimized parameters according to
different TRs at 7T and brain segmentation results were
compared.
|
1424. |
Localized Spectroscopy
Without J-modulation at Ultra High Field
Clark Lemke1, Uzay Emir1, Peter
Jezzard1, Stuart Clare1, and Jamie
Near2
1FMRIB, University of Oxford, Oxford,
Oxfordshire, United Kingdom, 2Douglas
Institute, McGill University, Verdun, Quebec, Canada
In vivo quantification of coupled metabolites is
hampered by J-modulation. J-modulation manifests as an
echo time (TE) dependent modulation on the metabolite
signal leading to increased signal loss over and beyond
other relaxation processes. Short TE spectroscopy avoids
the effects of J-modulation but is complicated by a
broad baseline extending over the relevant frequency
range. This baseline can lead to decreased accuracy of
metabolite quantification. Here we present a localized
metabolite quantification pulse sequence designed to
remove J-modulation at long TE (<40 ms) to avoid
baseline contamination. The sequence (PRESS-JR) is
presented with phantom measurements.
|
1425. |
Functional ASL at 9.4 T – a
comparison between balanced SSFP and GRE-EPI readout
Jonas Bause1,2, Philipp Ehses1,3,
G. Shajan1, Klaus Scheffler1,3,
and Rolf Pohmann1
1High-Field Magnetic Resonance, MPI for
biological Cybernetics, Tuebingen, BW, Germany, 2Graduate
Training Center of Neuroscience, International
Max-Planck Research School, Tuebingen, BW, Germany, 3Department
for Biomedical Magnetic Resonance, University of
Tuebingen, Tuebingen, BW, Germany
Functional ASL has a higher specificity and
reproducibility than BOLD fMRI. However, the perfusion
related signal is typically in the range of a few
percent and the spatial and temporal resolution of
arterial spin labeling imaging rather limited. ASL at
ultra-high field can benefit from higher intrinsic SNR
and increased longitudinal relaxation times. We
investigated bSSFP and GRE-EPI as possible readout
schemes for fASL studies at 9.4 T and were able to
measure the first time stimulus evoked perfusion changes
in the human motor cortex at this field strength.
|
1426. |
Tractography of the
trigeminal nerve using 7T MRI
Christophe Lenglet1, Julien Sein1,
Julian Tokarev2, Andrew W Grande3,
Bharathi Jagadeesan4, and Pierre-Francois Van
de Moortele1
1Center for Magnetic Resonance Research,
University of Minnesota, Minneapolis, MN, United States, 2University
of Minnesota, Minneapolis, MN, United States, 3Department
of Neurosurgery, University of Minnesota, Minneapolis,
MN, United States, 4Department
of Radiology, University of Minnesota, Minneapolis, MN,
United States
We performed ultra high-field (7T) diffusion MRI and
probabilistic tractography on the trigeminal nerve in a
series of normal volunteers. We were able to reconstruct
the detailed three-dimensional course of fiber pathways
from individual divisions of the trigeminal nerve, as
they travel within its ganglion and the nerve root to
the brain stem. This information can be useful to better
understand the etiology of Trigeminal Neuralgia, a
poorly understood neurological disorder, which is
characterized by extremely painful episodes of facial
pain produced by routine stimuli like light touch.
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1427. |
Physiologic noise at 7T:
PESTICA for 3T obtains signals for pulse and respiration at
ultra-high field
Erik Beall1 and
Mark Lowe1
1Imaging Institute, Cleveland Clinic,
Cleveland, OH, United States
Physiologic noise in BOLD acquisitions is problematic
for fMRI and connectivity analyses, and is an increasing
problem at higher field strengths. There is one existing
software package, PESTICA, that can obtain signals at 3T
with the same periodicity as parallel monitored pulse
and respiration signals and thus can be used in
physiologic corrections. PESTICA uses spatial priors
generated at 3T and we test PESTICA at 7T, finding
promising results.
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1428. |
QUANTITATIVE ANALYSIS OF
LATERAL GENICULATE NUCLEUS (LGN) IN GLAUCOMA USING 7.0T MRI
Hye-Jin Jeong1, Jong-Yeon Lee2,
Jong-Hwan Lee2, Sang-Han Choi1,
Young-BO Kim1, and Zang-Hee Cho1
1Neuroscience Research Institute, Gachon
University, Incheon, Korea, 2Department
of Ophthalmology, Gachon University Gil Hospital,
Incheon, Korea
Glaucoma is characterized by progressive degeneration of
retinal ganglion cells (RGC) and their axons. Recent
neuroimaging studies in human glaucoma have demonstrated
degenerative changes in the visual pathway of brain
including lateral geniculate nucleus (LGN). However, a
precise assessment of the LGN is still a technical
challenge due to anatomic characteristics. Therefore,
our aim was to investigate the LGN atrophy in patients
with open-angle glaucoma using high-resolution 7.0 Tesla
MR imaging and correlation with retinal nerve fiber
layer (RNFL) thickness
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1429. |
High Spatial Resolution
Ophthalmic MRI at 7.0 Tesla in Healthy Subjects and in
Patients with Intraocular Masses
Andreas Graessl1, Jan Rieger2,
Soenke Langner3, Paul Krueger3,
Oliver Stachs4, Michael Schwerter1,
Max Muhle1, and Thoralf Niendorf1
1Berlin Ultrahigh Field Facility (B.U.F.F.),
Max Delbrück Center for Molecular Medicine (MDC),
Berlin, Berlin, Germany, 2MRI.TOOLS
GmbH, Berlin, Berlin, Germany, 3University
of Greifswald, Institute for Diagnostic Radiology and
Neuroradiology, Greifswald, Germany, 4University
of Rostock, Department of Ophthalmology, Rostock,
Germany
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1430. |
HIGH RESOLUTION BILATERAL
HIP JOINT IMAGING AT 7 TESLA
Jutta Ellermann1, Mikko Nissi2,3,
Dingxing Wang4,5, Sebastian Schmitter6,
Peter Kollasch4, and Pierre-Francois Van De
Moortele6
1Department of Radiology, University of
Minnesota, Minneapolis, MN, United States, 2Department
of Orthopaedic Surgery, University of Minnesota, MN,
United States, 3CMRR,
MN, United States, 4Siemens
Medical Solutions, MN, United States, 5University
of Minnesota, MN, United States, 6CMRR,
University of Minnesota, MN, United States
Recent availability of arthroscopic treatment options
for young patients with femoroacetabular impingement has
increased the importance of high-resolution hip MRI as a
diagnostic tool. If left untreated, this condition can
lead to premature osteoarthritis. Due to SNR gains,
imaging the hip joints at 7 Tesla is expected to improve
diagnostic precision by accurately assessing the state
of the thin (1-2 mm) acetabular cartilage,. 7T data
obtained with multichannel transmit RF and transmit B1
shim methods suggests that non-enhanced bilateral hip
MRI at ultrahigh fields provide the necessary gains in
contrast and resolution for accurate diagnostic
evaluation of the acetabular cartilage.
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1431. |
En route to clinical
ultrahigh field musculoskeletal MR using multi-purpose
transceiver RF modules for spine und shoulder imaging at 7.0
T.
Andreas Graessl1, Soenke Langner2,
Marko Hoehne3, Matthias A Dieringer1,
and Thoralf Niendorf1,4
1Berlin Ultrahigh Field Facility (B.U.F.F.),
Max Delbrück Center for Molecular Medicine (MDC),
Berlin, Berlin, Germany, 2University
of Greifswald, Institute for Diagnostic Radiology and
Neuroradiology, Greifswald, Germany, 3Helios
Kliniken, Berlin-Buch, Germany, 4Experimental
and Clinical Research Center (ECRC), Charité Campus Buch,
Humboldt-University, Berlin, Berlin, Germany
Given the limited availability of RF coils for MSK-MR
and recognizing the versatile range of musculoskeletal
MR applications this work pursues modular RF transceiver
configurations which suite the geometrical needs of a
broad spectrum of musculoskeletal anatomy. The
applicability of the modular configurations tailored for
spine and shoulder imaging is demonstrated in healthy
subjects. The multi-purpose configurations afforded the
acquisition of sub-millimeter spatial resolution images
of the shoulder. The sensitivity of the modular spine
TX/RX configuration facilitated a spatial resolution as
low as (0.13x0.13x1) mm³ for 3D GRE. This resolution
helped to depict small structures such as the facet
joints.
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1432. |
In vivo {1H}-13C
NMR spectroscopy of the human calf on a 7-T whole-body MR
tomograph
Tanja Platt1, Andreas Korzowski1,
and Peter Bachert1
1Medical Physics in Radiology, German Cancer
Research Center, Heidelberg, Baden-Württemberg, Germany
13C NMR spectroscopy is applied to observe
various metabolites in vivo, e.g. triacylglycerides
(TAG). High field strengths and 1H
spin decoupling enhance signal and information content
of 13C
NMR spectra. In this study high resolution 1H–decoupled 13C
NMR spectra of the human calf were obtained on an
experimental 7–T whole–body MR tomograph.
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1433. |
T1 and
T2 relaxation
times of the human calf at 7 Tesla
Anja M. Marschar1, Mathies Breithaupt1,
Moritz C. Berger1, and Armin M. Nagel1
1Medical Physics in Radiology, German Cancer
Research Center (DKFZ), Heidelberg, Germany
On 7 Tesla we measured the relaxation times T1 and T2 of
the human calf with separate consideration of muscle
tissue and subcutaneous fat tissue. A saturation
recovery and spin echo sequence with non-equidistantly
adapted TI and TE (that match to T1 and T2 respectively)
was used to get a linear sampling on the magnitude axis.
For comparison with lower field strength, all
measurements were also carried out on a 3T scanner and
are compared with literature.
|
1434. |
Echo-planar spectroscopic 13C
and 31P
NMR imaging of human calf muscle in
vivo on a
whole–body 7-T MR tomograph
Andreas Korzowski1, Tanja Platt1,
and Peter Bachert1
1Dept. of Medical Physics in Radiology,
German Cancer Research Center (DKFZ), Heidelberg,
Baden-Württemberg, Germany
In this study an echo–planar spectroscopic imaging
(EPSI) technique was applied to obtain localized
high–resolution in vivo 13C
and 31P
NMR spectra from human calf muscle on a whole–body 7–T
MR tomograph. Fast spectroscopic imaging techniques such
as EPSI where information from one spatial direction is
simultaneously encoded with the spectral information
reduce the measurement time strongly.
|
1435. |
3D EPSI - Exploring the
potential of 3D spectroscopic imaging of the prostate at 7
tesla
Arjan D. Hendriks1,2, Tijl A. van der Velden1,
Mariska P. Luttje1, Vincent O. Boer1,
Peter R. Luijten1, and Dennis W.J. Klomp1
1Imaging Division, University Medical Center,
Utrecht, Netherlands, 2Biomedical
NMR, Department of Biomedical Engineering, Eindhoven
University of Technology, Eindhoven, Netherlands
To guide prostate cancer treatment, it is important to
know the aggressiveness of the prostate tumor in
question. Magnetic Resonance Spectroscopic Imaging (MRSI)
has great potential to determine this aggressiveness,
especially considering current progress of ultra-high
field MR systems in separating choline from polyamines.
A 3D EPSI acquisition & reconstruction method was
developed and compared with current 2D MRSI methods.
Found is that high field three-dimensional spectroscopic
imaging can be performed within the prostate, using an
EPSI sequence, avoiding extended scan time.
|
1436. |
En Route to Probing Human
Myocardial Microstructure in vivo Using Susceptibility Based
MRI at 7.0 T
Till Huelnhagen1, Fabian Hezel1,
and Thoralf Niendorf1,2
1Berlin Ultrahigh Field Facility (B.U.F.F.),
Max Delbrueck Center for Molecular Medicine, Berlin,
Germany, 2Experimental
and Clinical Research Center, a joint cooperation
between the Charite Medical Faculty and the Max
Delbrueck Center, Berlin, Germany
The complex microstructure of the myocardium is pivotal
for cardiac function and can provide important
information about the underlying (bio)physical
principles and (patho)physiological mechanisms. Probing
human myocardial fiber structure in vivo has been
described, but remains challenging due to cardiac and
respiratory motion. Susceptibility based MRI provides
excellent contrast which can be used to investigate
tissue microstructure and track fibers in the brain.
Recognizing this opportunity the work explores the
applicability of susceptibility weighted MRI for probing
human myocardial microstructure in vivo at 7.0 T.
|
1437. |
Detection of hepatic
glycogen by 1D ISIS localized 13C
MRS at 7T.
Martin Krssak1,2, Martin Gajdosik2,
Ladislav Valkovic2, Wolfgang Bogner2,
Michael Krebs1, Anton Luger1,
Siegfried Trattnig2, and Marek Chmelik2
1Division of Endocrinology and Metabolism,
Department of Internal Medicine III, Medical University
of Vienna, 1090, Austria, 2High
Field MR Centre, Department of Biomedical Imaging and
Image-Guided Therapy, Medical University of Vienna,
Wien, Austria
The aim of this study was to introduce and test the 13C
MRS localization scheme suitable for the measurement of
hepatic glycogen at 7T in short acquisition time. One
dimensional slice selective version of recently
introduced fully adiabatic extended ISIS sequence was
proposed and tested on phantom and in vivo on healthy
volunteers. 1D ISIS scheme applied at 7T presented
optimal localization performance and sufficient signal
to noise of natural abundance 1-13C hepatic
glycogen doublet in relatively short acquisition times
(4´16´´).
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