13:30 |
0662. |
Micro Magnetic Resonance x,y-Gradient
System for Microscopic Samples
-permission withheld
Markus V. Meissner1, Robert Ch. Meier1,
Peter T. While1, Ali Moazenzadeh2,
and Jan G. Korvink1,3
1Lab. for Simulation, IMTEK - University of
Freiburg, Freiburg, Germany, 2Lab.
for Microactuators, IMTEK - University of Freiburg,
Freiburg, Germany, 3Freiburg
Institute for Advanced Studies – FRIAS, University of
Freiburg, Freiburg, Germany
We present a micro-integrated gradient chip-design
manufactured by using multiple, wire-bonded conductors.
By placing the gradient conductors close to a
microscopic sample, a particular strong magnetic field
gradient can be achieved. The miniaturized gradient
coils are based on a customized coil design,
manufactured by using micro fabrication technology. A
chip design was studied, based on a sandwich structure,
consisting of straight, low profile wire-bonded gradient
conductors, embedded and aligned by using permanent dry
film photo-resist. The gradient conductors are
integrated on a 2cmx2cm large glass substrate and the
layer-based conductor alignment method enables
statically determined bond-wire fixation.
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13:42 |
0663. |
Genuine Minimum Power
Gradient Coil Design Accounting for Gaps Between Tracks or
Wires
Peter T. While1, Michael S. Poole2,
and Jan G. Korvink1,3
1Department of Microsystems Engineering (IMTEK),
Laboratory for Simulation, University of Freiburg,
Freiburg im Breisgau, Baden-Württemberg, Germany, 2Institute
of Neuroscience and Medicine - 4, Forschungszentrum
Jülich GmbH, Jülich, Nordrhein-Westfalen, Germany, 3Freiburg
Institute for Advanced Studies (FRIAS), University of
Freiburg, Freiburg im Breisgau, Baden-Württemberg,
Germany
Gradient coils are often designed in terms of a
continuous minimum power current density that is
discretized to obtain the locations of coil tracks or
wires. However, the existence of finite gaps between
these conductors and a maximum conductor width leads to
an underestimation of coil resistance. In this work, a
current density mapping is proposed that accounts for
these effects and is optimized to generate genuine
minimum power coils post-discretization (i.e. accounting
for build method). Many common coil types are surveyed
and it is demonstrated that up to a 30% reduction in
power dissipation is possible in certain cases.
|
13:54 |
0664.
|
Integrated Parallel
Reception, Excitation, and Shimming (IPRES)
Hui Han1, Allen W. Song1, and
Trong-Kha Truong1
1Brain Imaging and Analysis Center, Duke
University, Durham, NC, United States
A new general concept is proposed for integrated
parallel reception, excitation, and shimming (iPRES). It
uses a novel coil design allowing an RF current and a DC
current to flow in the same physical coil to perform
parallel excitation/reception and B0 shimming
with a unified coil array. To demonstrate its
feasibility, proof-of-concept phantom experiments were
performed with a two-coil array. The shim field induced
by individually optimized DC currents applied in both
coils was able to significantly reduce nonlinear B0 inhomogeneities
introduced in the phantom, demonstrating that parallel
excitation/reception and B0 shimming
can be performed with a unified coil system.
|
14:06 |
0665.
|
Combined Shim-RF Array for
Highly Efficient Shimming of the Brain at 7 Tesla
Jason P. Stockmann1, Thomas Witzel1,
James N. Blau1, Jonathan R. Polimeni1,
Wei Zhao1, Boris Keil1, and
Lawrence L. Wald1
1Athinoula A. Martinos Center for Biomedical
Imaging, Department of Radiology, Massachusetts General
Hospital, Charlestown, Massachusetts, United States
Multi-coil shimming shows great potential for canceling
B0 inhomogeneity at ultra-high field, but its
performance has been limited by the need to leave space
for RF receive coils, pushing the shim coils further
away from the body. We overcome this problem by
combining the shim and receive RF currents through a
single conductor thus optimizing the performance of both
systems by bringing them as close to the body as
possible. Experimental results show that shim-RF coils
provide equivalent SNR to conventional receive coils and
single loop shim structures can effectively shim the
brain with <5A current per loop.
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14:18 |
0666.
|
Matrix Gradient System:
Concept and Performance Evaluation
Feng Jia1, Gerrit Schultz1, Anna
M. Welz1, Sebastian Littin1, Hans
Weber1, Jürgen Hennig1, and Maxim
Zaitsev1
1Dept. of Radiology, Medical Physics,
University Medical Center Freiburg, Freiburg, Germany
Encoding with nonlinear encoding fields (SEMs) has
raised increasing interest in the past few years. Matrix
coils appear to offer a high flexibility in generating
customized SEMs and are particularly promising for
localized high resolution imaging applications such as
PatLoc or ExLoc. However, up to now, it is still an open
question of how to assess the performance of such matrix
coils. In this work we propose a new performance measure
that is oriented towards optimal local encoding. An
optimization problem is formulated that results in
high-performance cylindrical matrix coil designs with a
high number of elements. The results are tested and the
analysis reveals novel features of matrix coil designs.
|
14:30 |
0667. |
Dynamic Multi-Coil Shimming
of the Rat Brain at 11.7 Tesla
Christoph Juchem1, Basavaraju G. Sanganahalli1,
Peter Herman1, Peter B. Brown1,
Scott McIntyre1, Terence W. Nixon1,
and Robin A. de Graaf1
1MR Research Center (MRRC), Yale University,
New Haven, CT, United States
The in vivo rat model is a work horse in neuroscientific
and preclinical MR research, however, excellent magnetic
field homogeneity is required for meaningful results.
Dynamic multi-coil (DMC) shimming is shown to
successfully minimize magnetic field distortions
encountered in the rat brain at 11.7 Tesla. While EPI
with static, third order spherical harmonic shimming
suffers from signal loss and image deformation, the
brain outline is preserved with DMC-shimmed EPI. The
minimization of signal loss and the improvement of the
spatial accuracy of EPI with DMC shimming are expected
to critically benefit a wide range of preclinical and
neuroscientific MR research.
|
14:42 |
0668. |
Dynamic Field Monitoring by
20 Channel Field Probes Integrated with 12 Channel Head Coil
Ying-Hua Chu1, Yi-Cheng Hsu2,
Wen-Jui Kuo3, and Fa-Hsuan Lin1
1Institute of Biomedical Engineering,
National Taiwan University, Taipei, Taiwan, 2Department
of Mathematics, Nnational Taiwan University, Taipei,
Taiwan, 3Institute
of Neuroscience, National Yang-Ming University, Taipei,
Taiwan
We develop a 20-channel field probe system integrated
with a 12-channel head coil array to dynamically detect
the frequency fluctuations caused by the subject, eddy
current, or other systemic changes during the 3T MRI
scan. The frequency shift was continuously estimated by
the phase difference monitored by the field probes. This
information was found useful in dynamic tracking of the
magnetic field distribution and the k-space trajectory.
Our results suggest that, under the limit of a fixed
number of RF channels, an integrated RF field probe and
coil array system holds promise of high quality parallel
MRI.
|
14:54 |
0669.
|
Full 3rd Order
Real-Time Shim Feedback for Field Stabilization and Its
Application in Brain MRI at 7T
Yolanda Duerst1, Bertram J. Wilm1,
Benjamin E. Dietrich2, David Otto Brunner2,
Christoph Barmet2,3, Thomas Schmid1,
Signe Johanna Vannesjo1, and Klaas P.
Pruessmann1
1Institute for Biomedical Engineering,
University of Zurich and ETH Zurich, Zurich,
Switzerland, 2Institute
for Biomedical Engineering, University and ETH Zurich,
Zurich, Switzerland, 3Skope
Magnetic Resonance Technologies, Zurich, Switzerland
Spatio-temporal field fluctuations caused by hardware
imperfections or physiological motion can lead to signal
loss through increased T2* decay or off-resonant RF
pulses and severely degrade image quality. We present a
first implementation of a concurrent real-time feedback
system correcting for full 3rd order spherical harmonics
field changes. A proportional-integral controller was
used to address gradient and shim coils of a whole-body
scanner to actively compensate field fluctuations. The
control loop achieved robust field stabilization of
breathing induced field perturbations and significantly
enhanced image quality of a commonly used T2*-weighted
gradient-echo scan which otherwise strongly suffers from
breathing artifacts.
|
15:06 |
0670. |
A Low-Cost, Mechanically
Simple Apparatus for Measuring Eddy Currents
Kyle M. Gilbert1, L. Martyn Klassen1,
and Ravi S. Menon1
1Robarts Research Institute, The University
of Western Ontario, London, Ontario, Canada
A transmit/receive array is presented that allows for
the measurement of eddy currents of the zeroth and first
orders, simultaneously. The coil system is low-cost and
mechanically simple. The performance of the coil system
is evaluated based on metrics required to accurately
record the spatial and temporal variation of eddy
currents.
|
15:18 |
0671.
|
Digital Cross-Term
Pre-Emphasis for Higher-Order Dynamic Shimming
Signe Johanna Vannesjo1, Benjamin E. Dietrich1,
Matteo Pavan1, Christoph Barmet1,2,
and Klaas P. Pruessmann1
1Institute for Biomedical Engineering,
University and ETH Zurich, Zurich, Switzerland, 2Skope
Magnetic Resonance Technologies, Zurich, Switzerland
Dynamic shimming holds promise to improve B0 homogeneity
for a range of applications, however requires fast
updating of the shim fields. Eddy currents limit the
shim settling times and also produce strong cross-term
field components. Here we show the feasibility of
digital cross-term pre-emphasis applied to the input
shim waveforms. The pre-emphasis is calculated based on
shim impulse response functions (SIRFs) measured with a
dynamic field camera. It is shown that settling times
can be shortened and cross-term responses much reduced
with this approach. The digital pre-emphasis allows for
full flexibility in shaping the response, within
hardware limitations.
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