Sorting Out Some Artifacts |
Wednesday 22 April 2009 |
Room 314 |
16:00-18:00 |
Moderators: |
Brian A. Hargreaves and X. J. Zhou |
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16:00 |
567. |
Embedded PLACE Correction for
Geometric Distortion and N/2 Ghosting in Single-Shot
EPI |
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Qing-San Xiang1,
Frank Q. Ye2
1Radiology, University of British Columbia,
Vancouver, BC, Canada; 2Neurophysiology
Imaging Facility, National Institute of Mental
Health, NIH, Bethesda, MD, USA |
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Geometric distortion and
N/2 ghosting are two major artifacts in EPI. They
can be simultaneously and instantaneously suppressed
by a new method based upon Phase Labeling for
Additional Coordinate Encoding (PLACE). Since all
data are acquired within a single RF excitation, the
correction is instant and thus the new method is
termed iPLACE. A few central k-space lines are
collected 3 times. This allows an effective N/2
ghost suppression, as well as further distortion
correction. iPLACE has been demonstrated to be
effective by phantom experiments performed on a 4.7
T scanner. |
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16:12 |
568. |
Understanding the Origin of
Image Intensity Displacement in Spiral-In Versus
Spiral-Out Acquisitions |
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Kimberly D. Brewer1,2,
Chris V. Bowen2,3, Steven D. Beyea2,3
1Department of Physics, Dalhousie University,
Halifax, Nova Scotia, Canada; 2Institute
for Biodiagnostics (Atlantic), National Research
Council of Canada, Halifax, Nova Scotia, Canada;
3Departments of Physics, Radiology and
Biomedical Engineering, Dalhousie University,
Halifax, Nova Scotia, Canada |
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Pulse sequences using
reverse spiral trajectories (i.e. Spiral-In) are
commonly used to avoid signal loss and distortion in
regions with susceptibility field gradients (SFGs).
Although there have been theories postulated as to
why Spiral-In is superior to Spiral-Out, none of
them explain why Spiral-In continues to recover more
signal in SFG regions, even when acquired with an
acquisition window that begins after that of
Spiral-Out. We explored this phenomenon further
through use of a phantom that produces well-known
field patterns as well as computer simulations. |
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16:24 |
569. |
Simple Robust Estimation of
Gradient Delays for Spiral MRI |
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Ryan Keith Robison1,
James Grant Pipe1
1Keller Center for Imaging Innovation, Barrow
Neurological Institute, Phoenix, AZ, USA |
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Timing delays between
gradient transmission and data sampling are a major
source of artifact in spiral MRI. These delays
result most often from eddy currents, among other
things. Many of the common methods used to measure
these delays require specialized hardware, advanced
pulse sequences, or very small phantoms. A simple
technique is proposed to measure gradient delays
associated with a spiral sequence on all three
gradient axes in six excitations. |
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16:36 |
570. |
Eliminating Metal Artifact
Distortion Using 3D-PLACE |
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Michael Nicholas Hoff1,
Qing-San Xiang1,2
1Department of Physics, University of British
Columbia, Vancouver, BC, Canada; 2Department
of Radiology, University of British Columbia,
Vancouver, BC, Canada |
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A method is presented
which removes in-plane and through-plane distortion
stemming from MRI of a metallic hip prosthesis. Two
images are acquired using 3D turbo spin-echo
sequences differing only by added gradient lobes
along the frequency encoding (FE) direction, which
yield a relative phase ramp across the
field-of-view. The undistorted FE coordinate for
each voxel is encoded into the additional phase
information contained in the phase difference image.
Distortion correction of a Lego structure
surrounding the prosthesis is demonstrated. The
sequence modification is straightforward, the
required scan time is minimal, and phase unwrapping
is unnecessary for this technique. |
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16:48 |
571. |
A Method to Remove Nyquist
Ghosts from Echo Planar Images (EPI) Using UNFOLD |
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W. Scott Hoge1,
Huan Tan2, Robert A. Kraft2
1Radiology, Brigham and Women's Hospital,
Boston, MA, USA; 2Wake Forest University
School of Medicine, Winston-Salem, NC, USA |
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Nyquist ghosts are a
persistent artifact in echo planar imaging (EPI),
and occur when data sampled along positive and
negative read-out gradients is inconsistent.
Previous methods to correct these effects include
double-sampled EPI, which doubles the echo train
length leading to greater magnetic susceptibility
artifacts, and echo interleave strategies that carry
a cost of reduced temporal resolution. Here, we
present an approach using the slightly modified
trajectory common to interleave strategies, but
utilizing UNFOLD in place of interleaving to combine
the data. This has the advantage of greatly reducing
visible Nyquist ghosts while maintaining 90% of the
original temporal sampling bandwidth. |
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17:00 |
572. |
B1 Correction Using Dual Tau
Look-Locker (DτLL) |
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Trevor Wade1,2,
Brian Rutt1
1Robarts Research Institute, London, Ontario,
Canada; 2Biomedical Engineering,
University of Western Ontario, London, Ontario,
Canada |
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A new method of mapping
the transmit B1 field is introduced that is capable
of rapidly producing 3D B1 maps at low flip angles
without relying on the double angle assumption. It
is based on the accelerated 3D Look-Locker sequence
and has been compared to both the standard double
angle method as well as a double angle
implementation of the 3D Look-Locker sequence. |
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17:12 |
573. |
Sense Shimming (SSH), First
In-Vivo Results |
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Daniel Nicolas
Splitthoff1, Maxim Zaitsev1
1Dept. of Diagnostic Radiology, Medical
Physics, University Hospital Freiburg, Freiburg, BW,
Germany |
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Recently, a new shimming
method has been introduced, named Sense Shimming, or
SSH. Due to expected complication regarding chemical
shift artefacts and physiological noise, up to now
only phantom measurements have been shown. We here
present the first in-vivo measurements. |
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17:24 |
574. |
Simultaneous Fat Suppression
and Band Reduction with Large-Angle
Multiple-Acquisition BSSFP |
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Neal Kepler Bangerter1,2,
Garry E. Gold 3, Glen R. Morrell2,
Brian Andrew Hargreaves3
1Electrical
& Computer Engineering, Brigham Young University,
Provo, UT, USA; 2Radiology, University of
Utah, Salt Lake City, UT, USA; 3Radiology,
Stanford University, Stanford, CA, USA |
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Balanced SSFP (bSSFP) is
a fast and highly SNR-efficient imaging technique,
but can suffer from characteristic bands of signal
loss in the presence of field inhomogeneity.
Effective fat suppression with bSSFP is also
challenging in regions with large field
inhomogeneities. While techniques exist for both
banding artifact reduction and fat suppression with
bSSFP, they are sometimes incompatible and typically
require a significant increase in scan time. In this
work, we present a novel approach to simultaneous
fat suppression and banding artifact reduction in
bSSFP. |
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17:36 |
575. |
Oscillating Radial
Trajectories for Reduced Undersampling Artifacts |
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Rizwan Ahmad1,
Lee C. Potter2, Periannan Kuppusamy1
1Davis Heart and Lung Research Institute,
Department of Internal Medicine,, The Ohio State
University, Columbus, OH, USA; 2Department
of Electrical and Computer Engineering, The Ohio
State University, Columbus, OH, USA |
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We have proposed an
oscillating radial trajectory of k-space which
significantly improves the reconstruction quality as
compared to the traditional radial sampling. Adding
oscillations reduces the coherency of the radial
trajectory and hence minimizes the aliasing
artifacts. In contrast to the other methods for
generating randomized trajectories, the proposed
k-space trajectories are smooth and hence easy to
implement on a conventional MRI gradient coil
system. We present a systematic way of generating
oscillating radial trajectories and show an
improvement over the traditional radial sampling
using simulations. |
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17:48 |
576. |
Effects of Concomitant Fields
on Short-Time-Scale Noble Gas Diffusion Measurements |
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Michael Carl1,2,
John P. Mugler III3, Gordon D. Cates2,
Wilson Miller3
1GE Healthcare, Applied Science Lab,
Milwaukee, WI, USA; 2Physics, University
of Virginia, Charlottesville, VA, USA; 3Radiology,
University of Virginia, Charlottesville, VA, USA |
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In previous work we
described a specialized pulse sequence designed to
access very short diffusion times using noble-gas
NMR. In the present work we study the quantitative
effects that concomitant fields have on the
resulting diffusion measurements, and develop
strategies for minimizing or correcting for these
effects. We derived an approximate threshold
criterion to determine under what circumstances
concomitant field distortions remain insignificant
compared to the desired diffusion attenuation.
Phantom diffusion experiments were performed to
confirm our results. |
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