New Contrast
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Monday May 9th
Room 511D-F |
16:30 - 18:30 |
Moderators: |
Ludovic De Rochefort and Klaas Pruessmann |
16:30 |
120. |
SEMI-TWInS: Simultaneous
Extraction of Myelin and Iron using a T2*-Weighted
Imaging Sequence
Ferdinand Schweser1,2, Andreas Deistung1,
Berengar Wendel Lehr3, Karsten Sommer1,4,
and Jürgen R. Reichenbach1
1Medical Physics Group, Dept. of Diagnostic
and Interventional Radiology 1, Jena University
Hospital, Jena, Germany, 2School
of Medicine, Friedrich Schiller University of Jena,
Jena, Germany, 3Medical
Physics Group, Dept. of Diagnostic and Interventional
Radiology, Jena University Hospital, Jena, Germany, 4School
of Physics and Astronomy, Friedrich Schiller University
of Jena, Jena, Germany
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16:42 |
121. |
In vivo Evidence of
Susceptibility Anisotropy and Susceptibility Tensor Imaging
of Human Brain
Wei Li1, Bing Wu1, and Chunlei Liu1,2
1Brain Imaging & Analysis Center, Duke
University, Durham, NC, United States, 2Radiology,
Duke University, Durham, NC, United States
Previously, the magnetic susceptibility of brain tissue
is generally assumed to be isotopic. Recently, emerging
evidences from animal studies and in vitro brain
specimens started to show the directionality of
susceptibility. In this study, we demonstrated the
evidence of magnetic susceptibility anisotropy from in
vivo human brain by comparing susceptibility map with
the diffusion tensor imaging results and comparing
susceptibility obtained from different orientations.
Further, the susceptibility tensor is calculated, which
shows varied gray and white matter contrast among the
three principal eigenvalues. These results provide
convincing evidences that the magnetic susceptibility of
in vivo human brain is anisotropic.
|
16:54 |
122. |
Origin of phase contrast:
insight from susceptibility, R2* and element imaging by LA-ICP-MS
Ana-Maria Oros-Peusquens1, Andreas Matusch2,
Johannes Lindemeyer3, Sabine Johanna Becker4,
and Nadim Jon Shah1
1Institute of Neuroscience and Medicine
(INM-4), Research Centre Juelich, Juelich, NA, Germany, 2INM-2,
Research Centre Juelich, Germany, 3INM-4,
Research Centre Juelich, Germany, 4ZCH,
Research Centre Juelich
MR-based maps of susceptibility, field and R2*
distribution were compared to element imaging using
Laser Ablation Inductively Coupled Mass Spectrometry
(LA-ICP-MS). The distributions of carbon (C) and iron
(Fe), elements thought to be the main determinants of
susceptibility and phase contrast, show much more detail
than the susceptibility and field maps obtained from
MRI. A linear dependence between R2* and Fe
concentration has been confirmed in a limited, ROI-based
analysis. A clustering analysis of the distribution of
15 elements shows features which are unclear in the
phase or susceptibility distributions but can be found
in the mixed-contrast T2*-weighted high-resolution
images.
|
17:06 |
123. |
Active Contrast Modulation
of Iron Oxide Nanoparticles using Rotary Saturation
Bo Zhu1,2, Thomas Witzel1,2, Shan
Jiang3, Daniel G. Anderson3,
Robert S. Langer3, Bruce R Rosen1,2,
and Lawrence L Wald1,2
1Harvard-MIT Division of Health Sciences and
Technology, Massachusetts Institute of Technology,
Cambridge, MA, United States, 2Department
of Radiology, Athinoula A. Martinos Center for
Biomedical Imaging, Massachusetts General Hospital,
Charlestown, MA, United States, 3Department
of Chemical Engineering, Massachusetts Institute of
Technology, Cambridge, MA, United States
A novel contrast mechanism for imaging iron oxide
contrast agents is described based on the Rotary
Saturation effect, whereby the oscillating magnetic
fields generated from vibrating iron oxide nanoparticles
resonantly couples with the spin system to produce
tunable signal changes. We demonstrate this active
contrast modulation with a block-design experiment
interleaving vibration of the contrast agent on and off
resonance relative to the rotating frame resonance
frequency, and observe statistically significant signal
changes only for ROIs adjacent to the nanoparticles. We
envision contrast modulation of iron oxide nanoparticles
in-vivo using sound waves or endogenous motion to
generate the nanoparticle vibration.
|
17:18 |
124. |
A General T1 Relaxation
Model for Spin-Lock MRI using a Rotary Echo Pulse
Jing Yuan1, and Yi-Xiang Wang1
1Department of Imaging and Interventional
Radiology, The Chinese University of Hong Kong, Shatin,
New Territories, Hong Kong
T1ñ relaxation was conventionally described to follow a
purely monoexponential decay as a function of the spin
lock time. However, the validity of this monoexponential
decay may be violated in the presence of field
inhomogeneities, especially at extremely low spin lock
frequencies. T1ñ relaxation behavior using a rotary echo
spin lock pulse was studied using the Bloch Equation and
the rotation matrix transformation. A general analytical
expression was derived to describe the T1ñ relaxation at
different spin lock frequencies in the presence of B0
inhomogeneity, and verified experimentally by phantom
and in vivo imaging from 50Hz to 500Hz.
|
17:30 |
125. |
Comparing Electric
Properties Tomography at 1.5, 3 and 7 T
Astrid L.H.M.W. van Lier1, Tobias Voigt2,
Ulrich Katscher2, and Cornelis A.T. van den
Berg1
1Radiotherapy, UMC Utrecht, Utrecht,
Netherlands, 2Philips
Research Europe, Hamburg, Germany
Recently, the principle feasibility of Electrical
Properties Tomography has been shown at different field
strengths, 1.5T, 3T, and 7 T. To determine the optimal
field strength for EPT, a systematic study was performed
comparing phantom measurements and simulations. The
influence of SNR and the error induced by using the
transceiver phase instead of the transmit phase on the
reconstruction are evaluated.
|
17:42 |
126. |
Imaging Electrical
Properties of the Human Brain using a 16-channel Transceiver
Array Coil at 7T
Xiaotong Zhang1, Pierre-Francois Van de
Moortele2, Sebastian Schmitter2,
and Bin He1
1Department of Biomedical Engineering,
University of Minnesota, Minneapolis, Minnesota, United
States, 2Center
for Magnetic Resonance Research, University of
Minnesota, Minneapolis, Minnesota, United States
The electrical properties (EPs, conductivity and
permittivity) of brain tissues provide important
information for basic brain research and clinical
diagnosis of neurological disorders. They also play an
important role in SAR calculation. In this study, using
a 16-channel transceiver array coil at 7T and based on
existing B1-mapping technique, we have developed a novel
method to estimate both magnitude and absolute phase
distribution of transmit/receive B1 fields, and the
electrical conductivity and relative permittivity
values. We report our pilot results in a human brain for
electrical property imaging using a high field MRI
system.
|
17:54 |
127. |
In vivo Glioma
Characterization using MR Conductivity Imaging
Tobias Voigt1, Ole Väterlein2,
Christian Stehning1, Ulrich Katscher1,
and Jens Fiehler2
1Philips Research Laboratories, Hamburg,
Germany, 2Department
of Neuroradiology, University Medical Centre Hamburg-Eppendorf,
Hamburg, Germany
Conductivity imaging provides a new quantitative
contrast for MRI. In the presented study conductivity
imaging is applied in a routine clinical environment.
First clinical results of glioma patients are reported
and compared with healthy volunteers. In vivo
conductivity of glioma is found considerably higher than
healthy white matter conductivity.
|
18:06 |
128. |
Real-Time Conductivity
Mapping using Balanced SSFP and Phase-Based Reconstruction
Christian Stehning1, Tobias Ratko Voigt2,
and Ulrich Katscher1
1Philips Research Laboratories, Hamburg,
Germany, 2Institute
of Biomedical Engineering, University of Karlsruhe,
Karlsruhe, Germany
A volumetric, real-time conductivity mapping method
based on balanced SSFP and an image phase based
reconstruction is presented. It provides sufficient
temporal resolution to visualize the dissolving of salt
in a water phantom.
|
18:18 |
129. |
Panel Discussion
Richard W. Bowtell, Ludovic De Rochefort, Klaas Pruessmann &
Daniel K. Sodickson |
|