08:00 |
0993.
|
Application of a dipolar
model to inhomogeneous magnetization transfer (ihMT)
Gopal Varma1, Olivier M Girard2,
Valentin Prévost2, Aaron K Grant1,
Guillaume Duhamel2, and David C Alsop1
1Radiology, Division of MR Research, Beth
Israel Deaconess Medical Center, Harvard Medical School,
Boston, Massachusetts, United States, 2CRMBM
UMR 7339, CNRS and Aix-Marseille Université, Marseille,
France
The inhomogeneous magnetization transfer technique (ihMT)
has gained attention for producing myelin selective
images, but a model for its mechanism has not been
established. This work develops a model based on
existing applications of the Redfield-Provotorov theory
to regular MT that predicted a dipolar order. The
results from model fitting to mouse and human data
provide measurable values for a relaxation time of the
dipolar order, TD,
consistent with the observable ihMT signal. The
variation observed in TD between
different regions of interest might provide further
insight into the selectivity and/or optimization of the
ihMT technique.
|
08:12 |
0994. |
Towards a quantitative
theory for inhomogeneous magnetization transfer
Scott D. Swanson1, Dariya I. Malyarenko2,
and Mario L. Fabiilli2
1Department of Radiology, University of
Michigan, Ann Arbor, Michigan, United States, 2Department
of Radiology, University of Michigan, Michigan, United
States
ihMT theory
|
08:24 |
0995.
|
Further Evidence of an
Orientation Dependence of Magnetization Transfer Parameters
from Investigations in Post-Mortem Marmoset Brain
Henrik Marschner1, Riccardo Metere1,
Stefan Geyer1, André Pampel1, and
Harald E. Möller1
1Nuclear Magnetic Resonance, Max Planck
Institute for Human Cognitive and Brain Sciences,
Leipzig, Sachsen, Germany
We examine the apparent dependence of qMT parameters, in
particular those of the T2b relaxation time of bound
protons, on the white matter fiber orientation in a
Post-Mortem Marmoset Brain. The observed angular
dependence in the post-mortem data for highly ordered WM
supports the hypothesis of orientation dependence of the
RF absorption lineshape that was observed in human brain
in vivo. Here, variation of the orientation is achieved
by rotating the sample in the magnetic field.
|
08:36 |
0996. |
Exploring a Flexible Pulse
Design for Studying Magnetization Transfer
Peter van Gelderen1, Xu Jiang1,
and Jeff H Duyn1
1AMRI, LFMI, NINDS, National Institutes of
Health, Bethesda, MD, United States
Magnetization Transfer (MT) contrast is sensitive to
brain myelination but lacks specificity, while
quantification is difficult and requires lengthy
experiments, including T1 measurement. Pulsed MT
experiments may offer a simpler way to obtained
quantitative measures, such as bound pool fraction and
transfer rates. Here we explore a variation on a
binominal pulse design for optimizing the pulsed MT
experiment and demonstrate its application to study MT
contrast in white matter.
|
08:48 |
0997. |
Contrast Generation with a
Novel Adiabatic On-Resonance Magnetization Transfer
Preparation (MT-Prep)
Wolfgang G Rehwald1, David C Wendell2,
Elizabeth R Jenista2, Han W Kim2,
Enn-Ling Chen2, Igor Klem2, and
Raymond J Kim2
1Siemens Healthcare, Durham, NC, United
States, 2Cardiology,
Duke University Medical School, Durham, North Carolina,
United States
Magnetization transfer contrast could be a clinically
and technically advantageous alternative to T2-contrast.
It would be useful for imaging edema and creating
tissue-blood contrast, if its energy and power
requirements did not exceed the capabilities of most
clinical MRI scanners. To address this issue, we
designed an efficient adiabatic on-resonance MT module
that imparts significant MT-weighting while remaining
within the energy and power constraints of most clinical
MRI scanners. In ten cardiac patients, we compared this
module to standard high-power off-resonance MT
preparation and established its image quality and
contrast equivalence while only requiring a fraction of
its energy.
|
09:00 |
0998.
|
Study of Bound Proton T2
and Magnetization Transfer using Pulsed MT
Xu Jiang1,2, Peter van Gelderen1,
Xiaozhen Li1, Emily Leibovitch3,
Pascal Sati4, Afonso C. Silva5,
and Jeff H Duyn1
1AMRI, LFMI, NINDS, NIH, Bethesda, MD, United
States, 2Department
of Physics, University of Maryland, College Park, MD,
United States, 3Viral
Immunology Section, Neuroimmunology Branch, NINDS, NIH,
Bethesda, MD, United States, 4Translational
Neuroradiology Unit, NINDS, NIH, Bethesda, MD, United
States, 5CMU,
LFMI, NINDS, NIH, Bethesda, MD, United States
Accurate knowledge of the T2 of bound (non-water)
protons is very essential for optimization and
quantification of MT contrast. Using optimized, 2ms long
binomial MT pulses with varying amplitudes, and studying
delay-dependent saturation of mobile water protons, we
determined bound proton T2 to average 27μs, 17.5μs and
13.5μs in white matter, grey matter, and muscle tissue
in marmoset in vivo, while the exchange rates between
water and non-water protons were 13s-1, 30s-1, and 47s-1
respectively. The pulse-delay approach followed here
proved a sensitive way to study MT contrast and is
applicable to study of human brain at high field.
|
09:12 |
0999. |
A new MT signal at -1.6 ppm
via NOE-mediated saturation transfer
Xiao-Yong Zhang1, Hua Li1,
Junzhong Xu1, Jingping Xie1, John
C. Gore1, and Zhongliang Zu1
1Institute of Imaging Science, Vanderbilt
University, Nashville, TN, United States
Magnetization transfer (MT) provides a unique mechanism
for producing contrast and makes MRI sensitive to the
presence of metabolites, mobile macromolecules, and
semisolid macromolecules through their ‘magnetic
coupling’ effects on the water signal. Although the
nuclear Overhauser enhancement (NOE)-mediated MT signal
at -3.5 ppm has been recently studied, to date no in
vivo MT effect at -1.6 ppm has been reported. We report
a new MT signal MT at -1.6 ppm, which may reflect the
NOE effect between choline headgroup of membrane
phospholipids and water protons. The MT signal at -1.6
ppm could be used as a new biomarker in healthy rat
brain.
|
09:24 |
1000.
|
Oxidative stress sensitive
magnetization transfer MRI of prostate cancer
Rongwen Tain1,2, Michael Abern3,
Karen Xie1, X. Joe Zhou1,2, and
Kejia Cai1,2
1Radiology, College of Medicine, University
of Illinois at Chicago, Chicago, Illinois, United
States, 2Center
for MR Research, College of Medicine, University of
Illinois at Chicago, Chicago, Illinois, United States, 3Urology,
College of Medicine, University of Illinois at Chicago,
Chicago, Illinois, United States
Reduction-oxidation (Redox) imbalance due to oxidative
stress may occur in pathologies including cancer.
Developing imaging biomarkers for oxidative stress is a
key research area. Recently, we presented the first
non-invasive MRI method for mapping the tissue redox
state based on the endogenous Chemical Exchange
Saturation Transfer (CEST) contrast. It is well known
that magnetization transfer (MT) can occur via chemical
exchange (CEST) and/or dipole-dipole interactions
(Nuclear Overhauser Enhancement or NOE). This study on
ex vivo egg white tissues and in vivo prostate cancers
demonstrated that MT in the broad definition is
sensitive to oxidative stress through animal models.
|
09:36 |
1001. |
Assessment of Amide Proton
Transfer and Nuclear Overhauser Effects using long RF
Saturation at 3T in Clinical Brain Tumor Applications
Jochen Keupp1 and
Osamu Togao2
1Philips Research, Hamburg, Germany, 2Clinical
Radiology, Graduate School of Medical Science, Kyushu
University, Fukuoka, Japan
MTR asym can
be robustly and efficiently measured in clinical
settings, including 3D acquisitions with large coverage
in less than 5 minutes. On the other hand, MTR asym as
a measure for APT signal levels, was previously reported
to be biased by Nuclear Overhauser effects (NOE) at
opposite frequency offsets. The influence of NOE effects
may strongly depend on the main magnetic field (B 0)
and on saturation parameters. Most reported studies were
performed at ultra-high B 07T
and typically employed short RF saturation (T sat<1s)
and low saturation field amplitudes (e.g. B 1,rms=0.5
µT). In this study, a previously proposed APT protocol
(Tsat=2s; B 1,rms=2 µT) on 3.0T MRI systems is
applied for human brain tumor cases and analyzed for NOE
contributions using improved Z-spectral fitting methods.
It was hypothesized, that there is only a small or
negligible NOE contrast between NAWM and tumor tissue
using long saturation pulses at 3T. The study results
indicate that MTR asym in
combination with a specific protocol at 3T could be used
to assess APT signal levels in clinical applications
without significant interference of NOE effects.
|
09:48 |
1002. |
Amplifying ATP
Magnetization Exchange Effects by Band Inversion Transfer: A
31P NMR Study in Human Skeletal Muscle at 7T
Jimin Ren1,2, Baolian Yang3, A.
Dean Sherry1,4, and Craig R. Malloy1,5
1Advanced Imaging Research Center, University
of Texas Southwestern Medical Center, Dallas, Texas,
United States, 2Department
of Radiology, University of Texas Southwestern Medical
Center, Dallas, Texas, United States, 3Philips
Healthcare, Cleveland, Ohio, United States, 4Department
of Chemistry, University of Texas at Dallas, Richardson,
Texas, United States, 5VA
North Texas Health Care System, Dallas, Texas, United
States
31P magnetization transfer studies in animals and humans
suggest that transfer occurs not only between ATP and
exchanging metabolites such as phosphocreatine and
inorganic phosphate, but also among ATP spins. The
latter effect, although small, is most consistent with
31P-31P NOE. Here, we explore a strategy to amplify this
exchange effect within ATP by using a wideband
inversion. A four-fold increase in -ATP
signal reduction was observed by simultaneously
inverting Pi, PCr, -
and -ATP
using an adiabatic pulse, as compared to by conventional
frequency-selective inversion of only -ATP.
This observation is not consistent with known chemical
exchange pathways.
|
|