16:00 |
332. |
Observation of Frequency Shifts Induced by Chemical Exchange
in Brain Tissue
Karin Shmueli1,
Steve Dodd2, T-Q Li3, Jeff H. Duyn1
1Advanced MRI Section,
Laboratory of Functional and Molecular Imaging, National
Institute of Neurological Disorders and Stroke, National
Institutes of Health, Bethesda, MD, United States; 2Functional
and Molecular Metabolism Section, Laboratory of Functional
and Molecular Imaging, National Institute of Neurological
Disorders and Stroke, National Institutes of Health,
Bethesda, MD, United States; 3Department of
Medical Physics, Karolinska Huddinge, Stockholm, Sweden
Water-macromolecular exchange
has been proposed to explain brain gray and white matter
frequency (phase) contrast. We extended previous
observations of exchange-induced frequency shifts (fexch)
in protein solutions by performing chemical shift imaging
experiments using reference chemicals (TSP and dioxane) to
observe positive fexch in fixed human and fresh
pig brain tissue. Substantial negative GM-WM δfexch
was observed which was similar for all tissues and
references but opposite to in-vivo GM-WM frequency contrast,
implying that tissue magnetic susceptibility may have a
greater contribution. Exchange should therefore be included
in frequency contrast models but is insufficient to explain
in-vivo GM-WM phase contrast. |
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16:12 |
333. |
Classical
Interpretation of T1rho and T2rho Relaxation
Michael Carl1,
Mark Bydder2, Eric Han1, Graeme Bydder2
1GE
Healthcare, Waukesha, WI, United States; 2University
of California, San Diego,
San Diego, CA, United States
We present a simulation model
based solely on classical equations to study spin-lattice
relaxation in the rotating frame. Without the confound of a
quantum mechanical treatment, this model allows for an
intuitive understanding of spin locking such as T1rho
dispersion, oscillations caused by residual dipolar
interactions (RDI), and T2rho. |
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16:24 |
334. |
Quantitative T1rho Imaging Using Phase Cycling for B0 and B1
Field Inhomogeneity Compensation
Weitian Chen1, Atsushi Takahashi1,
Eric T. Han1
1MR Applied Science Lab, GE
Healthcare, Menlo Park, CA, United States
T1rho imaging is promising in
clinical applications such as early detection of
osteoarthritis. T1rho imaging, however, is sensitive to B0
and B1 RF field inhomogeneities. In this work, we report on
a phase cycling method to eliminate B1 RF inhomogeneity
effects in T1rho imaging. The presences of B0 field
inhomogeneity can compromise B1 RF inhomogeneity
compensation approaches. We present a method which combines
the phase cycling approach with a composite RF pulse scheme
proposed by Dixon et al for simultaneous compensation of B0
and B1 RF field inhomogeneity in T1rho imaging. The proposed
T1rho RF preparation methods can be combined with an SNR-efficient
3D T1rho imaging method MAPSS without compromising scan
time. |
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16:36 |
335. |
Quantitative Magnetization Transfer Imaging of Human Brain
at 3T Using Selective Inversion Recovery
Richard D.
Dortch1,2, Ke Li1,2, Ashish A. Tamhane3,
E B. Welch2,4, Dan F. Gochberg1,2,
John C. Gore1,2, Seth A. Smith1,2
1Department
of Radiology and Radiological Sciences, Vanderbilt
University, Nashville, TN, United States; 2Vanderbilt
University Institute of Imaging Science, Vanderbilt
University, Nashville, TN, United States; 3Department
of Biomedical Engineering, Illinois Institute of Technology,
Chicago, IL, United States; 4MR Clinical Science,
Philips Healthcare, Cleveland, OH, United States
Quantitative magnetization
transfer (qMT) yields quantitative information about
interactions between immobile macromolecular protons and
free water protons. Because of its relatively short scan
times, the pulsed, off-resonance saturation qMT approach is
most commonly employed on clinical systems; however, it
suffers from complicated data analysis and sensitivity to
macromolecular proton lineshape assumptions. The selective
inversion recovery (SIR) approach does not suffer from these
shortcomings, but has not been widely implemented on
clinical systems. In this study, the SIR approach was
implemented on a clinical 3T system. The resultant qMT
parameters in healthy brain were in good agreement with
previously published values. |
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16:48 |
336. |
Magnetization Transfer Mapping of Myelinated Fiber Tracts in
Living Mice at 9.4 T
Susann Boretius1,
Peter Dechent2, Jens Frahm1, Gunther
Helms2
1Biomedizinische NMR
Forschungs GmbH, Max-Planck-Institut für Biophysikalische
Chemie, Göttingen, Germany; 2MR-Research in
Neurology and Psychiatry, University Medical Center,
Göttingen, Germany
MRI of mouse models is an
integral part of translational research on white matter
diseases and myelin disorders. Thus, the delineation of
myelinated fiber tracts in mice becomes of growing interest.
Here we used in healthy adult mice a novel FLASH-based
parameter for magnetization transfer that was recently
established for human applications. In comparison to maps of
MT ratio and T1, this parameter provides an improved
gray-white matter contrast that allows for the visualization
of small neuronal fiber bundles such as the mammilothalamic
tract and fasciculus retroflexus. |
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17:00 |
337. |
Molecular
Mechanisms of Magnetization Transfer
Scott David Swanson1
1Department of
Radiology, University of Michigan, Ann Arbor, MI, United
States
We present a look at the
molecular mechanisms of MT in agarose and gelatin samples.
MT is found to be driven by whole water exchange in agarose
and proton exchange in gelatin. |
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17:12 |
338. |
CEST-Dixon
MRI for Sensitive and Accurate Measurement of Amide Proton
Transfer in Humans at 3T
Jochen Keupp1,
Holger Eggers1
1Philips Research
Europe, Hamburg, Germany
CEST-MRI based measurement of
endogenous proteins using the amide proton transfer (APT)
signal could find important clinical applications in
oncology (tumor metabolism) and in neurology (ischemic
acidosis). As APT-MRI is very sensitive to B0
inhomogeneity, we propose to apply multi gradient-echo
sequences and derive a B0 map by the Dixon
technique, as opposed to previously described methods like
full CEST-spectra interpolation or separate water resonance
mapping. Furthermore, technical limits for pulse lengths on
clinical scanners are addressed and a saturation of 1 second
is achieved (human head). Feasibility of APT-MRI within 6
minutes (SENSE R=3) is demonstrated in volunteers at 3T. |
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17:24 |
339. |
Detection
of Myo-Inositol In-Vivo Using MR Chemical Exchange
Saturation Transfer Imaging (MICEST)
Mohammad Haris1,
Kejia Cai1, Anup Singh1, Feliks Kogan1,
Walter Witschey1, Hari Hariharan1,
Ravinder Reddy1
1CMROI,
Department of Radiology, University of Pennsylvania,
Philadelphia, PA, United States
In the current study, we
demonstrated the mapping of Myo-inositol (MI) in human brain
at 7T by exploiting chemical exchange saturation transfer (CEST)
of labile hydroxyl proton (-OH) on the MI. The Z-spectrum of
MI showed an asymmetry around~0.625ppm downfield to the bulk
water resonance. The CEST imaging on healthy human brain
clearly shows the distribution of MICEST contrast in gray
and white matter regions and negligible contrast from
cerebrospinal fluid. |
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17:36 |
340. |
Differentiation Between Glioma and Radiation Necrosis Using
Molecular Imaging of Endogenous
Proteins and Peptides
Jinyuan Zhou1,
Erik Tryggestad2, Zhibo Wen1, Bachchu
Lal3, Tingting Zhou1, Rachely Grossman4,
Kun Yan1, Silun Wang1, De-Xue Fu5,
Eric Ford2, John Laterra3, Peter C.M.
van Zijl1
1Department
of Radiology, Johns Hopkins University, Baltimore, MD,
United States; 2Department of Radiation Oncology,
Johns Hopkins University, Baltimore, MD, United States;
3Department of Neurology, Kennedy Krieger Institute,
Baltimore, MD, United States; 4Department of
Neurosurgery, Johns Hopkins University, Baltimore, MD,
United States; 5Department of Oncology, Johns
Hopkins University, Baltimore, MD, United States
We show that it is possible
to differentiate between glioma and radiation necrosis using
the amide proton signals of endogenous cellular proteins and
peptides as imaging biomarker. Using a radiation necrosis
model (dose, 40 Gy; area, 10x10 mm2) and a SF188/V+ human
glioma model in rats, tumors and radiation necrosis had
similar conventional MRI features. However, gliomas were
consistently hyperintense on amide proton transfer (APT)
images, while radiation necrosis (observed about six months
post-radiation) was hypointense to isointense. APT MRI as an
imaging biomarker for tumor presence provides unique visual
information for assessing active tumor versus
treatment-related injury, such as radiation necrosis. |
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17:48 |
341. |
Fast T1
Mapping Using Modified Double-Inversion Recovery Pre-Pulse
Marcelo E.
Andia1, Rene M. Botnar1
1Division of
Imaging Sciences, Kings College London, London, United
Kingdom
In this work we present a new
technique for fast T1 estimation where the intensity of each
pixel is linearly related to its T1 value. The technique is
based on a modified Double Inversion Recovery pre-pulse and
only requires the acquisition of a single 2D or 3D dataset.
The technique was validated in a T1 phantom and in a
pre-clinical study of renal perfusion using a gadolinium
based contrast agent. Potential applications include fast T1
quantification in myocardial perfusion, infarct or fibrosis
imaging. |
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