16:00 |
0439.
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Simultaneous Quantitative
Mapping of T1, T2*, and Magnetic
Susceptibility with Multi-Echo MP2RAGE at 7 T
Riccardo Metere1, Harald E. Möller1,
Gunnar Krüger2,3, Tobias Kober2,3,
and Andreas Schäfer1
1Max Planck Institute for Human Cognitive and
Brain Sciences, Leipzig, Germany, 2Siemens
ACIT – CHUV Radiology, Siemens Healthcare IM BM PI &
Department of Radiology CHUV, Lausanne, Switzerland, 3LTS5,
École Polytechnique Fédérale de Lausanne, Lausanne,
Switzerland
Knowledge of the relaxation times is essential for
understanding the biophysical mechanisms underlying
image contrast, and can be related to tissue
composition. Quantitative experiments are essential for
cross-study comparisons, but often require longer
acquisition times. Using the prototype Multi-Echo (ME)
MP2RAGE pulse sequence, we show the possibility of
obtaining reliable T1, T2*, and
magnetic susceptibility maps that are inherently
co-registered. The acquisition time required for such
experiments is comparable to the time required for T1 map
acquisition with MP2RAGE. This result is obtained as a
trade-off between resolution and the parameters of the
multi-echo readouts.
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16:12 |
0440. |
Fast T1 Mapping
Using Slice-Shuffled Simultaneous Multi-Slice Inversion
Recovery EPI
Hua Wu1, Robert F Dougherty1, Adam
B Kerr2, Kangrong Zhu2, Matthew J
Middione3, and Aviv Mezer4
1Center for Cognitive and Neurobiological
Imaging, Stanford University, Stanford, CA, United
States, 2Electrical
Engineering, Stanford University, Stanford, CA, United
States, 3Applied
Sciences Laboratory West, GE Healthcare, Menlo Park, CA,
United States, 4Psychology,
Stanford University, Stanford, CA, United States
T1 mapping provides useful information for quantitative
MR. Gold-standard method using inversion recovery spin
echo sequence is robust but slow. EPI readout together
with simultaneous multi-slice excitation can greatly
accelerate the acquisition, and using a slice-shuffled
method can accelerate the sampling of the T1 recovery.
Here we test and validate fast T1 mapping methods using
a combination of simultaneous multi-slice excitation to
accelerate the cross-slice acquisition, in-plane
acceleration to shorten the readout, and slice-shuffling
to achieve rapid T1 recovery sampling.
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16:24 |
0441. |
T2-Snapshots imaging with
simultaneous multislice TESS acquisition
Orso Pusterla1, Francesco Santini1,
Rahel Heule1, and Oliver Bieri1
1Radiological Physics, Department of
Radiology, University of Basel Hospital, Basel,
Switzerland
Single slice triple echo steady-state (TESS) imaging has
demonstrated potential for robust highly B1-insensitive
T2 relaxometry in the human brain. In this work, a
Hadamard-encoding excitation scheme is investigated for
fast simultaneous multislice TESS acquisitions. The
achieved improvement in the signal-to-noise ratio was
invested into a reduction of the overall scan time per
slice yielding about 10 sec / slice. As a result,
simultaneous multislice TESS imaging is of high interest
for accurate T2 quantification in the clinical routine
offering full brain coverage within clinically
acceptable scan times.
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16:36 |
0442. |
Artifact-free T2* mapping
without post hoc corrections
Pippa Storey1, Yvonne W. Lui1, and
Dmitry S. Novikov1
1Radiology Department, New York University
School of Medicine, New York, NY, United States
Macroscopic susceptibility differences are a frequent
source of artifacts in T2* mapping, and post hoc
correction methods are often cumbersome or inaccurate.
We demonstrate that Fourier encoding is largely
insensitive to macroscopic phase gradients up to a
threshold determined by the Nyquist limit. Accurate T2*
maps can thus be obtained without post hoc correction
simply by acquiring data in 3D mode and truncating the
echo train where the local phase gradient exceeds the
threshold. This approach produces uniform T2* maps in
phantoms despite the presence of a ferromagnetic object,
and artifact-free T2* maps of the brain even near the
sinuses.
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16:48 |
0443. |
Fast dynamic measurements
of T1 relaxation
times: influence and correction of T2*
effects
Olaf Dietrich1, Maximilian Freiermuth1,
Linus Willerding2, Michael Peller1,
and Maximilian F Reiser1
1Josef Lissner Laboratory for Biomedical
Imaging, Institute for Clinical Radiology, LMU Ludwig
Maximilian University of Munich, Munich, Germany,2Department
of Internal Medicine III, LMU Ludwig Maximilian
University of Munich, Munich, Germany
The purpose of this study was to analyze and correct the
influence of contrast-agent induced T2* (transverse)
relaxation effects on the accuracy of fast dynamic 3D
gradient-echo T1 measurements with a combined
variable-flip-angle baseline measurement and subsequent
single-flip-angle measurements during the dynamic phase.
Previously proposed techniques for T1 quantitation
neglect the influence of transverse relaxation effects
on the measured signal during the dynamic phase and
result in systematically increased T1 values. We
demonstrate that the influence of transverse relaxation
can be expressed as a function of T1 leading to an
implicit expression for T1 that can be solved
numerically.
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17:00 |
0444.
|
B0 Correction
for Myelin Water Fraction Imaging Based on Multi-Slice MGRE
Acquisitions
Eva Alonso Ortiz1, Ives R. Levesque2,3,
and G. Bruce Pike4
1McConnell Brain Imaging Centre, Montreal
Neurological Institute, McGill University, Montreal,
Quebec, Canada, 2Medical
Physics Unit, Department of Oncology, McGill University,
Montreal, Quebec, Canada, 3Research
Institute of the McGill University Health Centre, McGill
University, Montreal, Quebec, Canada, 4Department
of Radiology and Hotchkiss Brain Institute, University
of Calgary, Alberta, Canada
Myelin water fraction (MWF) imaging based on
multi-component (MC) T2 analysis can be used to
quantitatively assess myelin. Recently, multi-gradient
echo (MGRE) sequences have been proposed for MCT2*-based
MWF mapping, due to their fast, whole-brain or
multi-slice imaging capability, low specific absorption
rate (SAR) and short echo spacing (ES). An important
caveat for MGRE imaging is the significant signal loss
caused by magnetic field inhomogeneities (ΔB0), making
proper ΔB0 correction necessary in order to avoid
inaccuracies in MWF maps. We propose a ΔB0 correction
method based on partial fits to MGRE data obtained for
the MWF-mapping itself.
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17:12 |
0445. |
Encoding with
Radiofrequency Spoiling, Equilibrium States and Inverse
Problem for Parametric Mapping
Ludovic de Rochefort1
1IR4M (Imagerie par Résonance Magnétique
Médicale et Multi-modalités), Univ. Paris-Sud, CNRS,
UMR8081, Orsay, France
Fast steady-state sequences often use RF spoiling to
modulate contrast in MRI. The dynamic equilibrium
depends on many parameters such as flip angle,
longitudinal and transverse relaxations, and diffusion.
Here it is shown that, extending the configuration state
formalism, RF spoiling can be described as an encoding
direction and equilibrium can be efficiently calculated
with relaxation and diffusion. The inverse problem can
then be solved to reconstruct associated parametric
maps. Theory, practical implementation as well as
proof-of-concept experiments on a clinical MRI system
are given introducing new methods for efficient
parametric mapping.
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17:24 |
0446. |
The effect of macroscopic
field gradients on the simultaneous estimation of reversible
and irreversible transverse relaxation rates
Mukund Balasubramanian1,2 and
Robert V. Mulkern1,2
1Department of Radiology, Boston Children's
Hospital, Boston, MA, United States, 2Harvard
Medical School, Boston, MA, United States
Pulse sequences such as GESFIDE and GESSE have enabled
the simultaneous measurement of irreversible and
reversible transverse relaxation rates. Reversible
relaxation is influenced by both macroscopic and
mesoscopic field inhomogeneities, with considerable
interest in separating effects of the former from the
latter. Here, we applied linear macroscopic gradients
during GESSE scans of the knee, where significant
mesoscopic field variations are induced by bone
trabeculae. We find that the sinc-term corrections that
have been proposed are not warranted and that the
recently-observed Gaussian behavior of GESSE time-domain
signals provides a better avenue for factoring out the
effects of macroscopic field variations.
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17:36 |
0447.
|
Simultaneous group-wise
rigid registration and Maximum Likelihood T1 estimation
for T1 mapping
Gabriel Ramos-Llordén1, Arnold J. den Dekker1,2,
Gwendolyn Van Steenkiste1, Johan Van
Audekerke3, Marleen Verhoye3, and
Jan Sijbers1
1iMinds-Vision Lab, University of Antwerp,
Antwerp, Belgium, 2Delft
Center for Systems and Control, Delft University of
Technology, Delft, Netherlands, 3Bio-Imaging
Lab, University of Antwerp, Antwerp, Belgium
In T1 mapping,
to prevent motion artifacts, alignment of the acquired T1 weighted
images is required. Commonly, image registration is
accomplished prior to T1 map
estimation. However, this two-step approach introduces
bias in the T1 estimation
due to inaccurate motion estimation and image
interpolation. We propose a simultaneous group-wise
rigid registration and T1 estimation
method using a Maximum Likelihood (ML) approach for
brain T1 mapping,
thereby constructing a unified framework and
circumventing the problems of the conventional two-step
approach. Results with synthetic and real data
demonstrate that the proposed method outperforms the
conventional two-step approach.
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17:48 |
0448.
|
Field Probes with In-Situ
Controllable Thermal Relaxation Times
David O. Brunner1, Simon Gross1,
Jennifer Nussbaum1, Benjamin E. Dietrich1,
Christoph Barmet1,2, and Klaas P. Pruessmann1
1Institute for Biomedical Engineering,
University and ETH Zurich, Zurich, Switzerland, 2Skope
Magnetic Resonance Technologies LLC, Zurich, Switzerland
For optimal performance, the T 1 and
T 2 relaxation
times of NMR based field sensors should be appropriately
chosen compared to the repetition time of their
re-excitation in the envisioned application. Too fast
relaxations would prevent acquiring long read-outs,
however too fast re-excitation would generate confounded
field values due to occurring spurious echoes in the
sensor. To date this is achieved by paramagnetic dopants
added when manufacturing the probes but in this work we
present an approach based on electrochemical reactions
allowing tuning the relaxation time of an existing
sensor between reversibly 3 ms and 60 ms.
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