16:30 |
99. |
Joint
Design of Dual-Band Large-Tip-Angle RF and Gradient
Waveforms in Parallel Excitation
William A. Grissom1,
Adam B. Kerr, Pascal P. Stang2, Greig C. Scott2,
Ileana Hancu3, Mika W. Vogel4, John M.
Pauly2
1Electrical
Engineering and Radiology, Stanford University, Stanford,
CA, United States; 2Electrical Engineering,
Stanford University, Stanford, CA, United States; 3GE
Global Research, Niskayuna, NY, United States; 4Advanced
Medical Applications Laboratory, GE Global Research, Munich,
Bavaria, Germany
We introduce a new framework
for optimizing the phase encoding locations of a 2D or 3D
parallel excitation pulse in the large-tip-angle regime. The
framework is analogous to the hard pulse approximation, and
yields a straightforward analytical relationship between the
pulses' spin-domain rotations and the phase encoding
locations. This relationship can be exploited to optimize
locations using gradient descent, or using optimization
transfer for monotonic, parameter-free optimization. We
apply our method to the design of dual-band (fat + water)
spin echo parallel excitation pulses along 3D rungs
trajectories. |
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16:42 |
100. |
Fast and
Accurate Large-Tip-Angle RF Pulse Design for Parallel
Excitation Using a Perturbation Analysis of the Bloch
Equation
Hai Zheng1,2,
Tiejun Zhao3, Tamer Ibrahim1, Fernando
Emilio Boada1
1MR
Research Center, University of Pittsburgh, Pittsburgh, PA,
United States; 2Department of Bioengineering,
University of Pittsburgh, Pittsburgh, PA, United States;
3Siemens Medical Systems, Malvern, PA, United
States
The design of RF pulses in
parallel excitation (PTX) commonly relies on the
small-tip-angle approximation, which, although efficient,
leads to distorted excitation patterns at large tip angles
because of the intrinsic nonlinear nature of the Bloch
equation. In this work, we introduce a fast and accurate
method for large-tip-angle PTX RF pulse design based on a
perturbation analysis (PTA) to the Bloch equation.
Experimental data at 7T as well as computer simulations
demonstrate the improvements produced by the proposed
techniques without the need of prohibitively long
calculation times. |
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16:54 |
101. |
Fast
High-Flip PTx Pulse Design to Mitigate B1+ Inhomogeneity
Using Composite Pulses at 7T
Rene Gumbrecht1,2,
Joonsung Lee1, Hans-Peter Fautz3, Dirk
Diehl4, Elfar Adalsteinsson1,5
1Electrical
Engineering and Computer Science, Massachusetts Institute of
Technology, Cambridge, MA, United States; 2Department
of Physics, Friedrich-Alexander-University, Erlangen,
Germany; 3Siemens Healthcare, Erlangen, Germany;
4Siemens Corporate Technology, Erlangen, Germany;
5Harvard-MIT Division of Health Sciences and
Technology, Massachusetts Institute of Technology,
Cambridge, MA, United States
Parallel RF transmission
offers flexible control of ma magnetization generation and
has been successfully applied at 7T for spatially tailored
excitations and mitigation of in-plane B1+ inhomogeneity for
slice-selection. Composite Pulses are known to have
favorable robustness properties for large-flip-angle
excitations in the presence of B1+ variations, but they have
not yet been demonstrated on pTx systems. We propose a
composite RF pulse design for pTx systems and demonstrate
the method for B1+ mitigation in a 90º excitation pulse
design. |
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17:06 |
102. |
Kt
Points: Fast Three-Dimensional Tailored RF Pulses for
Flip-Angle Homogenization Over an Extended Volume
Martijn Anton Cloos1,
Nicolas Boulant1, Michel Luong2,
Guillaume Ferrand2, Christopher J. Wiggins1,
Eric Giacomini1, Alain France2, Dennis
Le Bihan1, Alexis Amadon1
1CEA, DSV,
I2BM, NeuroSpin, LRMN, Gif-sur-Yvette, France; 2CEA,
DSM, IRFU, SACM, Gif-sur-Yvette, France
Transmit-SENSE gives the
opportunity to implement short excitation pulses with good
flip-angle homogeneity at high field. For slice-selective
pulses, this was previously demonstrated using a spoke
k-space trajectory. Here we present a novel pulse design
returning sub-millisecond pulses with excellent flip-angle
homogenization over an extended volume. Experimental results
are shown at 7T, demonstrating a 950-μs excitation pulse
producing a 15±1.1° flip-angle distribution over a 16-cm
spherical phantom having the same electrical properties as a
human head. |
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17:18 |
103. |
Inner-Volume-Imaging Using Three-Dimensional Parallel
Excitation
Johannes Thomas
Schneider1,2, Raffi Kalayciyan1,3,
Martin Haas2, Wolfgang Ruhm1, Olaf
Doessel3, Juergen Hennig2, Peter
Ullmann1
1Bruker
BioSpin MRI GmbH, Ettlingen, Germany; 2Dept. of
Diagnostic Radiology, Medical Physics, University Hospital
Freiburg, Freiburg, Germany; 3Institute of
Biomedical Engineering, Karlsruhe Institute of Technology,
Karlsruhe, Germany
This study presents the first
experimental realization of inner-volume-imaging using
three-dimensional parallel excitation of arbitrarily shaped
regions of interest. By using a temporally optimized 4-fold
undersampled 3D k-space trajectory consisting of
concentrical shells in combination with an 8-channel
transceive RF-array, 3D selective excitation of an arbitrary
volume could be achieved in only 5 ms. Featuring such short
durations 3D-selective pulses are now on the verge of being
used in common imaging sequences and have been successfully
applied in first experiments of inner-volume-imaging in
phantoms and fruits during this study. |
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17:30 |
104. |
SAR
Reduction by K-Space Adaptive RF Shimming
Hanno Homann1,
Kay Nehrke2, Ingmar Graesslin2, Olaf
Dössel1, Peter Börnert2
1Karlsruhe
University, Karlsruhe, Germany; 2Philips
Research, Hamburg, Germany
Parallel transmission allows
compensating for RF transmit field inhomogeneities and
simultaneous SAR reduction by RF shimming. This study
demonstrates that the trade-off between these two objectives
can be overcome by using several different, adapted RF
pulses: When sampling the center of the k-space, a highly
uniform but relatively SAR-intensive excitation is performed
to achieve optimal contrast. In the outer k-space, the
homogeneity requirement is relaxed to reduce the average
SAR. The concept is discussed theoretically;
proof-of-principle is given based on phantom and in vivo
images. |
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17:42 |
105. |
Parallel
Transmit RF Design with Local SAR Constraints
Joonsung Lee1, Matthias Gebhardt2,
Lawrence L. Wald3,4, Elfar Adalsteinsson1,4
1Electrical
engineering and computer science, Massachusetts Institute of
Technology, Cambridge, MA, United States; 2Siemens
Healthcare, Erlangen, Germany; 3Department of
Radiology, A. A. Martinos Center for Biomedical Imaging,
Cambridge, MA, United States; 4Harvard-MIT
Division of Health Sciences and Technology, Massachusetts
Institute of Technology, Cambridge, MA, United States
The model compression method
for local SAR esitmation dramatically decreases the
complexity of the prediction of the local SAR calculation
and enables the incorporation of local SAR constaints in pTX
MLS RF design. |
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17:54 |
106. |
RFuGE –an
Accelerated Imaging Method Combining Parallel Transmit RF
Encoding Plus Gradient Encoding with Compressed Sensing
Reconstruction
Muhammad Usman1,
Shaihan J. Malik2, Ulrich Katscher3,
Philip G. Batchelor1, Joseph V Hajnal2
1Imaging
Sciences, King's College London, London, United Kingdom;
2Robert Steiner MRI Unit, Imaging Sciences
Department, MRC Clinical Sciences Centre, Hammersmith
Hospital, Imperial College London, London, United Kingdom;
3Sector Medical Imaging Systems Philips Research
Europe, Hamburg, Germany
We describe a combination of
Parallel Transmit generated radiofrequency encoding and
undersampled gradient encoding that can be reconstructed
using compressed sensing to achieve accelerated imaging with
a non-linear encoding basis. The method, RF plus Gradient
Encoding, (RFuGE) has been tested in simulation and
successful reconstructions were achieved. |
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18:06 |
107. |
16-Channel Parallel Transmission in the Human Brain at 9.4
Tesla: Initial Results
Xiaoping Wu1,
J. Thomas Vaughan1, Kamil Ugurbil1,
Pierre-Francois Van de Moortele1
1CMRR,
University of Minnesota, Minneapolis, MN, United States
It has been shown that
parallel transmission (pTx), which consists of playing
different RF pulses through independent transmit (Tx)
channels, can be used to mitigate Tx B1 (B1+) nonuniformity
and to achieve more homogeneous spatially selective RF
excitation at high magnetic field. We have previously
reported a successful implementation of Transmit SENSE in
the human brain at 9.4 T with an 8 Tx channel system, which
required addressing methodological issues such as k-space
trajectory inaccuracies and large susceptibility induced
δB0. Recently, our 9.4T system has been upgraded with a 16
Tx channel console. Here we report preliminary results of 2D
(Transmit SENSE) and 3D (Spoke trajectories) pTx in the
human brain at 9.4 T using a 16-channel RF coil. |
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18:18 |
108. |
Self-Refocused Adiabatic Pulse for Spin Echo Imaging at 7T
Priti Balchandani1,
John Pauly2, Daniel Spielman1
1Radiology,
Stanford University, Stanford, CA, United States; 2Electrical
Engineering, Stanford University, Stanford, CA, United
States
Adiabatic 180° pulses may be
used to replace conventional 180° pulses in spin echo
sequences to provide greater immunity to the inhomogeneous B1-field
at 7T. However, because the spectral profile of an
adiabatic 180° pulse has non-linear phase, pairs of these
pulses are used for refocusing, resulting in increased SAR
and longer minimum echo times. We have used the adiabatic
SLR method to generate a matched-phase 90° for an adiabatic
180° pulse to obviate the need for a second 180° pulse. The
pulse pair was combined into a single self-refocused pulse
to achieve the minimum echo time, and phantom and in vivo
experiments were performed to validate pulse performance. |
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