10:00 |
0542.
|
Plug and Play Parallel
Transmission at 7 and 9.4 Tesla based on Principles from MR
Fingerprinting
Martijn A Cloos1, Christopher Wiggins2,
Graham Wiggins1, and Dan Sodickson1
1NYU Langone Medical Center, New York, NY,
United States, 2Scannexus,
Maastricht, Netherlands
Parallel transmission (PTX) is often proposed as a
framework for transmit non-uniformity mitigation in
ultra high field MRI. However, routine application of
PTX has hitherto been hampered by technical challenges.
In particular, optimal performance is contingent on
subject-specific transmit-sensitivity maps and tailored
RF-pulses, which impede the workflow and increase the
duration of the exam. In this work we demonstrate a
novel approach to transmit non-uniformity mitigation
inspired by the recently proposed MR Fingerprinting
method that enables simultaneous quantitative mapping of
the T1 relaxation and an array of transmit-sensitivity
profiles without prior calibration scans or tailored
RF-pulses in less than 15seconds.
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10:12 |
0543. |
Z-stacked RF array design
enhances parallel transmit multiband RF performance in whole
brain simultaneous multislice imaging at 7T
Xiaoping Wu1, Jinfeng Tian1,
Sebastian Schmitter1, Tommy Vaughan1,
Kamil Ugurbil1, and Pierre-Francois Van de
Moortele1
1CMRR, Radiology, University of Minnesota,
Minneapolis, Minnesota, United States
Simultaneous MultiSlice (SMS) MR imaging using MultiBand
(MB) RF pulses is becoming increasingly popular in
neuroimaging. Recently, there has been an interest in
utilizing multielement RF arrays combined with
multichannel (pTx) MB pulse design to reduce transmit B1
inhomogeneity and SAR for SMS/MB imaging. Meanwhile, it
has been shown that the use of transmit coil elements
that approximately align with the slice direction, such
as Z-stacked arrays with azimuthally distributed
elements in two rings displaced from each other along
the Z-direction versus axial slices, can provide
improved RF performance for pTx non-MB pulses at 3T and
7T, as compared to conventional single ring arrays. In
this study, we evaluate the performance of such transmit
coil element/slice geometries for achieving whole brain
SMS/MB imaging at 7T by designing pTx MB RF pulses based
on electromagnetic simulations.
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10:24 |
0544. |
High-Speed RF Modulation
System for 32 Parallel Transmission Channels at 7T
Samaneh Shooshtary1, Marcel Gratz2,
Mark E. Ladd2,3, and Klaus Solbach1
1High Frequency Technology, Duisburg-Essen
University, Duisburg, Germany, 2Erwin
L. Hahn Institute for Magnetic Resonance Imaging, Essen,
Germany, 3Medical
Physics in Radiology, German Cancer Research Center (DKFZ),
Heidelberg, Germany
High-field 7T MR systems increasingly apply multichannel
transmit systems to overcome artifacts resulting from
comparably short wavelengths inside the human tissue.
Individual phase and amplitude modulation for each
channel is required to gain the desired image
homogeneity. A high-speed digitally controlled modulator
system is presented for independent phase and magnitude
control of 32 transmit channels in a 7T MR-scanner, thus
allowing RF shimming and dynamic trajectories as well as
TX Sense. Experimental results show stability and
reproducibility of the RF signal while calibration of
imperfect amplitude- and phase tracking of I- and Q
components for 32 individual channels is demonstrated.
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10:36 |
0545.
|
Parallel transmission
approach for 7T based on optically controlled on-coil CMCD
amplifiers
Natalia Gudino1, Qi Duan1, Joe
Murphy-Boesch1, Jacco A de Zwart1,
Hellmut Merkle1, Peter Van Gelderen1,
and Jeff H Duyn1
1Advanced MRI section, LFMI, NINDS, National
Institutes of Health, Bethesda, MD, United States
An approach to perform parallel RF transmission with
on-coil CMCD amplifiers at 7T is evaluated. An optimized
2-channel prototype based on eGaN FET technology was
built and tested. Artifact-free images of a gel phantom
were obtained by transmitting with the array and
receiving signal with a detunable volume receive coil.
The results suggest that this technology provides a
practical solution for the use of multi-channel
B1-shimming and other parallel transmit applications at
high field.
|
10:48 |
0546.
|
Large-Signal
Characterization of Coupled RF Amplifiers for Parallel
Transmit
Michael Twieg1 and
Mark A Griswold1,2
1Dept. of Electrical Engineering and Computer
Science, Case Western Reserve University, Cleveland, OH,
United States, 2Dept.
of Radiology, Case Western Reserve University,
Cleveland, OH, United States
We present a fast and powerful method of experimentally
quantifying the effective open loop output impedance and
power efficiency of coupled power amplifier topologies
across their full control space. We demonstrate the use
of the method for characterizing a Current Mode Class D
(CMCD) amplifier at 10 MHz. The results demonstrate some
of the unique qualities associated with switch mode
power amplifiers, such as the complex nature of their
effective output impedance, and the ability to recover,
rather than dissipate, power coupled from other transmit
elements. This methodology greatly facilitates the
evaluation of amplifiers for parallel transmit
applications.
|
11:00 |
0547. |
A Comparison of Isolating
Amplifier Architectures
Neal Hollingsworth1, Katherine Moody1,
Jon-Fredrik Nielsen1, Douglas Noll1,
Mary Preston McDougall1,2, and Steven Wright1,2
1Electrical Engineering, Texas A&M
University, College Station, Texas, United States, 2Biomedical
Engineering, Texas A&M University, College Station,
Texas, United States
Transmit systems have historically been single channel
and used to excite a simple slice or slab, however the
desire to use spatially selective RF pulses has driven
an interest in using the Transmit SENSE to accelerate
excitation. This requires the array to have known and
stable patterns, but coupled arrays are sensitive to
varying loads. Current source and low output impedance
amplifiers have been suggested for decoupling transmit
arrays. We have constructed current source, ultra-low
output impedance, and standard power amplifiers to
investigate the strengths of different architectures by
comparing the peak-power and isolation of the different
amplifier architectures.
|
11:12 |
0548.
|
Design of a Robust
Decoupling Matrix for High Field Parallel Transmit Arrays
Zohaib Mahmood1, Bastien Guérin2,
Boris Keil2, Elfar Adalsteinsson1,3,
Lawrence L. Wald2,3, and Luca Daniel1
1Dept of Electrical Engineering & Computer
Science, Massachusetts Institute of Technology,
Cambridge, MA, United States, 2A.
A. Martinos Center for Biomedical Imaging, Dept. of
Radiology, Massachusetts General Hospital, Charlestown,
MA, United States, 3Harvard-MIT
Division of Health Sciences Technology, Cambridge, MA,
United States
We present a methodology to design a robust decoupling
matrix for high field parallel transmit arrays. The
matrix is placed between the power amplifiers and the
coupled coil and yields almost perfect decoupling of the
array and hence improves the power efficiency. We
demonstrate the methodology by designing a decoupling
matrix for a coupled 7T 4-channel head transmit-array.
Our design is robust with respect to component value
variations. A sensitivity analysis revealed that only
two lumped elements need to be implemented as variable
in order to guarantee good performance of the matrix
even in the presence of component values variations.
|
11:24 |
0549. |
Impact of coupling in Tx-array
coil design for transmit SENSE at 3T
Pei-Shan Wei1,2, Michael J. Smith2,
Christopher P. Bidinosti3, Jarod Matwiy2,
and Scott B. King1,2
1Department of Physics and Astronomy,
University of Manitoba, Winnipeg, Manitoba, Canada, 2National
Research Council of Canada, Winnipeg, Manitoba, Canada, 3Department
of Physics, University of Winnipeg, Winnipeg, Manitoba,
Canada
For determining an optimal Tx-SENSE Tx-array design, we
modeled Tx-arrays with and without proper mutual
inductance coupling and coil termination to compare
accuracy of excitation and SAR. We found that with
incorrect coupling models, average SAR was
over-estimated by as much as 23%, peak SAR
under-estimated by as much as 26%, and peak SAR/Average
SAR underestimated by as much as 40%. Therefore, proper
coupling in simulations is absolutely necessary for RF
coil designers to optimize the Tx-array design for Tx-SENSE
applications and for accurate prediction of peak local
SAR distribution.
|
11:36 |
0550. |
On the correction of cable
losses for in-situ subject-specific global Q matrix
calibration
Francesco Padormo1,2, Arian Beqiri1,
Shaihan J. Malik1, and Joseph V. Hajnal1,2
1Division of Imaging Sciences and Biomedical
Engineering, Kings College London, London, London,
United Kingdom, 2Centre
for the Developing Brain, Kings College London, London,
London, United Kingdom
In this work we demonstrate an improved model for global
Q matrix calculation using power monitoring hardware.
This model accounts for RF cable attenuation so that the
reconstructed global Q matrix is more accurate than
previous approaches.
|
11:48 |
0551. |
Power balance
considerations for RF transmit coil arrays
Andre Kuehne1,2, Sigrun Goluch1,2,
Ewald Moser1,2, and Elmar Laistler1,2
1Center for Medical Physics and Biomedical
Engineering, Medical University of Vienna, Vienna,
Vienna, Austria, 2MR
Center of Excellence, Medical University of Vienna,
Vienna, Vienna, Austria
The bower balance of an RF coil gives valuable insight
into its performance. For multi-channel arrays, the
amount of power deposited in the load, the coil itself
or radiated depends on the superposition of the
single-channel fields. In this work, the power
correlation matrix formalism is extended to encompass
all terms of the power balance, thus allowing
straight-forward evaluation of the power balance for any
excitation, worst-case estimates, and providing means to
verify EM simulation integrity.
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