TRADITIONAL POSTER - ismrm
TRADITIONAL POSTER - ismrm
TRADITIONAL POSTER - ismrm
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Poster Sessions<br />
average flip angle is used to calculate the transmit gain setting needed to produce the desired flip angle. This is shown here at 3 Tesla in the brain, shoulder,<br />
abdomen, breast, and wrist with a total scan time for a robust implementation of 1.6 seconds.<br />
2831. Fast and Robust B 1 Mapping at 7T by the Bloch-Siegert Method<br />
Mohammad Mehdi Khalighi 1 , Laura I. Sacolick 2 , W Thomas Dixon 3 , Ron D. Watkins 4 , Sonal Josan 4 , Brian<br />
K. Rutt 4<br />
1 Applied Science Lab, GE Healthcare, Menlo Park, CA, United States; 2 Imaging Technologies Lab, General Electric Global Research,<br />
Garching b. Munchen, Germany; 3 General Electric Global Research, Niskayuna, NY, United States; 4 Department of Radiology,<br />
Stanford University, Stanford, CA, United States<br />
B 1 + mapping is a critical step in the design of RF pulses for parallel transmit systems. We used the Bloch-Siegert (BS) B 1 + mapping method and a 2-channel<br />
parallel transmit enabled 7T scanner to produce fast, robust and accurate B 1 + maps through the human brain. Both B 1 + magnitude and phase are obtained<br />
from a single sequence, employing +/-4kHz off-resonance BS pulses. B 1 + magnitude and phase maps acquired with a 26s BS scan are compared with those<br />
acquired with a 640s classical double angle scan, showing that the BS method is a very good candidate for efficient B 1 + mapping at 7T.<br />
2832. Practical Vector B1 Mapping at 7T<br />
Douglas Kelley 1,2 , Janine Lupo 2<br />
1 Applied Science Laboratory, GE Healthcare, San Francisco, CA, United States; 2 Radiology and Biomedical Imaging, University of<br />
California, San Francisco, San Francisco, CA, United States<br />
Compensation of B1 variations in vivo requires mapping both the magnitude and the phase of each channel's RF magnetic field. Since the field distribution<br />
is strongly dependent on the specific size, shape, and positioning of the tissue, such mapping must be made for each subject. We present a practical method<br />
for acquiring these maps within 10 minutes in phantoms and human subjects at 7T.<br />
2833. Compressive B1 + Mapping: Towards Faster Transmit Coil Sensitivity Mapping<br />
Mariya Doneva 1 , Kay Nehrke 2 , Alfred Mertins 1 , Peter Börnert 2<br />
1 Institute for Signal Processing, University of Lübeck, Lübeck, Germany; 2 Philips Research Europe, Germany<br />
The potential to accelerate the B1 + mapping measurement by means of compressed sensing (CS) was investigated. Joint sparsity constraint accounting for<br />
the common sparsity support in different TX channels, and higher dimensional undersampling space, also including the coil dimension, allow for<br />
considerable acceleration even for the low resolution data acquired in B1 + mapping. The basic feasibility of the proposed method is evaluated on simulations<br />
and in vivo data from a 3T 8-channel parallel transmit system.<br />
2834. Simultaneuous B 0 and High Dynamic Range B 1 Mapping Using an Adiabatic Partial Passage Pulse<br />
Kim Shultz 1 , Greig Scott 1 , Joelle Barral 1 , John Pauly 1<br />
1 Electrical Engineering, Stanford University, Stanford, CA, United States<br />
We present a simultaneous δ B 0 and high-dynamic range B 1 mapping technique using an adiabatic partial passage pulse. The double angle method, the gold<br />
standard for B 1 mapping, requires 66% longer to acquire the same B 1 range. The high dynamic range is useful for mapping the fields from ablation wires or<br />
surface coils, where significant B 0 variation will also be present.<br />
2835. Fast B1+ Mapping with Validation for Parallel Transmit System in 7T<br />
Joonsung Lee 1 , Borjan Gagoski 1 , Rene Gumbrecht 1,2 , Hans-Peter Fautz 3 , Lawrence L. Wald 4,5 , Elfar<br />
Adalsteinsson 1,5<br />
1 Electrical engineering and computer science, Massachusetts Institute of Technology, Cambridge, MA, United States; 2 Physics,<br />
Friedrich-Alexander-University Erlangen, Erlangen, Germany; 3 Siemens Healthcare, Erlangen, Germany; 4 Department of Radiology,<br />
A. A. Martinos Center for Biomedical Imaging, Cambridge, MA, United States; 5 Harvard-MIT Division of Health Sciences and<br />
Technology, Massachusetts Institute of Technology, Cambridge, MA, United States<br />
We present a fast B1+ mapping method for parallel transmit system and validate the performance on water phantom in 7T. The measured flip angle matches<br />
with the flip angle simulated by the Bloch equation.<br />
2836. Image-Guided Radio-Frequency Gain Calibration for High-Field MRI<br />
Elodie Breton 1 , KellyAnne McGorty 1 , Graham C. Wiggins 1 , Leon Axel 1 , Daniel Kim 1<br />
1 Research Radiology - Center for Biomedical Imaging, New York University Langone Medical Center, New York, NY, United States<br />
The purpose of this study was to develop a rapid, image-guided RF transmitter gain calibration procedure for high-field MRI and evaluate its performance<br />
through phantom and in vivo experiments at 3T and 7T. Using a single-shot TurboFLASH pulse sequence, a series of “saturation-no-recovery” images was<br />
acquired by varying the flip angle of the preconditioning pulse. In the resulting images, the signal null occurs in regions where the flip angle of the<br />
preconditioning pulse is 90°, and the mean signal within a region-of-interest can be plotted as a function of the nominal flip angle to quantitatively calibrate<br />
the RF transmitter gain.<br />
2837. No Inversion Double Angle Look-Locker (NiDALL) for Flip Angle Mapping<br />
Trevor Wade 1,2 , Charles McKenzie 1,3 , Brian Rutt 4<br />
1 Imaging Research Laboratories, Robarts Research Institute, London, ON, Canada; 2 Biomedical Engineering, The University of<br />
Western Ontario, London, ON, Canada; 3 Medical Biophysics, The University of Western Ontario, London, ON, Canada; 4 Diagnostic<br />
Radiology and Richard M Lucas Center for Imaging, Stanford University, Stanford, CA, United States<br />
The double angle Look-Locker method is an efficient 3D method of mapping transmit B1 inhomogeneity. It makes uses inversion pulses and samples the<br />
recovering magnetization using SPGR trains at two different angles. This leads to two time constants that can be combined to find the achieved flip angle. If<br />
the SPGR trains at the two angles are interleaved the inversion pulses can be omitted entirely, and the same information can still be extracted. This reduces<br />
SAR, simplifies data analysis and still yields nearly the same performance in terms of measuring the flip angle.