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Sparsity-enforced Slice-selective MRI RF Excitation Pulse Design

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Date 2008 Sep 10
PMID 18779063
Citations 17
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Abstract

We introduce a novel algorithm for the design of fast slice-selective spatially-tailored magnetic resonance imaging (MRI) excitation pulses. This method, based on sparse approximation theory, uses a second-order cone optimization to place and modulate a small number of slice-selective sinc-like radio-frequency (RF) pulse segments ("spokes") in excitation k-space, enforcing sparsity on the number of spokes allowed while simultaneously encouraging those that remain to be placed and modulated in a way that best forms a user-defined in-plane target magnetization. Pulses are designed to mitigate B(1) inhomogeneity in a water phantom at 7 T and to produce highly-structured excitations in an oil phantom on an eight-channel parallel excitation system at 3 T. In each experiment, pulses generated by the sparsity-enforced method outperform those created via conventional Fourier-based techniques, e.g., when attempting to produce a uniform magnetization in the presence of severe B(1) inhomogeneity, a 5.7-ms 15-spoke pulse generated by the sparsity-enforced method produces an excitation with 1.28 times lower root mean square error than conventionally-designed 15-spoke pulses. To achieve this same level of uniformity, the conventional methods need to use 29-spoke pulses that are 7.8 ms long.

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References
1.
Collins C, Li S, Smith M . SAR and B1 field distributions in a heterogeneous human head model within a birdcage coil. Specific energy absorption rate. Magn Reson Med. 1998; 40(6):847-56. DOI: 10.1002/mrm.1910400610. View

2.
Hu X, Parrish T . Reduction of field of view for dynamic imaging. Magn Reson Med. 1994; 31(6):691-4. DOI: 10.1002/mrm.1910310618. View

3.
Sodickson D, Manning W . Simultaneous acquisition of spatial harmonics (SMASH): fast imaging with radiofrequency coil arrays. Magn Reson Med. 1997; 38(4):591-603. DOI: 10.1002/mrm.1910380414. View

4.
Saekho S, Yip C, Noll D, Boada F, Stenger V . Fast-kz three-dimensional tailored radiofrequency pulse for reduced B1 inhomogeneity. Magn Reson Med. 2006; 55(4):719-24. PMC: 3076290. DOI: 10.1002/mrm.20840. View

5.
Vaughan J, Garwood M, Collins C, Liu W, Delabarre L, Adriany G . 7T vs. 4T: RF power, homogeneity, and signal-to-noise comparison in head images. Magn Reson Med. 2001; 46(1):24-30. DOI: 10.1002/mrm.1156. View