Subject‐specific water‐selective imaging using parallel transmission

Spectral‐spatial excitation pulses are an efficient means of achieving water‐ or fat‐only imaging and can be used in conjunction with a variety of pulse sequences. However, the approach lacks reliability since its performance is dependent on the homogeneity of the static magnetic field. Sensitivity to static magnetic field variation can be reduced by designing pulses with wider frequency stop bands, but these require longer pulse durations. In the proposed method, spectral‐spatial pulses are optimized on a subject‐dependent basis to take into account measured subject‐specific static magnetic field variation. Extra control of the radiofrequency (RF) field from multichannel transmission is used to achieve this without increasing the length of the pulses. The method characterizes RF pulses using relatively few parameters and has been applied to abdominal imaging at 3 T with an eight‐channel system. In a comparison of standard and subject‐specific pulses on five healthy volunteers, the latter improved fat suppression in all subjects, with a reduction in RF power of 13% ± 6%. A forward model suggests that the mean flip angle in fat was reduced from 0.72° ± 0.55° to 0.12° ± 0.04° for a 20° excitation; uniformity of water excitation also improved, with the standard deviation divided by mean reduced from 0.26 ± 0.05 to 0.16 ± 0.05. Magn Reson Med, 2010. © 2010 Wiley‐Liss, Inc.

[1]  Johnpauly A k-Space Analysis of Small-Tip-Angle Excitation , 2012 .

[2]  Albert Macovski,et al.  A k-space analysis of small-tip-angle excitation. 1989. , 2011, Journal of magnetic resonance.

[3]  Shaihan J Malik,et al.  Optimal linear combinations of array elements for B1 mapping , 2009, Magnetic resonance in medicine.

[4]  Kawin Setsompop,et al.  Broadband slab selection with B  1+ mitigation at 7T via parallel spectral‐spatial excitation , 2009, Magnetic resonance in medicine.

[5]  Kay Nehrke,et al.  On the steady‐state properties of actual flip angle imaging (AFI) , 2009, Magnetic resonance in medicine.

[6]  Glen R Morrell,et al.  A phase‐sensitive method of flip angle mapping , 2008, Magnetic resonance in medicine.

[7]  O. Simonetti,et al.  Rapid phase-modulated water excitation steady-state free precession for fat suppressed cine cardiovascular MR , 2008, Journal of cardiovascular magnetic resonance : official journal of the Society for Cardiovascular Magnetic Resonance.

[8]  E. Adalsteinsson,et al.  Magnitude least squares optimization for parallel radio frequency excitation design demonstrated at 7 Tesla with eight channels , 2008, Magnetic resonance in medicine.

[9]  P. Börnert,et al.  Improved B1-Mapping for Multi RF Transmit Systems , 2008 .

[10]  D. Noll,et al.  Estimating K transmit B 1 + maps from K + 1 scans for parallel transmit MRI , 2008 .

[11]  K. Ugurbil,et al.  Very Fast Multi Channel B 1 Calibration at High Field in the Small Flip Angle Regime , 2008 .

[12]  P Röschmann,et al.  Eight‐channel transmit/receive body MRI coil at 3T , 2007, Magnetic resonance in medicine.

[13]  Vasily L Yarnykh,et al.  Actual flip‐angle imaging in the pulsed steady state: A method for rapid three‐dimensional mapping of the transmitted radiofrequency field , 2007, Magnetic resonance in medicine.

[14]  P. Börnert,et al.  A Minimum SAR RF Pulse Design Approach for Parallel Tx with Local Hot Spot Suppression and Exact Fidelity Constraint , 2007 .

[15]  K. Pruessmann,et al.  Increasing bandwidth of spatially selective transmit SENSE pulses using constrained optimization , 2007 .

[16]  Kawin Setsompop,et al.  Parallel RF transmission with eight channels at 3 Tesla , 2006, Magnetic resonance in medicine.

[17]  Douglas C Noll,et al.  Spatial domain method for the design of RF pulses in multicoil parallel excitation , 2006, Magnetic resonance in medicine.

[18]  Douglas C Noll,et al.  Fast‐kz three‐dimensional tailored radiofrequency pulse for reduced B1 inhomogeneity , 2006, Magnetic resonance in medicine.

[19]  G. Gold,et al.  Iterative decomposition of water and fat with echo asymmetry and least‐squares estimation (IDEAL): Application with fast spin‐echo imaging , 2005, Magnetic resonance in medicine.

[20]  Yudong Zhu,et al.  Parallel excitation with an array of transmit coils , 2004, Magnetic resonance in medicine.

[21]  T. Ibrahim,et al.  Effect of RF coil excitation on field inhomogeneity at ultra high fields: a field optimized TEM resonator. , 2001, Magnetic resonance imaging.

[22]  Y Zur Design of improved spectral‐spatial pulses for routine clinical use , 2000, Magnetic resonance in medicine.

[23]  Michael B. Smith,et al.  SAR and B1 field distributions in a heterogeneous human head model within a birdcage coil , 1998, Magnetic resonance in medicine.

[24]  Jianming Jin,et al.  On the SAR and field inhomogeneity of birdcage coils loaded with the human head , 1997, Magnetic resonance in medicine.

[25]  A Kerr,et al.  Consistent fat suppression with compensated spectral‐spatial pulses , 1997, Magnetic resonance in medicine.

[26]  C D Claussen,et al.  Highly selective water and fat imaging applying multislice sequences without sensitivity to B1 field inhomogeneities , 1997, Magnetic resonance in medicine.

[27]  J. Finn,et al.  Phase‐Modulated binomial RF pulses for fast spectrally‐selective musculoskeletal imaging , 1996, Magnetic resonance in medicine.

[28]  J. Pauly,et al.  Simultaneous spatial and spectral selective excitation , 1990, Magnetic resonance in medicine.

[29]  S J Riederer,et al.  Chemical shift selective MR imaging using a whole-body magnet. , 1986, Investigative radiology.

[30]  A. Haase,et al.  Chemical shift selective MR imaging using a whole-body magnet. , 1985, Radiology.

[31]  G M Bydder,et al.  MR Imaging: Clinical Use of the Inversion Recovery Sequence , 1985, Journal of computer assisted tomography.

[32]  W. T. Dixon Simple proton spectroscopic imaging. , 1984, Radiology.