Beyond k-space: spectral localization using higher order gradients.

Chemical shift imaging (CSI) often suffers from the inconvenient shape of its spatial response function (SRF), which affects both localization and signal-to-noise ratio. Replacing the magnetic field gradients for phase encoding by higher order magnetic fields allows a better adjustment of the SRF to the structures in the sample. We combined this principle with the SLOOP (spectral localization with optimal pointspread function) technique to simultaneously obtain spectra from several arbitrarily shaped compartments within a sample. Linear combinations of the fields of the shim coils are used to generate the pulsed fields for phase encoding. Their shapes are matched to the given sample geometry by numerical optimization. Using this method, spectra from a phantom were obtained that show a higher signal-to-noise ratio and a strongly reduced contamination compared to an equivalent CSI experiment.

[1]  W. Perman,et al.  Spatially resolved high resolution spectroscopy by “four-dimensional” NMR , 1983 .

[2]  David I. Hoult,et al.  The Ancient and Honourable Art of Shimming , 1990 .

[3]  P C Lauterbur,et al.  SLIM: Spectral localization by imaging , 1988, Magnetic resonance in medicine.

[4]  D. Hoult,et al.  Magnet field profiling: Analysis and correcting coil design , 1984, Magnetic resonance in medicine.

[5]  Marcel J. E. Golay,et al.  Field Homogenizing Coils for Nuclear Spin Resonance Instrumentation , 1958 .

[6]  Weston A. Anderson,et al.  Electrical Current Shims for Correcting Magnetic Fields , 1961 .

[7]  Thomas H. Mareci,et al.  High-resolution magnetic resonance spectra from a sensitive region defined with pulsed field gradients , 1984 .

[8]  Z H Cho,et al.  Localized volume selection technique using an additional radial gradient coil , 1989, Magnetic resonance in medicine.

[9]  D. Twieg The k-trajectory formulation of the NMR imaging process with applications in analysis and synthesis of imaging methods. , 1983, Medical physics.

[10]  A Haase,et al.  Localized spectroscopy from anatomically matched compartments: improved sensitivity and localization for cardiac 31P MRS in humans. , 1998, Journal of magnetic resonance.

[11]  J. Ra,et al.  Radial scanning technique for volume selective 31P spectroscopy , 1992, Magnetic resonance in medicine.

[12]  New spatial localization method using pulsed high‐order field gradients (SHOT: Selection with high‐order gradient) , 1991, Magnetic resonance in medicine.

[13]  D Hahn,et al.  Concentrations of human cardiac phosphorus metabolites determined by SLOOP 31P NMR spectroscopy , 1999, Magnetic resonance in medicine.

[14]  K. Uğurbil,et al.  NMR chemical shift imaging in three dimensions. , 1982, Proceedings of the National Academy of Sciences of the United States of America.

[15]  Michael A. Malcolm,et al.  Computer methods for mathematical computations , 1977 .

[16]  John S. Leigh,et al.  Transverse Hadamard spectroscopic imaging technique , 1990 .

[17]  A. Maudsley Fourier imaging using rf phase encoding , 1986, Magnetic Resonance in Medicine.

[18]  Thomas H. Mareci,et al.  Essential considerations for spectral localization using indirect gradient encoding of spatial information , 1991 .

[19]  Z P Liang,et al.  A generalized series approach to MR spectroscopic imaging. , 1991, IEEE transactions on medical imaging.

[20]  Andrew A. Maudsley,et al.  Sensitivity in fourier imaging , 1986 .

[21]  William H. Press,et al.  Numerical Recipes in FORTRAN - The Art of Scientific Computing, 2nd Edition , 1987 .

[22]  G. Arfken Mathematical Methods for Physicists , 1967 .

[23]  P. Jakob,et al.  Radial Spectroscopic Imaging , 1997 .

[24]  Markus von Kienlin,et al.  Spectral localization with optimal pointspread function , 1991 .