Reduction of RF penetration effects in high field imaging

A method of correcting for the RF inhomogeneity in the body by dielectric loading of the coil‐to‐shield space in an RF resonator (coil and shield assembly) is described. The presence of the RF coil and RF shield have significant effects on RF homogeneity. Based on theoretical calculations, a method for adjusting the RF homogeneity by manipulating the axial propagation constant, kz, is proposed. This is accomplished by loading the coil‐to‐shield space with dielectric material of suitable relative permittivity so as to increase kz and decrease the radial propagation constant, kp. In this manner, the radial wavelength (λp, = 2π/kp) can be increased relative to the body dimensions, and the field amplitude variations in the axial plane minimized. Theoretical calculations indicate that a value of between 30 and 40 for the relative permittivity of the dielectric material in the coil‐to‐shield space would reduce the RF field inhomogeneity from ±15% to about ±3% over a central 30‐cm‐diameter region of a homogeneous 40‐cm‐diameter body at both 64 and 170 MHz. The theoretical model was verified in laboratory measurements of the |B1|, field generated in a test coil at 170 MHz which was scaled to correspond to a body at 64 MHz. However, the improved RF field homogeneity would be accompanied by increased RF power requirements and reduced coil sensitivity. © 1992 Academic Press, Inc.

[1]  P. Bottomley A technique for the measurement of tissue impedance from 1 to 100 MHz using a vector impedance meter. , 1978, Journal of physics E: Scientific instruments.

[2]  P A Bottomley,et al.  RF magnetic field penetration, phase shift and power dissipation in biological tissue: implications for NMR imaging. , 1978, Physics in medicine and biology.

[3]  P. Lauterbur,et al.  The sensitivity of the zeugmatographic experiment involving human samples , 1979 .

[4]  R. Mark Henkelman,et al.  Absorption Of NMR Signals At High Frequencies In Physiological Phantoms , 1984, Medical Imaging.

[5]  W. Barber,et al.  Comparison of linear and circular polarization for magnetic resonance imaging , 1985 .

[6]  J. Schenck,et al.  An efficient, highly homogeneous radiofrequency coil for whole-body NMR imaging at 1.5 T , 1985 .

[7]  D. Hoult,et al.  The field dependence of NMR imaging. I. Laboratory assessment of signal‐to‐noise ratio and power deposition , 1986, Magnetic resonance in medicine.

[8]  A layer model for RF penetration, heating, and screening in NMR , 1988 .

[9]  J. Carlson,et al.  Radiofrequency field propagation in conductive NMR samples , 1988 .

[10]  P. Roemer,et al.  The NMR phased array , 1990, Magnetic resonance in medicine.

[11]  T K Foo,et al.  An analytical model for the design of RF resonators for MR body imaging , 1991, Magnetic resonance in medicine.

[12]  P B Roemer,et al.  Volume imaging with MR phased arrays , 1991, Magnetic resonance in medicine.