Abstract: An MRI system receive coil arrangement 3 for use with a main MRI scanner arrangement. The arrangement includes at least one primary receive coil 6 having a first impedance at a predetermined frequency and a first size defined by a cross-sectional area bounded by the primary receive coil and at least one auxiliary receive coil 7 having a second impedance at said predetermined frequency and a second size defined by a cross-sectional area bounded by the auxiliary receive coil wherein the first impedance is lower than the second impedance and the first size is larger than the second size.

Abstract: An MRI system coil insert 2 for use within a bore B of a main MRI system 1, the coil insert 2 comprising at least one gradient coil, for creating a spatially varying magnetic field along a respective axis and being arranged to be electrically driven at an ultrasonic frequency.

Abstract: An MRI system receive coil arrangement 3 for use with a main MRI scanner arrangement. The arrangement includes at least one primary receive coil 6 having a first impedance at a predetermined frequency and a first size defined by a cross-sectional area bounded by the primary receive coil and at least one auxiliary receive coil 7 having a second impedance at said predetermined frequency and a second size defined by a cross-sectional area bounded by the auxiliary receive coil wherein the first impedance is lower than the second impedance and the first size is larger than the second size.

Abstract: An MRI system coil insert 2 for use within a bore B of a main MRI system 1, the coil insert 2 comprising at least one gradient coil, for creating a spatially varying magnetic field along a respective axis and being arranged to be electrically driven at an ultrasonic frequency.

Abstract: In a method and apparatus for detection and spectral editing in MR spectroscopy by polarization transfer in which the high spin population difference of two or more energy levels of a particular nuclear spin system is transferred to the energy levels of an other nuclear spin system with lower spin population difference, all RF pulses to be irradiated are irradiated sequentially, i.e. with defined time interval to each other, so that at no time of the sequence are different RF pulses irradiated concurrently in an overlapping manner. The sequential succession of the RF pulses causes the polarization transfer between the two spin systems of atomic nuclei involved. The sequence of the RF pulses in each domain of the respective nuclei is completely symmetric.

Abstract: In a method and apparatus for detection and spectral editing in MR spectroscopy by polarization transfer in which the high spin population difference of two or more energy levels of a particular nuclear spin system is transferred to the energy levels of an other nuclear spin system with lower spin population difference, all RF pulses to be irradiated are irradiated sequentially, i.e. with defined time interval to each other, so that at no time of the sequence are different RF pulses irradiated concurrently in an overlapping manner. The sequential succession of the RF pulses causes the polarization transfer between the two spin systems of atomic nuclei involved. The sequence of the RF pulses in each domain of the respective nuclei is completely symmetric.