Method and apparatus for compensating for b1 inhomogeneity in magnetic resonance imaging by nonselective three-dimensional tailored RF pulses
A uniform, radio frequency pulse technology, applied in the direction of using nuclear magnetic resonance imaging system for measurement, magnetic resonance measurement, and analysis by nuclear magnetic resonance, can solve the problem of non-obvious B1 inhomogeneity
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[0047] figure 1 A very schematic illustration of a Magnetic Resonance Imaging (MRI) scanner comprising:
[0048] - a magnet M for generating a static, substantially uniform magnetic field B oriented along the direction z 0 , the patient's body (or a part of the patient's body) PB to be imaged is placed in the magnetic field;
[0049] - a radio frequency coil RFC for exposing the body to transverse radiofrequency pulses ("transverse" here means having 0 polarization, and thus in the x-y plane) and for detecting signals emitted by flipped nuclear spins within the body;
[0050] - three sets of gradient coils GC for generating gradient fields, i.e. magnetic fields oriented along the z-direction and varying linearly along corresponding spatial directions through the volume of interest (VOI);
[0051] - Oscillator OS, modulator and RF amplifier for generating radio frequency pulses supplied to the radio frequency coil. In parallel transmission, the number of times the radio fre...
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