Magnetic resonance imaging compensated for very rapid variations in static magnetic field

A magnetic resonance imaging apparatus which gathers MRI data over a sequence of measurement cycles, comprising:

• means for superimposing first magnetic gradient pulses on a nominally static magnetic field to selectively address NMR RF excitations for at least one predetermined volume;
• means for superimposing second magnetic gradient pulses on said static magnetic field at other times in a measurement cycle;
• means for performing at least one further of said measurement cycles during which at least one of said second gradient pulses is omitted so as to produce calibration data representative of the magnetic field then existing in the predetermined volume;
• and
• means for using said calibration data to produce MRI data compensated for phase angle errors which otherwise would be present due to undesirable changes with respect to time in the magnetic field actually present in said predetermined volume,
• wherein the MRI data is compensated for phase angle errors by applying to the measured image data the inverse of the phase angles determined during the at least one further of said measurement cycles.

A magnetic resonance imaging method, comprising the steps of:

• gathering MRI data from an imaged volume over a sequence of measurement cycles;
• performing at least one pair of further calibration measurement cycles, wherein the polarity of all gradient pulses utilized in one cycle is reversed for another cycle and the respectively corresponding phases of measured NMR RF responses obtained in said pair of cycles is subtracted to provide calibration data substantially without chemical shift artifact and in the absence of applied magnetic gradients to produce calibration data;
• and
• using said calibration data to produce MRI data compensated for errors which otherwise would be present due to undesirable changes with respect to time in the magnetic field actually present in said imaged volume.

A magnetic resonance imaging apparatus, comprising:

• means for gathering MRI data from an imaged volume over a sequence of measurement cycles;
• means for performing at least one pair of further calibration measurement cycles, wherein the polarity of all gradient pulses utilized in one cycle is reversed for another cycle and the respectively corresponding phases of measured NMR RF responses obtained in said pair of cycles is subtracted to provide calibration data substantially without chemical shift artifact and in the absence of applied magnetic gradients to produce calibration data;
• and
• means for using said calibration data to produce MRI data compensated for errors which otherwise would be present due to undesirable changes with respect to time in the magnetic field actually present in said imaged volume.

A magnetic resonance imaging method which gathers MRI data over a sequence of measurement cycles, comprising the steps of:

• generating MRI data for a predetermined volume by superimposing magnetic gradient pulses on a nominally static magnetic field during a plurality of measurement cycles;
• measuring variations in the static magnetic field with respect to time generated by the magnetic gradient pulses;
• and
• using the measured variations to produce MRI data compensated for errors which otherwise would be present in the magnetic field actually present in said predetermined volume due to the magnetic gradient pulses.

A magnetic resonance imaging apparatus which gathers MRI image data over a sequence of measurement cycles, comprising:

• means for generating MRI data in a predetermined volume by superimposing magnetic gradient pulses on a nominally static magnetic field during a sequence of measurement cycles;
• means for measuring variations in the static magnetic field with respect to time generated by the magnetic gradient pulses;
• and
• means for using the measured variations to produce MRI data compensated for errors which otherwise would be present in the magnetic field actually present in said predetermined volume due to the magnetic gradient pulses.