Method, apparatus and recording medium for measuring and correcting phase error in spins in a phase axis direction
AssigneeGE Medical Systems Global Technology Company, LLC
InventorsMitsuharu Miyoshi, Aki Yamazaki
Life of this patent
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Abstract
For the purpose of accurately measuring and correcting a phase error in spins in a phase axis direction, a gradient magnetic field having an integral value of zero is applied in the phase axis direction during a time period between first and second 180° excitations to read out a first spin echo SE1; a gradient magnetic field having an integral value of zero is applied in the phase axis direction during a time period between second and third 180° excitations to read out a second spin echo SE2; and a phase error due to an effect of residual magnetization Gp0 is determined based on these spin echoes.
Claims34
A phase error measuring method comprising the steps of:
- effecting a 90° excitation on object spins;
- effecting a first 180° excitation after a first time period from said 90° excitation;
- effecting a second 180° excitation after a second time period from said first 180° excitation;
- effecting a third 180° excitation after said second time period from said second 180° excitation;
- applying a first gradient magnetic field consisting of a first pulse of a first polarity, followed immediately by a second pulse of a second polarity, opposite to said first polarity followed immediately by a third pulse of said first polarity and having a time integral value of zero in a phase axis direction during the time period from said first 180° excitation to said second 180° excitation to generate a first spin echo signal with a first phase error determined by distance from a peak of said first spin echo and a point in time when the time integral of said first pulse and said second pulse are equal;
- applying a second gradient magnetic field consisting of a first pulse of a first polarity followed immediately by second pulse of a second polarity which is opposite to said polarity followed immediately by a third pulse of said polarity and having a time integral value of zero in the phase axis direction during the time period from said second 180° excitation to said third 180° excitation to generate a second spin echo signal with a second phase error determined by distance from a peak of said second spin echo and a point in time when the time integral of said first pulse and second pulse are equal;
- and
- determining a phase error of the spins in the phase axis direction due to residue magnetization or eddy current or combination thereof during the time period from said 90° excitation to said first 180° excitation based on calculation using said first phase error and said second phase error of said first and second spin echo signals.
A phase error measuring apparatus comprising:
- first means for effecting a 90° excitation on object spins, for effecting a first 180° excitation after a first time period from said 90° excitation, for effecting a second 180° excitation after a second time period from said first 180° excitation, and for effecting a third 180° excitation after said second time period from said second 180° excitation;
- second means for applying a first gradient magnetic field consisting of a first pulse of a first polarity, followed immediately by a second pulse of a second polarity opposite to said first polarity, followed immediately by a third pulse of said first polarity and having a time integral value of zero in a phase axis direction during time period from said first 180° excitation to said second 180° excitation to generate a first spin echo signal with a first phase error determined by distance from a peak of said first echo signal and a point in time when the time integral of said first pulse and said second pulse are equal, and for applying a second gradient magnetic field consisting of a first pulse of a first polarity followed immediately by a second pulse of a second polarity which is opposite to said first polarity followed immediately by a third pulse of said first polarity and having a time integral value of zero in the phase axis direction during the time period from said second 180° excitation to said third 180° excitation to generate a second spin echo signal with a second phase error determined by a distance from a peak of said second spin echo and a point in time when the time integral of said first pulse and second pulse are equal;
- and
- third means for determining a phase error of the spins in the phase axis direction due to residual magnetization or eddy current or combination thereof during the time period from said 90° excitation to said first 180° excitation based on calculation using said first phase error and said second phase error of said first and second spin echo signals.
A recording medium wherein being recorded in a computer readable manner with a program for causing a computer to execute the functions of:
- effecting a 90° excitation on object spins;
- effecting a first 180° excitation after a first time period from said 90° excitation;
- effecting a second 180° excitation after a second time period from said first 180° excitation;
- effecting a third 180° excitation after said second time period from said second 180° excitation;
- applying a first gradient magnetic field consisting of a first pulse of a second polarity followed immediately by a second pulse of a second polarity opposite to said first polarity, followed immediately by a third pulse of said first polarity and having a time integral value of zero in a phase axis direction during the time period from said first 180° excitation to said second 180° excitation to generate a first spin echo signal with a first phase error determined by distance from a peak of said first spin echo and a point in time when the time integral of said first pulse and said second pulse are equal;
- applying a second gradient magnetic field consisting of a first pulse of first polarity followed immediately by a second pulse of first polarity which is opposite to said polarity followed immediately by a third pulse of said selected first polarity and having a time integral value of zero in the phase axis direction during the time period from said second 180° excitation to said third 180° excitation to generate a second spin echo signal with a second phase error determined by distance from a peak of said second spin echo and a point in time when the time integral of said first pulse and second pulse are equal and
- determining a phase error of the spins in the phase axis direction due to residue magnetization or eddy current or combination thereof during the time period from said 90° excitation to said first 180° excitation based on calculation using said first phase error and said second phase error of said first and second spin echo signals.
A magnetic resonance imaging apparatus acquiring a magnetic resonance signal from a object using a static magnetic field, gradient magnetic fields, and a high frequency magnetic field, and constructing an image based on said acquired magnetic resonance signal, said apparatus comprising:
- first means for effecting a 90° excitation on object spins, for effecting a first 180° excitation after a first time period from said 90° excitation, for effecting a second 180° excitation after a second time period from said first 180° excitation, and for effecting a third 180° excitation after said second time period from said second 180° excitation;
- second means for applying a first gradient magnetic field consisting of a first pulse of first polarity, followed immediately by a second pulse of a second polarity opposite to said first polarity, followed immediately by a third pulse of said first polarity and having a time integral value of zero in a phase axis direction during time period from said first 180° excitation to said second 180° excitation to generate a first spin echo signal with a first phase error determined by distance from a peak of said first echo signal and a point in time when the time integral of said first pulse and said second pulse are equal, and for applying a second gradient magnetic field consisting of a first pulse of a first polarity followed immediately by a second pulse of a second polarity which is opposite to said first polarity followed immediately by a third pulse of said first polarity and having a time integral value of zero in the phase axis direction during the time period from said second 180° excitation to said third 180° excitation to generate a second spin echo signal with a second phase error determined by a distance from a peak of said second spin echo and a point in time when the time integral of said first pulse and said second pulse are equal;
- and
- third means for determining a phase error of the spins in the phase axis direction due to residual magnetization or eddy current or combination thereof during the time period from said 90° excitation to said first 180° excitation based on calculation using said first phase error and said second phase error of said first and second spin echo signals.
The apparatus of 27, further comprising:
- fourth means for applying crusher gradient magnetic fields in a frequency axis direction before and after each of said 180° excitations.
Dependencies are inferred from the claim text.