Magnetic resonance system and method for rephasing spin systems in slices in slice multiplexing measurement sequences for magnetic resonance imaging

• US 9,599,690 B2
• Filed: 09/04/2012
• Issued: 03/21/2017
• Est. Priority Date: 09/01/2011
• Status: Active Grant

• Current Assignee: Siemens Healthineers AG (Siemens AG)
• Original Assignee: Siemens AG
• Inventors: Feiweier, Thorsten
• Primary Examiner(s): Koval, Melissa
• Assistant Examiner(s): FETZNER, TIFFANY A
• Application Number:
  US13/602,686
• Publication Number:
  US 20130057280A1
• Time in Patent Office: 1,659 Days
• Field of Search: 324300-322, 600407-435
• US Class Current: 1/1
• CPC Class Codes: G01R 33/4835 of multiple slices
• CPC Class Codes: G01R 33/565 Correction of image distortions, e.g. due to magnetic field inhomogeneities

Abstract

In a method for rephasing a first spin system in a first slice with a first coherence curve and a second spin system of a second slice with a second coherence curve, in the generation of MR images with slice multiplexing, a first RF pulse deflects the spin system of the first slice and a second RF pulse deflects the spin system of the second slice. The beginning of the second RF pulse is time-shifted with respect to the beginning of the first RF pulse by a time period that is shorter than the duration of the first RF pulse. A rephasing correction impresses a correction phase on at least one of the spin systems, and signals of the spin systems are respectively detected. The coherence curves are rephased so detection of the signals occurs simultaneously.

Claims

1. A method configured for generating magnetic resonance (MR) images with slice multiplexing, comprising:

with a control computer, operating an MR data acquisition unit in order to generate a basic magnetic field having a basic field direction, and in order to radiate a first radio-frequency pulse that deflects a first nuclear spin system in a first slice of a subject, thereby giving said first spin system in said first slice a magnetization in a plane that is transverse to said basic field direction in which said magnetization has a phase that exhibits a phase evolution represented as a first coherence curve;

with said control computer, operating said MR data acquisition unit in order to radiate a second radio-frequency pulse that deflects a second spin system in a second slice of the subject, thereby giving said second spin system in said second slice a magnetization in another plane that is transverse to said basic field direction in which said magnetization has a phase that exhibits a phase evolution represented as a second coherence curve;

with said control computer, controlling operation of said MR data acquisition unit in order to cause a beginning of a second radio-frequency pulse to be time-shifted by a difference time period, with respect to a beginning of said first radio-frequency pulse, that is shorter than a duration of said first radio-frequency pulse;

with said control computer, operating said MR data acquisition unit in order to impress a correction phase on at least one of said first and second spin systems and in order to thereafter detect, in a given signal detection time period, a first signal representing said magnetization of said first nuclear spin system resulting from said deflection of said first nuclear spin system and in order to detect a second MR signal representing said magnetization of said second spin system resulting from said deflection of said second nuclear spin system;

with said control computer, operating said MR data acquisition unit in order to impress said correction phase, whereby each of said first and second coherence curves is rephased thereby causing detection of said first and second MR signals simultaneously in said given signal detection time period; and

from said control computer, making the detected first and second MR signals available in electronic form as a data file.

3. A method as claimed in claim 1 comprising, with said control computer, operating the MR data acquisition unit in order to radiate each of said first and second radio-frequency pulses with a time curve that is asymmetrical with respect to a point in time of a maximum amplitude of the respective first and second radio-frequency pulses.

4. A method as claimed in claim 1 comprising, with said control computer, impressing at least a portion of said correction phase by a modulation of at least one of said first and second radio-frequency pulses during the respective radiation thereof, said modulation being selected from the group consisting of amplitude modulation and phase modulation.

5. A method as claimed in claim 1 comprising, with said control computer, implementing said phase correction by operating the MR data acquisition unit in order to activate a correction magnetic field gradient.

6. A method as claimed in claim 5 comprising, with said control computer, operating the MR data acquisition unit in order to activate said correction magnetic field gradient with a non-linear spatial dependency.

7. A method as claimed in claim 1 comprising, with said control computer, operating the MR data acquisition unit in order to radiate said first radio-frequency pulse as a first refocusing pulse that generates a spin echo in said first slice, and in order to radiate said second radio-frequency pulse as a second refocusing pulse that generates a spin echo in said second slice.

8. A method as claimed in claim 1 wherein said difference time period is a first difference time period, and comprising, with said control computer, operating the MR data acquisition unit in order to:

excite said first nuclear spin system out of an idle state with said first radio-frequency excitation pulse;

excite said second nuclear spin system out of an idle state with said second radio-frequency excitation pulse; and

time shift a beginning of said second radio-frequency excitation pulse by a second difference time period with respect to a beginning of said first radio-frequency excitation pulse.

9. A method as claimed in claim 8 comprising with said control computer, setting said second difference time period to be longer than a duration of said first radio-frequency excitation pulse.

10. A method as claimed in claim 9 comprising, with said control computer, operating the MR data acquisition unit in order to activate a first correction magnetic field gradient between said first and second excitation pulses, and activating a second correction magnetic field gradient between either said second excitation pulse and said refocusing pulses, or after said refocusing pulses and before said detection time period.

11. A method as claimed in claim 8 comprising with said control computer, controlling said MR data acquisition unit to cause said second difference time period to satisfy a criterion selected from the group consisting of said second difference period being twice as long as said first difference time period, and said second difference time period being shorter than a duration of said first radio-frequency excitation pulse.

12. A method as claimed in claim 1 comprising, (b)with said control computer, operating the MR data acquisition unit in order to:

radiate said first radio-frequency pulse and a first refocusing pulse that generates a spin echo in said first slice;

radiate said second radio-frequency pulse and a second refocusing pulse that generates a spin echo in said second slice;

activate a first diffusion refocusing pulse that inverts dephasing of said first spin system;

activate a second diffusion refocusing pulse that inverts dephasing of said second spin system; and

time shift a beginning of said second diffusion refocusing pulse by a difference time period with respect to a beginning of said first diffusion refocusing pulse.

13. A method as claimed in claim 12 comprising, with said control computer, setting said difference time period between said second diffusion refocusing pulse in said beginning of said first diffusion refocusing pulse to be identical to said difference time period between said beginning of said second radio-frequency and said beginning of said first radio-frequency excitation pulse.

14. A method as claimed in claim 13 comprising, with said control computer, setting a direction of the time shift of said difference time period between said first and second diffusion refocusing pulses to be identical to a direction of the time shift of said difference time period between said first and second refocusing pulses.

15. A method as claimed in claim 1 comprising, with said control computer, operating the MR data acquisition unit in order to radiate said first radio-frequency pulse as a first excitation pulse that excites said first nuclear spin system out of an idle state, and in order to radiate said second radio-frequency pulse as a second excitation pulse that excites said second nuclear spin system out of an idle state.

2. A method as claimed in claim one comprising:

with said control computer, setting said difference time period, according to a to at least one of (1) total duration of radiating said first and second radio-frequency pulses and implementing said correction phase and said signal detection time period, (2) an amplitude of said first and second radio-frequency pulses, and (3) a signal strength of said radio-frequency pulses; and

with said control computer, selecting said correction phase dependent on at least one of said difference time period, said first coherence curve and said second coherence curve.

16. A magnetic resonance imaging system configured for generating magnetic resonance (MR) images with slice multiplexing, comprising:

an MR data acquisition unit comprising a basic field magnet and a radio-frequency radiator;

a control computer configured to operate said MR data acquisition unit in order to cause said basic field magnet to generate a basic magnetic field having a basic field direction, and in order to radiate a first radio-frequency pulse from said radio-frequency radiator that deflects a first nuclear spin system in a first slice of a subject, thereby giving said first spin system in said first slice a magnetization in a plane that is transverse to said basic field direction in which said magnetization has a phase that exhibits a phase evolution represented as a first coherence curve;

said control computer being configured to operate said MR data acquisition unit in order to radiate a second radio-frequency pulse from said radio-frequency radiator that deflects a second spin system in a second slice of the subject, thereby giving said second spin system in said second slice a magnetization in another plane that is transverse to said basic field direction in which said magnetization has a phase that exhibits a phase evolution represented as a second coherence curve;

said control computer being configured to control operation of said MR data acquisition unit in order to cause a beginning of said second radio-frequency pulse to be time-shifted by a difference time period, with respect to a beginning of said first radio-frequency pulse, that is shorter than a duration of said first radio-frequency pulse;

said control computer being configured to operate said MR data acquisition unit in order to impress a correction phase on at least one of said first and second spin systems, and in order to thereafter detect, in a given signal detection time period, a first signal representing said magnetization of said first nuclear spin system resulting from said deflection of said first nuclear spin system and to deflect a second MR signal representing said magnetization of said second spin system resulting from said deflection of said second nuclear spin system;

said control computer being configured to impress said correction phase in order to cause each of said first and second coherence curves to be rephased whereby detection of said first and second MR signals occurs simultaneously in said given signal detection time period; and

said control computer being configured to make the detected first and second MR signals available from said control computer in electronic form as a data file.