Radio frequency excitation method and device for magnetic resonance imaging system

• US 9,897,676 B2
• Filed: 03/21/2014
• Issued: 02/20/2018
• Est. Priority Date: 03/22/2013
• Status: Active Grant

• Current Assignee: Siemens Healthineers AG (Siemens AG)
• Original Assignee: Siemens AG
• Inventors: Huang, Yu Qing, Zhao, Cong
• Primary Examiner(s): Vargas, Dixomara
• Application Number:
  US14/221,614
• Publication Number:
  US 20140285193A1
• Time in Patent Office: 1,432 Days
• CPC Class Codes: G01R 33/4833 using spatially selective excitation of the volume of interest, e.g. selecting non-orthogonal or inclined slices
• CPC Class Codes: G01R 33/5616 using gradient refocusing, e.g. EPI
• CPC Class Codes: G01R 33/56341 Diffusion imaging

Abstract

In an RF excitation method and device for a magnetic resonance imaging system, the RF pulses are emitted in a STEAM sequence, the STEAM sequence including, in time order, a first 90-degree excitation pulse, a second 90-degree excitation pulse and a third 90-degree excitation pulse. Gradient pulses are activated that act in cooperation with the STEAM sequence, the gradient pulses including, in time order, a first gradient pulse, a second gradient pulse and a third gradient pulse. Each of the gradient pulses is activated simultaneously with the corresponding RF pulse. The direction of each of the gradient pulses is the vector sum of multiple gradient pulses in different directions, the directions of any two of the gradient pulses being the same and intersecting with the direction of another of the gradient pulses.

Claims

1. A method for acquiring magnetic resonance (MR) image data, comprising:

operating a radio-frequency (RF) radiator of an MR data acquisition unit to radiate RF pulses in a STEAM (Stimulated Echo Acquisition Mode) imaging sequence, said RF pulses comprising, in chronological order, a first 90°

excitation pulse, a second 90°

excitation pulse, and a third 90°

excitation pulse, each of which excites nuclear spins in an examination subject situated in the MR data acquisition unit;

operating a gradient system of the MR data acquisition unit to activate gradient pulses in synchronization with, and as an addition to, said STEAM imaging sequence, said gradient pulses comprising, in chronological order, a first gradient pulse, a second gradient and a third gradient pulse, said first, second and third gradient pulses being respectively simultaneously with said first, second and third 90°

RF excitation pulses;

operating said gradient system of said MR data acquisition unit to activate said first, second and third gradient pulses non-orthogonally with a respective direction of each of said first, second and third gradient pulses being a vector sum of multiple gradient pulses in different directions, with respective directions of any two of said gradient pulses being identical and intersecting with the direction of another of said gradient pulses, in order to reduce said imaging area compared to an imaging area produced by said STEAM imaging sequence without said addition; and

operating said MR data acquisition unit to acquire MR data resulting from the excited nuclear spins, transforming the acquired MR data into image data, and making the acquired MR image data available at an output of the MR data acquisition unit as an electronic signal.

2. A method as claimed in claim 1 comprising operating said gradient system of said MR data acquisition unit to activate said second gradient pulse and third gradient pulse in directions that are identical and that intersect with the direction of the first gradient pulse.

3. A method as claimed in claim 1 comprising operating the gradient system of said MR data acquisition unit to activate said second gradient pulse and said first gradient pulse in identical directions that intersect with the direction of the third gradient pulse.

4. A method as claimed in claim 1 comprising operating the gradient system of the MR data acquisition unit to activate the first gradient pulse and the third gradient pulse in identical directions that intersect with the direction of the second gradient pulse.

5. A method as claimed in claim 1 comprising operating the gradient system of the MR data acquisition unit to activate the first, second and third gradient pulses with respective directions of any two of said first, second and third gradient pulses being identical and orthogonal to the direction of another of the first, second and third gradient pulses.

6. A method as claimed in claim 1 comprising operating said RF radiator of said MR data acquisition unit with said STEAM imaging sequence as a DW STEAM EPI sequence.

7. A magnetic resonance (MR) apparatus comprising:

an MR data acquisition unit, in which an examination subject is situated, said MR data acquisition unit comprising a radio-frequency (RF) radiator and a gradient system;

a control unit configured to operate the RF radiator to radiate RF pulses in a STEAM (Stimulated Echo Acquisition Mode) imaging sequence, said RF pulses comprising, in chronological order, a first 90°

excitation pulse, a second 90°

excitation pulse, and a third 90°

excitation pulse, each of which excites nuclear spins in the examination subject situated in the MR data acquisition unit;

said control unit being configured to operate the gradient system to activate gradient pulses in synchronization with, and as an addition to, said STEAM imaging sequence, said gradient pulses comprising, in chronological order, a first gradient pulse, a second gradient and a third gradient pulse, said first, second and third gradient pulses being respectively simultaneously with said first, second and third 90°

RF excitation pulses;

said control unit being configured to operate the gradient system to activate said first, second and third gradient pulses non-orthogonally with a respective direction of each of said first, second and third gradient pulses being a vector sum of multiple gradient pulses in different directions, with respective directions of any two of said gradient pulses being identical and intersecting with the direction of another of said gradient pulses, in order to reduce said imaging area compared to an imaging area produced by said STEAM imaging sequence without said addition; and

said control unit being configured to operate said MR data acquisition unit to acquire MR image data resulting from the excited nuclear spins, transforming the acquired MR data into image data, and to make the image data available at an output of the MR data acquisition unit as an electronic signal.

8. An MR system as claimed in claim 7, wherein said control unit is configured to operate said gradient system of said MR data acquisition unit to activate said second gradient pulse and third gradient pulse in directions that are identical and that intersect with the direction of the first gradient pulse.

9. An MR system as claimed in claim 8, wherein said control unit is configured to operate the gradient system of said MR data acquisition unit to activate said second gradient pulse and said first gradient pulse in identical directions that intersect with the direction of the third gradient pulse.

10. An MR system as claimed in claim 8, wherein said control unit is configured to operate the gradient system of the MR data acquisition unit to activate the first gradient pulse and the third gradient pulse in identical directions that intersect with the direction of the second gradient pulse.

11. An MR system as claimed in claim 8, wherein said control unit is configured to operate the gradient system of the MR data acquisition unit to activate the first, second and third gradient pulses with respective directions of any two of said first, second and third gradient pulses being identical and orthogonal to the direction of another of the first, second and third gradient pulses.

12. An MR system as claimed in claim 8, wherein said control unit is configured to operate said RF radiator of said MR data acquisition unit with said STEAM imaging sequence as a DW STEAM EPI sequence.