Method and Apparatus for Compensating for B1 Inhomogeneity in Magnetic Resonance Imaging by Nonselective Tailored RF Pulses

• US 20130038326A1
• Filed: 04/12/2011
• Published: 02/14/2013
• Est. Priority Date: 04/15/2010
• Status: Active Grant

• Current Assignee: Commissariat a L'Energie Atomique (French Alternative Energies and Atomic Energy Commission)
• Original Assignee: Commissariat a L'Energie Atomique (French Alternative Energies and Atomic Energy Commission)
• Inventors: Cloos, Martijn, Amadon, Alexis
• Granted Patent: US 9,291,691 B2
• Time in Patent Office: Days
• US Class Current: 324/309
• CPC Class Codes: G01N 24/08 by using nuclear magnetic resonance G01N24/12 takes precedence
• CPC Class Codes: G01R 33/246 Spatial mapping of the RF magnetic field B1
• CPC Class Codes: G01R 33/34046 Volume type coils, e.g. bird-cage coils; Quadrature bird-cage coils; Circularly polarised coils
• CPC Class Codes: G01R 33/44 using nuclear magnetic resonance [NMR] G01R33/24, G01R33/62 take precedence
• CPC Class Codes: G01R 33/4818 MR characterised by data acquisition along a specific k-space trajectory or by the temporal order of k-space coverage, e.g. centric or segmented coverage of k-space
• CPC Class Codes: G01R 33/4822 in three dimensions
• 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 33/4836 using an RF pulse being spatially selective in more than one spatial dimension, e.g. a 2D pencil-beam excitation pulse
• CPC Class Codes: G01R 33/5659 caused by a distortion of the RF magnetic field, e.g. spatial inhomogeneities of the RF magnetic field G01R33/56509, G01R33/56518, G01R33/56536 take precedence
• CPC Class Codes: G01R 33/586 for optimal flip angle of RF pulses

Abstract

A method of exciting nuclear spins in a body, the method comprising the steps of: (a) immerging said body (PB) in a static magnetic field (B₀) for aligning nuclear spins along a magnetization axis (z), said static magnetic field being substantially uniform over at least a volume of interest (VOI) of said body; (b) exposing said body, or at least said volume of interest, to a time-varying magnetic field gradient having components (G_x, G_y, G_z) directed along at least three non-coplanar directions (x, y, z) and to a transverse radio-frequency field (B₁), whereby said time-varying magnetic field gradient defines a three-dimensional trajectory in k-space constituted by segments linking discrete points (k_T¹−k_T⁹), and said transverse radio-frequency field deposits radio-frequency energy along at least part of said trajectory for flipping said nuclear spins by a same predetermined flip angle, independently from their position within said volume of interest. A method of performing magnetic resonance imaging comprising a step of exciting nuclear spins in a body to be imaged, characterized in that said step is performed by carrying out a method. A magnetic resonance imaging scanner for carrying out such a method.

Claims

1. A method of exciting nuclear spins in a body, the method comprising the steps of:

(a) immerging said body (PB) in a static magnetic field (B₀) for aligning nuclear spins along a magnetization axis (z), said static magnetic field being substantially uniform over at least a volume of interest (VOI) of said body;

(b) exposing said body, or at least said volume of interest, to a time-varying magnetic field gradient having components (G_x, G_y, G_z) directed along at least three non-coplanar directions (x, y, z) and to a radio-frequency non-selective pulse having a transverse polarization (B₁), whereby said time-varying magnetic field gradient defines a three-dimensional trajectory in k-space constituted by straight segments linking discrete points (k_T¹-k_T⁹), and said radio-frequency non-selective pulse having a transverse polarization deposits radio-frequency energy along at least part of said trajectory;

the positions of said discrete points in k-space being determined, and the radio-frequency non-selective pulse having a transverse polarization being designed, for flipping said nuclear spins by a same predetermined flip angle, independently from their position within said volume of interest.

2. A method according to claim 1 wherein said time-varying magnetic field gradient consists of a sequence of magnetic field gradient pulses.

3. A method according to claim 2 wherein said radio-frequency non-selective pulse having a transverse polarization comprises transverse radio-frequency subpulses (P₁-P₁₀) interleaved with said magnetic field gradient pulses, whereby said radio-frequency subpulses deposit radio-frequency energy in said discrete points of k-space.

4. A method according to claim 3 wherein no radio frequency pulse is applied simultaneously to said magnetic field gradient pulses, whereby radio-frequency energy is only deposited in said discrete points of k-space.

5. A method according to claim 1, comprising using a plurality of independently driven antenna elements (D₁-D₈) for generating and applying said radio-frequency non-selective pulse having a transverse polarization.

6. A method according to claim 1, further comprising a preliminary step of determining said discrete points of k-space and the corresponding amount of radio-frequency energy by computing a three-dimensional Fourier transform of a predetermined excitation pattern, called a compensation pattern.

7. A method according to claim 6 wherein said preliminary step comprises the substeps of:

i. defining said volume of interest where a uniform target distribution of the nuclear spins'"'"' flip angle is wanted;

ii. determining the distribution of the nuclear spins'"'"' flip angle induced by a standard circularly polarized radio-frequency mode in said volume of interest; and

iii. taking, as said compensation pattern, the difference between said uniform target distribution of the nuclear spins flip angle and the distribution of the nuclear spins flip angle induced by said standard circularly polarized radio-frequency mode.

8. A method according to claim 7 wherein said substep ii. is performed by measurement.

9. A method according to claim 6 wherein said preliminary step further comprises determining at least some of said discrete points of excitation k-space as corresponding to a number of the most energetic components of the three-dimensional discrete Fourier transform of said compensation pattern.

10. A method according to claim 7 wherein said preliminary step further comprises a step of iteratively computing the phase and amplitude of said transverse radio-frequency subpulses, or of the contribution to said transverse radio-frequency subpulses generated by each of said independently driven antenna elements, in order to minimize the overall duration of application of said radio-frequency field under SAR constraints.

11. A method according to claim 1 wherein at least some of said discrete points of k-space belong to face centers of a parallelepiped containing the center of k-space and whose side size is approximately (2/λ

_obj), where λ

_obj is the RF wavelength in the body to be imaged.

12. A method according to claim 1 wherein said time-varying magnetic field gradient consists of a sequence of magnetic field gradient pulses directed along three perpendicular directions, one of which is parallel to said magnetization axis.

13. A method according to claim 1 wherein said radio-frequency non-selective pulse having a transverse polarization is constituted by a sequence of square subpulses each corresponding to one of said discrete points of excitation k-space, or to a segment linking two of said points.

14. A method of exciting nuclear spins in a human head, the method comprising the steps of:

(a) immerging said human head, or a portion thereof, in a static magnetic field for aligning nuclear spins along a magnetization axis substantially parallel to a cranio-caudal direction of said human head, said static magnetic field being substantially uniform over at least a volume of interest (VOI) of said human head;

(b) exposing at least said volume of interest, to a time-varying magnetic field gradient defining a bi-dimensional trajectory in k-space constituted by straight segments linking discrete points, and said radio-frequency non-selective pulse having a transverse polarization deposits radio-frequency energy along at least part of said trajectory;

the positions of said discrete points in k-space being determined, and the radio-frequency non-selective pulse having a transverse polarization being designed, for flipping said nuclear spins by a same predetermined flip angle, independently from their position within said volume of interest.

15. A method according to claim 14 wherein said time-varying magnetic field gradient has a first component directed along said cranio-caudal direction and a second