Three-dimensional spiral echo volume imaging

• US 5,532,595 A
• Filed: 04/18/1994
• Issued: 07/02/1996
• Est. Priority Date: 04/18/1994
• Status: Expired due to Term

• Current Assignee: Picker International, Inc. (Koninklijke Philips N.V.)
• Original Assignee: Picker International, Inc. (Koninklijke Philips N.V.)
• Inventors: Liu, Haiying, Lampman, David A.
• Primary Examiner(s): O'Shea, Sandra L.
• Assistant Examiner(s): ARANA, LOUIS M
• Application Number:
  US08/228,661
• Time in Patent Office: 806 Days
• Field of Search: 324/300, 324/306, 324/307, 324/309, 324/312, 324/314, 128/653.2, 128/653.3
• US Class Current: 324/309
• CPC Class Codes: G01R 33/446 Multifrequency selective RF pulses, e.g. multinuclear acquisition mode spatially selective RF pulses G01R33/4833
• CPC Class Codes: G01R 33/4824 using a non-Cartesian trajectory
• CPC Class Codes: G01R 33/561 by reduction of the scanning time, i.e. fast acquiring systems, e.g. using echo-planar pulse sequences

Abstract

Magnetic resonance imaging data of a volume of interest is collected by applying a radio frequency pulse (70, 96) and following the pulse with gradients applied along three axes (x,y,z). The gradients along x and y-axes are generally sinusoidal, which sinusoids increase and decrease in magnitude to define beat patterns of a common period. The period of the first and second gradients is an integer multiple of the gradient along the z-axis. In the embodiment of FIGS. 2A and 2B, the beats of the first and second gradients increase linearly and the third gradient oscillates in a linearly expanding generally sinusoidal pattern such that k-space is traversed by a trajectory that spirals around a series of spheres (50, 52, 54, 56, 58, 60) of progressively smaller radius. Blips or spikes (78) are preferably applied between each half cycle of the third gradient to step the trajectory to the radius of the next concentric sphere. In the embodiment of FIGS. 3A and 3B, the magnitude of the beats of the first and second gradients remain substantially constant and the gradient pulses along the third axis are applied generally between and at the mid-point of each beat such that the trajectory through k-space follows a series of parallel spirals lying along a cylinder. In the embodiment of FIGS. 4-4D, the beat patterns again increase linearly and the third gradient alternates polarity with each half beat such that the trajectory through k-space spirals around a series of concentric cones.

Claims

1. In an echo volume magnetic resonance imaging method in which selected dipoles in a volume of interest are induced to resonate by an RF pulse and in which a series of gradients are applied after the RF pulse and in the absence of any additional RF pulses such that resonance signal data is simultaneously detected and spatially encoded along a preselected data collection trajectory in three dimensions in k-space, the improvement comprising:

applying the magnetic field gradients such that the trajectory in k-space follows a three-dimensionally curving spiral trajectory through the three-dimensions.

2. In the echo volume method of magnetic resonance imaging as set forth in claim 1, the improvement further comprising:

configuring the magnetic field gradients such that the trajectory in k-space follows along ellipsoidal surfaces of multiple sizes.

6. In the echo volume magnetic resonance imaging method as set forth in claim 1, the improvement further comprising:

configuring the magnetic field gradients such that the trajectory through k-space extends along spiral paths lying on surfaces of cones.

7. The echo volume magnetic resonance imaging method as set forth in claim 6, the improvement further comprising:

configuring the magnetic field gradients such that the cones have a common apex and a range of cone angles.

3. In an echo volume imaging method in which selected dipoles in an entire volume of interest are induced to resonate by at least one RF pulse and in which a series of gradients are applied concurrently in the absence of RF pulses such that views of data are collected along a preselected data collection trajectory in three dimensions in k-space, the improvement comprising:

configuring the magnetic field gradients such that the trajectory in k-space follows spiraling paths which lie along a series of spheroidal surfaces of a multiplicity of radii.

4. In the echo volume imaging method as set forth in claim 3, the improvement further comprising:

configuring the magnetic field gradients such that the spheroidal surfaces are concentric spheres.

5. In the echo volume imaging method as set forth in claim 3, the improvement further comprising:

configuring the magnetic field gradients such that the spheroidal surfaces are non-concentric and touch a next larger spheroidal surface at one pole and a next smaller spheroidal surface at an opposite pole.

8. A method of echo volume magnetic resonance imaging comprising:

applying a radio frequency pulse to excite magnetic resonance in a volume of interest as a whole;

after exciting magnetic resonance in the whole volume, simultaneously sampling and spatially encoding the excited magnetic resonance in the absence of radio frequency pulses along a curving three-dimensional trajectory through k-space, including concurrently;

applying a first magnetic field gradient along a first axis, the first magnetic field gradient being generally sinusoidal and increasing and decreasing in magnitude in a beat pattern with a first period;

applying a second magnetic field gradient along a second axis, the second magnetic field gradient being generally sinusoidal and increasing and decreasing in magnitude in a beat pattern with the first period;

applying a third magnetic field gradient along a third axis, the third gradient having a second period, one of the first and second periods being an integer multiple of the other;

sampling magnetic resonance data at least during each half cycle of one of the first and second sinusoidal gradients;

reconstructing the sampled data into a volumetric magnetic resonance image representation.

9. The method as set forth in claim 8 wherein the beats of at least one of the first and second gradients decrease linearly in magnitude.

10. The method as set forth in claim 8 wherein the beats of at least one of the first and second gradients increase in magnitude linearly.

11. The method as set forth in claim 10 wherein the third gradient varies generally as a sinusoid having a half wavelength of the first period such that the time for applying one of the beats of the first and second gradients is the same as a half cycle of the third gradient.

12. The method as set forth in claim 11 wherein the third gradient is decreasing in magnitude with each half cycle.

13. The method as set forth in claim 11 wherein the third gradient is increasing in magnitude linearly with each half cycle.

14. The method as set forth in claim 13 wherein the magnitude of the beats of the first and second gradients is changing linearly such that k-space is sampled along a surface of a multiplicity of spheres of different radii.

15. The method as set forth in claim 14 wherein the third magnetic field gradient has a spike at each half cycle such that the trajectory steps between concentric spheres of different radii.

16. The method as set forth in claim 8 wherein the third gradient alternates polarity at the beginning and mid-point of each beat.

18. The method as set forth in claim 8 wherein the third gradient includes a series of gradient pulses applied between and at mid-points of each beat of the first and second gradients.

19. The method as set forth in claim 18 wherein the beats of the first and second gradients have substantially constant magnitudes and wherein the sinusoidally varying gradient of one of the first and second gradients changes phase by 180°

at a mid-point of each beat, such that k-space is traversed along parallel spiral paths of a cylindrical volume.

17. A method of echo volume imaging comprising:

applying a radio frequency pulse to excite magnetic resonance in a whole volume of interest;

in the absence of additional radio frequency pulses and before the excited resonance decays away, concurrently;

applying a first magnetic field gradient along a first axis, the first magnetic field gradient being generally sinusoidal and rapidly increasing and decreasing in magnitude in a beat pattern with a first periodicity;

applying a second magnetic field gradient along a second axis, the second magnetic field gradient being generally sinusoidal and increasing and decreasing in magnitude in a beat pattern with the first periodicity, the beats of the first and second gradients increasing or decreasing peak amplitudes, such that k-space is traversed along conical spirals;

applying a third magnetic field gradient along a third axis the third gradient having a second periodicity, one of the first and second periodicities being an integer multiple of the other, the third gradient alternating polarity adjacent the beginning and mid-point of each beat;

sampling the magnetic resonance such that the magnetic resonance is sampled along a spirally conical trajectory in k-space;

reconstructing the sampled data into a volumetric image representation.