Method for reversing residual transverse magnetization due to phase-encoding magnetic field gradients

• US 4,665,365 A
• Filed: 01/07/1985
• Issued: 05/12/1987
• Est. Priority Date: 01/07/1985
• Status: Expired due to Term

• Current Assignee: General Electric Company
• Original Assignee: General Electric Company
• Inventors: Glover, Gary H., Pelc, Norbert J.
• Primary Examiner(s): Levy, Stewart J.
• Assistant Examiner(s): Oldham, Scott M.
• Application Number:
  US06/689,428
• Time in Patent Office: 855 Days
• Field of Search: 324/300, 324/307, 324/309, 324/313, 324/314, 324/318, 324/322, 324/311
• US Class Current: 324/309
• CPC Class Codes: G01R 33/482 using a Cartesian trajectory

Abstract

A method for reversing residual transverse magnetization due to spatial encoding magnetic field gradient pulses, used in magnetic resonance imaging to encode spatial information, employs a reversing gradient pulse applied in the same direction as the encoding gradient pulse following the observation of the spin-echo signal. The encoding gradient pulse is applied following the 180° RF pulse to avoid the effects of imperfections associated therewith. In one embodiment, the amplitudes of the encoding and reversing gradient pulses are selected to be approximately the negatives of each other so as to substantially cancel the residual magnetization. In another embodiment, the amplitude of the reversing gradient pulse is selected such that the algebraic sum thereof with the corresponding amplitude of the encoding gradient pulse is a constant. In this case, the residual magnetization is not necessarily cancelled, but rather, is left in the same state after each view of the pulse sequence. The method is applicable to multiple-echo and driven equilibrium pulse sequences.

Claims

1. A method for undoing the effect of magnetic field gradients on the residual transverse magnetization in a pulse sequence useful for producing images of a study object positioned in a homogeneous magnetic field, which pulse sequence includes a predetermined plurality of sequentially implemented views, each of said views including at least one RF excitation pulse for exciting nuclear spins in the object, one 180°

RF pulse for generating a spin-echo signal, and at least one encoding magnetic field gradient pulse used to encode spatial information into said spin-echo signal, said method comprising the steps of;

applying said encoding magnetic field gradient pulse subsequent to the irradiation of the study object with said 180°

RF pulse, but prior to the occurrence of said spin-echo signal, said encoding magnetic field gradient pulse being applied along at least one directional axis of the study object; and

applying, following the occurrence of said spin-echo signal, a reversing magnetic field gradient pulse so as to undo the effects of said encoding magnetic field gradient pulse on any residual transverse magnitization, the amplitude of said reversing and encoding gradient pulses being selected such that the algebraic sum thereof along said one axis is equal to a constant.

2. The method of claim 1 wherein the amplitude of the reversing magnetic gradient pulse is selected to be substantially equal to the negative amplitude of the encoding pulse.

3. The method of claim 1 wherein each view includes a plurality of 180°

RF pulses and a corresponding plurality of spin-echo signals, said method further comprising the steps of applying an encoding magnetic gradient pulse before the occurrence of each of said spin-echo signals and a reversing magnetic field gradient pulse following the occurrence of each spin-echo signal, wherein the amplitudes of said encoding and reversing gradient pulses preceding and following each spin-echo signal in each view are selected such that the algebraic sum thereof is equal to a constant.

4. The method of claim 3 wherein the amplitude of the reversing magnetic gradient pulse is selected to be substantially equal to the negative amplitude of the encoding pulse.

5. The method of claim 1 wherein each view includes an odd plurality of 180°

RF pulses and a corresponding plurality of spin-echo signals, said method further comprising the step of applying an encoding magnetic field gradient subsequent to the application of said first 180°

RF pulse, but prior to the occurrence of the first spin-echo signal and applying a reversing magnetic field gradient pulse subsequent to the occurrence of the last spin-echo signal due to the application of the last one of said plurality of 180°

RF pulses, the amplitudes of said encoding and reversing magnetic field gradient pulses in each view being selected such that the algebraic sums thereof are equal to a constant.

6. The method of claim 5 wherein the amplitudes of the encoding and reversing magnetic gradient pulses are selected to be substantially identical.

7. The method of claim 1 wherein each view includes an even plurality of 180°

RF pulses and a corresponding plurality of spin-echo signals, said method further comprising the step of applying an encoding magnetic field gradient pulse subsequent to the application of said first 180°

RF pulse, but prior to the occurrence of the first spin-echo signal and reapplying a reversing magnetic field gradient pulse subsequent to the occurrence of the last spin-echo signal due to the application of the last one of plurality of 180°

RF pulses, wherein the algebraic sum of the amplitude of the encoding gradient and the negative amplitude of the reversing gradient in each view is equal to a constant.

8. The method of claim 7 wherein the amplitude of the encoding pulse and the negative amplitude of the reversing magnetic gradient pulse are selected to be substantially identical.

9. The method of claim 1 wherein said encoding gradient pulse comprises a phase-encoding gradient pulse.

10. The method of claim 1 wherein said pulse sequence comprises a multiple-angle projection reconstruction imaging method and wherein said encoding gradient pulse is a dephasing gradient which allows the spin echo to be detected in the presence of a read-out gradient.