Nuclear magnetic resonance apparatus and methods

• US 4,115,730 A
• Filed: 04/07/1977
• Issued: 09/19/1978
• Est. Priority Date: 04/14/1976
• Status: Expired due to Term

• Current Assignee: British Technology Group Ltd.
• Original Assignee: National Research Development Corporation
• Inventors: Mansfield, Peter
• Primary Examiner(s): Tokar, M.
• Application Number:
  US05/785,448
• Time in Patent Office: 530 Days
• Field of Search: 324/0.5 R, 324/0.5 A, 324/0.5 B
• US Class Current: 324/309
• CPC Class Codes: G01R 33/54 Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console

Abstract

A nuclear magnetic resonance spin density distribution in a sample is obtained for a selected plane or planes by placing the sample in a static magnetic field, applying a gradient to the field and simultaneously applying selective rf pulses to select a plane or planes in the sample, switching to an orthogonal gradient and simultaneously applying selective rf pulses to select strips in the selected plane or planes and then applying orthogonal field gradients to the sample of such relative magnitudes that each point of the selected strips is subjected to a resultant magnetic field of amplitude unique to that point. The free induction decay signal is then read out from the strips.

Claims

1. A method of obtaining a nuclear magnetic resonance spin density distribution of a sample which comprises maintaining a static magnetic field along one axis, applying a first magnetic field gradient to said static magnetic field to cause said field to vary along an axis selected from said one axis and an axis orthogonal thereto at the same time applying a selective excitation pulse so as to select at least one planar layer in the sample normal to the selected axis, removing said first magnetic field gradient and applying a second magnetic field gradient to said static magnetic field to cause said field to vary along an axis which is orthogonal to said selected axis and at the same time applying a selective excitation pulse to excite a series of strips in said at least one selected layer, and then simultaneously applying magnetic field gradients to said magnetic field to cause said field to vary in at least two of said orthogonal directions such that each point of the selected strips is subjected to a resultant magnetic field of amplitude unique to that point, and reading out the resulting free induction decay (FID) signal from said strips.

2. The method as claimed in claim 1 in which said first magnetic field gradient causes the static magnetic field to vary along its own axis.

3. The method as claimed in claim 1 in which said first magnetic field gradient causes the static magnetic field to vary along an axis orthogonal to the axis of the static magnetic field and the second magnetic field gradient causes the static magnetic field to vary along its own axis.

4. The method as claimed in claim 1 and including further steps in which the said simultaneously applied magnetic field gradients are periodically reversed to produce spin echoes.

5. The method as claimed in claim 1 and including the application of successive 180°

rf pulses to reverse the spins while maintaining said simultaneously applied magnetic field gradients so as to produce spin echoes.

6. The method as claimed in claim 1 in which the simultaneously applied magnetic field gradients cause the static mangetic field to vary in three orthogonal directions.

7. The method as claimed in claim 1 in which a plurality of planar layers are selected and the simultaneously applied magnetic field gradients cause the static magnetic field to vary in two directions orthogonal to its own direction and in which the resulting FID signals are read out individually from each of said selected layers.

8. The method as claimed in claim 1 and including the further step of Fourier transformation of said FID signal to yield a signal representing the magnetic resonance spin density distribution in the said strips.

9. The method as claimed in claim 1 in which the selective excitation pulses comprise a train of equally spaced short rf pulses followed by a short 90°

rf pulse whose phase is shifted 180°

from the phase of the pulse train.