Nuclear magnetic resonance systems

• US 4,379,262 A
• Filed: 08/05/1980
• Issued: 04/05/1983
• Est. Priority Date: 08/10/1979
• Status: Expired due to Term

• Current Assignee: Picker International, Inc. (Marconi Holdings Company Limited)
• Original Assignee: Picker International, Inc. (Marconi Holdings Company Limited)
• Inventors: Young, Ian R.
• Primary Examiner(s): Tokar, Michael J.
• Application Number:
  US06/175,672
• Time in Patent Office: 973 Days
• Field of Search: 324/300, 324/309, 324/310, 324/311, 324/313, 324/320
• US Class Current: 324/309
• CPC Class Codes: G01N 24/08 by using nuclear magnetic resonance G01N24/12 takes precedence
• CPC Class Codes: G01R 33/54 Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console

Abstract

The invention is suitable for a small nuclear magnetic resonance pulse head applicable to a part of the body in the manner of ultrasonic systems. The arrangement generates a field which varies in amplitude with distance from the head, being uniform at surfaces which intrude into the body. Resonance is excited in one such surface and a gradient restricts resonance to one line therein. The phase is then dispersed along the line and the signal sensed as a function of position therealong.

Claims

1. A nuclear magnetic resonance apparatus comprising:

first magnetic means for generating a steady magnetic field which bulges outwardly from one side of said first magnetic means so as to protrude into a body positioned adjacent said first magnetic means on said one side, thereby to establish therein a magnetic field which varies in strength with distance in at least a first direction in said body and is of constant strength in curved surfaces in said body;

means for preferentially exciting resonance of nuclei within the body lying in a selected one of said curved surfaces of constant magnetic field strength;

second magnetic means for applying a magnetic field having a gradient in a second direction orthogonal to said first direction, thereby to restrict resonance to a line in said one surface wherein said one surface intersects a surface in which the magnetic field produced by said second magnetic means is constant;

means for dispersing the phase of the resonance along said line; and

means for sensing the dispersed resonance as a function of position in said line.

3. An apparatus according to claim 1 wherein said first magnetic means comprises a U-shaped yoke and a coil arranged to energise the U-shaped yoke to provide, in an area adjacent the gap between the ends of the yoke, said steady magnetic field.

4. An apparatus according to claim 1 or claim 3 wherein said means for exciting resonance includes a coil system cooperating with drive circuits arranged to generate an RF field.

5. An apparatus according to claim 4 wherein said RF coil system also forms part of said means for sensing the dispersed resonance.

6. An apparatus according to claim 1 wherein said means for dispersing include means for generating a further magnetic field having a gradient substantially orthogonal to said first and second directions.

7. An apparatus according to claim 6 wherein said means for generating said further field include field coils.

8. An apparatus according to claim 1 including Fourier Transform means arranged to cooperate with the means for sensing the dispersed resonance to provide signals representing amplitudes of resonance for different positions in said line.

9. An apparatus according to claim 1 including a mobile probe which includes coils for generating said fields and sensing said resonance signals.

2. A method of examining a body by nuclear magnetic resonance, the method including:

applying to the body from one side only thereof a steady magnetic field which protrudes into the body from said one side so as to provide within the body a magnetic field which varies in strength with distance in at least a first direction in said body and which is of constant strength in curved surfaces in said body;

preferentially exciting resonance of nuclei within the body lying on selected one of said surfaces;

applying a second magnetic field to said body having a gradient in a second direction orthogonal to said first direction, thereby to restrict resonance to a line on said one surface wherein said one surface intersects a surface on which the second applied magnetic field is constant;

dispersing the phase of the resonance along said line; and

sensing the dispersed resonance as a function of position in said line.

10. A method according to claim 2 wherein said resonance is excited by application of an RF magnetic field having a first pulse envelope.

11. A method according to claim 10 wherein said first pulse envelope is followed by a second pulse envelope of said RF field to cause a spin echo of said resonance.

12. A method according to claim 11 wherein the first pulse envelope provides a π

/2 pulse and the second pulse envelope provides a π

pulse.

13. A method according to claim 11 or claim 12 wherein said second magnetic field is applied prior to said spin echo and the said dispersion is obtained by applying to said body, immediately following said spin echo, a third magnetic field having a gradient in a direction orthogonal to said first and second directions.