Imaging magnetic spin resonance method and apparatus

• US 4,748,409 A
• Filed: 12/09/1985
• Issued: 05/31/1988
• Est. Priority Date: 12/14/1984
• Status: Expired due to Term

• Current Assignee: Max-Planck-Gesellschaft Zur Foerderung Der Wissenschaften e.V. (Max-Planck-Gesellschaft zur Frderung der Wissenschaften e)
• Original Assignee: Max-Planck-Gesellschaft Zur Foerderung Der Wissenschaften e.V. (Max-Planck-Gesellschaft zur Frderung der Wissenschaften e)
• Inventors: Haenicke, Wolfgang, Matthaei, Dieter, Merboldt, Klaus-Dietmar, Frahm, Jens, Haase, Axel
• Primary Examiner(s): Tokar, Michael J.
• Application Number:
  US06/806,780
• Time in Patent Office: 904 Days
• Field of Search: 324/300, 324/307, 324/309, 324/311, 324/312, 324/313, 324/314, 324/318, 324/322, 128/653
• US Class Current: 324/309
• CPC Class Codes: G01R 33/482 using a Cartesian trajectory
• CPC Class Codes: G01R 33/4833 using spatially selective excitation of the volume of interest, e.g. selecting non-orthogonal or inclined slices

Abstract

A method and an apparatus for a locally resolved investigation of a speci, wherein the specimen is exposed to a constant magnetic field and a variable combination of three gradient magnetic fields directed substantially perpendicularly to each other and to a sequence of high-frequency (RF) pulses which contains three successive pulses with flip angles not equal to |m Pi|, and signals corresponding to a magnetic resonance of spin moments, in particular nuclear spin moments in said specimen are detected. The interval (tau) between the first and the second pulse is greater than T_2eff and smaller than 5T₂, and that the interval (T-tau) between the second and the third pulse is greater than T_2eff and smaller than 5T₁, wherein

m is an integer,

T₁ is the spin-lattice relaxation time,

T₂ is the spin-spin relaxation time and

T_2eff is the effective spin-spin relaxation time of the spins to be determined in the specimen.

At least one of said gradient fields is switched between the first and/or the second pulse and/or the second and the third pulse and/or after the third pulse, wherein at least one of the RF pulses is a frequency-selective pulse and at least one echo signal stimulated by the third pulse is detected and evaluated.

Claims

1. A method for locally resolved investigation of a specimen, in which the specimen is exposed to a constant magnetic field and a variable combinatio of three gradient magnetic fields directed substantially perpendicularly to each other and the specimen is subjected to a sequence of high-frequency pulses which sequence contains three successive pulses with flip angles differeing from 180 degrees and multiples thereof, and in which signals corresponding to a magnetic resonance of spin moments, in particular of nuclear spin moments, are measured, characterized in that

the interval (tau) between the first and the second of said three pulses is greater than T_2eff and smaller than 5T₂, and that the interval (T-tau) between the second and the third pulses is greater than T_2eff and smaller than 5T₁, wherein

T₁ is the spin-lattice relaxation time,

T₂ is the spin-spin relaxation time, and

T_2eff is the effective spin-spin relaxation time of the spinds to be determined in the specimen,

that at least one of the gradient fields is switched over during at least one of the following periods of time:

(a) between the first and the second pulses,

(b) between the second and the third pulses,

(c) after the third pulse,

that at least one of the pulses is a frequency-selective pulse and that at least one echo signal stimulated by the third pulse is detected and evaluated.

2. Method according to claim 1, characterized in that tau is smaller than 2T₂.

3. Method according to claim 1, characterized in that (T-tau) is smaller than 3T₂ .

4. Method according to claim 1, characterized in that the frequency-selective pulse is replaced by a sequence of separate single pulses which gives the necessary frequency selectivity.

5. Method according to claim 4, characterized in that at least two of the single pulses contain different carrier frequencies.

6. Method according to claim 4, characterized in that the single pulses contain the same carrier frequencies.

7. Method according to claim 6, characterized in that the single pulses are non-selective ("hard") pulses, i.e. a substantially rectangular envelope curve, have as short as possible a duration and as high as possible an amplitude and in themselves are not selective.

8. Method according to claim 1, characterized in that the at least one frequency-selective pulse is a frequency-modulated pulse.

9. Method according to claim 1, characterized in that the first pulse is a |90 degree| pulse (±

10%).

10. Method according to claim 1, characterized in that the second pulse is a |90 degree| pulse (±

50%).

11. Method according to claim 1, characterized in that the third pulse is a |90 degree| pulse (±

50%).

12. Method according to claim 1, characterized in that at least the first and the second pulse are substantially 90 degree pulses.

13. Method according to claim 1, characterized in that the third pulse is a pulse corresponding to a fraction of said flip angle, that the third pulse is followed by at least one further "fraction pulse" at a distance which is greater than the distance betweenthe first and second pulses, and that each stimulated echo following one of the further pulses is detected and evaluated.

14. Method according to claim 13, characterized in that the flip angle of each fraction pulse is less than 15 degrees.

15. Method according to claim 13, characterized in that the spacing of each fraction pulse from the preceding pulse is greater than 2 tau.

16. Method according to claim 13, characterized in that the flip angle of each further pulse is greater than the flip angle of each preceding pulse.

17. Method according to claim 1, characterized in that the first pulse is a slice pulse.

18. Method according to claim 1, characterized in that the second pulse is a slice pulse.

19. Method according to claim 1, characterized in that the second pulse is a slice pulse.

20. Method according to claim 17, characterized in that the remaining pulses of the three pulses are non-selective pulses.

21. Method according to claim 18, characterized in that the remaining pulses of the three pulses are non-selective pulses.

22. Method according to claim 19, characterized in that the remaining pulses of the three pulses are non-selective pulses.

23. Method according to claim 1, characterized in that one of the pulses is a slice pulse and another of the pulses is a fragment (zoom pulse).

24. Method according to claim 1, characterized in that at least one of the pulses is a resonance-line-selective pulse.

25. Method according to claim 1, characterized in that the first pulse is a resonance-line-selective pulse.

26. Method according to claim 1, characterized in that the first pulse is a slice pulse.

27. Method according to claim 1, characterized in that the first pulse is a fragment or zoom pulse.

28. Method according to claim 23, characterized in that the second pulse is a non-selective (hard) pulse.

29. Method according to claim 24, characterized in that the second pulse is a non-selective (hard) pulse.

30. Method according to claim 25, characterized in that the second pulse is a non-selective (hard) pulse.

31. Method according to claim 23, characterized in that the second pulse is a slice pulse.

32. Method according to claim 24, characterized in that the second pulse is a slice pulse.

33. Method according to claim 25, characterized in that the second pulse is a slice pulse.

34. Method according to claim 1, characterized in that the generation, observation and evaluation of stimulated echo signals is combined with other methods, in particular spinecho tomography methods, by adding 180 degrees pulses.

36. The method of claim 1, wherein at least one gradient field is switched over between said first and second pulses and between said second and third pulses.

37. The method of claim 1, wherein at least one graident field is switched over between said first and second pulses and after said third pulse.

38. The method of claim 1, wherein at least one gradient field is switched over between said second and third pulses and after said third pulse.

39. The method of claim 1, wherein at least one gradient field is switched over between said first and second pulses, and between said second and third pulses, and after said third pulse.

35. An apparatus for locally resolved investigation of a specimen, said apparatus comprising

means for exposing a specimen to a constant magnetic field and a variable combination of three gradient magnetic fields directed substantially perpendicularly to each other and to a sequence of high-frequency (RF) pulses which contains three successive pulses with flip angles differing from 180 degrees and multiples thereof, and

means (24,30,14) for detecting signals corresponding to a magnetic resonance of spin moments, in particular of nuclear spin moments in said specimen,

characterized in that

said exposing means (14,16,18,20,22,24,30) produces said sequence so that the interval (tau) between the first and the second of said three pulses is greater than T_2eff and smaller than 5T₂, and that the interval (T-tau) between the second and the third pulses is greater than T_2eff and smaller than 5T₁, wherein

T₁ is the spin-lattice relaxation time,

T₂ is the spin-spin relaxation time, and

T_2eff is the effective spin-spin relaxation time of the spins to be determined in the specimen,

said exposing means further effecting switching of at least one of said gradient fields during at least one of the following periods of time:

(a) between the first and the second pulses,

(b) between the second and the third pulses,

(c) after the third pulse,

wherein at least one of the RF pulses is a frequency-selective pulse and wherein said detecting means detects at least one echo signal, stimulated by the third pulse, for evaluation.