Method for reducing image artifacts due to periodic signal variations in NMR imaging

• US 4,663,591 A
• Filed: 08/16/1985
• Issued: 05/05/1987
• Est. Priority Date: 08/16/1985
• 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): Tokar, Michael J.
• Application Number:
  US06/766,733
• Time in Patent Office: 627 Days
• Field of Search: 324/300, 324/307, 324/309, 324/308, 324/312, 324/313, 324/318, 324/322, 128/653
• US Class Current: 324/309
• CPC Class Codes: G01R 33/56509 due to motion, displacement or flow, e.g. gradient moment nulling G01R33/567 takes precedence

Abstract

A method for reducing image artifacts due to signal variations in the course of examining a subject using nuclear magnetic resonance (NMR) techniques includes the acquisition of scan data for imaging the object. The scan data is composed of a number of views. The acquisition of each view includes the implementation of a pulse sequence to generate an NMR signal and application of a magnetic gradient along at least one dimensional axis of the object. The magnetic field gradient is characterized by a parameter (e.g., amplitude or direction) adjustable from view to view to encode spatial information into the NMR signal. The parameter value is selected just prior to implementation of the pulse sequence for that view and depends on the phase of the signal variation at that point in time. The final view order depends on the measured phase during the scan. In this manner, the view order can be continuously adjusted to obtain optimum artifact reduction. The method is applicable to various NMR imaging techniques, including Fourier transform and multiple angle projection reconstruction.

Claims

1. A method for reducing artifacts in a desired image due to substantially periodic signal variations while a portion of an object is being examined using nuclear magnetic resonance techniques, which techniques include measurement of imaging data about the object portion through the implementation of a plurality of views, each made up of at least one pulse sequence which includes irradiation of the object portion by an RF excitation pulse at the Larmor frequency to produce an NMR signal, application of a pulsed magnetic field gradient along at least one dimensional axis of the object, and acquisition of imaging data, said magnetic field gradient having a parameter value adjustable to have a different value in each view so as to encode spatial information into the NMR signal, said method comprising:

(a) Selecting a predetermined relationship between the signal variations and the parameter value of said magnetic field gradient, wherein selection of said relationship defines a correspondence between a desired parameter value to be implemented in a given pulse sequence and the phase of said signal variations;

(b) measuring the phase of said signal variations in the course of implementing said plurality of views; and

(c) selecting a non-monotonic temporal order of application of said magnetic field gradient so as to approximate said predetermined relationship, wherein said order is based on said phase measurements, thereby to reduce artifacts in said desired image.

2. The method of claim 1 wherein said signal variations are due to motion of the object being studied.

3. The method of claim 1 wherein said pulsed magnetic field gradient comprises a phase-encoding magnetic field gradient and wherein the adjustable parameter value comprises the time integral of the gradient pulse waveform.

4. The method of claim 3 wherein said time integral is controlled by the amplitude of said phase-encoding magnetic field gradient.

5. The method of claim 1 wherein said magnetic field gradient comprises a read-out magnetic field gradient and wherein the adjustable parameter value comprises the direction of said read-out gradient.

6. The method of claim 1 wherein the temporal order of said gradient parameter value applied in the course of implementing said plurality of views is selected such that said signal variations as a function of monotonically increasing gradient parameter value, averaged within each view, for views having more than one pulse sequence, are of a lower frequency than the actual frequency of the periodic signal variation, thereby to decrease displacement of the artifacts from the desired image.

7. The method of claim 6 wherein the temporal order of said gradient parameter applied in the course of implementing said plurality of views is selected such that when the measurements acquired in each pulse sequence are rearranged in order of monotonically increasing parameter value the signal variations, averaged within each view, for views with more than one pulse sequence, will appear to go through no more than one cycle.

8. The method of claim 1 wherein the temporal order of said gradient parameter applied in the course of implementing said plurality of views is selected such that said signal variations as a function of monotonically increasing gradient parameter value, averaged within each view, for views having more than one pulse sequence, are of a higher frequency than the actual frequency of the periodic signal variation, thereby to increase displacement of the artifacts from the desired image.

9. The method of claim 8 wherein the temporal order of said gradient parameter applied in the course of implementing said plurality of views is selected such that when the measurements acquired in each pulse sequence are rearranged in order of monotonically increasing parameter value the signal variations, averaged within each view, for views having more than one pulse sequence, will appear to go through N_v /2 cycles, where N_v is equal to the number of views comprising said plurality of views.

10. The method of claim 1 wherein, prior to the implementation of each pulse sequence, the phase of said signal variations is measured and a parameter value to be used is selected, wherein said selected parameter value depends on said phase measurement.

11. The method of claims 1, 3, 5, 8 or 10 wherein said step of selecting said predetermined relationship includes tabulating for a finite set of values of phase of said signal variations an entry containing the desired value of said gradient parameter and selecting the number of measurements to be made with each tabulated entry;

and wherein said step of selecting a temporal order comprises selecting from said tabulation the entry having a phase of signal variation closest to the phase of signal variation at the time the pulse sequence is implemented and wherein each entry in said tabulation is deleted after the requisite number of measurements with that entry have been made.

12. A method for reducing artifacts in a desired image due to substantially periodic signal variations while a portion of an object is being examined using nuclear magnetic resonance techniques, which techniques include measurement of imaging data about the object portion through the implementation of a plurality of views, each made up of at lease one pulse sequence which includes irradiation of the object portion by an RF excitation pulse at the Larmor frequency to produce an NMR signal, application of a pulsed magnetic field gradient along at least one dimensional axis of the object, and acquisition of imaging data, said magnetic field gradient having a parameter value adjustable to have a different value in each view so as to encode spatial information into the NMR signal, said method comprising:

(a) Selecting a predetermined relationship between the signal variations and the parameter value of said magnetic field gradient, wherein selection of said relationship defines a correspondence between a desired parameter value to be implemented in a given pulse sequence and the phase of said signal variations, and wherein said relationship is such that when the measurements of imaging data acquired in each pulse sequence are rearranged in order of monotonically increasing parameter value, the signal variations, averaged within each view, for views having more than one pulse sequence as a function of monotonically increasing gradient parameter are at a lower frequency than the actual frequency of the signal variations;

(b) measuring the phase of said signal variations in the course of implementing said plurality of views; and

(c) selecting a non-monotonic temporal order of application of said magnetic field gradient so as to approximate said predetermined relationship, wherein said order is based on said phase measurements, thereby to reduce artifacts in said desired image.

13. The method of claim 12 wherein said signal variations are due to motion of the object being studied.

14. The method of claim 12 wherein said pulsed magnetic field gradient comprises a phase-encoding magnetic field gradient and wherein the adjustable parameter value comprises the time integral of the gradient pulse waveform.

15. The method of claim 14 wherein said time integral is controlled by the amplitude of said phase-encoding magnetic field gradient.

16. The method of claim 12 wherein said magnetic field gradient comprises a read-out magnetic field gradient and wherein the adjustable parameter value comprises the direction of said read-out gradient.

17. The method of claim 12 wherein the temporal order of said gradient parameter applied in the course of implementing said plurality of views is selected such that when the measurements acquired in each pulse sequence are rearranged in order of monotonically increasing parameter value the signal variations, averaged within each view for views having more than one pulse sequence, will appear to go through no more than one cycle.

18. The method of claim 12 wherein, prior to the implementation of each pulse sequence, the phase of said signal variations is measured and a parameter value to be used is selected, wherein said selected parameter value depends on said phase measurement.

19. The method of claims 12, 14, 16 or 18 wherein said step of selecting said predetermined relationship includes tabulating for a finite set of values of phase of said signal variations an entry containing the desired value of said gradient parameter and selecting the number of measurements to be made with each tabulated entry;

and wherein said step of selecting a temporal order comprises selecting from said tabulation the entry having a phase of signal variation closest to the phase of signal variation at the time the pulse sequence is implemented and wherein each entry in said tabulation is deleted after the requisite number of measurements with that entry have been made.

20. A method for reducing artifacts in a desired image due to substantially periodic signal variations while a portion of an object is being examined using nuclear magnetic resonance techniques, which techniques include measurement of imaging data about the object portion through the implementation of a plurality of views, each made up of at least one pulse sequence which includes irradiation of the object portion by an RF excitation pulse at the Larmor frequency to produce an NMR signal, application of a pulsed magnetic field gradient along at least one dimensional axis of the object, and acquisition of imaging data, said magnetic field gradient having a parameter value adjustable to have a different value in each view so as to encode spatial information into the NMR signal, said method comprising:

(a) Selecting a predetermined relationship between the signal variations and the parameter value of said magnetic field gradient, wherein selection of said relationship defines a correspondence between a desired parameter value to be implemented in a given pulse sequence and the phase of said signal variations, and wherein said relationship is such that when the measurements of imaging data acquired in each pulse sequence are rearranged in order of monotonically increasing parameter value, the signal variations, averaged within each view, for views with more than one pulse sequence, as a function of gradient parameter are at a higher frequency than the actual frequency of the signal variations;

(b) measuring the phase of said signal variations in the course of implementing said plurality of views; and

(c) selecting a non-monotonic temporal order of application of said magnetic field gradient so as to approximate said predetermined relationship, wherein said order is based on said phase measurements, thereby to reduce artifacts in said desired image.

21. The method of claim 20 wherein said signal variations are due to motion of the object being studied.

22. The method of claim 20 wherein said pulsed magnetic field gradient comprises a phase-encoding magnetic field gradient and wherein the adjustable parameter value comprises the time integral of the gradient pulse waveform.

23. The method of claim 22 wherein said time integral is controlled by the amplitude of said phase-encoding magnetic field gradient.

24. The method of claim 20 wherein said magnetic field gradient comprises a read-out magnetic field gradient and wherein the adjustable parameter value comprises the direction of said read-out gradient.

25. The method of claim 20 wherein the temporal order of said gradient parameter applied in the course of implementing said plurality of views is selected such that when the measurements acquired in each pulse sequence are rearranged in order of monotonically incrasing parameter value the signal variations, averaged within each view, for views having more than one pulse sequence, will appear to go through N_v /2 cycles, where N_v is equal to the number of views comprising said plurality of views.

26. The method of claim 20 wherein, prior to the implementation of each pulse sequence, the phase of said signal variations is measured and a parameter value to be used is selected, wherein said selected parameter value depends on said phase measurement.

27. The method of claims 20, 22, 24 or 26 wherein said step of selecting said predetermined relationship includes tabulating for a finite set of values of phase of said signal variations an entry containing the desired value of said gradient parameter and selecting the number of measurements to be made with each tabulated entry;

and wherein said step of selecting a temporal order comprises selecting from said tabulation the entry having a phase of signal variation closest to the phase of signal variation at the time the pulse sequence is implemented and wherein each entry in said tabulation is deleted after the requisite number of measurements with that entry have been made.

32. The method of claim 25 wherein said magnetic field gradient comprises a read-out magnetic field gradient and wherein the adjustable parameter value comprises the direction of said read-out gradient.

28. A method for reducing artifacts in a desired image due to substantially periodic signal variations while a portion of an object is being examined using nuclear magnetic resonance techniques, which techniques include measurement of a set of imaging data about the object portion through the implementation of a plurality of views, each made up of at least one pulse sequence which includes irradiation of the object portion by an RF excitation pulse at the Larmor frequency to produce an NMR signal, application of a pulsed magnetic field gradient along at least one dimensional axis of the object, and acquisition of imaging data, said magnetic field gradient having a parameter value adjustable to have a different value in each view so as to encode spatial information into the NMR signal, said method comprising:

(a) Selecting a predetermined relationship between the signal variations and the parameter value of said magnetic field gradient, wherein selection of said relationship defines a correspondence between a desired parameter value to be implemented in a given pulse sequence and the phase of said signal variations;

(b) measuring the phase of said signal variations in the course of implementing said plurality of views;

(c) selecting a non-monotonic temporal order of application of said magnetic field gradient so as to approximate said predetermined relationship, wherein said order is based on said phase measurements; and

(d) selecting a subset of the imaging data acquired as a result of implementing said pulse sequences, said subset being smaller than the full set of imaging data, wherein the pulse sequences from which imaging data measurements are included in said subset are selected so as to more closely approximate said predetermined relationship, said subset being sufficient for constructing said desired image, thereby to reduce artifacts in said desired image.

29. The method of claim 28 wherein said signal variations are due to motion of the object being studied.

30. The method of claim 28 wherein said pulsed magnetic field gradient comprises a phase-encoding magnetic field gradient and wherein the adjustable parameter value comprises the time integral of the gradient pulse waveform.

31. The method of claim 30 wherein said time integral is controlled by the amplitude of said phase-encoding magnetic field gradient.

33. The method of claim 28 wherein the temporal order of said gradient parameter value applied in the course of implementing said plurality of views is selected such that said signal variations as a function of monotonically increasing gradient parameter value, for the pulse sequences from which imaging data is included in said subset, are such that said signal variations as a function of monotonically increasing gradient parameter value, averaged within each view for views having more than one pulse sequence, are of a lower frequency than the actual frequency of said periodic signal variations.

34. The method of claim 33 wherein the temporal order of said gradient parameter applied in the course of implementing said plurality of views is selected such that said signal variations as a function of monotonically increasing gradient parameter value, for the pulse sequences from which imaging data is included in said subset, are such that said signal variations as a function of monotonically increasing gradient parameter value, averaged within each view for views having more than one pulse sequence, will appear to go through no more than one cycle.

35. The method of claim 28 wherein the temporal order of said gradient parameter applied in the course of implementing said plurality of views is selected such that said signal variations as a function of monotonically increasing gradient parameter value, for the pulse sequences from which imaging data is included in said subset, are such that said signal variations as a function of monotonically increasing gradient parameter value, averaged within each view for views having more than one pulse sequence, are of a higher frequency than the actual frequrncy of the periodic signal variations, thereby to increase displacement of the artifacts from said desired image.

36. The method of claim 35 wherein the temporal order of said gradient parameter applied in the course of implementing said plurality of views is selected such that said signal variations as a function of monotonically increasing gradient parameter value, for the pulse sequences from which imaging data is included in said subset, are such that said signal variations as a function of monotonically increasing gradient parameter value, averaged within each view for views having more than one pulse sequence, will appear to go through N_v /2 cycles, where N_v is equal to the number of views comprising said plurality of views.

37. The method of claim 28 wherein, prior to the implementation of each pulse sequence, the phase of said signal variations is measured and a parameter value to be used is selected, wherein said selected parameter value depends on said phase measurement.

38. The method of claims 28, 30, 32, 33 or 37 further comprising the step of calculating a phase error for each pulse sequence, said phase error being equal to the difference between the phase of said signal variations at the time the pulse sequence was implemented and the phase of said signal variations corresponding to the gradient parameter value used, said correspondence being defined by said predetermined relationship.

39. The method of claims 38 wherein said step of selecting said predetermined relationship includes tabulating for a finite set of discrete values of phase of said signal variations an entry containing the desired value of said gradient parameter and selecting the number of measurements to be made with each tabulated entry;

and wherein said step of selecting a temporal order comprises;

(a) Selecting, for at least one of said pulse sequences, the entry from said tabulation having a phase of signal variation closest to the phase of signal variation at the time the pulse sequence is implemented and wherein each entry in said tabulation is deleted after the requisite number of measurements with that entry have been made; and

(b) selecting, for at least one of said pulse sequences, a value of said gradient parameter such that the resulting pulse sequence will have a phase error smaller in magnitude than the phase error for a previously implemented pulse sequence with the same gradient parameter.