Coincident multiple compton scatter nuclear medical imager

• US 6,484,051 B1
• Filed: 05/15/2001
• Issued: 11/19/2002
• Est. Priority Date: 05/15/2001
• Status: Expired due to Fees

• Current Assignee: James Daniel
• Original Assignee: James Daniel
• Inventors: Daniel, James
• Primary Examiner(s): Manuel, George
• Assistant Examiner(s): Shah, Devaang
• Application Number:
  US09/854,467
• Time in Patent Office: 553 Days
• Field of Search: 600/436, 250/363.03, 250/370.08, 250/370.09
• US Class Current: 600/436
• CPC Class Codes: A61B 6/037 Emission tomography
• CPC Class Codes: A61B 6/4258 for detecting non x-ray radiation, e.g. gamma radiation A61B6/037 takes precedence
• CPC Class Codes: A61B 6/508 for non-human patients
• CPC Class Codes: G01N 23/20 by using diffraction of the radiation by the materials, e.g. for investigating crystal structure; by using scattering of the radiation by the materials, e.g. for investigating non-crystalline materials; by using reflection of the radiation by the materials

Abstract

A Compton imager and method are provided for generating three-dimensional images. The Compton imager detects Compton scattering of simultaneously or nearly simultaneously emitted gamma rays produced by a radio-nuclide. A possible location of each radio-nuclide decay is defined by the intersection of Compton direction cones corresponding to the detected gamma rays. Three-dimensional images are generated by superposition of individual locations of separate radioactive decay locations.

Claims

1. An imaging device for generating three-dimensional images from a radio-nuclide emitting first, second and third initial gamma rays as simultaneous or nearly simultaneous emissions resulting from a single nuclear decay event, said imaging device comprising:

a position-sensitive gamma ray detector comprising at least one position sensitive layer, said detector being adapted to determine the locations of interaction sites at which gamma rays undergo one of Compton scatter and photoelectric interactions; and

a processor for determining a radio-nuclide location as a function of (i) at least two energy values corresponding to each of the first, second and third initial gamma rays,, (ii) detected locations of first interaction sites of the first, second and third initial gamma rays, respectively, and (iii) detected locations of second interactions sites of Compton scattered gamma rays corresponding to the first, second, and third initial gamma rays, respectively,

the at least two energy values being selected from the group consisting of the energy of a respective initial gamma ray, a first deposition energy of the respective initial gamma ray at the respective first interaction site, energy of said first Compton scattered gamma ray of a respective first initial gamma ray, and a second deposition energy of the corresponding Compton scattered gamma ray at the respective second interaction site, and said processor generating a three-dimensional image by superposition of individual radio-nuclide locations.

2. The device of claim 1, wherein said detector comprises a plurality of position-sensitive silicon detector layers.

3. The device of claim 1, wherein said processor determines a positron-emitting radio-nuclide location as an intersection of a Compton direction cone corresponding to the first initial gamma ray with a line joining a second initial gamma ray first interaction site and a third initial gamma ray first interaction site, said line joining first interaction sites of two 511 keV gamma rays produced in positron-electron annihilation.

4. The device of claim 1, wherein said processor determines the radio-nuclide location as a function of the location of each first interaction site, each second interaction site, and at least two energy values corresponding to each of the three initial gamma rays, said at least two energy values are selected from the group consisting of an initial gamma ray energy of the respective initial gamma rays, a first deposition energy of the respective gamma ray at the respective first interaction site, the energy of the first Compton scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the respective Compton scattered gamma ray at the respective second interaction site.

5. The device of claim 4, wherein said processor determines radio-nuclide location from a common point of intersection of three Compton direction cones, each Compton direction cone corresponding to one of the three initial gamma rays emitted as a function of a respective scattering angle, the location of the respective first interaction site and the location of the respective second interaction site.

6. A system for generating three-dimensional images, said system comprising:

a radio-nuclide emitting first, second and third initial gamma rays as simultaneous or nearly simultaneous emissions resulting from a single nuclear decay event;

a position-sensitive gamma ray detector adapted to determine the locations of multiple interaction sites at which gamma rays undergo one of Compton scatter and photoelectric interactions; and

a processor for determining a radio-nuclide location as a function of (i) at least two energy values corresponding to each of the first, second and third initial gamma rays, (ii) detected locations of first interaction sites of the first, second and third initial gamma rays, respectively, and (iii) detected locations of second interactions sites of Compton scattered gamma rays corresponding to the first, second, and third initial gamma rays, respectively,

the at least two energy values being selected from the group consisting of the energy of a respective initial gamma ray, a first deposition energy of the respective initial gamma ray at the respective first interaction site, the energy of the first Compton scattered gamma ray of the respective initial gamma ray, and a second deposition energy of the corresponding Compton scattered gamma ray at the respective second interaction site, said processor generating a three-dimensional image by superposition of individual radio-nuclide locations.

7. The method of claim 6, wherein said position-sensitive detector comprises a plurality of position-sensitive silicon detector layers.

8. The system of claim 6, wherein said radio-nuclide generates three coincident gamma rays during nuclear decay.

9. The system of claim 6, wherein said radio-nuclide generates a positron and said first initial gamma ray during nuclear decay, said positron annihilating with an electron generating said second and said third initial gamma rays.

10. The system of claim 9, wherein said processor determines the location of the radio-nuclide as an intersection of a Compton direction cone corresponding to the first initial gamma ray with a line joining the second initial gamma ray first interaction site and the third initial gamma ray first interaction site.

11. The system of claim 6, wherein said processor determines the location of the radio-nuclide as a function of the location of each first interaction site, each second interaction site, and at least two energy values corresponding to each of the three initial gamma rays, said at least two energy values are selected from the group consisting of the energy of the respective initial gamma ray, a first deposition energy of the respective gamma ray at the respective first interaction site, the energy of the first Compton scattered gamma ray of the respective initial gamma ray, and a second deposition energy of the respective Compton scattered gamma ray at the respective second interaction site.

12. The system of claim 11, wherein said processor determines the location of the radio-nuclide from a common point of intersection of three Compton direction cones, each Compton direction cone corresponding to one of the three initial gamma rays emitted as a function of a respective scattering angle, the location of the respective first interaction site and the location of the respective second interaction site.

13. An imaging device for generating three-dimensional images by detecting initial gamma rays emitted as simultaneous or nearly simultaneous emissions resulting from a single nuclear decay event of a radio-nuclide and three subsequent Compton scattered gamma rays resulting from Compton scattering of the respective initial gamma rays, said imaging device comprising:

a first position-sensitive detector for providing a Compton scattering medium for the initial gamma rays to interact at a respective first interaction site in said first position-sensitive detector and to thereby generate Compton scattered gamma rays, and for detecting a respective location of each first interaction site;

a second position-sensitive detector, surrounding said first position-sensitive detector, for detecting a respective location of a respective second interaction site in said second position-sensitive detector at which the Compton scattered gamma rays interact, said second position-sensitive detector permitting at least a portion of the energy associated with the scattered gamma rays to exit from said second position-sensitive detector; and

a processor for determining location of the radio-nuclide as a function of (i) at least two energy values corresponding to each of a first, second and third of the respective initial gamma rays, (ii) the respective locations of each detected first interaction sites, and (iii) the location of the second interaction site where the Compton scattered gamma rays corresponding to the respective initial gamma ray interacts with the second position-sensitive detector, said at least two energy values being selected from the group consisting of an initial gamma ray energy of the first initial gamma ray, a first deposition energy of the respective initial gamma ray at the respective first interaction site, the energy of the first Compton scattered gamma ray of the respective initial gamma ray, and a second deposition energy of a corresponding Compton scattered gamma ray of the first initial gamma ray, at the respective second interaction site, said processor for generating a three-dimensional image by superposition of individual locations of separate radioactive decay positions.

14. The imaging device of claim 13, wherein said first position-sensitive detector is further for detecting energy depositions at respective first interaction sites.

15. The imaging device of claim 13, wherein said second position-sensitive detector is further for detecting energy depositions at respective second interaction sites.

16. The imaging device of claim 13, wherein said first position-sensitive detector is disposed on said second position-sensitive detector to form a multi-layered array.

17. The imaging device of claim 13, wherein said first position-sensitive detector and said second array position-sensitive detection are disposed such that a large solid angle, e.g., greater than three π

steradians, is subtended by each said detector relative to a region-of-interest.

18. The imaging device of claim 13, wherein the single nuclear decay event results in three initial gamma rays and said processor determines the location of the radio-nuclide as a function of the (i) locations of each first interaction site, (ii) each second interaction site, and (iii) at least two energy values corresponding to three initial gamma rays, said at least two energy values are selected from the group consisting of the energy of the respective initial gamma rays, a first deposition energy of the respective gamma ray at the respective first interaction site, the energy of the first Compton scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the respective Compton scattered gamma ray at the respective second interaction site.

19. The imaging device of claim 18, wherein said processor is further for computing a respective scattering angle of the three initial gamma rays at the respective first interaction sites.

20. The imaging device of claim 19, wherein said processor determines the location of the radio-nuclide from a common point of intersection of three Compton direction cones, each cone corresponding to one of the three initial gamma rays emitted as a function of the respective scattering angle, the location of the respective first interaction site and the location of the respective second interaction site.

21. The imaging device of claim 13, wherein said processor determines the location of the radio-nuclide as a common point of an intersection of two Compton direction cones and a thin region-of-interest containing a radioactive substance that emits two coincident gamma rays, the Compton direction cones corresponding to the two coincident gamma rays, respectively, as a function of a respective scattering angle, the location of a respective first interaction site and the location of a respective second interaction site.

22. The imaging device of claim 13, wherein said processor determines the location of a positron-emitting radio-nuclide as an intersection of a Compton direction cone corresponding to the first initial gamma ray with a line joining the first interaction sites corresponding to a second initial gamma ray and a third initial gamma ray of the three initial gamma rays, said second and third initial gamma rays having energies of 511 keV.

23. The imaging device of claim 13, wherein said first position-sensitive detector array provides a three-dimensional position resolution at least one mm and an energy detection resolution of at least 2 keV.

24. The imaging device of claim 13, wherein said second position-sensitive detector provides position resolution of at least one mm.

25. The imaging device of claim 13, wherein said second position-sensitive detector comprises a high-Z detector, said high-Z detector selected to optimize the probability for a photoelectric effect interaction.

26. The imaging device of claim 13, wherein said first position-sensitive detector comprises silicon detectors.

27. The imaging device of claim 13, wherein said second position-sensitive detector comprises one of germanium and/or CdZnTe and/or CdTe and/or GaAs detectors.

28. The imaging device of claim 13, wherein said first position-sensitive detector is further for measuring an energy loss of the gamma rays at a respective first interaction site.

29. The imaging device of claim 13, wherein said second position-sensitive detector is further for measuring an energy loss of the Compton scattered gamma rays at a respective second interaction site.

30. The imaging device of claim 13, further comprising at least a third position-sensitive detector surrounding said second position-sensitive detector, said third position-sensitive detector for providing a gamma ray interaction media for the respective second Compton scattered gamma rays, thereby resulting in generating respective secondary Compton scattered gamma rays, and for detecting a respective location of a respective third interaction site along said third position-sensitive detector where the second Compton scattered gamma rays interact.

31. A method for generating three-dimensional images, said method comprising the steps of:

providing a radio-nuclide source generating three initial gamma rays as simultaneous or nearly simultaneous emissions resulting from a single nuclear decay event;

using a position-sensitive detector to detect locations of three first interaction sites at which the three initial gamma rays respectively interact with the position-sensitive detector;

generating three Compton scattered gamma rays from the three initial gamma rays, respectively, as a result of the three initial gamma rays interacting with the position-sensitive detector;

using the position-sensitive detector to detect locations of three second interaction sites where the three Compton scattered gamma rays interact with the position-sensitive detector, respectively;

determining the location of the radio-nuclide as a function of (i) at least two energy values corresponding to each of the three initial gamma rays, (ii) the location of each detected first interaction site, and (iii) the location of each detected second interaction site, the at least two energy values are selected from the group consisting of the respective energy of the respective initial gamma rays, a first deposition energy of the initial gamma rays at the respective first interaction sites, the energy of the first Compton scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the Compton scattered gamma rays at the respective second interaction sites; and

producing a three-dimensional image by superposition of individual locations of separate radioactive decay positions.

32. The method of claim 31, further comprising the step of measuring energy depositions at each first interaction sites from each of the three initial gamma rays, respectively.

33. The method of claim 31, further comprising the step of measuring energy depositions of each Compton-scattered gamma ray at each respective second interaction sites.

34. The method of claim 31, wherein said determining the location of the radio-nuclide step comprises determining scattering angles for the three initial gamma rays at the respective first interaction sites thereby providing for defining three Compton direction cones, one for each initial gamma ray, an intersection of the three Compton direction cones with each other defining the location of the radio-nuclide.

35. The method of claim 31, further comprising generating images of dynamic phenomena through time sequential acquisition of the three-dimensional images.

36. A method for generating three-dimensional images, said method comprising the steps of:

providing a radio-nuclide source generating nuclear decay as a positron and a first coincident gamma ray, the positron annihilating with an electron to thereby generate a second gamma ray and a third gamma ray;

using a position-sensitive detector to detect locations of first, second, and third gamma ray first interaction sites where the first, second and third gamma rays interact with the position-sensitive detector, respectively;

generating a first Compton scattered gamma ray from the first gamma ray, as a result of the first gamma ray interacting with the first position-sensitive detector;

using the position-sensitive detector to detect a location of a second interaction site where the first Compton scattered gamma ray interacts with the position-sensitive detector;

determining the location of the radio-nuclide as an intersection of a Compton direction gamma ray cone corresponding to the first gamma ray and a line connecting the second and third gamma ray first interaction sites; and

producing a three-dimensional image by superposition of individual locations of separate radioactive decay positions.

37. The method of claim 36, wherein the Compton direction cone satisfies a function of at least two energy values corresponding to the first gamma ray, the location of the first gamma ray first interaction, and the location of the second interaction site, the at least two energy values are selected from the group consisting of the energy of the first gamma ray, a first deposition energy of the first gamma ray at the first gamma ray first interaction site, the energy of the first Compton scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the first Compton scattered gamma ray at the second interaction site.

38. The method of claim 36, further comprising generating images of dynamic phenomena through time sequential acquisition of the three-dimensional images.

39. A method for generating three-dimensional images, said method comprising the steps of:

providing a radio-nuclide source generating nuclear decay as a first coincident gamma ray and a second coincident gamma ray;

administering the radio-nuclide source to a thin region-of-interest;

using a first position-sensitive detector to detect a location of a first gamma ray first interaction site where the first gamma ray interacts with the first position-sensitive detector and a location of a second gamma ray first interaction site where the second gamma ray interacts with the first position-sensitive detector;

generating a first Compton scattered gamma ray and a second Compton scattered gamma ray from the first gamma ray and second gamma ray, respectively, as a result of the first gamma ray and second gamma ray interacting with the first position-sensitive detector, respectively;

using a second position-sensitive detector to detect a first gamma ray second interaction site at which the first Compton scattered gamma ray interacts with the second position-sensitive detector and a second gamma ray second interaction site at which the second Compton scattered gamma ray interacts with the second position-sensitive detector;

determining the location of the radio-nuclide as an intersection of a first Compton direction cone corresponding to the first gamma ray, a second Compton direction cone corresponding to the second gamma ray, and the thin region-of-interest; and

producing a three-dimensional image by superposition of individual locations of separate radioactive decay positions.

40. The method of claim 39, wherein each Compton direction cones satisfies a function of at least two energy values corresponding to a respective gamma ray, the location of the respective first interaction site, and the location of the respective second interaction site, the at least two energy values are selected from the group consisting of the energy of the respective initial gamma ray, a first deposition energy of the respective gamma ray at the respective first interaction site, the energy of the first Compton scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the respective Compton scattered gamma ray at the respective second interaction site.

41. The method of claim 39, further comprising generating images of dynamic phenomena through time sequential acquisition of the three-dimensional images.

42. A system for generating three-dimensional images, said system comprising:

a radio-nuclide emitting a first, second and third initial gamma ray as simultaneous or nearly simultaneous emission resulting from a single nuclear decay event;

a first position-sensitive detector for providing a Compton scattering medium for the first, second and third initial gamma rays to interact, to thereby produce first, second, and third Compton scattered gamma rays, respectively, and for detecting a respective location of each of the first, second and third initial gamma rays at a first, second, and third initial gamma ray first interaction site, respectively, in said first position-sensitive detector;

a second position-sensitive detector surrounding said first position-sensitive for detecting locations of the first, second and third Compton scattered gamma rays at a first, second and third Compton gamma ray second interaction site, respectively, in said second position-sensitive detector, said second position-sensitive detector permitting at least a portion of the energy associated with the scattered gamma rays to exit from said second position-sensitive detector; and

a processor for determining a location of the radio-nuclide as a function of (i) at least two energy values corresponding to each of the three initial gamma rays, (ii) the locations of each detected first interaction sites, and (iii) the locations of the first Compton-scattered gamma ray second interaction sites, said at least two energy values are selected from the group consisting of the energy of the first respective gamma ray, a first deposition energy of the respective initial gamma ray at the respective first interaction site, the energy of the respective Compton scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the respective Compton scattered gamma ray at the respective second interaction site, said processor for generating a three-dimensional image by superposition of individual locations of separate radioactive decay positions.

43. The system of claim 42, wherein said radio-nuclide generates three coincident gamma rays during nuclear decay.

44. The system of claim 42, wherein said radio-nuclide generates a positron and said first initial gamma ray during nuclear decay, said positron annihilating with an electron generating said second and said third initial gamma rays.

45. The system of claim 44, wherein said processor determines the location of a positron-emitting radio-nuclide as an intersection of a Compton direction cone corresponding to the first initial gamma ray with a line joining the second initial gamma ray first interaction site and the third initial gamma ray first interaction site.

46. The system of claim 42, wherein said processor determines the location of the radio nuclide as a function of the location of each first interaction site, each second interaction site, and at least two energy values corresponding to each of the three initial gamma rays, said at least two energy values are selected from the group consisting of the energy of the respective initial gamma ray, a first deposition energy of the respective gamma ray at the respective first interaction site, the energy of the first Compton scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the respective Compton scattered gamma ray at the respective second interaction site.

47. The system of claim 46, wherein said processor determines the location of the radio-nuclide from a common point of intersection of three Compton direction cones, each Compton direction cone corresponding to one of the three initial gamma rays emitted as a function of a respective scattering angle, the location of the respective first interaction site and the location of the respective second interaction site.

48. The system of claim 42, further comprising at least a third position-sensitive detector surrounding said second position-sensitive detector, said third position-sensitive detector for providing a gamma ray interaction media for the Compton scattered gamma rays, thereby generating secondary Compton scattered gamma rays, respectively, and for detecting locations of the secondary Compton scattered gamma rays at a respective third interaction site in said third position-sensitive detector.

49. The system of claim 42, wherein respective energy losses L₁ and L₂ at the respective first and second interaction sites of each respective initial gamma ray and scattering angles at said respective second interaction sites are used to determine energies and direction cones of said respective initial gamma rays.

50. A method for generating three-dimensional images, said method comprising the steps of:

providing a radio-nuclide source generating three initial gamma rays as simultaneous or nearly simultaneous emissions resulting from a single nuclear decay event;

detecting locations of three first interaction sites at which the three initial gamma rays, respectively, interact with a single position-sensitive detector;

generating three Compton scattered gamma rays from the three initial gamma rays, respectively, as a result of the three initial gamma rays interacting with the position-sensitive detector;

detecting locations of three second interaction sites where the three Compton scattered gamma rays respectively interact with the positron-sensitive detector;

determining the location of the radio-nuclide as a function of (i) at least two energy values corresponding to each of the three initial gamma rays, (ii) the location of each detected first interaction site, and (iii) the location of each detected second interaction site, the at least two energy values are selected from the group consisting of the energy of the respective initial gamma rays, a first deposition energy of the initial gamma rays at the respective first interaction sites, the energy of the first Compton scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the Compton scattered gamma rays at the respective second interaction sites; and

producing a three-dimensional image by the superposition of individual locations of separate radioactive decay positions.

51. The method of claim 50, further comprising the step of measuring energy depositions at each first interaction site from each of the three initial gamma rays, respectively.

52. The method of claim 50, further comprising the step of measuring energy depositions of each respective Compton-scattered gamma ray at each respective second interaction site.

53. The method of claim 50 wherein said determining the location of the radio-nuclide step comprises determining scattering angles for the three initial gamma rays at the respective first interaction sites thereby providing for defining three Compton direction cones, one for each initial gamma ray, an intersection of the three Compton direction cones with each other defining the location of the radio-nuclide.

54. The method of claim 50, further comprising generating images of dynamic phenomena through time sequential acquisition of the three-dimensional images.

55. The method of claim 50, wherein the position-sensitive detector comprises a plurality of position-sensitive silicon detector layers.

56. A method for generating three-dimensional images, said method comprising the steps of:

providing a radio-nuclide source generating nuclear decay as a positron and a first coincident gamma ray, the positron annihilating with an electron to thereby generate a second gamma ray and a third gamma ray;

detecting locations of a first, second, and third gamma ray first interaction sites where the first, second and third gamma rays interact with a single position-sensitive detector, respectively;

generating a first Compton scattered gamma ray from the first gamma ray, as a result of the first gamma ray interacting with the position-sensitive detector;

detecting a location of a second interaction site where the first Compton scattered gamma ray interacts with the position-sensitive detector;

determining the location of the radio-nuclide as an intersection of a Compton direction gamma ray cone corresponding to the first gamma ray and a line connecting the second and third gamma ray first interaction sites, said second and third initial gamma rays having energies of 511 keV; and

producing a three-dimensional image by superposition of individual locations of separate radioactive decay positions.

57. The method of claim 56, further comprising the step of measuring energy depositions at each first interaction sites from each of the three initial gamma rays, respectively.

58. The method of claim 56, wherein the Compton direction cone satisfies a function of at least two energy values corresponding to the first gamma ray, the location of the first gamma ray first interaction, and the location of the second interaction site, the at least two energy values are selected from the group consisting of the energy of the first gamma ray, the deposition energy of the first gamma ray at the first gamma ray first interaction site, the energy of the first Compton-scattered gamma ray of the respective first initial gamma ray, and a second deposition energy of the first Compton scattered gamma ray at the second interaction site.

59. The method of claim 56, further comprising generating images of dynamic phenomena through time sequential acquisition of the three-dimensional images.