Magnetic resonance angiography method and apparatus employing an integration projection

• US 5,368,033 A
• Filed: 04/20/1993
• Issued: 11/29/1994
• Est. Priority Date: 04/20/1993
• Status: Expired due to Fees

• Current Assignee: North American Philips Corp. (Koninklijke Philips N.V.)
• Original Assignee: North American Philips Corp. (Koninklijke Philips N.V.)
• Inventors: Moshfeghi, Mehran
• Primary Examiner(s): Cohen, Lee S.
• Assistant Examiner(s): Casler, Brian L.
• Application Number:
  US08/049,907
• Time in Patent Office: 588 Days
• Field of Search: 128/653.2, 128/653.4, 364/413.15-413.20, 324/306, 382/6, 382/54
• US Class Current: 600/419
• CPC Class Codes: G01R 33/563 of moving material, e.g. flow contrast angiography
• CPC Class Codes: G06T 15/08 Volume rendering

Abstract

Magnetic Resonance Angiography (MRA) method and apparatus for determining an angiogram, in the form of a two-dimensional array of pixel intensities, from time-of-flight or phase contrast MRA volumetric image data utilizes a weighted sum, pixel by pixel, of integration projection (IP) and maximum intensity projection (MIP) 2D pixel arrays formed in the same viewing direction. The forming of the integration projection pixel array is preceded by optional background suppression and optional application of a depth cueing intensity weighting function varying along the viewing direction. The background suppression procedure contains a non-linear unsharp filtering portion followed by an intensity thresholding step.

Claims

1. An angiography method for determining a two-dimensional array of pixel intensities, said method comprising:

inducing radiation to exit from voxels of a region of a body under examination, said radiation having a characteristic influenced by any flowing blood within said voxels, said flowing blood being in cardiovascular structure including blood vessels, said voxels having center to center spacings in respective three mutually orthogonal directions;

receiving and sampling the radiation exiting from the voxels of said region to form a collection of signal samples;

converting said collection of signal samples into an initial three-dimensional array of voxel intensities, each dimension of said array corresponding to a different one of said three mutually orthogonal directions;

modifying the voxel intensities of a pre-depth-cued three-dimensional array of voxel intensities derived from said initial array in accordance with a depth cueing function applied in a given direction to form a three-dimensional depth-cued array of voxel intensities;

summing the intensities of voxels intercepted by or interpolated along respective parallel rays projected in said given direction through said depth-cued array of computed voxel intensities to form respective intensity sums for the respective rays, each of said rays being associated with a different one of the pixel intensities of the two-dimensional array to be determined; and

determining the values of the respective pixel intensities of said two-dimensional array as a function of the respective sums for the rays associated with the respective pixel intensities.

2. A method as claimed in claim 1, further comprising determining respective maximum intensities of voxels intercepted by or interpolated along said respective parallel rays associated with the respective pixel intensities and directed in said given direction, as projected through a pre-MIP three-dimensional array of voxel intensities derived from said initial three-dimensional array, and wherein said determining of the values of the respective pixel intensities of said two-dimensional array is by forming a weighted combination of said respective maximum intensities and said respective sums for the rays associated with said respective pixels.

3. A method as claimed in claim 2, wherein a pre-background-suppressed three-dimensional array is derived from said initial three-dimensional array and said pre-depth-cued three-dimensional array is derived from said pre-background-suppressed array by the following operations:

comparing the intensities of the voxels of said pre-background-suppressed array with a first intensity value to segment said voxels into flow voxels and background voxels;

forming a clipped array of voxels by replacing the flow voxels of said pre-background suppressed array with a second intensity value less than the first intensity value;

applying a low-pass spatial filter to said clipped array to form a smoothed clipped array;

subtracting said smoothed clipped array from said pre-background suppressed array, voxel by voxel to form a pre-thresholded array; and

intensity thresholding said pre-thresholded array with respect to a third intensity value to form said pre-depth-cued array.

4. A method as claimed in claim 3, wherein said induced and received radiation are MR spin resonance RF signals.

5. A method as claimed in claim 2, wherein said induced and received radiation are MR spin resonance RF signals.

6. A method as claimed in claim 1, wherein a pre-background-suppressed three-dimensional array is derived from said initial three-dimensional array and said pre-depth-cued three-dimensional array is derived from said pre-background-suppressed array by the following operations:

comparing the intensities of the voxels of said pre-background-suppressed array with a first intensity value to segment said voxels into flow voxels and background voxels;

forming a clipped array of voxels by replacing the flow voxels of said pre-background suppressed array with a second intensity value less than the first intensity value;

applying a low-pass spatial filter to said clipper array to form a smoothed clipped array;

subtracting said smoothed clipped array from said pre-background suppressed array, voxel by voxel to form a pre-thresholded array; and

intensity thresholding said pre-thresholded array with respect to a third intensity value to form said pre-depth-cued array.

7. A method as claimed in claim 6, wherein said induced and received radiation are MR spin resonance RF signals.

8. A method as claimed in claim 1, wherein said induced and received radiation are MR spin resonance RF signals.

9. An angiography method for determining a two-dimensional array of pixel intensities, said method comprising:

inducing radiation to exit from voxels of a region of a body under examination, said radiation having a characteristic influenced by any flowing blood within said voxels, said flowing blood being in cardiovascular structure including blood vessels, said voxels having center to center spacings in respective three mutually orthogonal directions;

receiving and sampling the radiation exiting from the voxels of said region to form a collection of signal samples;

converting said collection of signal samples into an initial three-dimensional array of voxel intensities, each dimension of said array corresponding to a different one of said three mutually orthogonal directions;

deriving a background suppressed three dimensional array by the following procedure from a pre-background-suppressed three-dimensional array derived from said initial three-dimensional array;

a) comparing the intensities of the voxels of said pre-background-suppressed array with a first intensity value to segment said voxels into flow voxels and background voxels;

b) forming a clipped array of voxels by replacing the flow voxels of said pre-background suppressed array with a second intensity value less than the first intensity value;

c) applying a low-pass spatial filter to said clipped array to form a smoothed clipped array;

d) subtracting said smoothed clipped array from said pre-background suppressed array, voxel by voxel to form a pre-thresholded array; and

e) intensity thresholding said pre-thresholded array with respect to a third intensity value to form said background suppressed array;

summing the intensities of voxels intercepted by or interpolated along respective parallel rays projected in a given direction through a pre-projection three dimensional array derived from said background suppressed array, to form respective intensity sums for the respective rays, each of said rays being associated with a different one of the pixel interstices of the two-dimensional array to be determined; and

,

determining the values of the respective pixel intensities of said two-dimensional array as a function of the respective sums for the rays associated with the respective pixel intensities.

10. A method as claimed in claim 9, further comprising determining respective maximum intensities of voxels intercepted by or interpolated along said respective parallel rays associated with the respective pixel intensities and directed in said given direction, as projected through a pre-MIP three-dimensional array of voxel intensities derived from said initial three-dimensional array, and wherein said determining of the values of the respective pixel intensities of said two-dimensional array is by forming a weighted combination of said respective maximum intensities and said respective sums for the rays associated with said respective pixel intensities.

11. A method as claimed in claim 10, wherein said induced and received radiation are MR spin resonance RF signals.

12. A method as claimed in claim 9, wherein said induced and received radiation are MR spin resonance RF signals.

13. An angiography apparatus for determining a two-dimensional array of pixels intensities, said apparatus comprising:

means for inducing radiation to exit from voxels of a region of a body under examination, said radiation having a characteristic influenced by any flowing blood within said voxels, said flowing blood being in cardiovascular structure including blood vessels, said voxels having center to center spacings in respective three mutually orthogonal directions;

means for receiving and sampling the radiation exiting from the voxels of said region to form a collection of signal samples;

means for converting said collection of signal samples into an initial three-dimensional array of voxel intensities, each dimension of said array corresponding to a different one of said three mutually orthogonal directions; and

image processing means comprising;

a) means for modifying the voxel intensities of a pre-depth-cued three-dimensional array of voxel intensities derived from said initial array in accordance with a depth cueing function applied in a given direction to form a three-dimensional depth cued array of voxel intensities;

b) means for summing the intensities of voxels intercepted by or interpolated onto respective parallel rays projected through said depth cued array of computed voxel intensities in said given direction, to form respective intensity sums for the respective rays, each of said rays being associated with a different one of the pixel intensities of the two-dimensional array to be determined; and

c) means for determining the values of the respective pixel intensities of said two-dimensional array as a function of the respective sums for the rays associated with the respective pixel intensities.

14. An apparatus as claimed in claim 13, wherein said image rendering means further comprises:

d) means for determining respective maximum intensities of voxels intercepted by or interpolated along said respective parallel rays associated with the respective pixel intensities and directed in said given direction, as projected through a pre-MIP three-dimensional array of voxel intensities derived from said initial three-dimensional array;

and wherein said means for determining the values of the respective pixels intensities of said two-dimensional array comprises means for forming a weighted combination of said respective maximum intensities and said respective sums for the rays associated with said respective pixels intensities.

15. An apparatus as claimed in claim 14, wherein a pre-background-suppressed three-dimensional array is derived from said initial three-dimensional array and further comprising background suppression means for deriving said pre-depth-cued three-dimensional array from said pre-background-suppressed array, said background suppression means comprising means for:

comparing the intensities of the voxel of said pre-background-suppressed array with a first intensity value to segment said voxels into flow voxels and background voxels;

forming a clipped array of voxels by replacing the flow voxels of said pre-background suppressed array with a second intensity value less than the first intensity value;

applying a low-pass spatial filter to said clipped array to form a smoothed clipped array;

subtracting said smoothed clipped array from said pre-background suppressed array, voxel by voxel to form a pre-thresholded array; and

intensity thresholding said pre-thresholded array with respect to a third intensity value to form said pre-depth-cured array.

16. An apparatus as claimed in claim 15, wherein said induced and received radiation are MR spin resonance RF signals.

17. An apparatus as claimed in claim 14, wherein said induced and received radiation are MR spin resonance RF signals.

18. An apparatus as claimed in claim 13, wherein a pre-background-suppressed three-dimensional array is derived from said initial three-dimensional array and wherein said image processing means further comprises background suppression means for converting said pre-background suppressed array to said pre-depth-cued array, said background suppression means comprising means for:

comparing the intensities of the voxels of said pre-background-suppressed array with a first intensity value to segment said voxels into flow voxels and background voxels;

forming a clipped array of voxels by replacing the flow voxels of said pre-background suppressed array with a second intensity value less than the first intensity value;

applying a low-pass spatial filter to said clipped array to form a smoothed clipped array;

subtracting said smoothed clipped array from said pre-background suppressed array, voxel by voxel to form a pre-thresholded array; and

intensity thresholding said pre-thresholded array with respect to a third intensity value to form said pre-depth-cued array.

19. An apparatus as claimed in claim 18, wherein said induced and received radiation are MR spin resonance RF signals.

20. An apparatus as claimed in claim 13, wherein said induced and received radiation are MR spin resonance RF signals.