Three dimensional image reconstruction from single plane X-ray fluorograms

• US 6,473,488 B2
• Filed: 12/20/2000
• Issued: 10/29/2002
• Est. Priority Date: 12/20/2000
• Status: Expired due to Term

• Current Assignee: International Business Machines Corporation
• Original Assignee: Cedara Software, Corp (International Business Machines Corporation)
• Inventors: Menhardt, Wido
• Primary Examiner(s): BRUCE, DAVID VERNON
• Application Number:
  US09/742,050
• Publication Number:
  US 20020106052A1
• Time in Patent Office: 678 Days
• Field of Search: 378/4, 378/10, 378/62, 378/98, 378/901
• US Class Current: 378/62
• CPC Class Codes: G06T 11/006 Inverse problem, transformation from projection-space into object-space, e.g. transform methods, back-projection, algebraic methods
• CPC Class Codes: G06T 2211/436 Limited angle
• CPC Class Codes: Y10S 378/901 Computer tomography program or processor

Abstract

A method is provided to reconstruct the three-dimensional image of an X-ray contrast agent-filled object having at least one plane of symmetry using a single plane two-dimensional X-ray projection. The projection is obtained by irradiating the object with X-rays substantially perpendicular to a selected plane of symmetry of the object. The absorbance value of each pixel in the projection, which is related to the distance travelled by the X-ray within the object, is then divided by 2 to define the z coordinates on each side of the x-y plane of symmetry of the object. The z coordinates together with the x,y coordinates of each pixel define the three-dimensional contour of the object.

Claims

1. A method for the three dimensional image reconstruction of single plane 2-dimensional X-ray image projection of an object having at least one plane of symmetry comprising:

a) substantially uniformly filling the object with an X-ray contrast agent said contrast agent having a pre-selected concentration and absorption coefficient;

b) irradiating said contrast agent-filled object with X-rays substantially perpendicular to said at least one plane of symmetry of the object;

c) detecting said X-rays transmitted through said contrast agent-filled object to define a 2-dimensional projection image with pixels (x,y) having an intensity related to the absorbance of said contrast agent-filled object;

d) processing said 2-dimensional projection image to reconstruct the 3-dimensional image of said object, said processing including determining a distance D(x,y) travelled by said X-rays in the contrast agent-filled object by dividing the absorbance corresponding to the intensity of each pixel (x,y) by the concentration of the contrast agent within said object and multiplying the result thus obtained by the absorption coefficient of said contrast agent;

dividing said distance D(x,y) by 2 to define a (+z) coordinate (equals to +D(x,y)/2) and a (−

z) coordinate (equals to −

D(x,y)/2) for each pixel (x,y);

such that for each pixel (x,y) there is;

1) a (+z) coordinate=+D(x,y)/2 and

2) a (−

z) coordinate=−

D(x,y)/2;

e) using the x,y,z coordinates thus determined to reconstruct the 3 dimensional image in a 3-dimensional axis system in which the x-y plane is parallel to the plane of symmetry of said object.

3. The method of claim 1 further comprising the step of storing the reconstructed 3-dimensional image.

4. The method of claim 3 further comprising the step of displaying the image on a display screen.

5. The method of claim 4 wherein the concentration of the contrast agent is determined by integrating the absorbance over all pixels of the 2-dimensional projection image;

dividing the integrated absorbance by the absorption coefficient of the X-ray contrast agent and multiplying the result thus obtained by the volume of said object.

6. The method of claim 4 wherein the concentration of the contrast agent is determined by obtaining a first projection image perpendicular to the plane of symmetry;

measuring the maximum width of said projection;

obtaining a second projection parallel to the plane of symmetry and measuring the maximum absorbance of said projection;

dividing the absorbance by said maximum width and multiplying the result thus obtained by the absorption coefficient of the X-ray contrast agent.

7. The method of claim 5 wherein the object is an organ.

8. The method of claim 7 wherein the organ is the left ventricle of a mammalian heart.

9. The method of claim 8 wherein the mode of filling the organ with an X-ray contrast agent is selected from IV, IC, and IA.

10. The method of claim 9 wherein the mode of X-ray contrast agent injection is IV.

11. The method of claim 10 wherein the X-ray contrast agent is an Iodine containing compound.

12. The method of claim 8 wherein the volume of said left ventricle is calculated by applying the formula $V=\frac{8}{}$

S23

 



π



 



L

wherein V is the volume, S is the surface of the final 2-dimensional projection image and L is the length of the principal axis of said left ventricle as measured on said image.

13. The method of claim 1 wherein said X-rays are detected with an X-ray sensitive screen substantially parallel to said selected plane of symmetry.

14. The method of claim 1 wherein said X-rays are detected with an X-ray sensitive screen substantially non-parallel to said selected plane of symmetry.

15. The method of claim 14 wherein said 2-dimensional image is projected into a plane parallel to said plane of symmetry in a direction orthogonal to said plane parallel to said plane of symmetry prior to reconstructing the 3-dimensional image.

16. The method of claim 8 wherein said selected plane of symmetry is coincident with the anterior-posterior (A-P) plane of said ventricle.

17. The method of claim 8 wherein said mask and live images are acquired at the end diastolic part of the cardiac cycle.

19. The method of claim 6 wherein the object is an organ.

2. A method for the three dimensional image reconstruction of single plane 2-dimensional X-ray image projection of an object having at least one plane of symmetry comprising:

a) irradiating said object with X-rays substantially perpendicular to said at least one plane of symmetry of the object;

b) detecting said X-rays transmitted through said object to define a 2-dimensional projection mask image with pixels (x,y) having an intensity related to the absorbance of said object;

c) substantially uniformly filling the object with an X-ray contrast agent said contrast agent having a pre-selected concentration and absorption coefficient;

d) irradiating said contrast agent-filled object with X-rays substantially perpendicular to said at least one plane of symmetry of the object;

e) detecting said X-rays transmitted through said contrast agent-filled object to define a 2-dimensional projection live image with pixels (x,y) having an intensity related to the absorbance of said contrast agent-filled object;

f) subtracting said mask image from said live image to obtain a 2- dimensional final image;

d) processing said 2-dimensional final image to reconstruct the 3-dimensional image of said object, said processing including determining a distance D(x,y) travelled by said X-rays in the contrast agent-filled object by dividing the absorbance corresponding to the intensity of each pixel (x,y) by the concentration of the contrast agent within said object and multiplying the result thus obtained by the absorption coefficient of said contrast agent;

dividing said distance D(x,y) by 2 to define a (+z) coordinate (equals to +D(x,y)/2) and a (−

z) coordinate (equals to −

D(x,y)/2) for each pixel (x,y);

such that for each pixel (x,y) there is;

1) a (+z) coordinate=+D(x,y)/2 and

2) a (−

z) coordinate=−

D(x,y)/2;

e) using the x,y,z coordinates thus determined to reconstruct the 3-dimensional image in a 3-dimensional axis system in which the x-y plane is parallel to the plane of symmetry of said object.

18. The method of claim 2 further comprising the step of storing the reconstructed 3-dimensional image.

20. The method of claim 2 wherein said X-rays are detected with an X-ray sensitive screen substantially parallel to said selected plane of symmetry.

21. The method of claim 2 wherein said X-rays are detected with an X-ray sensitive screen substantially non-parallel to said selected plane of symmetry.