Reduction of hitlist size in spiral cone beam CT by use of local radon origins

• US 5,901,196 A
• Filed: 09/30/1997
• Issued: 05/04/1999
• Est. Priority Date: 09/30/1997
• Status: Expired due to Term

• Current Assignee: Siemens Medical Solutions USA Incorporated (Siemens AG)
• Original Assignee: Siemens Corporate Research Incorporated (Siemens AG)
• Inventors: Samarasekera, Supun, Sauer, Frank, Tam, Kwok
• Primary Examiner(s): Bruce, David Vernon
• Application Number:
  US08/940,489
• Time in Patent Office: 581 Days
• Field of Search: 378/4, 378/15, 378/901
• US Class Current: 378/4
• CPC Class Codes: A61B 6/027 characterised by the use of a particular data acquisition trajectory, e.g. helical or spiral
• CPC Class Codes: G01N 2223/419 computed tomograph
• CPC Class Codes: G01N 23/046 using tomography, e.g. computed tomography [CT]
• CPC Class Codes: Y10S 378/901 Computer tomography program or processor

Abstract

A method and apparatus for reconstructing an image of an object using a three dimensional (3D) computerized tomographic (CT) imager having a cone beam radiation source and detector arrangement for acquiring measurement data. The source and detector arrangement is operated at a plurality of source positions along a spiral scan path so as to acquire a corresponding plurality of sets of measurement data representative of radiation attenuation caused by the object. Image reconstruction processing information required for processing of the acquired measurement data in a Radon space partitioned by plurality of vertically oriented coaxial φ-planes for reconstructing the image, is pre-calculated and stored in a hitlist. The stored information is pre-calculated on less that all of the φ-planes, but due to a symmetry that is induced in the reconstruction processing, the stored information can be used for calculating Radon data for all of the φ-planes that partition the Radon space. The size of the hitlist is thus reduced by a factor equal to the number of φ-planes for which the stored information is re-used, e.g., 360 for 1/2 degree φ-plane spacing and storage of reconstruction processing information for a single φ-plane.

Claims

1. A method of operating a 3D CT imaging apparatus having a cone beam radiation source and detector arrangement, for reconstructing an image of an object that is scanned by said source and detector arrangement, comprising the following steps:

operating said source and detector arrangement at a plurality of source positions along a spiral scan path so as to acquire a corresponding plurality of sets of measurement data representative of radiation attenuation caused by said object, and

processing the acquired measurement data using pre-calculated and stored image reconstruction processing information that was calculated on less that all of a plurality of vertically oriented coaxial φ

-planes that partition Radon space, for developing numerical values for Radon data samples on all of said φ

-planes that partition the Radon space.

2. The method of claim 1, wherein said processing step comprises,

using pre-calculated image reconstruction processing information calculated on a single φ

-plane, for determining a numerical value for the Radon data samples for all of the φ

-planes.

3. The method of claim 1, wherein said processing step comprises,

inducing a symmetry into the image reconstruction processing of the measurement data so that a correspondence is developed between the relative source positions and Radon data samples over a plurality of φ

-planes.

4. The method of claim 3, wherein said inducing step comprises establishing on each of successive ones of the φ

-planes a local Radon origin, which Radon origins are independent of each other.

5. The method of claim 4, wherein said establishing step comprises,

shifting the Radon origin for each of successive ones of said φ

-planes an amount corresponding to an amount of z-axis shift that a projection of the spiral scan path experiences between the successive φ

-planes.

6. The method of claim 4, including a further processing step of performing two-step Radon inversion processing of the Radon data to develop image reconstruction data in a coordinate system having a global origin, wherein the shift of the local Radon origins of the φ

-planes are compensated for during the Radon inversion processing.

7. The method of claim 6, wherein said two-step Radon inversion processing includes a first step for backprojecting the Radon data for each of said successive φ

-planes to make 2D images on grids (z,r'"'"') of φ

-planes having local origins which are already part of a global grid, the z-axis shift of the Radon origin for each of said successive φ

-planes that are input to the Radon inversion processing being taken into account by introducing a Δ

z offset into the coordinate variables of the backprojecting processing that corresponds to the amount of z-axis shift of the Radon origin of each of the φ

-planes.

8. The method of claim 6, wherein said two-step Radon inversion processing includes a first step for backprojecting the Radon data for each of said successive φ

-planes to make 2D images on grids (z,r'"'"') of φ

-planes having local origins which are shifted along with the local Radon origins of the φ

-planes that are input to the Radon inversion processing, and then, before one performs a second step of the two-step inversion processing, shifting in the z-axis direction the backprojection results from the first step, in order to compensate for the previous z-shift of the local origins.

9. The method of claim 8, wherein said shifting of the backprojection results comprises interpolating new image values that are shifted in the z-axis direction from 2d images that resulted from the first backprojection step.

10. The method of claim 1, wherein said processing step comprises,

organizing the pre-calculated image reconstruction processing information into a database.

11. The method of claim 10, wherein said processing step comprises,

organizing the pre-calculated image reconstruction processing information into a database sortable by sample points in Radon space, so that less than all of the maximum samples of Radon data will be determined, thereby reconstructing the image in a desired resolution that is less than a maximum resolution.

12. A method of operating a 3D CT imaging apparatus having a cone beam radiation source and detector arrangement, for reconstructing an image of an object that is scanned by said source and detector arrangement, comprising the following steps:

before the acquisition of measurement data during an imaging operation of the apparatus,

pre-calculating and storing image reconstruction processing information required for processing of the acquired measurement data in Radon space partitioned by a set of vertically oriented co-axial φ

-planes to develop contributions to the final reconstruction of the image, which information is calculated on less than all of said φ

-planes; and

during the imaging operation of the apparatus,

operating said source and detector arrangement at a plurality of source positions along a scan path so as to acquire a corresponding plurality of sets of said measurement data, and

processing the acquired measurement data using said pre-calculated image reconstruction processing information on said single φ

-plane in a relative way to determine Radon data for other ones of the φ

-planes and reconstructing the image.

13. The method of claim 12, wherein said processing step comprises,

inducing a symmetry into the image reconstruction processing of the measurement data so that a correspondence is developed between the relative source positions and Radon data samples over a plurality of φ

-planes.

14. The method of claim 13, wherein said inducing step comprises establishing on each of successive ones of the φ

-planes a local Radon origin, which Radon origins are independent of each other.

15. The method of claim 14, wherein said establishing step comprises,

shifting the Radon origin for each of successive ones of said φ

-planes an amount corresponding to an amount of z-axis shift that a projection of a spiral scan path experiences between the successive φ

-planes.

16. The method of claim 14, including a further processing step of performing two-step Radon inversion processing of the Radon data to develop image reconstruction data in a coordinate system having a global origin, wherein the shift of the local Radon origins of the φ

-planes that are input to the Radon inversion processing are compensated for during the Radon inversion processing.

17. The method of claim 16, wherein said two-step Radon inversion processing includes a first step for backprojecting the Radon data for each of said successive φ

-planes to make 2D images on grids (z,r'"'"') of φ

-planes having local origins which are already part of a global grid, the z-axis shift of the Radon origin for each of said successive φ

-planes that are input to the Radon inversion processing being taken into account by introducing a Δ

z offset into the coordinate variables of the backprojecting processing that corresponds to the amount of z-axis shift of the Radon origin of each of the φ

-planes.

18. The method of claim 16, wherein said two-step Radon inversion processing includes a first step for backprojecting the Radon data for each of said successive φ

-planes to make 2D images on grids (z,r'"'"') of φ

-planes having local origins which are shifted along with the local Radon origins of the φ

-planes that are input to the Radon inversion processing, and then, before one performs a second step of the two-step inversion processing, shifting in the z-axis direction the backprojection results from the first step, in order to compensate for the previous z-shift of the local origins.

19. The method of claim 18, wherein said shifting of the backprojection results comprises interpolating new image values that are shifted in the z-axis-direction from 2D images that resulted from the first backprojection step.

20. The method of claim 12, wherein said processing step includes the further step of,

inducing a symmetry into the image reconstruction processing of the measurement data so that a spatial correspondence is developed between the position of samples on either side of a local origin in a projection of a spiral scan path onto a φ

-plane.

21. The method of claim 12, wherein said pre-calculating and storing step comprises,

calculating as said image reconstruction processing information that information which is determined by predetermined geometric parameters of the scan path and the detector, and a desired sampling of the scan path and Radon space.

22. The method of claim 12, wherein said pre-calculating and storing step comprises,

organizing the pre-calculated image reconstruction processing information into a database.

23. The method of claim 22, wherein said organizing step comprises,

organizing the pre-calculated image reconstruction processing information into a database sortable by sample points in Radon space, so that less than all of the maximum samples of Radon data will be determined, thereby reconstructing the image in a desired resolution that is less than a maximum resolution.

24. The method of claim 12, wherein said pre-calculating and storing step comprises,

calculating as said image reconstruction processing information that information which calculates Radon data on a single given φ

-plane.

25. The method of claim 24, wherein said processing step comprises using the information calculated on said single given φ

-plane to determine Radon data for all of the remaining φ

-planes.

26. A scanning and data acquisition apparatus for three dimensional (3D) computerized tomography (CT) imaging of an object in a field of view radially centered on a predetermined axis, comprising:

an energy source (10) for emitting energy in the form of a cone beam;

an area detector (12) for detecting as measurement data cone beam energy after attenuation by passage through an object to be imaged;

a manipulator (6) for movably positioning said source and detector along a scan path relative to the object, to cause irradiation of said object by said source at multiple source positions along said scan path about said object, said detector acquiring a corresponding set of measurement data at each said source position;

control means (8) for defining the scan path as a plurality of spaced stages on a predetermined geometric surface surrounding the field of view, with each of a plurality of planes that pass through the field of view and intersect the scan path in at least one point as well as the area detector, being useful for calculating Radon data at a given one of a plurality of Radon sample points that sample a Radon space partitioned by a set of vertically oriented co-axial φ

-planes;

image reconstruction processing means (18) including means for calculating Radon data for each of said Radon sample points by processing multiple ones of the sets of measurement data, for developing image data; and

display means (28) responsive to said image data for displaying a reconstructed image of the object;

wherein said image reconstruction processing means (18) includes a database (21) of reconstruction processing information that is calculated on less than all of said φ

-planes, which information is pre-calculated and stored before acquisition of the measurement data, and then used by said image reconstruction processing means (18) during imaging operation of said apparatus for facilitating processing of the measurement data to calculate the Radon data for all of the φ

-planes.

27. Apparatus in accordance with claim 26, wherein said image reconstruction processing means (18) includes Radon derivative calculating means (20) responsive to the image reconstruction processing information stored in said database (21) for calculating Radon derivative data for each of said Radon sample points in Radon space by processing line integral values from multiple ones of the sets of measurement data.

28. Apparatus in accordance with claim 27, wherein said image reconstruction processing means (18) includes Radon derivative data converting means (22) responsive to the image reconstruction processing information stored in said database (21) and said Radon derivative data for calculating Radon data at equally spaced polar grid points.

29. Apparatus in accordance with claim 27, wherein said image reconstruction processing means (18) includes inverse transformation processing means (24) responsive to said Radon data at equally spaced polar grid points for performing a 3D inverse Radon transformation of said Radon data to develop said image data.

30. Apparatus in accordance with claim 26, wherein said image reconstruction processing means (18) includes a two-step Radon inversion processor (24) which independently processes each of said φ

-planes of Radon data, for developing said image data.