Square wave cone beam scanning trajectory for data completeness in three-dimensional computerized tomography

• US 5,073,910 A
• Filed: 08/27/1990
• Issued: 12/17/1991
• Est. Priority Date: 08/27/1990
• Status: Expired due to Fees

• Current Assignee: General Electric Company
• Original Assignee: General Electric Company
• Inventors: Eberhard, Jeffrey W., Hedengren, Kristina H. V.
• Primary Examiner(s): Howell, Janice A.
• Assistant Examiner(s): CHU, KIM KWOK
• Application Number:
  US07/572,651
• Time in Patent Office: 477 Days
• Field of Search: 378/4, 378/9, 378/10, 378/22, 378/901, 378/99, 378/11, 378/13, 378/17, 378/23
• US Class Current: 378/4
• 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 configuration for three-dimensional cone beam computerized tomography imaging which allows a complete data set to be acquired in a practical manner, while providing fast data acquisition to minimize motion artifacts. An object within a field of view such that every plane passing through the field of view passes through the source scanning trajectory at least once.

Claims

1. A scanning and data acquisition method for three-dimensional computerized tomography (CT) imaging of a field of view containing at least a portion of an object illuminated by a cone beam source, said method comprising:

defining a source scanning trajectory as a path traversed by said source;

employing the cone beam source fixed with reference to a two-dimensional array detector with both source and detector movably positioned relative to the object in order to scan about the object;

specifying the source scanning trajectory as a square wave on a cylindrical surface surrounding the field of view such that each plane passing through the field of view intersects the scanning trajectory in at least one point; and

scanning at a plurality of positions along the source scanning trajectory to obtain cone beam projection data.

2. A method in accordance with claim 1, which comprises specifying the source scanning trajectory as any even number of square wave cycles on the cylindrical surface.

3. A method in accordance with claim 2, which comprises specifying the source scanning trajectory as two complete square wave cycles on the cylindrical surface.

4. A method in accordance with claim 1, which comprises specifying the source scanning trajectory as any odd number of square wave cycles on the cylindrical surface.

5. A method in accordance with claim 4, which comprises specifying the source scanning trajectory as three complete square wave cycles on the cylindrical surface.

6. A method in accordance with claim 1, which comprises moving the source along the scanning trajectory in a continuous scan.

7. A method in accordance with claim 1, which comprises moving the source along the scanning trajectory in a step-wise scan.

8. A method in accordance with claim 1, which comprises maintaining the source and detector in stationary positions while translating and rotating the object so as to effect relative movement of the source with reference to the object.

9. A method in accordance with claim 1, which comprises maintaining the object in stationary positions while moving the source and detector so as to effect relative movement of the source with reference to the object.

10. A method in accordance with claim 2 wherein the field of view is cylindrical and has a radius no greater than r_o and a length no greater than ±

A_o, which comprises defining the scanning trajectory as

space="preserve" listing-type="equation">x(θ

)=r.sub.p cos θ

space="preserve" listing-type="equation">y(θ

)=r.sub.p sin θ

##EQU7## where r.sub.p is the radius of the scanning trajectory, A.sub.p is the amplitude of the scanning trajectory; and

the following conditions are met;

##EQU8##

11. A method in accordance with claim 3 wherein the field of view is cylindrical and has a radius no greater than r_o and a length no greater than ±

A_o, which comprises defining the scanning trajectory as

space="preserve" listing-type="equation">x(θ

)=r.sub.p cos θ

space="preserve" listing-type="equation">y(θ

)=r.sub.p sin θ

##EQU9## where r.sub.p is the radius of the scanning trajectory, A.sub.p is the amplitude of the scanning trajectory; and

the following conditions are met;

12. α

=β

=1. 34 ##EQU10##

14. A system in accordance with claim 12, wherein the source scanning trajectory is specified by any even number of square wave cycles on the cylindrical surface.

16. A system in accordance with claim 12, wherein the source scanning trajectory is specified by any odd number of square wave cycles on the cylindrical surface.

18. A system in accordance with claim 12, wherein said scanning means is operable to move said source relative to the object along the source scanning trajectory in a continuous scan.

19. A system in accordance with claim 12, wherein said scanning means is operable to move said source relative to the object along the scanning trajectory in a stepwise scan.

20. A system in accordance with claim 12, wherein said scanning element comprises a two-axis CNC part manipulator connected to the object for translating and rotating the object while said source and detector remain stationary.

21. A system in accordance with claim 12, wherein said scanning element comprises a two-axis CNC part manipulator connected to said source and detector for translating and rotating said source and detector about the object while the object remain stationary.

22. A system in accordance with claim 14, wherein the field of view is cylindrical and has a radius no greater than r_o and a length no greater than ±

A_o, and wherein the scanning trajectory is defined as

space="preserve" listing-type="equation">x(θ

)=r.sub.p cos θ

space="preserve" listing-type="equation">y(θ

)=r.sub.p sin θ

##EQU11## where r.sub.p is the radius of the scanning trajectory, A.sub.p is the amplitude of the scanning trajectory; and

the following conditions are met;

##EQU12##

23. A system in accordance with claim 14, wherein the field of view is cylindrical and has a radius no greater than r_o and a length no greater than ±

A_o, and wherein the scanning trajectory is defined as

space="preserve" listing-type="equation">x(θ

)=r.sub.p cos θ

space="preserve" listing-type="equation">y(θ

)=r.sub.p sin θ

##EQU13## where r.sub.p is the radius of the scanning trajectory, A.sub.p is the amplitude of the scanning trajectory; and

the following conditions are met;

13. A scanning and data acquisition system for three-dimensional computerized tomography (CT) imaging of a field of view containing at least a portion of an object illuminated by a cone beam source, said system comprising:

a cone beam source;

a two-dimensional array detector fixed in spaced alignment with reference to said source and both the detector and the source rotatably mounted to scan the object in order to acquire cone beam projection data; and

scanning means for effecting relative motion between said source and the object, said source moving relative to the object along a source scanning trajectory specified as a square wave on a cylindrical surface surrounding the field of view such that each plane passing through the field of view intersects the scanning trajectory in at least one point; and

means for acquiring cone beam projection data with said source at a plurality of positions on the scanning trajectory.

15. A system in accordance with claim 13, wherein the source scanning trajectory is specified by two complete square wave cycles on the cylindrical surface.

17. A method in accordance with claim 15, wherein the source scanning trajectory is specified by three complete square wave cycles on the cylindrical surface.

24. α

=β

=1. 34 ##EQU14##