Electron beam computed tomographic scanner system with helical or tilted target, collimator, and detector components to eliminate cone beam error and to scan continuously moving objects

• US 6,735,271 B1
• Filed: 11/28/2000
• Issued: 05/11/2004
• Est. Priority Date: 11/28/2000
• Status: Expired due to Fees

• Current Assignee: GE Medical Systems Global Technology Company LLC (GE Healthcare Technologies, Inc.)
• Original Assignee: GE Medical Systems Global Technology Company LLC (GE Healthcare Technologies, Inc.)
• Inventors: Rand, Roy E., Boyd, Douglas P., Harman, Jonathan
• Primary Examiner(s): Dunn, Drew A.
• Assistant Examiner(s): THOMAS, COURTNEY D
• Application Number:
  US09/728,481
• Time in Patent Office: 1,260 Days
• Field of Search: 378/4, 378/15, 378/137, 378/901, 378/10
• 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: A61B 6/032 Transmission computed tomography [CT]
• CPC Class Codes: A61B 6/4028 resulting in acquisition of views from substantially different positions, e.g. EBCT
• CPC Class Codes: A61B 6/4085 Cone-beams
• CPC Class Codes: G01N 2223/419 computed tomograph
• CPC Class Codes: G01N 2223/612 biological material
• CPC Class Codes: G01N 23/046 using tomography, e.g. computed tomography [CT]
• CPC Class Codes: G06T 11/005 Specific pre-processing for tomographic reconstruction, e.g. calibration, source positioning, rebinning, scatter correction, retrospective gating
• CPC Class Codes: G06T 2211/428 Real-time
• CPC Class Codes: G21K 1/06 using diffraction, refraction or reflection, e.g. monochromators G21K1/10, G21K7/00 take precedence

Abstract

A scanning electron beam computed tomographic system eliminates axial offset between target and detector by disposing the target, collimator, and detector such that active portions of the target and detector are always diametrically opposite each other. This result is achieved by providing a helical target, collimator, and detector, or by providing planar target, collimator, and detector components that are inclined relative to the vertical axis such that active portions of the target and detector are always diametrically opposite each other. Either configuration eliminates cone beam error and the necessity to correct for same. Further, the system can provide multi-slice scanning of an object that is in constant motion at a critical velocity, without having to interpolate data. Conventional helical scanning may still be undertaken. Detector elements can be disposed axially to improve signal/noise ratio and to produce a cone beam cancellation effect.

Claims

1. In a scanning electron beam computed tomographic system in which an electron beam is scanned across a target with a constant velocity to emit a fan beam of X-rays some of which X-rays may pass through an area defined by a reconstruction radius and having an object therein to be detected by a detector array, a method of eliminating cone beam error, comprising the following steps:

(a) configuring and disposing said target and said detector array such that active regions of said target and said detector array are always diametrically opposite from each other;

wherein step (a) includes providing a planar target and a planar detector array and tilting said target and said detector array relative to a transverse axis that may include a vertical axis of said system to approximate a true helix configuration.

2. In a scanning electron beam computed tomographic system in which an electron beam is scanned across a target with a constant velocity to emit a fan beam of X-rays some of which X-rays may pass through an area defined by a reconstruction radius and having an object therein to be detected by a detector array, a method of eliminating cone beam error, comprising the following steps:

(a) configuring and disposing said target and said detector array such that active regions of said target and said detector array are always diametrically opposite from each other;

(b) moving said object along a z-axis of said system with an object velocity equal to a critical velocity Vcrit during helical mode operation of said system;

wherein discrete equally-spaced slices of said object may be scanned without need to interpolate scan data acquired by said system.

3. The method of claim 2, wherein said object is moved with said velocity Vcrit relative to a stationary said system.

4. The method of claim 2, wherein said system is moved with said velocity Vcrit relative to a stationary said object.

5. The method of claim 4, wherein said object is moved with velocity less than approximately half Vcrit relative to a stationary said system.

6. The method of claim 4, wherein said system is moved with said velocity less than approximately half a constant critical velocity Vcrit relative to a stationary said object.

7. In a scanning electron beam computed tomographic system operated in helical mode in which an electron beam is scanned across a target with a constant velocity to emit a fan beam of X-rays some of which X-rays may pass through an area defined by a reconstruction radius and having an object therein to be detected by a detector array, a method of acquiring scan data without a need to interpolate said data, the method comprising the following steps:

(a) configuring and disposing said target and said detector array such that active regions of said target and said detector array are always diametrically opposite from each other;

(b) providing relative movement of said object to said system along a z-axis of said system at a critical velocity Vcrit;

wherein equally spaced object slices are acquired without need to interpolate said data.

8. The method of claim 7, wherein step (a) includes providing a helical shaped said target and providing a helical shaped said detector array.

9. The method of claim 7, wherein step (a) includes providing a planar target and a planar detector array and tilting said target and said detector array relative to a transverse axis that may include a vertical axis of said system to approximate a true helix configuration.

10. The method of claim 7, wherein step (a) includes providing a detector array including elements disposed along an axial axis of said system.

11. A scanning electron beam computed tomographic system in which cone beam error is eliminated, comprising:

a helical shaped target;

a helical shaped detector array;

said target and said detector array disposed such that active regions of said target and active regions of said array are always diametrically opposite one another;

means for generating and sweeping an electron beam across said target with a constant velocity to emit a fan beam of X-rays some of which X-rays may pass through an area defined by a reconstruction radius and having an object therein to be detected by said detector array;

means for moving said object relative to a z-axis of said system with an velocity less than or equal to a critical velocity Vcrit;

wherein in helical mode operation of said system, if said velocity=Vcrit,scan data representing equally spaced slices of said object are obtained without need to interpolate said data.

12. The system of claim 11, wherein said means for moving has a characteristic selected from a group consisting of (i) said object is moved and said system is stationary, and (ii) said system is moved and said object is stationary.

13. A scanning electron beam computed tomographic system in which cone beam error is eliminating, comprising:

a planar target tilted with respect to a transverse axis that may include a vertical axis of said system to approximate a true helix;

a planar detector array tilted with respect to the same axis of said system to approximate a true helix;

said target and said detector array disposed such that active regions of said target and active regions of said array are always diametrically opposite one another; and

means for generating and sweeping an electron beam across said target with a constant velocity to emit a fan beam of X-rays some of which X-rays may pass through an area defined by a reconstruction radius and having an object therein to be detected by said detector array.

14. The system of claim 13, further including:

means for moving said object relative to a z-axis of said system with a velocity less than or equal to a critical velocity Vcrit;

wherein in helical mode operation of said system, if said velocity=Vcrit scan data representing equally spaced slices of said object are obtained without need to interpolate said data.

15. The system of claim 13, wherein said detector array includes elements displaced along an axial axis of said system.