Coherent-scatter computer tomograph

• US 7,590,215 B2
• Filed: 06/01/2005
• Issued: 09/15/2009
• Est. Priority Date: 06/07/2004
• Status: Expired due to Fees

• Current Assignee: Koninklijke Philips Electronics N.V. (Koninklijke Philips N.V.)
• Original Assignee: Koninklijke Philips Electronics N.V. (Koninklijke Philips N.V.)
• Inventors: Schlomka, Jens-Peter
• Primary Examiner(s): Glick; Edward J
• Assistant Examiner(s): Taningco; Alexander H
• Application Number:
  US11/569,806
• Publication Number:
  US 20080285706A1
• Time in Patent Office: 1,567 Days
• Field of Search: 378/4, 378/5
• US Class Current: 378/4
• CPC Class Codes: A61B 6/032 Transmission computed tomography [CT]
• CPC Class Codes: A61B 6/06 Diaphragms
• CPC Class Codes: A61B 6/4291 the detector being combined with a grid or grating
• CPC Class Codes: A61B 6/483 involving scattered radiation
• CPC Class Codes: G01N 23/207 Diffractometry using detectors, e.g. using a probe in a central position and one or more displaceable detectors in circumferential positions

Abstract

Conventional CSCT may require a complex reconstruction involving a large number of calculations. According to an exemplary embodiment of the present invention, additional collimators are used in combination with energy revolving detectors, which may allow that a CSCT image may be reconstructed by a simple superposition of images obtained from different viewing angles in a direct tomography data acquisition scheme. Advantageously, a reconstruction may be avoided. Advantageously, this may allow for an improved image quality while reducing an amount of calculations required for generating the output image.

Claims

1. A computer tomography apparatus for examination of an object of interest, the computer tomography apparatus comprising:

a source of radiation;

a scatter radiation detector for receiving a scatter radiation scattered by the object of interest, said detector being arranged opposite to the source of radiation with an offset with respect to a fan plane which extends through the object of interest and the source of radiation; and

a first collimator comprised of;

a second collimator focused at the source of radiation; and

a third collimator focused at the section of the object of interest;

wherein the scatter radiation detector has a plurality of detector regions organized substantially as a detector matrix comprised of matrix elements defined by horizontal and vertical detector lines, each of the plurality of detector regions having at least one energy resolving detector element;

wherein the first collimator is adapted such that radiation impinging on the at least one energy resolving detector element of a respective region of the plurality of regions is substantially restricted to scatter radiation scattered from a predetermined section of the object of interest, the dimensions of which correspond substantially to a matrix element of said detector matrix;

wherein the source of radiation is adapted such that a fan beam of radiation is applied to the object of interest in the fan plane.

2. The computer tomography apparatus of claim 1,

wherein the second and third collimators are arranged one after another with respect to the source of radiation.

3. The computer tomography apparatus of claim 1,

wherein the second collimator has first lamellae which are focused at the source of radiation and are arranged substantially perpendicular to the fan plane such that radiation impinging on the at least one first detector element in the region of the plurality of regions associated with the second collimator is restricted to radiation having a first predetermined angle with respect to the source of radiation;

and

wherein the third collimator has second lamellae which are focused at the section of the object of interest such that radiation impinging on the at least one first detector element in the region of the plurality of regions associated with the third collimator is restricted to radiation having a second predetermined angle with respect to the section of the object of interest.

4. The computer tomography apparatus of claim 1, wherein the second and third collimators are together implemented by means of a slot collimator comprising holes which, for each respective region, are respectively focused in the fan-plane at the source of radiation and out of the fan-plane defines a fixed scatter angle and a section within the section of the object of interest from which radiation can reach a detector element.

5. The computer tomography apparatus of claim 1, further comprising:

a primary radiation detector;

wherein the primary radiation detector is arranged opposite to the source of radiation in the fan plane for receiving a primary radiation attenuated by the object of interest.

6. The computer tomography apparatus of claim 5, wherein the at least one energy resolving detector element is a direct-converting semiconductor cell;

and

wherein the primary radiation detector comprises scintillator cells.

7. The computer tomography apparatus of claim 1, further comprising a calculation unit;

wherein the calculation unit is adapted to generate a first output image without performing a reconstruction.

8. The computer tomography apparatus of claim 7, wherein the calculation unit is further adapted to generate the first output image by superposing second images corresponding to readouts of the scatter radiation detector obtained from different viewing angles with respect to the object of interest.

9. The computer tomography apparatus of claim 7, wherein the calculation unit is further adapted to perform at least one of an attenuation correction and a primary radiation intensity correction.

10. A computer tomography apparatus for determining a first output image by using readouts from a scatter radiation detector, the computer tomography apparatus having:

a source of radiation;

a scatter radiation detector for receiving a scatter radiation scattered by the object of interest wherein the scatter radiation detector has a plurality of detector regions organized substantially as a detector matrix comprised of matrix elements defined by horizontal and vertical detector lines;

wherein each of the plurality of detector regions has at least one energy resolving detector element;

a first collimator comprised of a second collimator focused at the source of radiation and a third collimator focused at a section of the object of interest;

wherein the first collimator is adapted such that radiation impinging on the at least one energy resolving detector element of a respective region of the plurality of regions is substantially restricted to scatter radiation scattered from a predetermined section of the object of interest, the dimensions of which correspond substantially to a matrix element of said detector matrix;

wherein the scatter radiation detector is arranged opposite to the source of radiation with an offset with respect to a fan plane;

wherein the fan plane extends through the object of interest and the source of radiation;

wherein the scatter radiation detector has a plurality of regions;

wherein each of the regions has at least one first detector element;

wherein the at least one first detector element is an energy resolving detector element;

wherein the first collimator is adapted such that scatter radiation impinging on the at least one first detector element of a respective region of the plurality of regions is substantially restricted to radiation scattered from a predetermined section of the object of interest; and

wherein the source of radiation is adapted such that a fan beam of radiation is applied to the object of interest in the fan plane; and

a data processing device comprising;

a memory for storing the readouts from the scatter radiation detector; and

a processor which is adapted to perform at least the following operation;

generating a first output image from the readouts without performing a reconstruction.

11. The data processing device of claim 10, wherein the processor is further adapted to generate the first output image by superposing second images corresponding to readouts of the radiation detector obtained from different viewing angles with respect to the object of interest.

12. The data processing device of claim 10, wherein the processor is further adapted to perform at least one of an attenuation correction and a primary radiation intensity correction.

13. A method of performing a fan-beam coherent scatter computer tomography scan with a computer tomography apparatus for examination of an object of interest, the method comprising the steps of:

providing a source of radiation;

providing a scatter radiation detector for receiving a scatter radiation scattered by the object of interest, wherein the scatter radiation detector has a plurality of detector regions organized substantially as a detector matrix comprised of matrix elements defined by horizontal and vertical detector lines;

providing a first collimator comprised of a second collimator focused at the source of radiation and a third collimator focused at a section of the object of interest, wherein the first collimator is adapted such that radiation impinging on the at least one energy resolving detector element of a respective region of the plurality of regions is substantially restricted to scatter radiation scattered from a predetermined section of the object of interest, the dimensions of which correspond substantially to a matrix element of said detector matrix;

energizing the source of radiation to generate a fan beam of radiation;

determining readouts from the scatter radiation detector;

generating a first output image from the readouts by superimposing images without performing a reconstruction.

14. The method of claim 13, wherein the step of generating a first output image from the readouts without performing a reconstruction further comprises the steps of:

superposing second images corresponding to readouts of the radiation detector obtained from different viewing angles with respect to the object of interest; and

performing at least one of an attenuation correction and a primary radiation intensity correction.

15. The method of claim 14, further comprising the steps of:

determining attenuation coefficients of the object of interest by using readouts of a primary radiation detector arranged in the fan plane;

determining parameters for the absorption correction of the readouts from the scatter radiation detector on the basis of the attenuation coefficients.

16. The method of claim 13, wherein the source of radiation is operated such that the primary radiation detector and the scatter radiation detector are subjected to the fan beam radiation emitted from the source of radiation essentially at the same time.

17. The method of claim 13, wherein the scatter radiation detector is arranged opposite to the source of radiation with an offset with respect to a fan plane.

18. The method of claim 13, wherein the fan plane extends through the object of interest and the source of radiation.

19. The method of claim 13, wherein the scatter radiation detector has a plurality regions.

20. The method of claim 13, wherein each of the regions has at least one first detector element.

21. The method of claim 13, wherein the at least one first detector element is an energy resolving detector element.

22. The method of claim 13, wherein the first collimator is adapted such that radiation impinging on the at least one first detector element of a respective region of the plurality of regions is substantially restricted to scatter radiation scattered from a predetermined section of the object of interest.

23. The method of claim 13, wherein the source of radiation is adapted such that a fan beam of radiation is applied to the object of interest in the fan plane.