Method for reconstructing tomograms from detector measured data of a tomography unit

• US 20060013354A1
• Filed: 07/15/2005
• Published: 01/19/2006
• Est. Priority Date: 07/16/2004
• Status: Abandoned Application

• Current Assignee: Siemens AG
• Original Assignee: Siemens AG
• Inventors: Heismann, Bjoern
• Application Number:
  US11/181,734
• Publication Number:
  US 20060013354A1
• Time in Patent Office: Days
• 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 6/482 involving multiple energy imaging
• 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 2211/408 Dual energy
• CPC Class Codes: G06T 2211/424 Iterative

Abstract

A reconstruction method is used in computed tomography, wherein an examination object is scanned with a beam that rotates during scanning about a system axis. In the method, firstly the absorption coefficients of subvolumes relatively remote from the system axis are determined. Subsequently the absorption coefficients of the subvolumes situated relatively nearer to the system axis are determined iteratively, taking account of the absorption coefficients already calculated.

Claims

1. A reconstruction method in computed tomography, comprising:

scanning an examination object with a beam that rotates during scanning about a system axis;

determining absorption coefficients of subvolumes that are relatively remote from the system axis; and

subsequently determining absorption coefficients of subvolumes relatively nearer to the system axis, iteratively, taking account of the absorption coefficients already calculated.

2. The method as claimed in claim 1, wherein the method is respectively carried out per se for at least one of an individual slice plane and a number of individual slice planes, independently of one another.

3. The method as claimed in claim 1, wherein spiral scanning takes place and it is carried out for complete scanning volumes of at least substantially cylindrical design by firstly calculating subvolumes at the edge using rays at the edge and subsequently iteratively calculating subvolumes, lying relatively further inside and approaching one another in relation to the system axis, with reference to their absorption coefficients, doing so in each case by taking account of the already calculated absorption coefficients lying relatively further outside.

4. The method as claimed in claim 1, wherein at least one of multirow detectors, multifocus systems and multitube systems are used.

15. The method as claimed in claim 2, wherein the absorption coefficients ({right arrow over (μ

)}_s) of the shell segments is calculated iteratively using the following formula;

${\stackrel{\to <br><br>}{\mathrm{\mu <br><br>}}}_s=L_s^{-1}\left({\stackrel{\to <br><br>}{A}}_s-\underset{i=1}{\overset{s-1}{\sum <br><br>}}<br><br>L_{s,i}<br><br>\text{\hspace{1em}<br><br>}<br><br>{\stackrel{\to <br><br>}{\mathrm{\mu <br><br>}}}_i\right),$

L_s being the path length matrix of the defining ray of the shell s, L_s,i being the path length matrices of the rays i=1 . . . s lying further outside with reference to the system axis, and A_s being the partial sinogram belonging to the shell S_s.

16. The method as claimed in claim 1, wherein the subvolumes are of rectangular formation in section perpendicular to the system axis.

17. The method as claimed in claim 1, wherein the subvolumes are of hexagonal formation in section perpendicular to the system axis.

18. The method as claimed in claim 1, wherein, during the iterative measurement of the absorption coefficients, their energy dependence is taken into account.

19. The method as claimed in claim 18, wherein use is made for this purpose of the energy-dependent variation in the intensity of radiation after passage through the examination object.

20. The method as claimed in claim 18, wherein, use is made for this purpose of the total variation in intensity of at least two rays having a known different energy spectrum on the same beam path.

21. The method as claimed in claim 20, wherein at least two radiation sources are used which have different spectra, and which are arranged in such a way that they revolve on the same track during the scanning of the examination object.

22. The method as claimed in claim 1, wherein the examination object is scanned with a beam of known energy spectrum, and the varied energy spectrum of each ray is measured after passage through the examination object.

23. The method as claimed in claim 22, wherein the energy spectrum includes at least two mean energies.

24. The method as claimed in claim 18, wherein an intensity value of a primary color is assigned per energy to the value of the energy-dependent absorption coefficients when displaying the CT tomograms, a color display of the CT image resulting therefrom.

5. A method for reconstructing tomographs from detector measured data of a tomography unit, comprising:

moving at least one radiation source about a system axis;

measuring, using at least one oppositely situated at least single row detector, measures absorption of the radiation, emanating from the radiation source after the penetration of an examination object, the radiation source revolving around the examination object on an imaginary cylindrical surface and in the process scanning the examination object, which lies in a scanning volume formed by the rays, with a beam, the scanning volume being divided into a multiplicity of subvolumes;

using a ray in the beam that is remote from the system axis and whose absorption is used to determine absorption coefficients of the subvolumes penetrated by this ray; and

subsequently, iteratively using rays relatively closer to the system axis and using their measured absorption in order to determine as yet unknown absorption coefficients of as yet unconsidered subvolumes, taking account of already known absorption coefficients of already calculated subvolumes.

6. The method as claimed in claim 5, wherein

the scanning volume is divided into a multiplicity of concentric shells, and the shells are subdivided in turn into shell segments, wherein firstly the absorption coefficients of relatively outer segments are determined, and thereupon the absorption coefficients of the shell segments lying relatively further inside, are determined iteratively taking account of the absorption coefficients, calculated meanwhile of shell segments lying relatively further outside, until the center of the scanning volume is reached.

7. The method as claimed in claim 6, wherein the shells are divided into individual shell segments of identical thickness in the radial direction.

8. The method as claimed in claim 6, wherein the shells are divided into individual shell segments of identical length in the circumferential direction.

9. The method as claimed in claim 6, wherein the individual shell segments have an identical cross-sectional surface perpendicular to the system axis.

10. The method as claimed in claim 6, wherein the individual shell segments sweep over a segment angle of identical size.

11. The method as claimed in claim 6, wherein, proceeding from the focus to a specific detector element, each ray is assigned a shell at a constant distance from the system axis.

12. The method as claimed in claim 6, wherein each ray of the beam describes a tangent circle with all the perpendicular feet relative to the system axis, and the shell segments that have an outer circular segment and an inner circular segment, the shell segments being arranged in such a way that the tangent circle lies centrally between the outer circular segment and inner circular segment.

13. The method as claimed in claim 6, wherein each shell segment has an imaginary centroid line that corresponds to a circular segment of concentrically arranged circles about the system axis.

14. The method as claimed in claim 6, wherein each shell segment has an imaginary centroid line that corresponds to a segment of concentrically arranged helical lines about the system axis.

26. The method as claimed in claim 7, wherein the shells are divided into individual shell segments of identical length in the circumferential direction.

25. A tomography unit for reconstructing tomograms from detector measured data, comprising:

at least one radiation source, movable about a system axis;

at least one oppositely situated, at least single row detector that measures the absorption of the radiation, emanating from the radiation source, after penetration of an examination object, wherein at least the radiation source revolves around the examination object on an imaginary cylindrical surface and scans the examination object, which lies in a scanning volume formed by the rays, with a beam; and

means for determining absorption coefficients of subvolumes that are relatively remote from the system axis and subsequently determining absorption coefficients of subvolumes relatively nearer to the system axis, iteratively, taking account of the absorption coefficients already calculated.

27. The tomography unit as claimed in claim 25, further comprising:

means for controlling the tomography unit and for collecting and computationally processing detector output data,

reconstructing tomographic images and displaying the images.