Patent Number: 
Section: claims

1. Apparatus for imaging a body, comprising:a camera head positioned in a location and configured to detect radiation emitted from regions in the body so as to produce sliced images of radiation intensity emitted from a three dimensional structure of the regions, the camera head comprising:a two-dimensional array of D CdZnTe (CZT) detector elements, wherein D is an integer greater than 1, the array of D detector elements being defined by two orthogonal repetition vectors, the elements being mounted in the camera head and being respectively coupled to D electrodes, each electrode being configured to output signals indicative of intensities of radiation that are incident on a given detector element; andD adjustable collimators disposed respectively, in a collimator array defined by two orthogonal repetition vectors, in registration between the D detector elements and the body so as to define respective regions of the body from which the radiation emitted is incident on the detector elements, each of the adjustable collimators having N dimensional configurations defining different respective volumes of each of the regions, wherein N is an integer greater than 1, wherein each of the collimators is in registration with each of the detector elements so that the emitted radiation from the body traverses the collimators to impinge on the detector elements and wherein for each collimator the respective volumes of each of the regions have a respective common axis of symmetry which is normal to the two orthogonal repetition vectors, wherein each collimator comprises a respective different cavity which is configured to receive liquid opaque to the radiation; anda processor which is configured:to receive DN signals from the D electrodes corresponding to the respective volumes of each collimator while the camera head is in the location and while the respective common axis of symmetry of each collimator is fixed and while the adjustable collimators are in the N different dimensional configurations,to process the signals in order to form a three dimensional image of the body comprising a number of volume elements from which the radiation is emitted, andto produce sliced images of the three dimensional image while the two-dimensional array of CZT detector elements and the respective common axis of symmetry of each collimator are fixed with respect to the body,wherein the number of volume elements is a function of D and N. 2. The apparatus according to claim 1, wherein each collimator comprises a first collimator channel aligned with a second collimator channel and separated therefrom by an adjustable gap. 3. The apparatus according to claim 2, wherein the first collimator channel is aligned with one of the detector elements and is separated therefrom by a variable gap. 4. The apparatus according to claim 3, wherein the processor is coupled to adjust at least one of the variable gap and the adjustable gap. 5. The apparatus according to claim 2, wherein the first and second collimator channels comprise different cross-sectional areas. 6. The apparatus according to claim 1, wherein the liquid comprises mercury. 7. The apparatus according to claim 1, wherein each respective different cavity alters a length of each collimator on receipt of the liquid. 8. The apparatus according to claim 1, wherein each respective cavity comprises a different first cylinder and a different second cylinder having a different cross- section from the respective different first cylinder, and wherein each collimator on receipt of the liquid changes from the respective different first cylinder to the respective different second cylinder. 9. The apparatus according to claim 1, wherein the emitted radiation comprises gamma rays. 10. The apparatus according to claim 1, wherein the processor is configured to generate a representation of radioisotopes in the body in response to an intensity of the radiation. 11. The apparatus according to claim 1, wherein the processor is coupled to compute the number of the volume elements iteratively, so as to determine a largest number of the volume elements. 12. The apparatus according to claim 1, wherein the different respective volumes comprise respective first volumes and respective second volumes, and wherein the respective first volumes include the respective second volumes. 13. The apparatus according to claim 12, wherein the respective first volumes comprise respective first conic volumes, and wherein the respective second volumes comprise respective second conic volumes concentric with the respective first conic volumes. 14. The apparatus according to claim 1, wherein each respective different cavity comprises a plurality of isolated sub-compartments, each sub-compartment being independently filled with the liquid to form the N dimensional configuration, and so that each respective different cavity is operative in the N dimensional configurations in non-horizontal orientations. 15. The apparatus according to claim 1, wherein the volume elements are uniquely identifiable by an ordered triple (i, j, k) wherein i, j, k are positive integers having respective values 1, . . . , I; 1, . . . , J; and 1, . . . , K; and wherein a number IJK of volume elements is a function of DN proportionality coefficients βi,j,kd,n for each of the volume elements, wherein d, n are positive integers respectively identifying a particular detector element and a particular configuration of the adjustable collimators, d, n having respective values 1, . . . , D; 1, . . . N, each proportionality coefficient being a ratio between the emitted radiation from a given volume element of the body and the radiation received by a given detector element for a respective collimator having a given dimensional configuration. 16. The apparatus according to claim 15, wherein βi,j,kd,n=αi,j,kd,n·θi,j,kd,n·Vi,j,kd,n wherein:αi,j,kd,n is an attenuation factor between volume element (i, j, k) and detector d in collimator dimensional configuration n, θi,j,kd,n is a solid angle in which volume element (i, j, k) is viewed from detector d in collimator dimensional configuration n, and Vi,j,kd,n is a volume fraction of volume element (i, j, k) enclosed by the body as viewed from detector d in collimator dimensional configuration n. 17. The apparatus according to claim 16, wherein the processor is configured:to calculate values of βi,j,kd,n, αi,j,kd,n, θi,j,kd,n, and Vi,j,kd,n in response to geometrical relations between positions of the body, the D detector elements and the N dimensional configurations of the collimators, and wherein processing the signals comprises evaluating DN simultaneous linear equations:      S          d      ,      n        =            ∑              i        ,        j        ,        k              ⁢                  ⁢                  α                  i          ,          j          ,          k                          d          ,          n                    ·              C                  i          ,          j          ,          k                    ·              θ                  i          ,          j          ,          k                          d          ,          n                    ·              V                  i          ,          j          ,          k                          d          ,          n                    wherein Sd,n is a total radiation intensity received by detector d in collimator configuration n, andwherein Ci,j,k is an average radioisotope concentration in volume element (i, j, k). 18. A method for imaging a body, comprising:configuring a camera head to detect radiation emitted from regions in the body so as to produce sliced images of radiation intensity emitted from a three dimensional structure of the regions, the camera head comprising:a two-dimensional array of D CdZnTe (CZT) detector elements, wherein D is an integer greater than 1, the array of D detector elements being defined by two orthogonal repetition vectors and being mounted in the camera head, the elements being respectively coupled to D electrodes, each electrode being configured to output signals indicative of intensities of radiation that are incident on a given detector element, andD adjustable collimators respectively disposed, in a collimator array defined by the two orthogonal repetition vectors, in registration between the D detector elements and the body so as to define respective regions of the body from which the radiation emitted is incident on the detector elements, each of the adjustable collimators having N dimensional configurations defining different respective volumes of each of the regions, wherein N is an integer greater than 1, and wherein each of the collimators is in registration with each of the detector elements so that the emitted radiation from the body traverses the collimators to impinge on the detector elements, wherein for each collimator the respective volumes of each of the regions have a respective common axis of symmetry which is normal to the two orthogonal repetition vectors, and wherein each collimator comprises a respective different cavity which is configured to receive a liquid opaque to the radiation;positioning the camera in a location;receiving DN signals from the electrodes corresponding to the respective volumes of each collimator while the camera head is in the location and while the respective common axis of symmetry of each collimator is fixed and while the adjustable collimators are in the N different dimensional configuration;processing the signals in order to form a three dimensional image of the body comprising a number of volume elements from which the radiation is emitted, wherein the number is a function of D and N; andproducing sliced images of the three dimensional image while the two-dimensional array of CZT detector elements and the respective common axis of symmetry of each collimator are fixed with respect to the body. 19. The method according to claim 18, wherein each collimator comprises a first collimator channel aligned with a second collimator channel and separated therefrom by an adjustable gap. 20. The method according to claim 19, wherein the first collimator channel is aligned with one of the detector elements and is separated therefrom by a variable gap. 21. The method according to claim 20, and comprising adjusting at least one of the variable gap and the adjustable gap. 22. The method according to claim 19, wherein the first and second collimator channels comprise different cross-sectional areas. 23. The method according to claim 18, wherein the liquid comprises mercury. 24. The method according to claim 18, wherein each respective different cavity alters a length of each collimator on receipt of the liquid. 25. The method according to claim 18, wherein each respective different cavity comprises a respective different first cylinder and a respective different second cylinder having a different cross-section from the respective different first cylinder, and wherein on receipt of the liquid, each collimator changes from the respective different first cylinder to the respective different second cylinder. 26. The method according to claim 18, wherein the emitted radiation comprises gamma rays. 27. The method according to claim 18, and comprising generating a representation of radioisotopes in the body in response to an intensity of the radiation. 28. The method according to claim 18, wherein processing the signals comprises computing the number iteratively, so as to determine a largest number of the volume elements. 29. The method according to claim 18, wherein each respective different cavity comprises a plurality of isolated sub-compartments, each sub-compartment being independently filled with the liquid to form the N dimensional configurations, so that each respective different cavity is operative in the N dimensional configurations in non-horizontal orientations. 30. The method according to claim 18, wherein the different respective volumes comprise respective first volumes and respective second volumes, and wherein the respective first volumes include the respective second volumes. 31. The method according to claim 30, wherein the respective first volumes comprise respective first conic volumes, and wherein the respective second volumes comprise respective second conic volumes concentric with the respective first conic volumes. 32. The method according to claim 18, wherein the volume elements are uniquely identifiable by an ordered triple (i, j, k) wherein i, j, k are positive integers having respective values 1, . . . , I; 1, . . . , J; and 1, . . . , K; and wherein a number IJK of volume elements is a function of DN proportionality coefficients βi,j,kd,n for each of the volume elements, wherein d, n are positive integers respectively identifying a particular detector element and a particular configuration of the adjustable collimators, d, n having respective values 1, . . . , D; 1, . . . N, each proportionality coefficient being a ratio between the emitted radiation from a given volume element of the body and the radiation received by a given detector element for a respective collimator having a given dimensional configuration. 33. The method according to claim 32, wherein βi,j,kd,n=αi,j,kd,n·θi,j,kd,n·Vi,j,kd,n wherein:αi,j,kd,n is an attenuation factor between volume element (i, j, k) and detector d in collimator dimensional configuration n,θi,j,kd,n is a solid angle in which volume element (i, j, k) is viewed from detector d in collimator dimensional configuration n, andVi,j,kd,n is a volume fraction of volume element (i, j, k) enclosed by the body as viewed from detector d in collimator dimensional configuration n. 34. The method according to claim 33, and comprising:calculating values of βi,j,kd,n, αi,j,kd,n, θi,j,kd,n, and Vi,j,kd,n in response to geometrical relations between positions of the body, the D detector elements and the N dimensional configurations of the collimators,and wherein processing the signals comprises evaluating DN simultaneous linear equations:      S          d      ,      n        =            ∑              i        ,        j        ,        k              ⁢                  ⁢                  α                  i          ,          j          ,          k                          d          ,          n                    ·              C                  i          ,          j          ,          k                    ·              θ                  i          ,          j          ,          k                          d          ,          n                    ·              V                  i          ,          j          ,          k                          d          ,          n                    wherein Sd,n is a total radiation intensity received by detector d in collimator configuration n, andwherein Ci,j,k is an average radioisotope concentration in volume element (i, j, k).