초록

A detector module for a CT imaging system includes a scintillator to convert x-rays to optical photons. The scintillator is optically coupled to a solid-state photomultiplier with internal gain to receive the optical photons and convert them into a corresponding electrical signal output.

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What is claimed is: 1. A CT imaging system comprising: a gantry having a bore therethrough designed to receive a patient being translated through the bore; an x-ray source disposed in the gantry and configured to emit x-rays toward the patient; and a detector module disposed in the gantry to receiv

What is claimed is: 1. A CT imaging system comprising: a gantry having a bore therethrough designed to receive a patient being translated through the bore; an x-ray source disposed in the gantry and configured to emit x-rays toward the patient; and a detector module disposed in the gantry to receive x-rays attenuated by the patient, the detector module comprising: a scintillator configured to absorb the x-rays and to convert the x-rays into optical photons; and a solid-state photomultiplier (SSPM) configured to receive the optical photons and to convert the optical photons into corresponding electrical signals. 2. The CT imaging system of claim 1 wherein the scintillator comprises a material having a decay time of approximately less than 50 nanoseconds. 3. The CT imaging system of claim 2 wherein the scintillator material is a ceramic material having a decay time of approximately less than 50 nanoseconds. 4. The CT imaging system of claim 3 wherein the ceramic material comprises one of LYSO, LaBr3, and (LuxTb1-x-yCey)3Al5O12 (i.e., LuTAG), where "x" ranges from 0.5 to 1.5 and "y" ranges from 0.01 to 0.15. 5. The CT imaging system of claim 1 wherein the scintillator is a pixelated scintillator having a plurality of scintillation elements. 6. The CT imaging system of claim 5 wherein the SSPM further comprises a plurality of pixels, the pixels being coupled to the scintillation elements to receive optical photons therefrom. 7. The CT imaging system of claim 6 wherein each of the plurality of SSPM pixels further comprises: an array of microcells configured to operate in Geiger-mode and to convert the optical photons into corresponding electrical signals; and a conductive grid connected to the array of microcells, the conductive grid configured to combine the electrical charges and output a single electrical signal from the SSPM pixel. 8. The CT imaging system of claim 1 wherein the detector module further comprises readout electronics coupled to the SSPM to digitize the electrical signals output therefrom. 9. The CT imaging system of claim 8 wherein the readout electronics are configured to characterize the x-rays absorbed by the scintillator as high energy or low energy based on an intensity of the electrical signals output by the SSPM. 10. The CT imaging system of claim 8 wherein the readout electronics are configured to count x-ray photons. 11. An energy discriminating CT detector module comprising: a scintillator to receive x-rays and convert the x-rays into optical photons; and a solid-state photosensor with internal gain, the solid-state photosensor optically coupled to the scintillator to receive the optical photons therefrom and configured to convert the optical photons into an electrical signal output. 12. The energy discriminating detector module of claim 11 further comprising a data acquisition system (DAS) coupled to the solid-state photosensor, the DAS configured to receive the electrical signal output and to perform processing thereon. 13. The energy discriminating detector module of claim 12 wherein the DAS is configured to separate the x-rays into a plurality of energy bins to count photons in the x-rays, the plurality of energy bins comprising at least a high energy bin and a low energy bin. 14. The energy discriminating detector module of claim 11 wherein the solid-state photosensor further comprises at least one pixel. 15. The energy discriminating detector module of claim 14 wherein the at least one pixel further comprises a plurality of Geiger-mode avalanche photodiodes (APDs) configured to receive the optical photons from the scintillator and to produce corresponding electrical charges therefrom. 16. The energy discriminating detector module of claim 15 wherein the at least one pixel is configured to sum the electrical charges produced by the Geiger-mode APDs and generate the electrical signal output based on the sum. 17. The energy discriminating detector module of claim 16 wherein the electrical signal output is proportional to the number of Geiger-mode APDs caused to fire by the optical photons received thereby. 18. The energy discriminating detector module of claim 11 wherein the scintillator is a pixelated scintillator and comprises a material having a decay time of less than 50 nanoseconds. 19. A method for constructing a photon counting and energy discriminating, CT detector, the method comprising the steps of: forming a scintillator to receive x-rays and convert the x-rays into optical photons; and coupling a solid-state photomultiplier (SSPM) with internal gain to the scintillator to receive the optical photons and convert the optical photons into a corresponding electrical signal output. 20. The method of claim 19 further comprising the step of electrically connecting a data acquisition system (DAS) to the SSPM to receive the electrical signal output therefrom. 21. The method of claim 19 wherein forming the scintillator further comprises the step of forming the scintillator of a material having a fluorescent decay time of approximately less than 50 nanoseconds.