Photon counting type X-ray computed tomography apparatus and method for correcting scattered radiation
View Patent ↗A CT apparatus includes: a tube that produces an X-ray photon whose highest energy is higher than highest peak energy of characteristic X-rays; a detecting material; a unit that produces a first attenuation coefficient map which corresponds to a first energy region including the highest peak energy of the characteristic X-rays; a unit that transforms the first attenuation coefficient map into a second attenuation coefficient map of a second energy region; a unit that produces a scattered photon distribution of scattered X-ray photons on the basis of the second attenuation coefficient map; and a unit that produces data before reconstruction on the basis of the detected X-ray photon which corresponds to the second energy region, corrects and processes the data before reconstruction with the scattered photon distribution so as to produce corrected data, and reconstructs an image corresponding to the second energy region for which scattered radiation is corrected.
1. A photon counting type X-ray computed tomography apparatus comprising:
an X-ray tube configured to produce an X-ray photon whose highest energy is higher than highest peak energy of characteristic X-rays;
an X-ray detecting material configured to detect the X-ray photon;
an attenuation coefficient map producing unit configured to produce a first attenuation coefficient map which corresponds to a first energy region including the highest peak energy of the characteristic X-rays;
an attenuation coefficient map transforming unit configured to transform the first attenuation coefficient map into a second attenuation coefficient map of a second energy region which is different from the first energy region;
a simulation performing unit configured to perform a simulation of scattered radiation on the basis of the second attenuation coefficient map so as to produce a scattered photon distribution of scattered X-ray photons; and
an image reconstructing unit configured to produce data before reconstruction on the basis of the detected X-ray photon which corresponds to the second energy region, to correct and process the data before reconstruction with the scattered photon distribution so as to produce corrected data, and to reconstruct an image corresponding to the second energy region for which scattered radiation is corrected.
2. The photon counting type X-ray computed tomography apparatus according to claim 1 , wherein
the simulation performing unit produces the scattered photon distribution by making a plurality of X-ray photons emitted by the X-ray tube move ahead by a unit distance for calculating a scattering probability and a scattering angle and by carrying out a process for making the plural X-ray photons move ahead by a unit distance until, as a result of the calculation, the plural X-ray photons reach out of a calculation range.
3. The photon counting type X-ray computed tomography apparatus according to claim 2 , wherein
the simulation performing unit sets a threshold to energy of the X-ray photons in the simulation of scattered radiation.
4. The photon counting type X-ray computed tomography apparatus according to claim 2 , wherein
the simulation performing unit limits the number of times of scattering of the X-ray photons in the simulation of scattered radiation.
5. The photon counting type X-ray computed tomography apparatus according to claim 2 , wherein
the simulation performing unit limits a calculation range in the simulation of scattered radiation.
6. The photon counting type X-ray computed tomography apparatus according to claim 1 , wherein
the X-ray tube produces an X-ray photon in such a way that the highest energy is around the highest peak energy of the characteristic X-rays.
7. A method for correcting scattered radiation comprising:
producing an X-ray photon whose highest energy is higher than highest peak energy of characteristic X-rays from an X-ray tube;
detecting the X-ray photon by means of an X-ray detecting material;
producing a first attenuation coefficient map which corresponds to a first energy region including the highest peak energy of the characteristic X-rays;
transforming the first attenuation coefficient map into a second attenuation coefficient map of a second energy region which is different from the first energy region;
performing a simulation of scattered radiation on the basis of the second attenuation coefficient map so as to produce a scattered photon distribution of scattered X-ray photons; and
producing data before reconstruction on the basis of the detected X-ray photon which corresponds to the second energy region, correcting and processing the data before reconstruction with the scattered photon distribution so as to produce corrected data, and reconstructing an image corresponding to the second energy region for which scattered radiation is corrected.
8. The method for correcting scattered radiation according to claim 7 further comprising, for producing the scattered photon distribution:
making a plurality of X-ray photons emitted by the X-ray tube move ahead by a unit distance for calculating a scattering probability and a scattering angle; and
carrying out a process for making the plural X-ray photons move ahead by a unit distance until, as a result of the calculation, the plural X-ray photons reach out of a calculation range.
9. The method for correcting scattered radiation according to claim 8 , wherein
a threshold is set to energy of the X-ray photons in the simulation of scattered radiation.
10. The method for correcting scattered radiation according to claim 8 , wherein
the number of times of scattering of the X-ray photons is limited in the simulation of scattered radiation.
11. The method for correcting scattered radiation according to claim 8 , wherein
a calculation range is limited in the simulation of scattered radiation.
12. The method for correcting scattered radiation according to claim 7 , wherein
the X-ray tube produces an X-ray photon in such a way that the highest energy is around the highest peak energy of the characteristic X-rays.