Phantom, radiographic imaging device, and calibration method for photon counting detector

1. A phantom used in acquisition of calibration data for a photon counting detector that outputs an electric signal based on photon energy of incident radiation,

the phantom comprising a first basis material,

wherein the first basis material varies in thickness in a stepwise fashion in a direction perpendicular to a radiation field of the radiation, and

wherein the phantom includes a plurality of elliptic cylinders stacked one on another, each cylinder comprising the first basis material, and the plurality of elliptic cylinders varying in length along a minor axis of each elliptic cylinder.

2. The phantom according to claim 1 , wherein when N is the number of steps in the direction perpendicular to the radiation field, an i-th ellipse from one end of the direction perpendicular to the radiation field has a minor axis with a length that is i/N times a length of a major axis thereof.

3. The phantom according to 1, wherein the first basis material is moved in the direction perpendicular to the radiation field.

4. A radiographic imaging device, comprising:

a photon counting detector that outputs an electric signal based on photon energy of incident radiation; and

a storage for storing calibration data acquired using the phantom according to claim 1 .

5. The phantom according to claim 1 , wherein when N is the number of steps in the direction perpendicular to the radiation field, in an i-th step from one end of the direction perpendicular to the radiation field, a thickness of the first basis material in a direction in which the radiation passes through the first basis material is i/N times a length in which the radiation passes through the radiation filed.

6. The phantom according to claim 5 , wherein a center of the thickness of the first basis material in the direction in which the radiation passes through the first basis material passes through a contact point between the radiation field and a tangent to the radiation field passing through a focal point of the radiation, and creates an arc that is centered around the focal point.

7. A phantom used in acquisition of calibration data for a photon counting detector that outputs an electric signal based on photon energy of incident radiation, the phantom comprising a first basis material,

wherein the first basis material varies in thickness in a stepwise fashion in a direction perpendicular to a radiation field of the radiation, and in each step, the step decreases in thickness with distance from a center of the radiation field in a direction of arrangement of detection elements of the photon counting detector, and

wherein when N is the number of steps in the direction perpendicular to the radiation field, in an i-th step from one end of the direction perpendicular to the radiation field, a thickness of the first basis material in a direction in which the radiation passes through the first basis material is i/N times a length in which the radiation passes through the radiation field.

8. The phantom according to claim 7 , wherein a center of the thickness of the first basis material in the direction in which the radiation passes through the first basis material passes through a contact point between the radiation field and a tangent to the radiation field passing through a focal point of the radiation, and creates an arc that is centered around the focal point.

9. A method for calibrating a photon counting detector that outputs an electric signal based on photon energy of incident radiation, the method comprising the step of acquiring calibration data for the photon counting detector by using a phantom that includes a first basis material varying in thickness in a stepwise fashion in a direction perpendicular to a radiation field of the radiation and, in each step, the step decreasing in thickness with distance from a center of the radiation field in a direction of arrangement of detection elements of the photon counting detector,

when N is the number of steps in the direction perpendicular to the radiation field, in an i-th step from one end of the direction perpendicular to the radiation field, a thickness of the first basis material in a direction in which the radiation passes through the first basis material is i/N times a length in which the radiation passes through the radiation field.

10. The method according to claim 9 , wherein a center of the thickness of the first basis material in the direction in which the radiation passes through the first basis material passes through a contact point between the radiation field and a tangent to the radiation field passing through a focal point of the radiation, and creates an arc that is centered around the focal point.

11. The method according to claim 9 , further comprising:

moving the first basis material in the direction perpendicular to the radiation field.

12. The method according to claim 9 , wherein

a cross section shape of the first basis material in the radiation field is an ellipse with a minor axis extending along radiation passing though the center of the radiation field,

the minor axis varies in length from one step to another in the direction perpendicular to the radiation field, and

the ellipse has a major axis equal in length in all steps in the direction perpendicular to the radiation field.

13. The method according to claim 12 , wherein when N is the number of steps in the direction perpendicular to the radiation field, an i-th ellipse from one end of the direction perpendicular to the radiation field has a minor axis with a length that is i/N times a length of a major axis thereof.