IP Library Granted Patent US 10,271,811
Granted Patent B2
US 10,271,811 · App. 15/210,657 · Granted Apr 30, 2019

Scatter simulation with a radiative transfer equation using direct integral spherical harmonics method for computed tomography

Inventors: Yujie Lu (Vernon Hills, IL); Yu Zou (Naperville, IL); Xiaolan Wang (Buffalo Grove, IL); Zhou Yu (Wilmette, IL); Richard Thompson (Hawthorn Woods, IL)
Assignee: TOSHIBA MEDICAL SYSTEMS CORPORATION
A61B6/5282A61B6/032A61B6/483A61B6/583A61B6/4435
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Quick Facts
Patent No.
US 10,271,811
App. No.
15/210,657
Granted
Apr 30, 2019
Kind
B2
Abstract

A method and apparatus is provided to calculate scatter using a method to determine primary X-ray flux, first-scatter flux, and multiple-scatter flux using an integral formulation of a radiative transfer equation and using spherical-harmonic expansion. The integral for the primary X-ray flux does not include a spherical-harmonic expansion. The integral for the first-scatter flux includes an angle-dependent scatter cross-section. The integral for the multiple-scatter flux is performed iteratively, includes spherical harmonics, and includes a scatter cross-section expanded using Legendre polynomials. The integrals of attenuation along propagation rays can be accelerated using material decomposition of the attenuation coefficients. An anti-scatter-grid term can be included in the integrals to account for the effects of an anti-scatter grid on the fluxes prior to detection of the X-rays.

Claims (65)

1. An apparatus, comprising:

circuitry configured to

obtain projection data representing an intensity of X-ray radiation detected at a plurality of detector elements,

obtain a model of an object between an X-ray source generating the X-ray radiation and the plurality of detector elements, the model representing a spatial distribution of material components of the object,

determine, using the model and a radiative transfer equation, scattered X-ray data representing an intensity of scattered X-ray radiation detected at the plurality of detector elements, the radiative transfer equation being expressed as an integral equation including a first portion corresponding to a primary flux and a second portion corresponding to a scatter flux, the scattered X-ray data being determined by

integrating an attenuation from the X-ray source to a detection location or a first scatter location to calculate the first portion for generation of the primary flux, and

iteratively calculating a multiple-scatter flux from a first order scatter calculated based on the primary flux at the first scatter location, using position dependent cross-sections and spherical-harmonic components to calculate the second portion for generation of the scatter,

correct the projection data based on the scattered X-ray data to obtain scatter corrected projection data, and

reconstruct an image of the object from the scatter-corrected projection data; and

a display configured to display the reconstructed image of the object.

2. The apparatus according to claim 1 , wherein the circuitry is further configured to iteratively calculate the multiple-scatter flux by

iteratively updating the multiple-scatter flux, which is decomposed into a plurality of multiple-scatter spherical-harmonic components, by integrating products of respective spherical-harmonic components of a previous iteration of the multiple-scatter flux at a scatter location of the previous iteration with corresponding spherical-harmonic components of the predefined scatter cross-section at a scatter location of a next iteration to generate the multiple-scatter flux of the next iteration, wherein

the multiple-scatter flux of a first iteration is the first-scatter flux and a scatter location of the first iteration is the first scatter location.

3. The apparatus according to claim 2 , wherein the circuitry is further configured to calculate the scattered X-ray data by

the iteratively updating of the multiple-scatter flux using spherical-harmonic components of the predefined scatter cross-section that are obtained by using a Legendre polynomial to expand the predefined scatter cross-section.

4. The apparatus according to claim 2 , wherein the circuitry is further configured to calculate the scattered X-ray data by the updating of the multiple-scatter flux, including integrating an attenuation from the scatter location of the previous iteration to the scatter location of the next iteration.

5. The apparatus according to claim 1 , wherein the circuitry is further configured to calculate the scattered X-ray data by the integrating of the attenuation from the X-ray source to the detection location or the first scatter location, including a material decomposition of the attenuation into a plurality of material components.

6. The apparatus according to claim 5 , wherein the circuitry is further configured to calculate the scattered X-ray data by the integrating of the attenuation from the X-ray source to the detection location or the first scatter location, including precomputing the plurality of material attenuation components and storing the plurality of material attenuation components in a memory.

7. The apparatus according to claim 1 , wherein the circuitry is further configured to determine the predefined scatter cross-sections at respective scatter locations of the iterations of the iteratively updating of the multiple-scatter flux using corresponding scatter locations on the spatial distribution of the material components of the object represented by the model and predetermined scatter cross-sections of the material components of the object.

8. The apparatus according to claim 1 , wherein the circuitry is further configured to obtain the model of the object by

correcting scatter in the projection data using a kernel-based method to generate corrected projection data,

reconstructing a computed tomography image of the object to generate the model of the object, and

performing material decomposition to generate the material components of the object for the model.

9. The apparatus according to claim 2 , wherein the circuitry is further configured to calculate the scattered X-ray data by

correcting the first-scatter flux at the plurality of detector elements to account for an effect of an anti-scatter grid, and

correcting the multiple-scatter flux at the plurality of detector elements to account for the effect of the anti-scatter grid.

10. The apparatus according to claim 1 , further comprising:

a gantry including a rotating member;

the X-ray source radiating X-rays, the X-ray source fixed to the rotating member; and

the plurality of detector elements fixed to the rotating member and arranged diametrically opposed to the X-ray source, wherein

the obtaining of the projection data is performed by detecting, at the plurality of detector elements, X-ray radiation from the X-ray source to generate the projection data.

11. An apparatus, comprising:

circuitry configured to

obtain projection data representing an intensity of X-ray radiation detected at a plurality of detector elements,

obtain a model of an object between an X-ray source generating the X-ray radiation and the plurality of detector elements, the model representing a spatial distribution of material components of the object,

determine, using the model and a radiative transfer equation, scattered X-ray data representing an intensity of scattered X-ray radiation detected at the plurality of detector elements, the radiative transfer equation being expressed as an integral equation including a first portion corresponding to a primary flux and a second portion corresponding to a scatter flux, the scattered X-ray data being determined by

integrating an attenuation from the X-ray source to a detection location or a first scatter location to calculate the first portion for generation of the primary flux, and

iteratively calculating a multiple-scatter flux from a first order scatter calculated based on the primary flux at the first scatter location, using position dependent cross-sections and spherical-harmonic components to calculate the second portion for generation of the scatter,

correct the projection data based on the scattered X-ray data to obtain scatter-corrected projection data, and

reconstruct an image of the object from the scatter corrected projection data; and

a display configured to display the reconstructed image of the object.

12. A method, comprising:

obtaining projection data representing an intensity of X-ray radiation detected at a plurality of detector elements,

obtaining a model of an object between an X-ray source generating the X-ray radiation and the plurality of detector elements, the model representing a spatial distribution of material components of the object,

determining, using the model and a radiative transfer equation, scattered X-ray data representing an intensity of scattered X-ray radiation detected at the plurality of detector elements, the radiative transfer equation being expressed as an integral equation including a first portion corresponding to a primary flux and a second portion corresponding to a scatter flux, by integrating a radiative transfer equation, wherein the determining of the scattered X-ray data includes

integrating an attenuation from the X-ray source to a detection location or a first scatter location to calculate the first portion for generation of the primary flux, and

iteratively calculating a multiple-scatter flux from a first order scatter calculated based on the primary flux at the first scatter location, using position dependent cross-sections and spherical-harmonic components to calculate the second portion for generation of the scatter

correcting the projection data based on the scattered X-ray data to obtain scatter corrected projection data, and

reconstructing an image of the object from the scatter corrected projection data, and

displaying the reconstructed image of the object.

13. The method according to claim 12 , wherein the iteratively calculating the multiple-scatter flux includes

iteratively updating the multiple-scatter flux, which is decomposed into a plurality of multiple-scatter spherical-harmonic components, by integrating products of respective spherical-harmonic components of a previous iteration of the multiple-scatter flux at a scatter location of the previous iteration with corresponding spherical-harmonic components of the predefined scatter cross-section at a scatter location of a next iteration to generate the multiple-scatter flux of the next iteration, wherein

the multiple-scatter flux of a first iteration is the first-scatter flux and a scatter location of the first iteration is the first scatter location.

14. The method according to claim 13 , wherein the iteratively updating of the multiple-scatter flux is performed using spherical-harmonic components of the predefined scatter cross-section that are obtained by using a Legendre polynomial to expand the predefined scatter cross-section.

15. The method according to claim 13 , wherein the updating of the multiple-scatter flux includes integrating an attenuation from the scatter location of the previous iteration to the scatter location of the next iteration.

16. The method according to claim 12 , wherein the integrating of the attenuation from the X-ray source to the detection location or the first scatter location includes a material decomposition of the attenuation into a plurality of material components.

17. The method according to claim 16 , wherein the integrating of the attenuation from the X-ray source to the detection location or the first scatter location includes precomputing the plurality of material attenuation components and storing the plurality of material attenuation components in a memory.

18. The method according to claim 12 , wherein the obtaining of the model of the object further includes

correcting scatter in the projection data using a kernel-based method to generate corrected projection data,

reconstructing a computed tomography image of the object to generate the model of the object, and

performing material decomposition to generate the material components of the object for the model.

19. The method according to claim 13 , wherein the determining of the scattered X-ray data further includes

correcting the first-scatter flux at the plurality of detector elements to account for an effect of an anti-scatter grid, and

correcting the multiple-scatter flux at the plurality of detector elements to account for the effect of the anti-scatter grid.

20. A non-transitory computer readable storage medium including executable instructions, wherein the instructions, when executed by circuitry, cause the circuitry to perform the method according to claim 12 .

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 2, 2016
From: LU, YUJIE; ZOU, YU; WANG, XIAOLAN; YU, ZHOU; THOMPSON, RICHARD
To: TOSHIBA MEDICAL SYSTEMS CORPORATION
Reel/Frame 039316/0331 →
Continuity (1)
Related Publication 20180014806A1 · Jan 18, 2018