IP Library › Granted Patent US 9,437,016
Granted Patent B2
US 9,437,016 · App. 13/960,819 · Granted Sep 6, 2016

Image domain pansharpening method and system for spectral CT with large pixel energy discriminating detectors

Inventors: David Rigie (Chicago, IL); Patrick La Riviere (Chicago, IL); Adam Petschke (Lake Bluff, IL)
Assignees: Toshiba Medical Systems Corporation; The University of Chicago
G06T11/008A61B6/4241G06T3/4061G06T5/003G06T5/50G06T2207/10081G06T2207/10108G06T2210/41
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Quick Facts
Patent No.
US 9,437,016
App. No.
13/960,819
Filed
Aug 7, 2013
Granted
Sep 6, 2016
Kind
B2
Art Unit
2667
USPC
382/131
Abstract

A hybrid CT dataset is obtained from a combination of a integrating detector and a photon-counting detector. The hybrid CT dataset contains low-resolution photon-counting data and high-resolution integrating data. High-resolution panchromatic images are generated from the high-resolution integrating data, and low-resolution spectral images are generated from the low-resolution photon-counting data. The high-resolution panchromatic images inherit the resolution properties of the integrating detector while the low-resolution spectral images inherit the spectral information of the photon-counting detector. Subsequently, the low resolution spectral images are pansharpened based upon at least one high resolution panchromatic image that lacks spectral information according to a pansharpening algorithm.

Claims (32)

1. A method of improving a spectral image, comprising;

reconstructing a whole high-resolution panchromatic image based upon energy integration data from energy integrating detectors;

reconstructing at least one whole low-resolution spectral image based upon spectral energy data from photon counting detectors; and

pansharpening at least the one whole low-resolution spectral image using the whole high-resolution panchromatic image to generate a high-resolution spectral image as a pansharpened image, wherein a first flux rate of X ray entering the photon counting detectors is lower than a second flux rate of X ray entering the energy integrating detectors.

2. The method of improving a spectral image according to claim 1 further comprising an additional steps of:

acquiring the energy integration data at the energy integrating detectors having a second detector element size;

acquiring the spectral energy data at the photon counting detectors having a first detector element size that is larger than the second detector element size.

3. The method of improving a spectral image according to claim 2 wherein said acquiring the spectral energy data and said acquiring the energy integration data utilize two separate sources.

4. The method of improving a spectral image according to claim 1 further comprising an additional step of iteratively reconstructing an image using the high-resolution spectral image as a seed image.

5. The method of improving a spectral image according to claim 1 wherein said pansharpening uses a predetermined algorithm as described by

E (ƒ i )=λ 1 ∫ Ω ∥∇ƒ i −α(∇ I pam )∥ 2 dxdy+λ 2 ∫ Ω (ƒ i −M i ) 2 dxdy

where I pan is the panchromatic image, M i is i'th channel of the whole low-resolution spectral image, f i is the i'th channel of the pansharpened image, E is minimizing energy functional, λ 1 is predetermined first coefficient value for weighing the gradient matching term for resolution recovery, λ 2 is predetermined second coefficient value for keeping gray level faithful, Ω just means the area to integrate over, ∇ is gradient, dx is a location along a predetermined x axis, dy is a location along a predetermined y axis.

6. A system for improving a spectral image, comprising;

energy integrating detectors for acquiring energy integration data;

photon counting detectors for acquiring spectral energy data;

a data storing unit for storing the energy integration data and the spectral energy data, wherein a first flux rate of X ray entering said photon counting detectors is lower than a second flux rate of X ray entering said energy integrating detectors;

an image reconstruction unit connected to said data storing unit for reconstructing a high-resolution panchromatic image from the energy integration data and reconstructing at least one whole low-resolution spectral image from the spectral energy data; and

an image pansharpening unit connected to said image reconstruction unit for pansharpening the whole low-resolution spectral image using the whole high-resolution panchromatic image to generate at least one high-resolution spectral image.

7. The system for improving a spectral image according to claim 6 wherein said photon counting detectors have a first detector element size that is smaller than a second detector element size of said energy integrating detectors, the first detector element size being effectively combined to have a third element size that is larger than the second detector element size.

8. The system for improving a spectral image according to claim 6 wherein said photon counting detectors have a first detector element size that is larger than a second detector element size of said energy integrating detectors.

9. The system for improving a spectral image according to claim 6 further comprising a first source for said photon counting detectors and a second source for energy integration detectors.

10. The system for improving a spectral image according to claim 9 wherein said first source and said second source are located at a predetermined angle along the predetermined trajectory.

11. The system for improving a spectral image according to claim 6 wherein said image reconstruction unit iteratively reconstructs an image using the whole high-resolution spectral image as a seed image.

12. The system for improving a spectral image according to claim 6 wherein said image pansharpening unit for pansharpening according to a predetermined algorithm as described by

E (ƒ i )=λ 1 ∫ Ω ∥∇ƒ i −α(∇ I pam )∥ 2 dxdy+λ 2 ∫ Ω (ƒ i −M i ) 2 dxdy

where I pan is the panchromatic image, M i is i'th channel of the whole low-resolution spectral image, f i is the i'th channel of the pansharpened image, E is minimizing energy functional, λ 1 is predetermined first coefficient value for weighing the gradient matching term for resolution recovery, λ 2 is predetermined second coefficient value for keeping gray level faithful, Ω just means the area to integrate over, ∇ is gradient, dx is a location along a predetermined x axis, dy is a location along a predetermined y axis.

13. A system for improving a spectral image, comprising;

energy integrating detectors in a first predetermined detector size for acquiring energy integration data;

photon counting detectors in with a second predetermined detector size with thick anti-scatter grids for acquiring spectral energy data, the second predetermined detector size being substantially larger than the first predetermined detector size, wherein a first flux rate of X ray entering said photon counting detectors is lower than a second flux rate of X ray entering said energy integrating detectors;

a data storing unit for storing the energy integration data and the spectral energy data;

an image reconstruction unit connected to said data storing unit for reconstructing a whole high-resolution panchromatic image from the energy integration data and reconstructing at least one whole low-resolution spectral image from the spectral energy data; and

an image pansharpening unit connected to said image reconstruction unit for pansharpening the whole low-resolution spectral image using the whole high-resolution panchromatic image to generate at least one high-resolution spectral image.

Assignments (5)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 24, 2014
From: TOSHIBA MEDICAL SYSTEMS CORPORATION
To: CHICAGO, THE UNIVERSITY OF; TOSHIBA MEDICAL SYSTEMS CORPORATION
Reel/Frame 034249/0754 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 13, 2014
From: THE UNIVERSITY OF CHICAGO
To: TOSHIBA MEDICAL SYSTEMS CORPORATION; THE UNIVERSITY OF CHICAGO
Reel/Frame 033938/0041 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 13, 2014
From: PETSCHKE, ADAM
To: TOSHIBA MEDICAL SYSTEMS CORPORATION
Reel/Frame 032876/0127 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 13, 2014
From: RIGIE, DAVID; RIVIERE, PATRICK LA
To: CHICAGO, THE UNIVERSITY OF
Reel/Frame 032876/0324 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 9, 2013
From: RIGIE, DAVID; RIVIERE, PATRICK LA; PETSCHKE, ADAM
To: THE UNIVERSITY OF CHICAGO; TOSHIBA MEDICAL SYSTEMS CORPORATION
Reel/Frame 031165/0552 →
Continuity (1)
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