Position calculation and energy correction in the digital scintillation camera

• US 5,576,547 A
• Filed: 12/23/1994
• Issued: 11/19/1996
• Est. Priority Date: 07/27/1993
• Status: Expired due to Term

• Current Assignee: Triumph State Bank (Trimont Bancorporation)
• Original Assignee: Park Medical Systems Incorporated
• Inventors: Ferreira, Abel, Lucic, Miljenko, Bartulovic, Vuk
• Primary Examiner(s): Willis, Davis L.
• Assistant Examiner(s): HANIG, RICHARD E
• Application Number:
  US08/362,900
• Time in Patent Office: 697 Days
• Field of Search: 250/369, 250/363.09, 250/363.07, 250/252.1
• US Class Current: 250/369
• CPC Class Codes: G01T 1/1642 using a scintillation crystal and position sensing photodetector arrays, e.g. ANGER cameras
• CPC Class Codes: G01T 1/208 Circuits specially adapted for scintillation detectors, e.g. for the photo-multiplier section
• CPC Class Codes: G01T 1/40 Stabilisation of spectrometers

Abstract

For accurate position calculation of scintillation events in a gamma camera, photodetector signals are processed based on small groups of photodetectors surrounding the scintillations. Relative position correction and energy correction is carried out based on rough position values relative to the group of photodetectors, taking into consideration the number of the center photodetector and the sum of all photodetector signals in the group.

Claims

1. A method of producing a position value signal in a scintillation camera having a scintillator, light detectors optically coupled to said scintillator for producing light detector signals, the method comprising the steps of:

(a) determining from said light detector signals a center light detector receiving a maximum amount of light from a scintillation;

(b) selecting a group of light detectors surrounding said center light detector;

(c) calculating based on values from said group of surrounding light detectors a relative coordinate of a scintillation relative to said center light detector;

(d) providing a transformation value table for a matrix of positions of scintillations within a scope of each of said center light detectors; and

(e) transforming said relative coordinate of said scintillation using one of said transformation values from said table, said one of said transformation values having a position in said matrix corresponding to said coordinates, to obtain a value for generating said position value signal.

2. The method as claimed in claim 1, further comprising the step of adding a base coordinate of said center light detector to said position value signal to obtain a global position value signal.

3. The method as claimed in claim 1, wherein said step (d) comprises the steps of acquiring scintillation data using a structured phantom in front of said camera to obtain point position data for a known structure fixed array, and generating said transformation values based on distortion values of said position data corresponding to points of said array surrounding each position in said matrix as well as distances between each position in said matrix and the surrounding points of said array.

4. The method as claimed in claim 3, wherein said step (d) further comprises the steps of acquiring flood image intensity data, and adding to said transformation values a uniformity factor calculated based on a local gradient of said intensity data such that said transformation values also help to displace scintillation position value signals from bright spots to dimmer spots to reduce intensity anomalies in an image based on said position values.

5. The method as claimed in claim 4, further comprising the step of adding a base coordinate of said center light detector to said position value signal to obtain a global position value signal.

6. The method as claimed in claim 1, wherein said step (d) comprises the steps of acquiring flood image intensity data, and generating said transformation values based on a local gradient of said intensity data such that said transformation values help to displace scintillation position value signals from bright spots to dimmer spots to reduce intensity anomalies in an image based on said position values.

7. The method as claimed in claim 1, wherein said step (d) comprises providing a transformation value table for a plurality of scintillation energies for a matrix of positions of scintillations within a scope of each of said center light detectors, and said step (e) comprises transforming said relative coordinate of said scintillation using an interpolated value of two of said transformation values having a position in said matrix corresponding to said coordinates and relating to energies proximate an expected energy of said scintillation, to obtain a value for generating said position value signal.

8. The method as claimed in claim 5, wherein said step (d) comprises providing a transformation value table for a plurality of scintillation energies for a matrix of positions of scintillations within a scope of each of said center light detectors, and said step (e) comprises transforming said relative coordinate of said scintillation using an interpolated value of two of said transformation values having a position in said matrix corresponding to said coordinates and relating to energies proximate an expected energy of said scintillation, to obtain a value for generating said position value signal.

9. The method as claimed in claim 1, wherein said step (a) comprises randomly choosing between one of said light detectors receiving a maximum amount of light from a scintillation and neighbouring ones of said light detectors receiving almost as much light as said maximum amount, whereby scintillations occurring near a boundary between two or more of said light detectors will have a randomly selected center light detector yielding a gradual overlap from one tiled image to the other.

10. The method as claimed in claim 9, wherein said random selection is achieved by adding a small random variance to one of said light detector signals associated with said center photodetector signal for the purposes of determining whether said small random variance changes said determination of said center light detector, said small random variance ranging from a small negative value to a small positive value.

11. A method of producing and filtering a position value signal in a scintillation camera having a scintillator, light detectors optically coupled to said scintillator for producing light detector signals, the method comprising the steps of:

(a) determining from said light detector signals a center light detector receiving a maximum amount of light from a scintillation;

(b) selecting a group of light detectors surrounding said center light detector;

(c) calculating based on values from said group of surrounding light detectors relative coordinates of a scintillation relative to said center light detector;

(d) calculating a sum of said light detector signals from said group of surrounding light detectors and from said center light detector;

(e) providing an energy correction value table for a matrix of positions of scintillations within a scope of each of said center light detectors;

(f) applying one of said correction values to said sum to obtain a corrected energy sum value, said one of said correction values having a position in said matrix corresponding to said coordinate of said scintillation; and

(g) filtering said relative coordinates for each scintillation based on said corrected energy sum value.

12. The method as claimed in claim 11, wherein said step (e) comprises the steps of acquiring scintillation data with a gamma ray source of known energy without use of phantoms or collimators to obtain a statistically large number of scintillation data for each position within said matrix, recording the energy of said scintillation data for each said position in the form of an energy histogram, and computing said energy correction value for said matrix using said histograms.

13. The method as claimed in claim 11, wherein said step (a) comprises randomly choosing between one of said light detectors receiving a maximum amount of light from a scintillation and neighbouring ones of said light detectors receiving almost as much light as said maximum amount, whereby scintillations occurring near a boundary between two or more of said light detectors will have a randomly selected center light detector yielding a gradual overlap from one tiled image to the other.

14. The method as claimed in claim 11, wherein said random selection is achieved by adding a small random variance to one of said light detector signals associated with said center photodetector signal for the purposes of determining whether said small random variance changes said determination of said center light detector, said small random variance ranging from a small negative value to a small positive value.