High resolution 3-D position sensitive detector for gamma rays

• US 6,770,884 B2
• Filed: 07/11/2002
• Issued: 08/03/2004
• Est. Priority Date: 07/11/2002
• Status: Expired due to Fees

• Current Assignee: Advanced Applied Physics Solutions, Inc.
• Original Assignee: TRIUMF
• Inventors: Bryman, Douglas
• Primary Examiner(s): GAGLIARDI, ALBERT J
• Application Number:
  US10/192,614
• Publication Number:
  US 20040007670A1
• Time in Patent Office: 754 Days
• Field of Search: 250/366, 250/369, 250/370.11, 250/370.1, 250/361.R, 250/389
• US Class Current: 250/366
• CPC Class Codes: G01T 1/1603 with a combination of at least two different types of detector see provisionally also G01T1/16
• CPC Class Codes: G01T 1/2914 Measurement of spatial distribution of radiation
• CPC Class Codes: G01T 1/2935 using ionisation detectors
• CPC Class Codes: G01T 1/2978 Hybrid imaging systems, e.g. using a position sensitive detector (camera) to determine the distribution in one direction and using mechanical movement of the detector or the subject in the other direction or using a camera to determine the distribution in two dimensions and using movement of the camera or the subject to increase the field of view G01T1/2985 takes precedence

Abstract

A method and apparatus for determining the position of a gamma ray interaction are disclosed. A medium that emits light in response to an interaction between a gamma ray and the medium is provided. A plurality of photodetectors is used to detect the light and determine a first three-dimensional position of the interaction. A field is produced in the medium that dire ionization electrons resulting from the interaction to a collector. A portion of a shutter system that corresponds to the interaction is opened. The shutter selectively blocks and permits the passage of the ionization electrons to the collector. A second three-dimensional position of the interaction is determined by localizing a two-dimensional position of the interaction in the collector and determining a third dimension based on a time of arrival of the ionization electrons relative to when the light is detected.

Claims

1. A method for determining the position of a gamma ray interactions, the method comprising:

emitting light in a medium in response to an interaction between a gamma ray and the medium;

determining when light has been emitted from the medium and a first three-dimensional position of the interaction using a plurality of photodetectors;

producing a drift field in the medium that directs ionization electrons resulting from the interaction to a collector; and

determining a second three dimensional position of the interaction by localizing the position of the interaction in two dimensions in the collector based on a position of the ionization electrons collected in the collector and determining a third dimension based on a time of arrival of the ionization electrons relative to when the light is detected.

2. The method according to claim 1, wherein the medium is a liquid.

3. The method according to claim 2, where the medium is at least one of liquid xenon (Xe), liquid krypton (Kr) and liquid argon (Ar).

4. The method according to claim 1, wherein the medium is a noble gas.

5. The method according to claim 1, wherein the collector comprises a two-dimensional collection electrode array.

6. The method according to claim 1, wherein the drift field is established to provide a constant velocity in the medium.

7. The method according to claim 6, wherein the medium is liquid xenon and the drift field set to 1 kV/cm causing the ionization electrons to drift at a speed of 0.2 cm/μ

s.

8. The method according to claim 1, wherein the photodetectors are at least one of photo-multiplier tubes, position sensitive photo multipliers, photodiodes, avalanche photodiodes, hybrid photodiodes, and visible light photodetectors.

9. The method of claim 1, further comprising:

opening a portion of a shutter system that corresponds to an approximate position of the interaction and an approximate time of arrival of the ionization electrons, wherein the shutter system selectively blocks and permits the passage of the ionization electrons to the collector.

10. The method according to claim 9, wherein the portion of the shutter system is opened based on an expected time of arrival of the ionization electrons at the collector.

11. The method of claim 1, further comprising:

collecting data from the plurality of photodetectors and the collector; and

processing the data off-line to determine the second three-dimensional position of the interaction.

12. The method according to claim 1, wherein a distribution of the light detected by the plurality of photodetectors is used to determine the first three-dimensional position.

13. The method according to claim 1, wherein a difference of times at which the light arrives at the plurality of photodetectors is used to determine the first three-dimensional position.

14. The method according to claim 1, wherein a distribution of the light detected by the plurality of photodetectors and a difference of times at which the light arrives at the plurality of photodetectors are used to determine the first three-dimensional position.

15. A gamma ray detector for determining the position of gamma ray interaction, the detector comprising:

an active region containing a medium for emitting light and ionization electrons in response to an interaction between a gamma ray and the medium;

a plurality of photodetectors to determine when light has been emitted from the medium and a first three-dimensional position of the interaction;

a collector that is used to determine a second three-dimensional position of the interaction by localizing the position of the interaction in two dimensions in the collector based on a position of the ionization electrons collected in the collector and a third dimension based on a time of arrival of the ionization electrons relative to when the light is detected; and

a plurality of field wires to produce a drift field in the medium that directs the ionization electrons resulting from the interaction to the collector.

16. The gamma ray detector according to claim 15, wherein the medium is a liquid.

17. The gamma ray detector according to claim 16, wherein the medium is at least one of liquid xenon (Xe), liquid krypton (Kr) and liquid argon.

18. The gamma ray detector according to claim 15, wherein the medium is a noble gas.

19. The gamma ray detector according to claim 15, wherein the drift field is established to provide a constant velocity in the medium.

20. The gamma ray detector according to claim 19, wherein the medium is liquid xenon and the drift field set to 1 kV/cm causing the ionization electrons to drift at a speed of 0.2 cm/μ

s.

21. The gamma ray detector according to claim 15, wherein the photodetectors are at least one of photo-multiplier tubes, position sensitive photo multipliers, photodiodes, avalanche photodiodes, hybrid photodiodes, and visible light photodetectors.

22. The gamma ray detector according to claim 15, further comprising:

a shutter system that selectively blocks and permits the passage of the ionization electrons to the collector, wherein a portion of the shutter system corresponding to an approximate position of the interaction in two dimensions and an approximate time of arrival of the ionization corresponding to the third dimension is opened to allow the ionization electrons to pass to the collector; and

a triggering system that determines the portion of the shutter system that is opened and a time period that the shutter is opened based on light signals detected by the plurality of the photodetectors.

23. The gamma ray detector according to claim 15, wherein the collector comprises a two-dimensional collection electrode array that localizes the position of the interaction in the two dimensions.

24. The gamma ray detector according to claim 15, further comprising:

a processor that collects data from the plurality of photodetectors and the collector and processes the data off-line to determine the second three-dimensional position of the interaction.

25. The gamma ray detector according to claim 15, wherein a distribution of the light detected by the plurality of photodetectors is used to determine the first three-dimensional position.

26. The gamma ray detector according to claim 15, wherein a difference of times at which the light arrives at the plurality of photodetectors is used to determine the first three-dimensional position.

27. The gamma ray detector according to claim 15, wherein a distribution of the light detected by the plurality of photodetectors and a difference of times at which the light arrives at the plurality of photodetectors are used to determine the first three-dimensional position.