Unidimensional array 3-D position sensitive ionization detector

• US 20050205796A1
• Filed: 03/18/2005
• Published: 09/22/2005
• Est. Priority Date: 03/19/2004
• Status: Active Grant

• Current Assignee: Advanced Applied Physics Solutions, Inc.
• Original Assignee: Advanced Applied Physics Solutions, Inc.
• Inventors: Bryman, Douglas
• Granted Patent: US 7,518,117 B2
• Time in Patent Office: Days
• US Class Current: 250/370.110
• 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 1/204 the detector being a liquid
• CPC Class Codes: G01T 1/2935 using ionisation detectors

Abstract

The present invention provides an improved gamma ray detector module and a method of operating such a detector module for more accurately determining the position of a gamma ray interaction within the detector. The detector module includes an induction array arranged at an offset angle relative other arrays utilized in the detector, whereby the relative timing of the detection of ionization electrons by the induction array and a collector or anode indicate at least one coordinate corresponding to the location of the interaction that produced the ionization electron. This secondary locating apparatus and method supplements or replaces conventional locating apparatus and methods for improving the accuracy or reducing the complexity of the detection apparatus.

Claims

1. A method for determining the position of energetic particle interactions within a detector, the method comprising:

providing a drift medium within the detector;

allowing an energetic particle to interact with the drift medium and thereby produce ionization electrons at an interaction location;

generating an interaction signal indicating that an interaction between the energetic particle and the drift medium has occurred;

establishing a drift field within the drift medium whereby the ionization electrons are directed toward an induction array and a collector; and

detecting the ionization electrons at the induction array for determining at least one coordinate corresponding to the interaction location.

2. The method according to claim 1, wherein:

the drift medium is a scintillating liquid.

3. The method according to claim 2, wherein:

the drift 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 drift 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 induces movement of the ionization electrons through the drift medium at a drift velocity.

7. The method according to claim 1, wherein:

the drift medium is liquid xenon; and

the drift field is approximately 1 kV/cm.

8. The method according to claim 1, wherein:

the drift medium is liquid xenon; and

the drift field produces drift velocity of approximately 0.2 cm/μ

s in the ionization electrons.

9. The method according to claim 1, wherein:

the drift medium is a scintillating medium and the interaction between the energetic particle and the drift medium emits scintillation light, the scintillation light being detected by photodetectors provided around the drift medium to generate the interaction signal;

and further wherein the photodetectors are selected from a group consisting of photomultiplier tubes, position sensitive photo multipliers, photodiodes, avalanche photodiodes, hybrid photodiodes and visible light photodetectors.

10. The method of claim 1, further comprising:

providing a shield array between the interaction location and the induction array;

opening a portion of the shield array system corresponding to the first plurality of coordinates during a period of time during which the ionization electron is expected to reach the shield array, thereby selectively allowing the ionization electrons to pass through the shield array and move toward a portion of the induction array.

11. The method according to claim 10, wherein:

the portion of the shield array is opened based on an expected time of arrival of the ionization electrons at the collector as determined from the interaction signal.

12. The method of claim 9, further comprising:

collecting data from the photodetectors and the collector; and

processing the collected data off-line to calculate a three-dimensional approximation of the interaction location.

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

an active region containing a drift medium that will emit ionization electrons in response to an interaction between the drift medium and a gamma ray at an interaction location;

a device for detecting the interaction for setting an initial time in response to the interaction;

an energizable array for inducing a drift field in the drift medium, the drift field being sufficient to induce the ionization electrons to move through the drift medium at a drift velocity toward a selective shield array, an induction array and a collector, wherein the induction array is arranged in an offset alignment relative to the shield array and the collector; and

a processor for calculating at least one coordinate of the interaction location based on detection of the ionization electrons by the induction array.

14. The gamma ray detector according to claim 13, wherein:

the drift medium is a noble liquid.

15. The gamma ray detector according to claim 13, wherein:

the drift medium is a gas through which ionization electrons can be induced to move with a drift velocity of at least 0.1 cm/μ

s.

16. The gamma ray detector according to claim 13, wherein:

energizable array is biased to induce a drift field sufficient to move the ionization electrons through the drift medium at a substantially constant drift velocity.

17. The gamma ray detector according to claim 14, wherein:

the medium is liquid xenon; and

the drift velocity is about 0.2 cm/μ

s.

18. The gamma ray detector according to claim 13, wherein:

the drift medium is a scintillating medium and the device for detecting the interaction includes a plurality of photodetectors arranged around the drift medium, the photodetectors being selected from a group consisting of photo-multiplier tubes, position sensitive photo multipliers, photodiodes, avalanche photodiodes, hybrid photodiodes and visible light photodetectors.

19. The gamma ray detector according to claim 13, further comprising:

an actuation system for selectively deactivating a portion of the shield array based on a first interaction location calculated in response to detection of the interaction and the induced drift velocity of the ionization electrons, thereby allowing the ionization electrons to pass through the shield array.

20. The gamma ray detector according to claim 13, wherein:

the energizable array surrounds the shield array;

the shield array surrounds the collector, the energizable array, shield array and the collector being configured in a substantially parallel and coaxial arrangement;

the active region is an annular region between the energizable array and the shield array; and

the induction array is arranged between the shield array and the collector, elements of the induction array being arranged at an offset angle relative to the collector whereby a distance between an element of the induction array and the collector may be represented by a linear function of a z-axis position along the collector.

21. A gamma ray detector system comprising:

a plurality of gamma ray detectors according to claim 20;

the plurality of gamma ray detectors being arranged in an array within a gamma ray detector module; and

a plurality of gamma ray detector modules arranged in a predetermined pattern around a target region, wherein the target region is arranged and configured for positioning an object relative to the gamma ray detector modules.