IP Library Granted Patent US 7,626,178
Granted Patent B2
US 7,626,178 · App. 11/949,095 · Granted Dec 1, 2009

Integrated neutron-gamma radiation detector with adaptively selected gamma threshold

View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 7,626,178
App. No.
11/949,095
Granted
Dec 1, 2009
Kind
B2
Abstract

An integrated radiation detector having a pulse-mode operating photosensor optically coupled to a gamma sensing element and a neutron sensing element is disclosed. The detector includes pulse shape and processing electronics package that uses an analog to digital converter (ADC) and a charge to digital converter (QDC) to determine scintillation decay times and classify radiation interactions by radiation type. The pulse shape and processing electronics package determines a maximum gamma energy from the spectrum associated with gamma rays detected by the gamma sensing element to adaptively select a gamma threshold for the neutron sensing element. A light pulse attributed to the neutron sensing element is a valid neutron event when the amplitude of the light pulse is above the gamma threshold.

Claims (30)

1. An integrated neutron-gamma radiation detector, comprising:

a gamma sensing element;

a neutron sensing element;

a photosensor optically coupled to both the gamma sensing element and the neutron sensing element; and

pulse shape and processing electronics package coupled to the photosensor for determining a maximum gamma energy associated with the gamma sensing element,

wherein a gamma threshold for the neutron sensing element is determined from the gamma sensing element based on the maximum gamma energy present in a radiation field, and

wherein a light pulse emitted by the neutron sensing element is counted as a valid neutron event when an amplitude of the light pulse is above the gamma threshold.

2. The detector according to claim 1 , wherein the gamma sensing element comprises a sensor formed of materials comprising: a crystalline form of at least one of LaBr 3 , LaCl 3 , LaI 3 ; a solid solution of at least one of LaBr 3 , LaCl 3 , LaI 3 ; and a form of a dense, bright and fast scintillator material.

3. The detector according to claim 1 , wherein the neutron sensing element comprises a sensor formed of at least one of: LiF/ZnS, LiF/ZnS:Ag and a mixture of a Lithium based powder material comprising scintillator particles.

4. The detector according to claim 1 , wherein the photosensor comprises at least one of a photomultiplier tube, a photodiode and an avalanche photodiode.

5. The detector according to claim 1 , wherein the pulse shape and processing electronics package comprises an analog-to-digital converter (ADC) and a charge-to-digital converter (QDC), and wherein an integration time for at least one of the QDC and the ADC is selected for controlling pulse shape discrimination to account for a scintillation decay time associated with the gamma sensing element and the neutron sensing element.

6. The detector according to claim 5 , wherein an integration time for the ADC is about 50 nanoseconds.

7. The detector according to claim 5 , wherein an integration time for the QDC is about 500 nanoseconds.

8. A method for adaptively selecting a gamma threshold in an integrated neutron-gamma radiation detector, the detector comprising a gamma sensing element, a neutron sensing element, a photosensor optically coupled to the gamma sensing element and the neutron sensing element, and a pulse shape and processing electronics package coupled to the photosensor, the method comprising the steps of:

determining a maximum gamma energy associated with gamma rays detected by the gamma sensing element;

selecting a gamma threshold for the neutron sensing element based on the maximum gamma energy as determined by the gamma sensing element,

whereby a light pulse emitted by the neutron sensing element is counted as a valid neutron event when an amplitude of the light pulse is above the gamma threshold.

9. The method according to claim 8 , wherein the gamma sensing element comprises a sensor formed of materials comprising: a crystalline form of at least one of LaBr 3 , LaCl 3 , LaI 3 ; a solid solution of at least one of LaBr 3 , LaCl 3 , LaI 3 ; and a form of a dense, bright and fast scintillator material.

10. The method according to claim 8 , wherein the neutron sensing element comprises a sensor formed of at least one of: LiF/ZnS, LiF/ZnS:Ag and a mixture of a Lithium based powder material comprising scintillator particles.

11. The method according to claim 8 , wherein the photosensor comprises at least one of a photomultiplier tube, a photodiode and an avalanche photodiode.

12. The method according to claim 8 , further comprising the steps of:

determining a signal amplitude V 0 for each detected interaction;

determining a signal charge Q for each detected interaction; and

classifying each radiation interaction according to radiation type by evaluating the signal amplitude V 0 and the signal charge Q.

13. The method according to claim 12 , wherein evaluating the signal amplitude V 0 and the signal charge Q comprises forming a ratio (Q/V 0 ).

14. The method according to claim 13 , wherein the ratio provides for determining a scintillation decay time for the gamma sensing element and the neutron sensing element.

15. The method according to claim 14 , wherein a scintillation decay time for the neutron sensing element is separated from the scintillation decay time for the gamma sensing element by a factor greater than one.

16. The method according to claim 8 , wherein the pulse shape and processing electronics package comprises an analog-to-digital converter (ADC) and a charge-to-digital converter (QDC), and wherein an integration time for at least one of the QDC and the ADC is selected for controlling pulse shape discrimination to account for a scintillation decay time associated with the gamma sensing element and the neutron sensing element.

17. The method as in claim 16 , wherein an integration time for the ADC is about 50 nanoseconds.

18. The method as in claim 16 , wherein an integration time for the QDC is about 500 nanoseconds.

Assignments (3)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jan 16, 2020
From: GENERAL ELECTRIC COMPANY
To: BAKER HUGHES, A GE COMPANY, LLC
Reel/Frame 051624/0123 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 6, 2007
From: IVAN, ADRIAN; DUCLOS, STEVEN JUDE; MCDEVITT, DANIEL BRUNO; WILLIAMS, JAMES RICHARD; CLOTHIER, BRENT ALLEN; GORDON, JEFFREY SEYMOUR
To: GENERAL ELECTRIC COMPANY
Reel/Frame 020203/0828 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 3, 2007
From: IVAN, ADRIAN; DUCLOS, STEVEN JUDE; MCDEVITT, DANIEL BRUNO; WILLIAMS, JAMES RICHARD; CLOTHIER, BRENT ALLEN; GORDON, JEFFREY SEYMOUR
To: GENERAL ELECTRIC COMPANY
Reel/Frame 020185/0313 →