IP Library Granted Patent US 9,835,741
Granted Patent B1
US 9,835,741 · App. 14/327,438 · Granted Dec 5, 2017

Single volume fission energy neutron detector

Inventors: Erik Brubaker (Oakland, CA); Peter Marleau (Dublin, CA)
Assignee: National Technology & Engineering Solutions of Sandia, LLC
G01T3/06G01T3/08
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Quick Facts
Patent No.
US 9,835,741
App. No.
14/327,438
Granted
Dec 5, 2017
Kind
B1
Abstract

A single volume fission energy neutron detector is described herein. The detector includes a single volume of scintillator. A photodetector is positioned adjacent to a surface of the scintillator, wherein the photodetector has relatively small spatial resolution corresponding thereto and relatively small temporal resolution corresponding thereto. Based upon values read out from detection bins of the photodetector, kinematics of a neutron that interacted with scintillating material of the scintillator are reconstructed. Based upon the kinematics (of the neutron and other detected neutrons), a location of material from which the neutron was emitted is ascertained, and an image of the material is generated.

Claims (38)

1. A single volume fission energy neutron detection system, the system comprising:

a scintillator block;

a photodetector, wherein the photodetector is located adjacent to the scintillator block, the photodetector comprises:

detection bins; and

a readout circuit that reads respective values from the position bins; and

a computing system that is configured to estimate kinematics of a neutron that has interacted with scintillating material of the scintillator block at least twice, the computing system estimates the kinematics of the neutron based upon the respective values from the detection bins read out by the readout circuit, the kinematics of the neutron indicative of:

a type of material of a target from which the neutron was emitted; and

a location of the target relative to the scintillator block.

2. The system of claim 1 , the computing system is further configured to output data that identifies the type of the material of the target based upon the kinematics of the neutron.

3. The system of claim 1 , the computing system is further configured to generate an image of the target based upon the kinematics of the neutron.

4. The system of claim 1 , the readout circuit is configured to readout values from detection bins at a time resolution of between 35 picoseconds and 2 nanoseconds.

5. The system of claim 1 , the scintillator block comprises an organic scintillator.

6. The system of claim 1 , wherein the computing system is configured to estimate locations of interactions of the neutron in the scintillator block based upon the values from the detection bins read out by the readout circuit, the computing system configured to estimate the kinematics of the neutron based upon the locations of the interactions of the neutron in the scintillator block.

7. The system of claim 1 , wherein the computing system is configured to estimate times of interactions of the neutron in the scintillator block based upon the values from the detection bins read out by the readout circuit, the computing system configured to estimate the kinematics of the neutron based upon the times of the interactions of the neutron in the scintillator block.

8. The system of claim 1 , wherein resolution of the detection bins is between about 1 mm×1 mm and about 1 cm×1 cm.

9. The system of claim 1 , wherein the computing system is configured to execute a maximum likelihood fit algorithm to estimate the kinematics of the neutron.

10. The system of claim 1 , wherein the computing system disambiguates between gamma interactions and neutron interactions based upon the values read from the detection bins by the readout circuit.

11. The system of claim 1 , further comprising at least one other photodetector, the at least one other photodetector positioned orthogonal to the photodetector.

12. The system of claim 1 , further comprising at least one other photodetector, the at least one other photodetector positioned on an opposing side of the scintillator block from the photodetector.

13. A method executed by a computing system, the method comprising:

receiving data from a photodetector;

estimating, by a processor, respective locations of interactions of a neutron in a scintillator block based upon the data received from the photodetector, wherein the scintillator is located adjacent to the photodetector; and

estimating, by the processor, kinematics of the neutron based upon the estimated location of interactions of the neutron in the scintillator block, wherein the kinematics of the neutron are indicative of:

a type of material of a target from which the neutron was emitted; and

a location of the target relative to the scintillator block.

14. The method of claim 13 , further comprising:

estimating respective times of the interactions of the neutron in the scintillator block based upon the data received from the photodetector; and

estimating the kinematics of the neutron based upon the estimated times of the interactions of the neutron in the scintillator block.

15. The method of claim 14 , wherein the data received from the photodetector comprises first data pertaining to a first interaction between the neutron and the scintillator block and second data pertaining to a second interaction between the neutron and the scintillator block, and further wherein estimating the kinematics of the neutron comprises:

estimating a velocity of the neutron between the first interaction and the second interaction based upon a first location of the first interaction and a second location of the second interaction and a first time of the first interaction and a second time of the second interaction, wherein the first time and first location of the first interaction are determined based upon a first volume of photons captured by a plurality of detection bins included in the photodetector and the second time and second location of the second interaction are determined based upon a second volume of photons captured by the plurality of detection bins included in the photodetector.

16. The method of claim 15 , further comprising identifying the type of material of the target based upon the velocity of the neutron between the first interaction and the second interaction in the scintillator block.

17. The method of claim 13 , further comprising:

generating an image that is indicative of a location of the target from which the neutron was emitted.

18. The method of claim 13 , wherein a maximum likelihood fit algorithm is used to estimate the locations of the interactions.

19. The method of claim 13 , where coded aperture imaging is used to estimate the locations of the interactions.

20. A computer-readable storage medium comprising instructions that, when executed by a processor, cause the processor to perform acts comprising:

receiving data from a photodetector that is adjacent to a surface of a scintillator block; and

reconstructing kinematics of a neutron that interacted multiple times with scintillating material in the scintillator block, the reconstructing based upon the data received from the photodetector, the kinematics indicative of a location of a material from which the neutron was emitted.

Assignments (4)
CHANGE OF NAME Recorded Oct 10, 2017
From: SANDIA CORPORATION
To: NATIONAL TECHNOLOGY & ENGINEERING SOLUTIONS OF SANDIA, LLC
Reel/Frame 044217/0346 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Aug 10, 2015
From: BRUBAKER, ERIK; MARLEAU, PETER
To: SANDIA CORPORATION
Reel/Frame 036291/0852 →
CONFIRMATORY LICENSE Recorded Mar 26, 2015
From: SANDIA CORPORATION
To: U.S. DEPARTMENT OF ENERGY
Reel/Frame 035258/0815 →
CONFIRMATORY LICENSE Recorded Mar 26, 2015
From: SANDIA CORPORATION
To: U.S. DEPARTMENT OF ENERGY
Reel/Frame 035259/0604 →