Sensor fusion with muon detector arrays to augment tomographic imaging using ambient cosmic rays

Patent metadata

Field	Value
Publication number	US-9939537-B2
Application number	US-201615065638-A
Country	US
Kind code	B2
Filing date	Mar 9, 2016
Priority date	Mar 10, 2015
Publication date	Apr 10, 2018
Grant date	Apr 10, 2018

Abstract

Techniques, systems and apparatus are described for operating a multimode passive detection system (MMPDS). A multimode passive detection system includes charged particle tracking detectors to measure cosmic ray-based charged particle trajectories in a volume of interest. The multimode passive detection system includes fission product detectors to detect cosmic ray-based charged particle induced fission in a fissile material present in the volume of interest.

First claim

What is claimed is:

1. A multimode passive detection system, comprising:
charged particle tracking detectors to measure cosmic ray-based charged particle trajectories in a volume of interest;
fission product detectors to detect cosmic ray-based charged particle induced fission in a fissile material present in the volume of interest;
a conditioning circuitry electrically coupled to the charged particle tracking detectors to detect pulses from the charged particle tracking detectors, wherein the pulses correspond to passage of the cosmic ray-based charged particle through the charged particle tracking detectors;
the conditioning circuitry comprising a time to digital converter including a processor and a memory having instructions stored thereupon, wherein the instructions upon execution by the processor configures the time to digital converter to:
generate timing information associated with pulses detected by the conditioning circuitry; and
dynamically adjust threshold levels to improve detection of pulses corresponding to passage of the cosmic ray-based charged particle through the charged particle tracking detectors.

2. The system of claim 1 , wherein the charged particle tracking detectors include drift tubes.

3. The system of claim 1 , wherein the charged particle tracking detectors are configured to detect muons.

4. The system of claim 3 , wherein the fission product detectors include neutron detectors to detect neutron produced when muons interact with the nucleus of the fissile material.

5. The system of claim 4 , wherein the fission product detectors include spectroscopic gamma detectors to detect gamma rays emitted when muons interact with the nucleus of the fissile material.

6. The system of claim 1 , comprising:
a data merger for merging signals from the charged particle tracking detectors and the fission product detectors into a data stream.

7. The system of claim 1 , comprising:
a data processing system to analyze signals from the charged particle tracking detectors and the fission product detectors and to identify the fissile material in the volume of interest as a special nuclear material.

8. The system of claim 7 , wherein the special nuclear material includes fissionable 235 Uranium and 239 Plutonium.

9. The system of claim 1 , wherein the charged particle tracking detectors and the fission product detectors are integrated into a single detection system.

10. The system of claim 1 , further including at least two mobile platforms positioned to support the charged particle tracking detectors and the fission product detectors, and to enable mobile deployment of the multimode passive detection system.

11. The system of claim 10 , wherein the at least two mobile platforms are adjustable in at least two planes.

12. A method of performing cosmic ray based tomographic imaging, the method comprising:
measuring, by charged particle tracking detectors, trajectories of cosmic ray-based charged particles entering and exiting a volume of interest;
detecting, by fission product detectors, cosmic ray-based charged particle induced fission in a fissile material present in the volume of interest;
detecting, using a conditioning circuitry, pulses from the charged particle tracking detectors, wherein the pulses correspond to passage of the cosmic ray-based charged particles through the charged particle tracking detectors;
generate, using a time to digital converter, timing information associated with pulses detected by the conditioning circuitry; and
dynamically adjusting threshold levels to improve detection of pulses corresponding to passage of the cosmic ray-based charged particles through the charged particle tracking detectors.

13. The method of claim 12 , wherein the measuring is performed by the charged particle tracking detectors that include drift tubes.

14. The method of claim 12 , wherein the measuring includes measuring trajectories of the cosmic ray-based charged particles that enter and stop in the fissile material present in the volume of interest.

15. The method of claim 12 , wherein the measuring includes measuring trajectories of the cosmic ray-based charged particles that include negatively charged muons.

16. The method of claim 15 , wherein the detecting includes using the fission product detectors that include neutron detectors to detect neutrons from the nuclear chain reaction generated initiated when muons induce a fission in the nucleus of the fissile material.

17. The method of claim 16 , wherein the detecting includes using the fission product detectors that include gamma detectors to detect gammas emitted by muon induced fission.

18. The method of claim 12 , comprising:
merging, by a data merger, signals from the charged particle tracking detectors and the fission product detectors into a data stream.

19. The method of claim 12 , comprising:
analyzing, by a data processing system, signals from the charged particle tracking detectors and the fission product detectors to identify the fissile material in the volume of interest as a special nuclear material.

20. The method of claim 19 , wherein the special nuclear material includes fissionable 235 Uranium and 239 Plutonium.

21. A portable multi-detection mode system, comprising:
a mobile platform comprising a plurality of sections movable to be positioned at different sides of an object under suspicion;
a set of charged particle detectors supported by the mobile platform such that at least one charged particle detector is positioned two of the sections of the mobile platform;
one or both of the following detector sets:
(a) a set of fast neutron detectors positioned at different sides of the object under suspicion, or
(b) a set of gamma ray detectors positioned at different sides of the object under suspicion;

detector electronic circuitry coupled to the set of charged particle detectors, and to the set of fast neutron detectors or the set of gamma ray detectors to produce electrical responses corresponding to detected charged particles, neutrons or gamma rays, the detector electronic circuitry further configured to detect pulses from the set of charged particle detectors, wherein the pulses correspond to passage of a cosmic ray-based charged particle through the set of charged particle detectors;
the detector electronic circuitry further comprising a time to digital converter including a processor and a memory having instructions stored thereupon, wherein the instructions upon execution by the processor configures the time to digital converter to:
generate timing information associated with pulses detected by the conditioning circuitry; and
dynamically adjust threshold levels to improve detection of pulses corresponding to passage of the cosmic ray-based charged particle through the set of charged particle detectors.

Assignees

• Decision Sciences Int Corp

Inventors

• Sossong Michael James

Classifications

• G01T1/167

  Measuring radioactive content of objects, e.g. contamination (whole body counters G01T1/163) · CPC title

• G01V5/0075

  Physics · mapped topic

• G01T3/008 Primary

  using an ionisation chamber filled with a gas, liquid or solid, e.g. frozen liquid, dielectric (G01T3/006 takes precedence) · CPC title

• G01V5/26

  Passive interrogation, i.e. by measuring radiation emitted by objects or goods · CPC title