Methods and systems for time-of-flight neutron interrogation for material discrimination

• US 9,123,519 B2
• Filed: 05/31/2013
• Issued: 09/01/2015
• Est. Priority Date: 06/01/2012
• Status: Expired due to Fees

• Current Assignee: Rapiscan Systems Incorporated (OSI Systems Incorporated)
• Original Assignee: Rapiscan Systems Incorporated (OSI Systems Incorporated)
• Inventors: Bendahan, Joseph, Solovyev, Vladimir
• Primary Examiner(s): Porta, David
• Assistant Examiner(s): FEIN, ABRA S
• Application Number:
  US13/907,811
• Publication Number:
  US 20130327948A1
• Time in Patent Office: 823 Days
• Field of Search: 250/390.04, 250/390.08
• US Class Current: 1/1
• CPC Class Codes: G01N 23/222 using neutron activation analysis [NAA]
• CPC Class Codes: G01V 5/234 Measuring induced radiation, e.g. thermal neutron activation analysis
• CPC Class Codes: H05H 3/06 Generating neutron beams targets for producing nuclear reactions H05H6/00; neutron sources G21G4/02

Abstract

The present invention provides a Time-of-Flight based neutron inspection system. The system employs a collimated beam of fast neutrons for targeted interrogation of suspect areas in cargo. Elemental composition is determined as a function of depth. Analysis is then used to determine the presence of contraband. The system may be used for secondary inspection for material discrimination to reduce false alarm rate and high cost and time associated with manual unpacking.

Claims

1. A system for inspecting a suspect area in an object, comprising:

a nano-second pulsed deuteron generator configured to generate at least 10⁹ neutrons/second, said nano-second pulsed deuteron generator comprising an ion source to produce a pulsed beam of deuterium ions and an ion filter, chopper and buncher for shaping the pulsed beam of deuterium ions into a narrow pulse width;

a tritium target, which produces pulsed neutrons upon being impinged by the pulsed beam of deuterium ions and wherein a current of the pulsed beam of deuteron ions impinging on the tritium target is in the range of 100 μ

A;

a movable collimator configured to generate a collimated beam of pulsed neutrons and aim the pulsed neutrons at the suspect area;

gamma ray detectors to detect gamma rays produced after an interaction of pulsed neutrons with the suspect area; and

a processing unit that analyzes time-of flight (ToF) data from the gamma ray detectors to determine identities of materials in the suspect area.

2. The system of claim 1 wherein the processing unit uses said ToF data to map signals from gamma ray detectors into elements of the suspect area as a function of depth.

3. The system of claim 1, wherein an accelerating voltage is in a 100 to 300 kV range.

4. The system of claim 1, wherein the ion source is a positive ion source.

5. The system of claim 1, wherein the tritium target comprises multiple targets.

6. The system of claim 1, wherein the tritium target comprises a rotating target.

7. A system for inspecting a suspect area in an object, comprising:

a pulsed deuteron generator configured to generate neutrons, said pulsed deuteron generator comprising an ion source to produce a pulsed beam of deuterium ions, wherein the pulsed deuteron generator is shielded to reduce a dose outside the collimated beam of pulsed neutrons and reduce gamma ray background and wherein said shielding has a total thickness of approximately 75 cm;

a tritium target, which, when impinged upon by the pulsed beam of deuterium ions, generates pulsed neutrons;

a movable collimator configured to generate a collimated beam of pulsed neutrons directed toward the suspect area;

gamma ray detectors to detect gamma rays produced after an interaction of the pulsed neutrons with the suspect area; and

a processing unit that analyzes time-of flight (ToF) data from the gamma ray detectors to determine identities of materials in the suspect area.

8. A system for inspecting a suspect area in an object, the system comprising:

a d-T neutron generator configured to produce neutrons and corresponding alpha particles;

a neutron beam collimator to collimate the neutrons into a collimated beam and direct the neutrons at the suspect area, wherein said neutron beam collimator is shielded, using layers comprising at least one of borated polyethylene, tungsten, steel, copper and lead, to reduce neutron leakage and gamma rays produced in the collimator;

an alpha-particle detector placed 180-degrees relative to the suspect area to detect alpha particles and determine a time of generation of said neutrons, wherein the alpha-particle detector is collimated to substantially a same angular opening as the neutron beam collimator;

gamma-ray detectors configured to detect gamma rays produced after an interaction of neutrons with the suspect area, wherein said gamma ray detectors are shielded to prevent thermal and epi-thermal capture; and

a processing unit to determine an elemental composition of the suspect area as a function of depth based on the time of generation of the neutrons and a time spectrum of the gamma rays produced.

9. The system of claim 8, wherein a total neutron output of the neutron generator is in a range of 10⁹ neutrons per second.

10. The system of claim 8, wherein a size of the collimated beam that impinges on the suspect area is at least 1 cm, when a high deuteron beam current is used.

11. The system of claim 8, wherein the alpha-particle detector is placed at a distance in the range of 25 cm from the object.

12. The system of claim 8, wherein the alpha detector comprises a multi-segmented detector.

13. The system of claim 8, wherein the d-T neutron generator rotates along its long axis to aim neutrons at the suspect area.

14. The system of claim 8, wherein the d-T neutron generator comprises shielding to reduce a dose outside the collimated beam and wherein said shielding has a total thickness of approximately 50 cm.

15. The system of claim 8, wherein a total overall length of the collimator is at least 75 cm.

16. The system of claim 8, wherein the system comprises a primary inspection subsystem and a secondary inspection subsystem, wherein suspect areas are identified by the primary inspection subsystem system and wherein the system determines an optimal position and rotation angle of the object for inspecting the suspect areas with collimated neutrons.