High Z material detection system and method

• US 7,470,905 B1
• Filed: 11/29/2007
• Issued: 12/30/2008
• Est. Priority Date: 01/04/2007
• Status: Expired due to Fees

• Current Assignee: CeLight, Inc.
• Original Assignee: CeLight, Inc.
• Inventors: Shpantzer, Isaac, Goldberg, Jacques, Reingand, Nadejda, Achiam, Yaakov
• Primary Examiner(s): Vanore; David A.
• Application Number:
  US11/947,058
• Time in Patent Office: 397 Days
• Field of Search: None
• US Class Current: 250/358.1
• CPC Class Codes: G01T 1/2935 using ionisation detectors

Abstract

A method and system for high Z substance revealing using muon detection technique is presented. Natural muon coordinate and incidence angle are measured above and below the interrogated volume. The data on muons trajectory change caused by the presence of high Z material and the muons time of flight between the upper and lower muon detectors are used for the decision making on the presence of a nuclear substance inside the volume. The system is adapted for performing measurements on moving objects such as moving trucks.

Claims

1. A system for a high Z material detection, comprising:

at least a first muon detector and a second muon detector positioned essentially parallel to each other, the first muon detector is indicative of an incidence angle, and the second muon detector is indicative of an actual leaving angle for each muon passing the system;

a digital signal processing unit for

storing a data on the incidence and the actual leaving angle for muons passing the system during an exposure time T;

calculating an actual statistics of the actual leaving angles and an expected statistics of expected leaving angles, wherein the expected statistics of the expected leaving angle is estimated assuming absence of the high Z material in between the first and the second muon detector;

finding a difference between the actual and the expected statistics; and

determining a presence of the high Z material inside the system when the difference is above a predetermined difference value.

2. The system according to claim 1, wherein

the actual statistics and the expected statistics are an actual and expected distribution widths.

3. The system according to claim 2, wherein the predetermined difference value is 1 mrad.

4. The system according to claim 1, wherein the predetermined difference value depends on the exposure time T.

5. The system according to claim 1, wherein

the predetermined difference value providing probability of a positive detection above 90%.

6. The system according to claim 1, wherein

the first and the second muon detectors are flat detectors of at least 1 square meters each.

7. The system according to claim 1, wherein

the measurement time T is at least one minute.

8. The system according to claim 1, wherein

the first and the second muon detectors each comprises an angular measuring unit for angular measurement of a muon trajectory with an accuracy of at least 1 mrad.

9. The system according to claim 1, wherein

the first and the second muon detectors each comprises a coordinate measuring unit for coordinate measurement for each muon passing the system with a resolution of at least 2 mm.

10. The system according to claim 1, further comprising:

a time measuring unit to measure a time of flight of each muon between the first and the second muon detectors; and

the digital signal processing unit being used for computation of a muon velocity basing on the measured time of flight and for calculation of the expected statistics depending on the computed muon velocity.

11. The system according to claim 10, wherein

a contribution of muons having the measured time of flight larger than a predetermined time of flight value is eliminated from consideration by the digital signal processing unit when determining the presence of high Z material in the system.

12. The system according to claim 10, wherein

the time measuring unit is a clock associated with the first and the second muon detector, the clock being initiated by a muon penetrating the first muon detector and being stopped by the muon leaving the second muon detector.

13. The system according to claim 12, wherein

a time resolution of the clock is 1 ns or better.

14. The system according to claim 1, wherein

the first and the second muon detectors each comprises a scintillator counter for measurement of a time for each muon passing each detector.

15. The system according to claim 1, wherein

the first and the second muon detectors each comprises at least two flat wire detectors.

16. The system according to claim 15, wherein

the wire detector is a gas chamber with at least one wire grid.

17. The system according to claim 1, further comprising

an indication system to produce a signal when the presence of the high Z material in the system is suspected.

18. The system according to claim 1, further comprising

a position measuring unit for measuring a position of a vehicle moving in between the first and the second muon detector;

the digital signal processing unit storing the position of the vehicle associated with each muons entering the system during the exposure time T;

performing calculation of the actual statistics of the actual leaving angle basing on statistics of muon penetration of each part of the moving vehicle.

19. A method for high Z material revealing, comprising:

continuously measuring an incident angle of each incoming muon by a first detector;

estimating an expected statistics of an expected leaving angle at a second detector for each incoming muon;

continuously measuring an actual leaving angle for each incoming muon by the second detector;

storing a data on the incident, the actual and the expected leaving angles;

calculating an actual statistics of the actual leaving angle;

finding a difference between the expected and the actual statistics; and

determining a presence of high Z material in between the first and the second muon detector when the difference exceeds a predetermined difference value.

20. The method according to claim 19, further comprising:

measuring a time of flight for each muon registered by the first muon detector, and calculating the expected statistics depending on the muon time of flight.