Adaptive Cargo Inspection Based on Multi-Energy Betatron

• US 20190129060A1
• Filed: 10/28/2017
• Published: 05/02/2019
• Est. Priority Date: 10/28/2017
• Status: Active Grant

• Current Assignee: Radiabeam Technologies, LLC
• Original Assignee: Radiabeam Technologies, LLC
• Inventors: Arodzero, Anatoli, Kutsaev, Sergey V., Ziskin, Vitaliy, Boucher, Salime, O'Shea, Finn
• Granted Patent: US 10,641,918 B2
• Time in Patent Office: Days
• CPC Class Codes: G01V 5/224 Multiple energy techniques using one type of radiation, e.g. X-rays of different energies

Abstract

The present disclosure relates generally to methods and apparatus for cargo inspection and, more particularly, to X-ray based inspection systems providing radiographic imaging and material discrimination with adaptive control of X-ray source dependent upon characteristics of the cargo under inspection. X-rays are generated utilizing a dual energy interlaced betatron by generation of X-ray pulses with lower- and higher-energies during the same betatron acceleration cycle.

Claims

1. A system for cargo inspection comprising:

a betatron accelerating a beam of electrons internal to said betatron;

a Bremsstrahlung conversion target located internal to said betatron and positioned to overlap the path of said beam of electrons at a specific electron orbit;

said beam of electrons producing a beam of X-rays when said electron beam interacts with said Bremsstrahlung conversion target;

a collimator rigidly attached to said betatron and positioned between said betatron and said cargo forming a fan beam of said beam of X-rays incident upon said cargo wherein said cargo is sampled in a slice bounded by said fan beam of said beam of X-rays;

a variable magnetic field generator proximal to said betatron producing a time dependent magnetic field internal to said betatron wherein said magnetic field modifies the electron orbits near the Bremsstrahlung conversion target;

a first modification to said time dependent field internal such that said electron beam partially intercepts radially said Bremsstrahlung conversion target producing a first pulse of X-rays with a first end-point energy;

a second modification to said time dependent field internal following said first modification such that said electron beam continues to circulate within said betatron but does not intercept said Bremsstrahlung conversion target;

a radiation detector positioned distal from said betatron and intercepting said first pulse of X-rays and receiving the part of the first pulse of X-rays that pass through said cargo;

a third modification to said time dependent field internal following said second modification such that said electron beam intercepts said Bremsstrahlung conversion target producing a second pulse of X-rays with a second end-point energy;

said radiation detector receiving the part of the second pulse of X-rays that pass through said cargo from said second pulse of X-rays;

wherein said first pulse of X-rays and said second pulse of X-rays are generated from the same acceleration cycle of said betatron;

said cargo translated relative to said fan beam of said beam of X-rays and perpendicular to the plane of said fan beam of X-rays and repeating first and second pulse production and measurement for subsequent inspection slices of said cargo;

a processor for receiving data from said radiation detector;

said processor using said data to derive relative attenuation of said first pulse of X-ray and said second pulse of X-rays transmitted through said cargo, said relative attenuation computed for each said first and said second pulse of said penetrating radiation transmitted through said cargo; and

said processor deriving a material characteristic of multiple sections of said cargo.

2. The system of claim 1 wherein:

said first modification to said time dependent field internal producing said first pulse of X-rays with pulse duration greater than 10 microseconds;

said third modification to said time dependent field producing said second pulse of X-rays with a pulse duration greater than 10 microseconds.

3. The system of claim 2 wherein:

said radiation detector is an X-ray detector operating in a photon counting mode.

4. The system of claim 3 wherein:

said radiation detector is a scintillation detector.

5. The system of claim 1 further comprising:

said radiation detector is a linear array of radiation detectors spatial distributed in the plane of said fan-beam of penetrating radiation.

6. The system of claim 3 wherein:

said radiation detector comprises an array of direct conversion detectors.

7. The system of claim 2 wherein:

said first modification to said time dependent field internal producing said first pulse of X-rays with pulse duration less than 1000 microseconds;

said third modification to said time dependent field producing said second pulse of X-rays with a pulse duration less than 1000 microseconds.

8. The system of claim 2 further comprising:

a forth modification to said time dependent field internal to said betatron modifying the electron orbits such that said electron beam intercepts said Bremsstrahlung conversion target producing a third pulse of X-rays with a higher end-point energy than said first pulse of X-rays and a lower end-point energy than said second pulse of X-rays;

wherein said third modification to said time dependent field internal following said second modification such that said electron beam partially intercepts said Bremsstrahlung conversion target producing a second pulse of X-rays with a second end-point energy;

said radiation detector receiving the part of the third pulse of X-rays that pass through said cargo;

wherein said first pulse of X-rays and said second pulse of X-rays and said third pulse of X-rays are generated from the same acceleration cycle of said betatron;

wherein said first pulse of X-rays occurs first followed by said third pulse of X-rays followed by said second pulse of X-rays;

said cargo translated relative to said fan beam of said penetrating radiation and perpendicular to the plane of said fan beam of X-rays and repeating first, third and second pulse production and measurement for subsequent inspection slices of said cargo;

said processor using said data to derive relative attenuation of said beam of X-rays transmitted through said cargo, said relative attenuation computed for each said first, said third and said second pulse of X-rays transmitted through said cargo.

9. The system of claim 1 further comprising:

said processor computing a modified range of X-ray energies for material decomposition from one slice of said cargo and modifying said variable magnetic field generator to apply new timing to said variable magnetic field generator to produce a new first X-ray end-point energy and a new second X-ray end-point energy within a subsequent betatron acceleration cycle corresponding to said modified range of X-ray energies.

10. The system of claim 9 wherein:

said first X-ray end-point energy is modified in real time based upon data from said radiation detector;

such that said first X-ray end-point energy modification is configured based upon said measured data from said X-ray detector from the previously sampled X-ray transmission characteristics by modification in the timing of activation of said variable magnetic field generator.

11. The system of claim 9 wherein:

said second X-ray end-point energy is modified in real time based upon data from said radiation detector;

such that said second X-ray end-point energy modification is configured based upon said measured data from said X-ray detector from the previously sampled X-ray transmission characteristics by modification in the timing of activation of said variable magnetic field generator.

12. The system of claim 1 wherein:

said first modification to said time dependent field internal producing said first pulse of X-rays with pulse duration less than 10 nanoseconds;

said third modification to said time dependent field producing said second pulse of X-rays with a pulse duration less than 10 nanoseconds.

13. The system of claim 12 wherein:

said radiation detector is a Scintillation-Cherenkov detector producing a scintillation signal component and a Cherenkov signal component.

14. The system of claim 12 further comprising:

a forth modification to said time dependent field internal to said betatron modifying the electron orbits such that said electron beam intercepts said Bremsstrahlung conversion target producing a third pulse of X-rays with a higher end-point energy than said first pulse of X-rays and a lower end-point energy than said second pulse of X-rays;

wherein said third modification to said time dependent field internal following said second modification such that said electron beam partially intercepts said Bremsstrahlung conversion target producing a second pulse of X-rays with a second end-point energy;

said radiation detector receiving the part of the third pulse of X-rays that pass through said cargo;

wherein said first pulse of X-rays and said second pulse of X-rays and said third pulse of X-rays are generated from the same acceleration cycle of said betatron;

wherein said first pulse of X-rays occurs first followed by said third pulse of X-rays followed by said second pulse of X-rays;

said cargo translated relative to said fan beam of said penetrating radiation and perpendicular to the plane of said fan beam of X-rays and repeating first, third and second pulse production and measurement for subsequent inspection slices of said cargo;

said processor using said data to derive relative attenuation of said beam of X-rays transmitted through said cargo, said relative attenuation computed for each said first, said third and said second pulse of X-rays transmitted through said cargo.

15. The system of claim 13 wherein:

said processor computes a high energy component for said radiation detector data based on said Cherenkov detector signal and a low energy component based on said scintillation detector signal.

16. The system of claim 12 further comprising:

said processor computing an optimal range of X-ray energies for material decomposition from one slice of said cargo and modifying said variable magnetic field generator to apply new timing to said variable magnetic field generator to produce a new first X-ray end-point energy and a new second X-ray end-point energy corresponding to said optimal range of X-ray energies.

17. The system of claim 1 wherein:

said first modification to said time dependent field internal producing said first pulse of X-rays with pulse duration less than 50 nanoseconds;

said third modification to said time dependent field producing said second pulse of X-rays with a pulse duration less than 50 nanoseconds.

18. A multi-energy betatron comprising:

a betatron accelerating a beam of electrons internal to said betatron;

said betatron having a distal exit port for accelerated electrons;

a variable magnetic field generator internal to said betatron producing a time dependent magnetic field internal to said betatron wherein said magnetic field modifies the electron orbits near the distal radii of said betatron;

a first modification to said time dependent magnetic field internal to said betatron modifying the electron orbits such that said electron beam partially intercepts radially said distal exit port producing a first pulse of electrons with a lower energy and said electron beam partially bypasses said distal exit port;

said time dependent field internal to said betatron modifying the electron orbits such that said electron beam intercepts said distal exit port producing a second pulse of electrons with a higher energy;

wherein said first pulse of electrons and said second pulse of electrons are generated from the same acceleration cycle of said betatron.

19. A multi-energy X-ray generation system comprising:

a betatron accelerating a beam of electrons internal to said betatron;

a Bremsstrahlung conversion target located internal to said betatron and positioned to overlap the path of said beam of electrons at a specific electron orbit;

said beam of electrons producing a beam of X-rays when said electron beam interacts with said Bremsstrahlung conversion target;

a variable magnetic field generator internal to said betatron producing a time dependent magnetic field internal to said betatron wherein said magnetic field modifies the electron orbits near the Bremsstrahlung conversion target;

said time dependent field internal to said betatron modifying the electron orbits such that said electron beam partially intercepts radially said Bremsstrahlung conversion target producing a first pulse of X-rays with a lower end-point energy and said electron beam partially bypasses said Bremsstrahlung conversion target;

said time dependent field internal to said betatron modifying the electron orbits such that said electron beam intercepts said Bremsstrahlung conversion target producing a second pulse of X-rays with a higher end-point energy;

wherein said first pulse of X-rays and said second pulse of X-rays are generated from the same acceleration cycle of said betatron.