Systems and methods for generating X-rays and neutrons using a single linear accelerator
View Patent ↗Systems and methods for generating X-rays and neutrons using a single linear accelerator are disclosed. Such system and methods may interrogate an object at times with X-rays and at other times with neutrons, e.g., after suspicious material is detected based on the X-rays. A system may include a single linear accelerator for generating first and second electron beams; first and second targets; a magnet configured to control irradiation of the first and second targets by the first and second electron beams; and a controller that (a) causes the linear accelerator to generate the first electron beam and causes the magnet to direct the beam to first target to generate X-rays; and (b) causes the linear accelerator to generate the second electron beam and causes the magnet to direct the beam to the second target to generate neutrons.
1. A system for interrogating an object, the system comprising:
a single linear accelerator configured to generate first and second electron beams respectively having first and second energies;
first and second targets;
a magnet configured to control irradiation of the first and second targets by the first and second electron beams; and
a controller in operable communication with the linear accelerator and with the magnet, the controller configured to:
(a) cause the linear accelerator to generate the first electron beam at a first time and cause the magnet to direct the first electron beam to the first target so as to generate a first X-ray beam that has a first X-ray energy and irradiates the object; and
(b) cause the linear accelerator to generate the second electron beam at a second time and cause the magnet to direct the second electron beam to the second target so as to generate a neutron beam that irradiates the object.
2. The system of claim 1 , wherein the magnet is configured to deflect the second electron beam to irradiate the second target responsive to a control signal from the controller.
3. The system of claim 2 , wherein the magnet is configured to allow the first electron beam to irradiate the first target without deflection responsive to a control signal from the controller.
4. The system of claim 1 , wherein the controller is configured to interleave the first X-ray beam and the neutron beam by repeating (a) and (b).
5. The system of claim 1 , further comprising an X-ray detector configured to detect a percent transmission of the first X-ray beam through the object.
6. The system of claim 5 , wherein the controller is in operable communication with the detector and is configured to perform (b) when the percent transmission is less than a predetermined threshold.
7. The system of claim 1 , wherein the linear accelerator is further configured to generate a third electron beam having a third energy, and wherein the controller is further configured to (c) cause the linear accelerator to generate the third electron beam at a third time and cause the magnet to direct the third electron beam to the first target so as to generate a second X-ray beam that has a second X-ray energy and irradiates the object.
8. The system of claim 7 , wherein the controller is configured to interleave the first and second X-ray beams and the neutron beam by repeating (a), (b), and (c).
9. The system of claim 7 , further comprising an X-ray detector configured to detect percent transmissions of the first and second X-ray beams through the object.
10. The system of claim 9 , wherein the controller is in operable communication with the detector and is configured to perform (b) when the percent transmissions are less than a predetermined threshold.
11. The system of claim 1 , wherein the linear accelerator and the first and second targets all share a common vacuum.
12. The system of claim 1 , wherein the controller is further configured to select a dose of the first X-ray beam by selecting one of a beam current and a pulse width of the first electron beam, and to select a dose of the neutron beam by selecting one of a beam current and a pulse width of the second electron beam.
13. The system of claim 1 , wherein the first and second energies are different from one another.
14. A method of interrogating an object, the method comprising:
generating with a single linear accelerator first and second electron beams respectively having first and second energies;
directing the first electron beam to a first target so as to generate a first X-ray beam having a first X-ray energy at a first time;
irradiating the object with the first X-ray beam;
directing the second electron beam to a second target so as to generate a neutron beam at a second time; and
irradiating the object with the neutron beam.
15. The method of claim 14 , wherein directing the second electron beam to the second target comprises deflecting the second electron beam with a magnet.
16. The method of claim 15 , wherein directing the first electron beam to the first target comprises allowing the first electron beam to travel undeflected from the single linear accelerator to the first target.
17. The method of claim 16 , comprising interleaving the first and second electron beams and directing the first and second electron beams to the first and second targets in synchrony with the interleaving.
18. The method of claim 15 , wherein the first and second energies are different from one another.
19. The method of claim 14 , further comprising detecting a percent transmission of the first X-ray beam through the object.
20. The method of claim 19 , wherein the second electron beam is generated and directed to the target when the detected percent transmission is less than a predetermined threshold.
21. The method of claim 14 , further comprising:
generating with the single linear accelerator a third electron beam having a third energy;
directing the third electron beam to the first target so as to generate a second X-ray beam having a second X-ray energy; and
irradiating the object at a third time with the second X-ray beam.
22. The method of claim 21 , further comprising interleaving the first, second, and third electron beams generated by the single linear accelerator and controlling direction of the first, second, and third electron beams to the first and second targets in synchrony with the interleaving.
23. The method of claim 21 , further comprising detecting a percent transmission of the first and second X-ray beams through the object.
24. The method of claim 23 , wherein the second electron beam is generated and directed to the second target when the percent transmission less than a predetermined threshold.
25. The method of claim 14 , wherein the linear accelerator and the first and second targets all share a common vacuum.
26. The method of claim 14 , further comprising selecting a dose of the first X-ray beam by selecting one of a beam current and a pulse width of the first electron beam, and selecting a dose of the neutron beam by selecting one of a beam current and a pulse width of the second electron beam.