Traveling wave linear accelerator based x-ray source using pulse width to modulate pulse-to-pulse dosage
Provided herein are systems and methods for operating a traveling wave linear accelerator to generate stable electron beams at two or more different intensities by varying the number of electrons injected into the accelerator structure during each pulse by varying the width of the beam pulse, i.e., pulse width.
1. A traveling wave linear accelerator comprising:
an electron gun modulator to adjust a pulse width and a beam injection time of a beam of electrons from an electron gun;
a signal backplane connected to the electron gun modulator;
a radio frequency (RF) source, connected to the signal backplane, to generate an RF pulse having an RF rise time; and
an intensity controller connected to the signal backplane and operatively associated with the electron gun modulator and the RF source, the intensity controller to:
receive an intensity adjustment command to implement a particular intensity adjustment;
compute the RF rise time to be used by the RF source and the pulse width and the beam injection time to be used by the electron gun modulator based at least in part on the intensity adjustment command, wherein a combination of the computed RF rise time, the computed pulse width and the computed beam injection time is to suppress a beam loading transient and produce the particular intensity adjustment;
transmit a first signal for the computed pulse width and the computed beam injection time to the electron gun modulator; and
transmit a second signal for the computed RF rise time to the RF source;
wherein the RF source is to receive the second signal for the computed RF rise time and adjust the RF rise time of the RF pulse and the electron gun modulator is to receive the first signal for the computed pulse width and the computed beam injection time and adjust the pulse width and the beam injection time of the beam of electrons such that the traveling wave linear accelerator generates an output dose rate of electrons in accordance with the particular intensity adjustment.
2. The traveling wave linear accelerator of claim 1 , wherein an energy of the output dose rate is stable.
3. The traveling wave linear accelerator of claim 1 , wherein the intensity controller further comprises an input device to receive the intensity adjustment command.
4. The traveling wave linear accelerator of claim 1 , wherein the intensity controller is to compute the pulse width and the beam injection time using a lookup table.
5. The traveling wave linear accelerator of claim 1 , wherein the intensity controller is to compute the pulse width and the beam injection time on a pulse-to-pulse basis.
6. The traveling wave linear accelerator of claim 5 , wherein an intensity of the output dose rate of a first pulse is different from an intensity of the output dose rate of a second pulse.
7. The traveling wave linear accelerator of claim 6 , wherein, during a single energy operation, an energy of the first pulse is substantially the same as an energy of the second pulse.
8. The traveling wave linear accelerator of claim 6 , wherein, during an interleaved energy operation, an energy of the first pulse is different from an energy of the second pulse.
9. The traveling wave linear accelerator of claim 8 , wherein, during the interleaved energy operation, an energy of a third pulse is substantially the same as the energy of the first pulse.
10. The traveling wave linear accelerator of claim 1 , wherein the intensity controller is to compute the beam injection time such that a transient energy of the beam of electrons is centered around a steady state energy.
11. The traveling wave linear accelerator of claim 1 , wherein the RF source comprises a klystron that is to receive a generated signal having a frequency determined by a frequency controller and to generate an electromagnetic wave.
12. The traveling wave linear accelerator of claim 11 , further comprising an accelerator structure to receive the electromagnetic wave from the klystron and the electrons having the adjusted pulse width and beam injection time and to accelerate electrons and the electromagnetic wave to generate the output dose rate of electrons.
13. The traveling wave linear accelerator of claim 1 , wherein the RF source comprises a magnetron to receive a generated signal having a frequency determined by a frequency controller and to generate an electromagnetic wave.
14. The traveling wave linear accelerator of claim 13 , further comprising an accelerator structure to receive the electromagnetic wave from the magnetron and the electrons having the adjusted pulse width and beam injection time and to accelerate electrons and the electromagnetic wave to generate the output dose rate of electrons.
15. A method comprising:
receiving an intensity adjustment command to implement a particular intensity adjustment at an intensity controller of a traveling wave linear accelerator;
computing a radio frequency (RF) rise time, a pulse width and a beam injection time at the intensity controller based on the intensity adjustment command, wherein a combination of the computed RF rise time, the computed pulse width and the computed beam injection time is to suppress a beam loading transient and produce the particular intensity adjustment;
adjusting a setting of an electron gun modulator to produce the computed pulse width and the computed beam injection time of electrons from an electron gun;
adjusting a setting of an RF source to produce the computed RF rise time; and
generating an output dose rate of electrons in accordance with the particular intensity adjustment using the traveling wave linear accelerator.
16. The method of claim 15 , wherein an energy of the output dose rate is stable.
17. The method of claim 15 , wherein the receiving comprises receiving the intensity adjustment command from an input device on the intensity controller.
18. The method of claim 15 , wherein the computing comprises computing the pulse width and the beam injection timing using a lookup table.
19. The method of claim 15 , wherein, during a single energy operation, an energy of a first pulse is substantially the same as an energy of a second pulse.
20. The method of claim 15 , wherein, during an interleaved energy operation, an energy of a first pulse is different from an energy of a second pulse, and wherein the pulse width and the beam injection time are rapidly adjusted on a pulse-to-pulse basis to provide multi-energy interleaving.
21. A non-transitory computer readable medium comprising instructions that, when executed by a processor of a traveling wave linear accelerator, cause the processor to perform operations comprising:
receiving an intensity adjustment command to implement a particular intensity adjustment by the processor of the traveling wave linear accelerator;
computing, by the processor, a radio frequency (RF) rise time, a pulse width and a beam injection time based on the intensity adjustment command, wherein a combination of the computed RF rise time, the computed pulse width and the computed beam injection time is to suppress a beam loading transient and produce the particular intensity adjustment;
adjusting a setting of an electron gun modulator to produce the computed pulse width and the computed beam injection time of electrons from an electron gun;
adjusting a setting of an RF source to produce the computed RF rise time; and
generating an output dose rate of electrons in accordance with the particular intensity adjustment using the traveling wave linear accelerator.
22. The non-transitory computer readable medium of claim 21 , wherein the computer readable medium and the processor comprise a programmable logic controller or personal computer.
23. The non-transitory computer readable medium of claim 22 , wherein the traveling wave linear accelerator further comprises an intensity controller integrated in the programmable logic controller or the personal computer, the intensity controller to receive the intensity adjustment command and to compute the pulse width and the beam injection time.
24. The non-transitory computer readable medium of claim 21 , wherein the traveling wave linear accelerator further comprises an electron gun modulator to adjust the pulse width and the beam injection time of electrons from the electron gun using the computed pulse width and the computed beam injection time.
25. The non-transitory computer readable medium of claim 21 , wherein the computer readable medium and the processor comprise a programmable logic controller or personal computer and an intensity controller,
wherein the intensity controller is separate from the programmable logic controller or personal computer, the intensity controller to receive the intensity adjustment command and to compute the pulse width and the beam injection time.
26. A multi-energy traveling wave linear accelerator comprising:
a signal backplane;
an intensity controller, connected to the signal backplane, comprising a processor to:
receive an intensity adjustment command to implement a particular intensity adjustment; and
compute a radio frequency (RF) rise time, a pulse width and a beam injection time based on the intensity adjustment command, wherein a combination of the computed rise time, the computed pulse width and the computed beam injection time is to suppress a beam loading transient and produce the particular intensity adjustment;
an RF source, connected to the signal backplane, to output an RF pulse having the computed RF rise time; and
an electron gun modulator, connected to the signal backplane, to cause an electron gun of the multi-energy traveling wave linear accelerator to output a beam of electrons having the computed pulse width and the computed beam injection, and further to cause the traveling wave linear accelerator to generate an output dose rate of electrons in accordance with the particular intensity adjustment.
27. The traveling wave linear accelerator of claim 26 , wherein the processor comprises a programmable logic controller.
28. The traveling wave linear accelerator of claim 1 , wherein the intensity controller is to execute a programmed routine.
29. The traveling wave linear accelerator of claim 1 , wherein the intensity controller further comprises a computer readable medium.
30. The traveling wave linear accelerator of claim 1 , wherein the traveling wave linear accelerator is a multi-energy traveling wave linear accelerator.
31. The method of claim 15 , wherein the traveling wave linear accelerator is a multi-energy traveling wave linear accelerator.
32. The non-transitory computer readable medium of claim 21 , wherein the traveling wave linear accelerator is a multi-energy traveling wave linear accelerator.
33. The traveling wave linear accelerator of claim 1 , wherein a combination of the computed RF rise time, the computed pulse width and the computed beam injection time are to produce the particular intensity adjustment without causing adjustment of an energy of the beam of electrons.