Interleaving multi-energy x-ray energy operation of a standing wave linear accelerator
View Patent ↗The disclosure relates to systems and methods for interleaving operation of a standing wave linear accelerator (LINAC) for use in providing electrons of at least two different energy ranges, which can be contacted with x-ray targets to generate x-rays of at least two different energy ranges. The LINAC can be operated to output electrons at different energies by varying the power of the electromagnetic wave input to the LINAC, or by using a detunable side cavity which includes an activatable window.
1. A method, comprising:
coupling an electromagnetic wave into an accelerator,
wherein said accelerator comprises a plurality of main cavities and a plurality of side cavities,
wherein each side cavity of said plurality of side cavities communicates with two neighboring main cavities of said plurality of main cavities, and
wherein at least one side cavity of said plurality of side cavities comprises an activatable window positioned in said at least one side cavity; and
injecting a first set of electrons into a longitudinal passageway positioned along a longitudinal axis of said accelerator,
wherein said longitudinal passageway communicates with said plurality of main cavities,
wherein said first set of electrons is accelerated by said electromagnetic wave in a region of said longitudinal passageway in communication with at least one of said plurality of main cavities, and
wherein said first set of electrons is emitted from said accelerator at a first energy when said activatable window is not activated;
activating said activatable window by injecting charge carriers into said activatable window; and
injecting a second set of electrons into said longitudinal passageway,
wherein said second set of electrons is emitted from said accelerator at a second energy when said activatable window is activated.
2. The method of claim 1 , wherein activating said activatable window further comprises injecting the charge carriers through PIN diodes arranged around a periphery of said activatable window.
3. The method of claim 1 , wherein said at least one side cavity comprises a longitudinal axis, and wherein said at least one side cavity is positioned such that said longitudinal axis of said at least one side cavity is perpendicular to said longitudinal axis of said accelerator.
4. The method of claim 3 , wherein said at least one side cavity comprising said activatable window has a substantially cylindrical cross-section.
5. The method of claim 4 , wherein said at least one side cavity comprising said activatable window comprises a resonant TE01 waveguide.
6. The method of claim 5 , wherein said resonant TE01 waveguide has a length approximately equal to a guided wavelength of the electromagnetic wave.
7. The method of claim 5 , wherein said resonant TE01 waveguide has a length approximately equal to a half of a guided wavelength of the electromagnetic wave.
8. The method of claim 3 , wherein said activatable window is positioned near an end of said at least one side cavity.
9. The method of claim 8 , wherein the accelerator comprises a thermal conductor positioned between said activatable window and said end of said at least one side cavity.
10. The method of claim 1 , wherein, when said activatable window is not activated, said activatable window transmits more than 50% of a component of said electromagnetic wave which is fed into said at least one side cavity comprising said activatable window, and wherein said activating said activatable window causes said activatable window to transmit less than 50% of a component of said electromagnetic wave.
11. A standing wave linear accelerator, comprising:
a plurality of main cavities and a plurality of side cavities,
wherein each side cavity of said plurality of side cavities communicates with two neighboring main cavities of said plurality of main cavities, and
wherein at least one side cavity of said plurality of side cavities comprises an activatable window positioned in said at least one side cavity, thereby providing at least one detunable side cavity, wherein said activatable window comprises a doped silicon wafer window, and
wherein said at least one detunable side cavity is configured such that a standing wave is disrupted in main cavities of said plurality of main cavities located downstream of said at least one detunable side cavity when said activatable window is activated.
12. The standing wave linear accelerator of claim 11 , wherein said activatable window is activated by injecting charge carriers into said activatable window.
13. The standing wave linear accelerator of claim 11 , wherein said at least one side cavity comprising said activatable window has a cylindrical cross-section.
14. The standing wave linear accelerator of claim 13 , wherein said at least one side cavity comprising said activatable window comprises a resonant TE01 waveguide.
15. The standing wave linear accelerator of claim 14 , wherein said resonant TE01 waveguide has a length approximately equal to a guided wavelength of the electromagnetic wave.
16. The standing wave linear accelerator of claim 14 , wherein said resonant TE01 waveguide has a length approximately equal to a half of a guided wavelength of the electromagnetic wave.
17. The standing wave linear accelerator of claim 13 , wherein said activatable window is positioned near an end of said at least one side cavity.
18. The standing wave linear accelerator of claim 17 , further comprising a thermal conductor positioned between said activatable window and said end of said at least one side cavity.
19. A standing wave linear accelerator, comprising:
a plurality of main cavities and a plurality of side cavities,
wherein each side cavity of said plurality of side cavities communicates with two neighboring main cavities of said plurality of main cavities, and
wherein at least one side cavity of said plurality of side cavities comprises an activatable window positioned in said at least one side cavity, thereby providing at least one detunable side cavity, wherein said activatable window comprises a plasma switch, and
wherein said at least one detunable side cavity is configured such that a standing wave is disrupted in main cavities of said plurality of main cavities located downstream of said at least one detunable side cavity when said activatable window is activated.