Variable energy linear accelerator

• US 6,407,505 B1
• Filed: 02/01/2001
• Issued: 06/18/2002
• Est. Priority Date: 02/01/2001
• Status: Expired due to Term

• Current Assignee: Siemens Medical Solutions USA Incorporated (Siemens AG)
• Original Assignee: Siemens Medical Solutions USA Incorporated (Siemens AG)
• Inventors: Bertsche, Kirk Joseph
• Primary Examiner(s): Anderson, Bruce
• Assistant Examiner(s): Wells, Nikita
• Application Number:
  US09/775,526
• Time in Patent Office: 502 Days
• Field of Search: 315/5.41, 315/5.42, 315/5.46, 315/505
• US Class Current: 315/5.41
• CPC Class Codes: H05H 9/04 Standing-wave linear accelerators

Abstract

A device for use in a linear accelerator operable to accelerate charged particles along a beam axis. The device includes a first end section, a second end section, and a transition section interposed between the first and second end sections. The sections are coupled together to form a plurality of accelerating cavities aligned along the beam axis. The first and second sections are configured to operate in a fixed collective resonant mode and the transition section is tunable such that resonant modes of the transition section may be tuned to lie at generally the same frequency as the resonant mode of the first and second sections.

Claims

1. A device for use in a linear accelerator operable to accelerate charged particles along a beam axis, the device comprising a first end section, a second end section, and a transition section interposed between the first and second end sections, the sections being connected together to form a plurality of accelerating cavities aligned along said beam axis and coupling cavities, wherein the first and second sections are configured to operate in fixed collective resonant modes and the transition section is tunable such that different resonant modes of the transition section may be tuned to lie at generally the same frequency as the resonant modes of the first and second sections.

2. The device of claim 1 wherein the transition section is tunable to resonate in two different collective modes.

3. The device of claim 1 wherein the device is configured for use in medical applications.

4. The device of claim 1 wherein the transition section comprises two half-cavities, each of the half cavities being connected with a half cavity from one of the end sections to form an accelerating cavity.

5. The device of claim 4 wherein the transition section is tunable to operate in two different collective modes.

6. The device of claim 5 wherein one of the collective modes allows each of the half-cavities of the transition section to resonate generally in phase and the other of the modes allows the half-cavities to resonate generally 180 degrees out of phase.

7. The device of claim 5 wherein one of the modes is a π

operating mode and the other mode is a 0 operating mode.

8. The device of claim 4 wherein the accelerating cavities located at ends of the transition section include two tuning devices.

9. The device of claim 4 wherein the half-cavities of the transition section are coupled through an opening in a cavity wall common to the half-cavities.

10. The device of claim 1 wherein the transition section comprises one full cavity and two half-cavities.

11. The device of claim 10 wherein the accelerating cavities at the ends of the transition section include two tuning devices.

12. The device of claim 11 wherein each tuning device is disposed within one of the half-cavities.

13. The device of claim 10 wherein the transition section is configured to operate in a π

mode and a π

/2 mode.

14. The device of claim 10 wherein the transition section is configured to operate in a 0 mode and a π

/2 mode.

15. The device of claim 1 wherein the transition section comprises three full cavities and two half-cavities.

16. The device of claim 15 wherein the transition section is configured to operate in π

/2 mode and π

/4 mode.

17. The device of claim 15 wherein the transition section is configured to operate in π

/2 mode and 3π

/4 mode.

18. The device of claim 1 wherein the transition section comprises one accelerating cavity and two half-cavities, each half cavity being coupled to the accelerating cavity of the transition section through a side coupling cavity.

19. The device of claim 1 wherein the fixed collective resonant mode of the first and second end sections is a π

/2 mode.

20. A system for delivering charged particles, the system comprising:

a particle accelerator having an input for connection to a source of charged particles and a beam path extending to an exit window, the particle accelerator comprising a first end section, a second end section, and a transition section interposed between the first and second end sections, the sections being connected together to form a plurality of accelerating cavities aligned along said beam path, wherein the first and second sections are configured to operate in fixed collective resonant modes and the transition section is tunable such that resonant modes of the transition section may be tuned to lie at generally the same frequency as the resonant modes of the first and second sections; and

a signal source for energy transfer engagement with the charged particles within the particle accelerator.

21. The system of claim 20 wherein the transition section is tunable to resonate in two different collective modes.

22. The system of claim 20 wherein the device is configured for use in medical applications.

23. The system of claim 20 wherein the transition section comprises two half-cavities, each of the half cavities being coupled with a half cavity from one of the end sections to form an accelerating cavity.

24. The system of claim 23 wherein the transition section is tunable to operate in two different collective modes.

25. The system of claim 24 wherein one of the collective modes allows each of the half-cavities of the transition section to resonate generally in phase and the other of the modes allows the half-cavities to resonate generally 180 degrees out of phase.

26. The system of claim 24 wherein one of the modes is a π

operating mode and the other mode is a 0 operating mode.

27. The system of claim 23 wherein the transition section comprises two tuning devices.

28. The system of claim 27 wherein the transition section comprises two deformable cavities.

29. The system of claim 23 wherein the half-cavities of the transition section are coupled through an opening in a common cavity wall separating the half-cavities.

30. The system of claim 20 wherein the transition section comprises one accelerating cavity and two half-cavities.

31. The system of claim 30 wherein the transition section comprises two tuning devices.

32. The system of claim 31 wherein each of the tuning devices is disposed within one of the half-cavities.

33. The system of claim 31 wherein the transition section is configured to operate in a π

mode and a π

/2 mode.

34. The system of claim 31 wherein the transition section is configured to operate in a 0 mode and a π

/2 mode.

35. The system of claim 20 wherein the transition section comprises three accelerating cavities and two half-cavities.

36. The system of claim 35 wherein the transition section is configured to operate in π

/2 mode and π

/4 mode.

37. The system of claim 35 wherein the transition section is configured to operate in π

/2 mode and 3π

/4 mode.

38. The system of claim 20 wherein the transition section comprises one accelerating cavity and two half-cavities, each half cavity being coupled to the accelerating cavity of the transition section through a side coupling cavity.

39. The device of claim 20 wherein the fixed collective resonant mode of the first and second end sections is a π

/2 mode.

40. A device for use in a linear accelerator operable to accelerate charged particles along a beam axis, the device comprising first and second sections, the sections being connected together to form a plurality of accelerating cavities aligned along said beam axis and coupling cavities, wherein the first section is configured to operate in fixed collective resonant modes and the second section is tunable such that different resonant modes of the transition section may be tuned to lie at generally the same frequency as the resonant mode of the first section.