RADIO FREQUENCY CAVITIES

• US 20170273168A1
• Filed: 11/24/2015
• Published: 09/21/2017
• Est. Priority Date: 11/25/2014
• Status: Active Grant

• Current Assignee: Oxford University Innovation Limited (University of Oxford)
• Original Assignee: Oxford University Innovation Limited (University of Oxford)
• Inventors: Konoplev, Ivan, Burt, Graeme
• Granted Patent: US 10,237,963 B2
• Time in Patent Office: Days
• CPC Class Codes: H05H 13/10 Accelerators comprising one or more linear accelerating sections and bending magnets or the like to return the charged particles in a trajectory parallel to the first accelerating section, e.g. microtrons or rhodotrons
• CPC Class Codes: H05H 2007/227 power coupling, e.g. coupling loops
• CPC Class Codes: H05H 7/06 Two-beam arrangements; Multi-beam arrangements storage rings; Electron rings
• CPC Class Codes: H05H 7/22 Details of linear accelerators, e.g. drift tubes H05H7/02 - H05H7/20 take precedence

Abstract

A radio-frequency (RF) cavity apparatus for accelerating charged particles includes first and second cavity arms. The first and second cavity arms have respective first and second axes of rotational symmetry and each cavity arm includes at least one cell. The first and second cavity arms are connected by a resonance coupler. The cell(s) of the first cavity aim have an axial dimensional parameter that is equal to a corresponding axial dimensional parameter of the cell(s) of the second cavity arm, and the cell(s) of the first cavity arm have at least one non-axial dimensional parameter that differs from corresponding non-axial dimensional parameter(s) of the cell(s) of the second cavity arm.

Claims

1. A radio-frequency (RF) cavity apparatus for accelerating charged particles, comprising first and second cavity arms, the first and second cavity arms having respective first and second axes of rotational symmetry and each cavity arm comprising at least one cell, wherein the first and second cavity aims are connected by a resonance coupler, wherein the cell(s) of the first cavity arm have an axial dimensional parameter that is equal to a corresponding axial dimensional parameter of the cell(s) of the second cavity arm, and wherein the cell(s) of the first cavity arm have at least one non-axial dimensional parameter that differs from corresponding non-axial dimensional parameter(s) of the cell(s) of the second cavity arm.

2. The cavity apparatus as claimed in claim 1, wherein more than one non-axial dimensional parameter differs between the cell(s) of the first and second cavity arms.

3. The cavity apparatus as claimed in claim 1, wherein the or each non-axial parameter is selected from a group consisting of:

a maximum width of a cell;

a maximum radius of a cell;

a minimum width of a cell;

a minimum radius of a cell; and

a curvature of a cell wall.

4. The cavity apparatus as claimed in claim 1, wherein the non-axial dimensional parameter(s) are one or more of the major and minor axes of one or more ellipses, where the ellipses correspond to portions of a cavity wall along an axial cross-section of a cell.

5. The cavity apparatus as claimed in claim 1, wherein the difference between the or each of the non-axial dimensional parameters of the cell(s) of the first cavity arm and the corresponding non-axial dimensional parameter(s) of the cell(s) of the second cavity arm, expressed as a percentage of the former, is less than about 5%, preferably less than about 3%, more preferably less than about 1%, and most preferably less than about 0.5%.

6. The cavity apparatus as claimed in claim 1, wherein the axial dimensional parameter is the length of each cell.

8. The cavity apparatus as claimed in claim 1, wherein the axial dimensional parameter value of the cell(s) of the first and second cavity arms is selected so as to support a fundamental mode in the range of about 100 MHz-10 GHz, preferably about 500 MHz-5 GHz, more preferably about 1-2.5 GHz, and most preferably about 1.3 GHz.

20. The cavity apparatus as claimed in claim 1, wherein resonance coupler is configured to strongly couple eigenmodes which have the same frequencies and to weakly couple eigenmodes which have different frequencies.

21. The cavity apparatus as claimed in claim 1, wherein the resonance coupler comprises a single coupling cell which is connected to one end of each of the cavity arms.

22. The cavity apparatus as claimed in claim 21, wherein the single coupling cell is racetrack- or oblong-shaped.

7. (canceled)

9-19. -19. (canceled)

23-35. -35. (canceled)

36. A method of recovering energy from a charged particle beam comprising:

generating a charged particle beam;

passing the charged particle beam through a first cavity aim of a radio-frequency (RF) cavity apparatus, the first cavity arm being arranged to apply an electric and/or magnetic field to accelerate the charged particle beam;

passing the charged particle beam through a second cavity arm of the radio-frequency (RF) cavity apparatus, the second cavity arm being arranged to apply an electric and/or magnetic field to decelerate the charged particle beam after it has interacted;

wherein the first and second cavity arms are connected by a resonance coupler, wherein the cell(s) of the first cavity arm have an axial dimensional parameter that is equal to a

corresponding axial dimensional parameter of the cell(s) of the second cavity arm, and wherein the cell(s) of the first cavity arm have at least one non-axial dimensional parameter that differs from corresponding non-axial dimensional parameter(s) of the cell(s) of the second cavity arm.

37. The method as claimed in claim 36, wherein more than one non-axial dimensional parameter differs between the cell(s) of the first and second cavity arms.

38. The method as claimed in claim 36, wherein the or each non-axial parameter is selected from a group consisting of:

a maximum width of a cell;

a maximum radius of a cell;

a minimum width of a cell;

a minimum radius of a cell; and

a curvature of a cell wall.

39. The method as claimed in claim 36, wherein the non-axial dimensional parameter(s) are one or more of the major and minor axes of one or more ellipses, where the ellipses correspond to portions of a cavity wall along an axial cross-section of a cell.

40. The method as claimed in claim 36, wherein the difference between the or each of the non-axial dimensional parameters of the cell(s) of the first cavity arm and the corresponding non-axial dimensional parameter(s) of the cell(s) of the second cavity arm, expressed as a percentage of the former, is less than about 5%, preferably less than about 3%, more preferably less than about 1%, and most preferably less than about 0.5%.

41. The method as claimed in claim 36, wherein the axial dimensional parameter is the length of each cell.

43. The method as claimed in claim 36, wherein the axial dimensional parameter value of the cell(s) of the first and second cavity arms is selected so as to support a fundamental mode in the range of about 100 MHz-10 GHz, preferably about 500 MHz-5 GHz, more preferably about 1-2.5 GHz, and most preferably about 1.3 GHz.

55. The method as claimed in claim 36, wherein the resonance coupler comprises a single coupling cell which is connected to one end of each of the cavity arms.

56. The method as claimed in claim 55, wherein the single coupling cell is racetrack- or oblong-shaped.

57. The method as claimed in claim 36, wherein the resonance coupler is configured to strongly couple eigenmodes which have the same frequencies and to weakly couple eigenmodes which have different frequencies.

42. (canceled)

44-54. -54. (canceled)

58-70. -70. (canceled)