Standing wave particle beam accelerator with switchable beam energy

• US 6,366,021 B1
• Filed: 01/06/2000
• Issued: 04/02/2002
• Est. Priority Date: 01/06/2000
• Status: Expired due to Fees

• Current Assignee: Varian Medical Systems Incorporated (Siemens AG)
• Original Assignee: Varian Medical Systems Incorporated (Siemens AG)
• Inventors: Meddaugh, Gard E., Kalkanis, Gregory
• Primary Examiner(s): Wong, Don
• Assistant Examiner(s): VO, TUYET THI
• Application Number:
  US09/479,466
• Time in Patent Office: 817 Days
• Field of Search: 315/5.41, 315/5.42, 315/500, 315/501, 315/506, 315/507, 315/3.39
• US Class Current: 315/5.41
• CPC Class Codes: H01J 2223/20 Cavity resonators; Adjustment or tuning thereof
• CPC Class Codes: H05H 7/18 Cavities; Resonators travelling-wave tubes H01J23/18; hyperfrequency cavities in general H01P7/04, H01P7/06
• CPC Class Codes: H05H 9/04 Standing-wave linear accelerators

Abstract

A standing wave particle beam accelerator in which the electric fields in one side coupling cavity are switched by inserting two probes of selected diameter to provide different upstream and downstream electric field coupling to adjacent coupled accelerator cavities.

Claims

1. In an accelerator for accelerating a particle beam, a chain of resonant electromagnetic cavities coupled in series along an axis and resonant at approximately the same frequency,

a cylindrical coupling cavity coupled to each of at least two intermediate adjacent cavities through irises,

conductors extending parallel to the axis into said coupling cavity with their ends spaced from one another,

at least first and second probes mounted for independent radial insertion into said coupling cavity at a radial angle with respect to one another, and with their ends adjacent and selectively coupled to one or the other of said conductors to change the distribution of electromagnetic fields in the cavity whereby the electromagnetic field coupling between said two adjacent cavities is changed with the selective insertion of said probes to thereby change the energy of the particle beam from a first value with both probes retracted and uncoupled to a second value with only one probe inserted and coupled to one conductor and a third value with only the other probe inserted and coupled to one the or the other conductor.

2. The accelerator of claim 1 in which said first and second probes are both on one side of the longitudinal centerline of the coupling cavity.

3. The accelerator of claim 1 in which said first and second probes are on opposite sides of the longitudinal centerline of the coupling cavity.

4. The accelerator of claims 1, 2 or 3 wherein the coupling of the electromagnetic fields to the two adjacent cavities is through irises and the probes change the distribution of electromagnetic field with respect to the irises.

5. The accelerator of claims 1, 2 or 3 an which the diameter of the first and second probes is selected to control the frequency of the cavity.