Radio frequency focused drift tube linear accelerator

• US 5,523,659 A
• Filed: 08/18/1994
• Issued: 06/04/1996
• Est. Priority Date: 08/18/1994
• Status: Expired due to Fees

• Current Assignee: Swenson, Donald A.
• Original Assignee: Swenson, Donald A.
• Inventors: Swenson, Donald A.
• Primary Examiner(s): O'Shea, Sandra L.
• Assistant Examiner(s): NING, JOHN K
• Application Number:
  US08/292,487
• Time in Patent Office: 656 Days
• Field of Search: 315/5.34, 315/5.41, 315/500, 315/505, 315/506, 315/507
• US Class Current: 315/506
• CPC Class Codes: H05H 7/22 Details of linear accelerators, e.g. drift tubes H05H7/02 - H05H7/20 take precedence
• CPC Class Codes: H05H 9/00 Linear accelerators

Abstract

A drift tube linac incorporates rf-electric quadrupole focusing by employing drift tubes with only one drift-tube stem per particle wavelength and in which the lowest frequency RF cavity mode has a transverse magnetic field (TM₀₁₀ -mode). Each drift tube comprises two separate electrodes that form a capacitor that couples to the axial electric field of the primary cavity mode. The electrodes operate at different electrical potentials, as determined by the RF fields in the cavity, and are supported by a single stem along the axis of a cylindrical cavity. Each electrode supports two fingers pointing towards the opposite end of the drift tube, forming a four fingered geometry that produces an RF quadrupole field distribution along its axis. The fundamental periodicity of the structure is equal to the particle wavelength (βλ) where β is the particle velocity in units of the velocity of light and λ is the free space wavelength of the rf. The particles traverse two distinct regions, namely the gaps between drift tubes, where the acceleration takes place, and the regions inside the drift tubes, where the RF focusing takes place. The linac of the present invention transforms the reverse fields into transverse fields for focusing such that the beam is not decelerated.

Claims

1. A drift tube linear accelerator comprising

a cylindrical tank excited with RF fields in the TM₀₁₀ RF cavity mode, said tank having an input for receiving a particle beam and an output for emitting said particle beam at a higher energy level;

a plurality of drift tubes axially arranged in said tank, said plurality of drift tubes being configured to define an acceleration gap between each drift tube, wherein said particle beam is accelerated as it traverses through said gap and wherein said particle beam is focused as it traverses through said drift tube, said drift tube comprising;

a first electrode supporting a first pair of fingers protruding substantially into the center of said drift tube from a first end of said drift tube, said first pair of fingers lying in a first plane;

a second electrode supporting a second pair of fingers protruding substantially into the center of said drift tube from a second end of said drift tube opposite of said first end, said second pair of fingers lying in a second plane substantially perpendicular to said first plane; and

means for supporting said first electrode and said second electrode along said axis of said tank;

wherein said pairs of fingers form a four finger geometry and wherein said first and second electrodes have alternating RF electrical potentials of different magnitudes, said potential differences establishing RF electric quadrupole fields in a region between said pairs of fingers, said focusing of said particle beam resulting from said RF electric quadrupole fields.

2. The drift tube linear accelerator of claim 1, wherein said four finger geometries are oriented at a fundamental periodicity substantially equal to twice the particle wavelength, said distance between acceleration gaps being substantially equal to one particle wavelength.

3. The drift tube linear accelerator of claim 1, wherein said four finger geometry is oriented such that the fundamental periodicity of said four finger geometries is an even integral multiple of the particle wavelength.

4. The drift tube linear accelerator of claim 1, wherein the lengths of said drift tubes and said acceleration gaps are increased such that the fundamental periodicity of said distance between said acceleration gaps is an integral multiple of the particle wavelength.

5. The drift tube linear accelerator of claim 1, wherein said means for supporting said first electrode and said second electrode comprises ceramic rings supported at midplane by a metallic ring on a single stem, wherein said stem conducts dissipated power from said electrodes and said rings, said metallic ring and said stem being cooled by water.

6. The drift tube linear accelerator of claim 1, wherein an appropriately shaped conductor joins said first electrode with said second electrode, said conductor being supported from said tank wall by one or more stems.

7. The drift tube linear accelerator of claim 1, wherein each said electrode is supported independently from said tank wall by a single stem.

8. The drift tube linear accelerator of claim 1, wherein said accelerator operates in the range of about 200 MHZ to about 450 MHz.

9. The drift tube linear accelerator of claim 1, wherein said accelerator operates at a frequency substantially greater than 400 MHz.

10. The drift tube linear accelerator of claim 1, wherein said outer walls of said tank include post couplers to stabilize longitudinally distributed electromagnetic energy within said tank.