Method and apparatus for inductive amplification of ion beam energy

• US 8,558,461 B2
• Filed: 07/16/2010
• Issued: 10/15/2013
• Est. Priority Date: 07/20/2009
• Status: Expired due to Fees

• Current Assignee: Leland Stanford Junior University (Stanford University)
• Original Assignee: Board of Trustees of the Leland Stanford Junior University (Stanford Management Co.)
• Inventors: Cappelli, Mark A., Rieker, Gregory, Poehlmann-Martins, Flavio
• Primary Examiner(s): A, Minh D
• Application Number:
  US12/804,269
• Publication Number:
  US 20110011729A1
• Time in Patent Office: 1,187 Days
• Field of Search: 315/111.21, 315/111.31, 315/111.41, 315/111.51, 315/111.61, 315/111.71, 315/111.81, 315/111.91
• US Class Current: 315/111.51
• CPC Class Codes: H05H 15/00 Methods or devices for acceleration of charged particles not otherwise provided for , e.g. wakefield accelerators

Abstract

Accelerated charged particles are provided by inductive amplification of particle energy in connection with a deflagration-mode plasma discharge. The deflagration mode discharge tends to increase particle energy relative to other operating modes. Inductive amplification of particle energy further increases output particle velocity. Inductive amplification can occur by formation of a current loop in the plasma discharge, and/or by a sudden increase in inductance due to collapse of the current distribution of the plasma discharge. Applications include particle therapy and production of radio-isotopes.

Claims

1. A method for producing accelerated charged particles, the method comprising:

providing a plasma discharge operating in a deflagration mode and having a gas flow that defines upstream and downstream directions; and

inductively coupling energy to charged particles of the plasma discharge to provide accelerated charged particles as an output;

wherein the inductively coupling energy to charged particles is provided at least in part by formation of a current loop having an inductively amplified circulating current in or passing through part of the plasma discharge.

2. The method of claim 1, wherein an inductance of the current loop is smaller than an inductance of a current distribution prior to formation of the current loop.

3. The method of claim 1, wherein the coupling energy to charged particles is provided at least in part by application of a magnetic field.

4. The method of claim 1, wherein the plasma discharge is formed by energizing electrodes prior to providing input gas or no more than 200 μ

s after providing input gas.

5. A method for radio-isotope production comprising

providing accelerated charged particles according to the method of claim 1;

and

delivering the accelerated charged particles to a target for radio-isotope production.

6. A method for producing accelerated charged particles, the method comprising:

providing a plasma discharge operating in a deflagration mode and having a gas flow that defines upstream and downstream directions; and

inductively coupling energy to charged particles of the plasma discharge to provide accelerated charged particles as an output;

wherein the inductively coupling energy to charged particles is provided at least in part by collapse of a current distribution of the plasma discharge from a first configuration to a second configuration having greater self-inductance than the first configuration.

7. The method of claim 6, wherein the second configuration is localized at a downstream part of the first configuration.

8. A method for radio-isotope production comprising

providing accelerated charged particles according to the method of claim 6;

and

delivering the accelerated charged particles to a target for radio-isotope production.

9. Apparatus for producing accelerated charged particles, the apparatus comprising:

a plasma discharge source capable of operating in a deflagration mode and having a gas flow that defines upstream and downstream directions; and

an inductive coupling subsystem capable of inductively coupling energy to charged particles of the plasma discharge to provide accelerated charged particles as an output;

wherein an electrode length of the plasma discharge source is within about 20% of a length of the plasma discharge when inductive coupling of energy to charged particles of the plasma discharge occurs.

10. The apparatus of claim 9, wherein a circuit inductance of said apparatus is 500 nH or more.

11. The apparatus of claim 9, wherein the apparatus includes electrodes for the plasma discharge having inductance per unit length that decreases in the downstream direction.

12. The apparatus of claim 11, wherein an inductance per unit length at a downstream location of the plasma discharge is 50% or less of an inductance per unit length at an upstream location of the plasma discharge.

13. The apparatus of claim 9, wherein an electrical ringing frequency of the apparatus is 50 kHz or greater.

14. The apparatus of claim 9, further comprising a particle source disposed at a downstream location of the plasma discharge.

15. Apparatus for radio-isotope production including the apparatus for producing accelerated charged particles of claim 9.

16. Apparatus for producing accelerated charged particles, the apparatus comprising:

a plasma discharge source capable of operating in a deflagration mode and having a gas flow that defines upstream and downstream directions; and

an inductive coupling subsystem capable of inductively coupling energy to charged particles of the plasma discharge to provide accelerated charged particles as an output;

wherein the apparatus has a circuit inductance of 50 nH or less, and includes electrodes for the plasma discharge having inductance per unit length of 450 nH/m or more.

17. Apparatus for radio-isotope production including a plasma source of accelerated charged particles capable of operating in a deflagration mode to provide a particle beam having an ion beam average current of 50 μ

A or more, where particles contributing to the ion beam average current have energy between 300 keV and 5 MeV.