Compact cold, weak-focusing, superconducting cyclotron

• US 8,525,447 B2
• Filed: 11/22/2010
• Issued: 09/03/2013
• Est. Priority Date: 11/22/2010
• Status: Active Grant

• Current Assignee: Massachusetts Institute of Technology
• Original Assignee: Massachusetts Institute of Technology
• Inventors: Antaya, Timothy A.
• Primary Examiner(s): Jackson, Jr., Jerome
• Assistant Examiner(s): LOTTER, DAVID E
• Application Number:
  US12/951,968
• Publication Number:
  US 20120126726A1
• Time in Patent Office: 1,016 Days
• Field of Search: 315/502
• US Class Current: 315/502
• CPC Class Codes: H05H 13/005 Cyclotrons

Abstract

A compact, cold, weak-focusing superconducting cyclotron can include at least two superconducting coils on opposite sides of a median acceleration plane. A magnetic yoke surrounds the coils and contains an acceleration chamber. The magnetic yoke is in thermal contact with the superconducting coils, and the median acceleration plane extends through the acceleration chamber. A cryogenic refrigerator is thermally coupled both with the superconducting coils and with the magnetic yoke.

Claims

1. A compact, cold, weak-focusing superconducting cyclotron comprising:

at least two superconducting coils, centered around a central axis with outer surfaces remote from the central axis, wherein the coils are on opposite sides of a median acceleration plane and have opposed median-acceleration-plane-facing surfaces;

a magnetic yoke surrounding the coils and in physical contact with the coils across the outer surface of each coil and across the median-acceleration-plane-facing surface of each coil to substantially reduce or eliminate strain on the coils due to decentering forces and without an intervening cryostat between the magnetic yoke and the coils, wherein the magnetic yoke contains an acceleration chamber, wherein the magnetic yoke is in thermal contact with the superconducting coils, wherein the median acceleration plane extends through the acceleration chamber, and wherein the superconducting coils and the physically coupled magnetic yoke are configured to generate a magnetic field that reaches at least 6 Tesla in the median acceleration plane;

a cryogenic refrigerator physically and thermally coupled with the superconducting coils and with the magnetic yoke; and

a cryostat mounted outside the magnetic yoke and containing the coils and the magnetic yoke inside a thermally insulated volume in which the coils and the magnetic yoke can be maintained at cryogenic temperatures by the cryogenic refrigerator.

2. The cyclotron of claim 1, wherein the superconducting coils are physically supported by the magnetic yoke.

3. The cyclotron of claim 1, further comprising a pair of electrodes coupled with a radiofrequency voltage source and mounted in the acceleration chamber to accelerate ions orbiting in the acceleration chamber.

4. The cyclotron of claim 3, further comprising a thermally insulating structure separating the electrodes from the magnetic yoke and the superconducting coils.

5. The cyclotron of claim 1, wherein the magnetic yoke includes a pair of poles on opposite sides of the median acceleration plane, wherein each pole is structured to produce a radially decreasing magnetic field across the median acceleration plane from an inner radius for ion introduction to an outer radius for ion extraction.

6. The cyclotron of claim 5, wherein the magnetic yoke includes a radially extending vacuum feed-through port providing access through the magnetic yoke to the acceleration chamber, and wherein a separation gap between the poles decreases over the vacuum feed-through port.

7. The cyclotron of claim 5, wherein the poles extend radially about 10 cm from a central axis to the superconducting coils.

8. The cyclotron of claim 7, wherein each pole has a profile including stages that can be designated A, B, C and D, wherein stages A, B, C and D extend radially outward from a central axis in alphabetical order, and wherein the poles are separated by about 7 cm at stage B.

9. The cyclotron of claim 8, wherein the poles are separated by about 1.6 cm at stage D.

10. The cyclotron of claim 9, wherein the poles are separated by about 5 cm at each of stages A and C.

11. The cyclotron of claim 10, wherein the superconducting coils are separated by about 7 cm.

12. The cyclotron of claim 11, wherein each of stages A, B, C and D extend across a radial distance from the central axis that is substantially the same as the radial distance over with the other stages extend.

13. The cyclotron of claim 5, wherein the magnetic yoke is structured to contribute no more than 2.5 Tesla to the median acceleration plane when the magnetic yoke is fully magnetized.

14. The cyclotron of claim 13, wherein the superconducting coils are structured to contribute at least 3 Tesla to the median acceleration plane.

15. The cyclotron of claim 1, wherein the superconducting coils comprise a material that is superconducting at a temperature of at least 4 K.

16. The cyclotron of claim 1, wherein the magnetic yoke comprises iron.

17. A method for ion acceleration comprising:

employing a cyclotron comprising;

a) at least two superconducting coils, centered around a central axis with outer surfaces remote from the central axis, wherein the coils are on opposite sides of a median acceleration plane and have opposed median-acceleration-plane-facing surfaces;

b) a magnetic yoke surrounding the coils, and in physical contact with the coils across the outer surface of each coil and across the median-acceleration-plane-facing surface of each coil to substantially reduce or eliminate strain on the coils due to decentering forces and without an intervening cryostat between the magnetic yoke and the coils, wherein the magnetic yoke contains an acceleration chamber, wherein the magnetic yoke is in thermal contact with the superconducting coils, wherein the median acceleration plane extends through the acceleration chamber, and wherein the superconducting coils and the physically coupled magnetic yoke are configured to generate a magnetic field that reaches at least 6 Tesla in the median acceleration plane;

c) a cryogenic refrigerator physically and thermally coupled with the superconducting coils and with the magnetic yoke;

d) an electrode coupled with a radiofrequency voltage source and mounted in the acceleration chamber; and

e) a cryostat mounted outside the magnetic yoke and containing the coils and the magnetic yoke;

introducing an ion into the median acceleration plane at an inner radius;

providing a radiofrequency voltage from the radiofrequency voltage source to the electrode to accelerate the ion in an expanding orbit across the median acceleration plane;

cooling the superconducting coils and the magnetic yoke with the cryogenic refrigerator, wherein the superconducting coils are cooled to a temperature no greater than their superconducting transition temperature, and wherein the magnetic yoke is cooled to a temperature no greater than 100 K;

providing a voltage to the cooled superconducting coils to generate a superconducting current in the superconducting coils that produces a magnetic field reaching at least 6 Tesla in the median acceleration plane from the superconducting coils and from the yoke; and

extracting the accelerated ion from acceleration chamber at an outer radius.

18. The method of claim 17, wherein the electrode is maintained at a temperature at least 40 K higher than the magnetic yoke and the superconducting coils.

19. The method of claim 17, wherein the magnetic field produced in the median acceleration plane decreases with radius from the inner radius for ion introduction to the outer radius for ion extraction.

20. The method of claim 17, wherein the magnetic field produced in the median acceleration plane reaches at least 8 Tesla.

21. The method of claim 20, wherein at least 5 Tesla of the field of at least 8 Tesla is produced by the superconducting coils.

22. The method of claim 17, wherein the superconducting coils are centered about a central axis, and wherein the produced magnetic field is substantially axially symmetric about the central axis from the inner radius for ion introduction to the outer radius for ion extraction.

23. The method of claim 17, wherein the ion is accelerated at a fixed frequency from the inner radius for ion introduction to the outer radius for ion extraction.

24. A cyclotron positioned about a central axis, the cyclotron comprising:

an ion source at an inner radius from the central axis for introducing into an acceleration chamber an ion to be accelerated by the cyclotron in a median acceleration plane inside the acceleration chamber;

an ion extraction apparatus at an outer radius from the central axis for extracting the ion from the acceleration chamber;

an electrode including a pair of plates, one on each side of the median acceleration plane for orbitally accelerating the ion from the inner radius to the outer radius;

a pair of electrically conductive coils centered about the central axis and configured to generate a magnetic field in the acceleration chamber;

a magnetic yoke surrounding the electrode and the electrically conductive coils and including a pair of poles joined at a perimeter and separated on opposite sides of the electrode across a pole gap, wherein the magnetic yoke defines a vacuum feed-through port that provides access to the electrode, and wherein the pole gap narrows at angles from the central axis that cross the vacuum feed-through port and expands at angles from the central axis that are away from the vacuum feed-through port; and

an electrically conductive conduit that extends through the vacuum feed-through port and is coupled with the electrode.