Compact isochronal cyclotron

• US 5,521,469 A
• Filed: 05/12/1994
• Issued: 05/28/1996
• Est. Priority Date: 11/22/1991
• Status: Expired due to Term

• Current Assignee: Ion Beam Applications s.a.
• Original Assignee: Ion Beam Applications s.a.
• Inventors: Laisne, Andre E. P.
• Primary Examiner(s): O'Shea, Sandra L.
• Assistant Examiner(s): NING, JOHN K
• Application Number:
  US08/240,786
• Time in Patent Office: 747 Days
• Field of Search: 313/62, 313/507, 315/502, 335/216, 335/299
• US Class Current: 315/502
• CPC Class Codes: H05H 13/00 Magnetic resonance accelerators; Cyclotrons strophotrons, turbine tubes H01J25/62

Abstract

A superconducting or non-superconducting compact isochronic cyclotron in which the particle beam is sectorally focused. The cyclotron comprising a solenoid forming a magnetic circuit which is energized by at least one pair of circular main coils surrounding the solenoid poles. The magnetic circuit includes at least three pairs of sectors known as "hills", where the air gap is reduced, separated by sector-shaped spaces known as "valleys", where the air gap is larger. The air gap between the hills has a substantially elliptical curved profile which completely closes off the radial end of the hills at the center plane.

Claims

1. A compact isochronal cyclotron in which the particle beam is focused by sectors, comprising an electromagnet having two poles, said poles defining a mid-plane and constituting a magnetic circuit which includes at least three pairs of sectors (3 and 3'"'"') called "hills" where the air gap is reduced, these being separated by spaces in the form of sectors (4) called "valleys" where the air gap has a greater dimension and which is energized by at least one pair of main circular coils (6) surrounding the poles of the electromagnet, this cyclotron being characterized in that the air gap (8) located between the two hills (3 and 3'"'"') has an essentially elliptical changing profile which tends towards complete closure at the radial extremity of the hills, called the hill radius (R_c), on the mid-plane (10).

2. Cyclotron according to claim 1, characterized in that the air gap (8) between two hills (3 and 3'"'"') closes up completely at the hill radius (R_c) on the mid-plane (10).

3. Cyclotron according to claim 1, characterized in that the air gap (8) between two hills (3 and 3'"'"') has a slight opening, at the hill radius (R_c), preferably less than the vertical dimension of the beam to be extracted.

4. Cyclotron according to claim 2, characterized in that a magnetic shunt (9) produced in continuity with the poles of the electromagnet is placed between each pair of hills (3 and 3'"'"') beyond the radial extremity (R_c) of the hills.

5. Cyclotron according to claim 4, characterized in that at least one magnetic shunt (9) is equipped with at least one opening (11) so as to enable the extracted beam to pass.

6. Cyclotron according to claim 4, characterized in that the magnetic shunts (9) are in the form of a metal screen having a thickness lying between 2 and 10 mm and preferably of the order of 6.5 mm.

7. Cyclotron according to claim 1, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

9. Cyclotron according to claim 3, characterized in that a magnetic shunt (9) produced in continuity with the poles of the electromagnet is placed between each pair of hills (3 and 3'"'"') beyond the radial extremity (R_c) of the hills.

10. Cyclotron according to claim 9, characterized in that at least one magnetic shunt (9) is equipped with at least one opening (11) so as to enable the extracted beam to pass.

11. Cyclotron according to claim 5, characterized in that the magnetic shunts (9) are in the form of a metal screen having a thickness lying between 2 and 10 mm and preferably of the order of 6.5 mm.

12. Cyclotron according to claim 10, characterized in that the magnetic shunts (9) are in the form of a metal screen having a thickness lying between 2 and 10 mm and preferably of the order of 6.5 mm.

13. Cyclotron according to claim 2, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

14. Cyclotron according to claim 3, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

15. Cyclotron according to claim 4, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

16. Cyclotron according to claim 5, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

17. Cyclotron according to claim 6, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

18. Cyclotron according to claim 9, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

19. Cyclotron according to claim 10, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

20. Cyclotron according to claim 11, characterized in that the extraction system associated with the cyclotron is composed of a single electrostatic deflector followed by preferably two or three focusing electrostatic channels.

8. A method for accelerating protons to an energy greater than 150 MeV comprising subjecting the protons to a magnetic field provided by a magnetic circuit which includes at least three pairs of sectors (3 and 3'"'"') called "hills" where the air gap is reduced, these being separated by spaces in the form of sectors (4) called "valleys" where the air gap has a greater dimension and which is energized by at least one pair of main circular coils (6) surrounding the poles of the electromagnet, said poles defining a mid-plane, this cyclotron being characterized in that the air gap (8) located between two hills (3 and 3'"'"') has an essentially elliptical changing profile which tends towards complete closure at the radial extremity of the hills, called the hill radius (R_c), on the mid-plane (10).