Achromatic and uncoupled medical gantry

• US 8,063,381 B2
• Filed: 03/13/2009
• Issued: 11/22/2011
• Est. Priority Date: 03/13/2009
• Status: Active Grant

• Current Assignee: Brookhaven Science Associates, LLC (Government of the United States of America)
• Original Assignee: Brookhaven Science Associates, LLC (Government of the United States of America)
• Inventors: Kayran, Dmitry, Tsoupas, Nicholaos, Litvinenko, Vladimir, MacKay, William W.
• Primary Examiner(s): Kim; Robert
• Assistant Examiner(s): LOGIE, MICHAEL J
• Application Number:
  US12/403,486
• Publication Number:
  US 20100230620A1
• Time in Patent Office: 984 Days
• Field of Search: None
• US Class Current: 250/396.ML
• CPC Class Codes: A61N 2005/1087 Ions; Protons
• CPC Class Codes: A61N 5/10 X-ray therapy; Gamma-ray therapy; Particle-irradiation therapy A61N5/01 takes precedence
• CPC Class Codes: A61N 5/1081 Rotating beam systems with a specific mechanical construction, e.g. gantries
• CPC Class Codes: H05H 7/04 Magnet systems , e.g. undulators, wigglers free-electron laser H01S3/0903; Energisation thereof

Abstract

A medical gantry that focus the beam from the beginning of the gantry to the exit of the gantry independent of the rotation angle of the gantry by keeping the beam achromatic and uncoupled, thus, avoiding the use of collimators or rotators, or additional equipment to control the beam divergence, which may cause beam intensity loss or additional time in irradiation of the patient, or disadvantageously increase the overall gantry size inapplicable for the use in the medical treatment facility.

Claims

1. A particle therapy gantry for delivering a particle beam to a patient comprising:

a beam tube defining a particle beam path;

a plurality of dipole magnets sequentially arranged along the beam tube for guiding the particle beam along the particle beam path; and

a plurality of quadrupole magnets that provide a fully achromatic and uncoupled beam transport for the unconstrained particle beam at the gantry entrance to the gantry isocenter;

wherein the size and shape of the particle beam is independent of the angle of gantry rotation, and wherein the gantry can be rotated by any angle between 0 and 360 with respect to a fixed incoming beam line

wherein the plurality of quadrupoles comprises six quadrupoles arranged in three quadrupole pairs with each quadrupole pair symmetrically arranged about the center between each pair of dipole magnets adjacent to the three quadrupole pairs.

2. A gantry as defined in claim 1, wherein a plurality of dipole magnets comprises three dipole magnets positioned sequentially from the gantry entrance that bend the particle beam along the defined particle beam path by angles that provide a translation of the beam in the direction of the isocenter.

3. A gantry as defined in claim 2, wherein each quadrupole pair is excited at the same strength to achieve the achromatic conditions and to satisfy the condition R_x=R_y.

4. A gantry as defined in claim 3, wherein the strength and the location of the plurality of quadrupoles is determined by the achromaticity condition R₁₆=0 and R₂₆=0, the mirror symmetry of the particle beam, which requires that R₁₁=R₂₂ and R₃₃=R₄₄, and the decoupling condition R_x=R_y.

5. A gantry as defined in claim 3, further comprises a quadrupole magnet placed in the center between the first and second dipole magnet to provide additional control on the .beta, functions to reduce the aperture of the second dipole magnet.

6. A gantry as defined in claim 5, wherein the strength and the location of the plurality of quadrupoles is determined by the achromaticity condition R₁₆=0 and R₂₆=0, the mirror symmetry of the particle beam, which requires that R₁₁=R₂₂ and R₃₃=R₄₄, and the decoupling condition R_x=R_y.

7. A gantry as defined in claim 5, wherein the strength and the location of the plurality of quadrupoles maintain the .beta, functions of less than about 30 m between the first and the second dipoles.

8. A gantry as defined in claim 7, the strength and the location of the plurality of quadrupoles maintain the .beta, functions of less than about 5.5 m at the exit of the third dipole.

9. A gantry as defined in claim 5, wherein the drift between the first and the second dipole magnet is about 5 m.

10. A gantry as defined in claim 3, further comprises a quadrupole magnet placed in the center between the second and third dipole magnet to provide additional control on the .beta, functions to reduce the aperture of the third dipole magnet.

11. A gantry as defined in claim 10, wherein the strength and the location of the plurality of quadrupoles is determined by the achromaticity condition R₁₆=0 and R₂₆=0, the mirror symmetry of the particle beam, which requires that R₁₁=R₂₂ and R₃₃=R₄₄, and the decoupling condition R_x=R_y.

12. A gantry as defined in claim 10, wherein the strength and the location of the plurality of quadrupoles maintain the .beta, functions of less than about 30 m between the second and the third dipoles.

13. A gantry as defined in claim 12, the strength and the location of the plurality of quadrupoles maintain the .beta, functions of less than about 5.5 m at the exit of the third dipole.

14. A gantry as defined in claim 3, further comprises a quadrupole magnet placed in the center between each pair of dipole magnets to provide additional control on the .beta, functions to reduce the aperture of the second and third dipole magnets.

15. A gantry as defined in claim 14, wherein the strength and the location of the plurality of quadrupoles is determined by the achromaticity condition R₁₆=0 and R₂₆=0, the mirror symmetry of the particle beam, which requires that R₁₁=R₂₂ and R₃₃=R₄₄, and the decoupling condition R_x=R_y.

16. A gantry as defined in claim 14, wherein the strength and the location of the plurality of quadrupoles maintain the .beta, functions of less than about 30 m between the second and the third dipoles.

17. A gantry as defined in claim 16, the strength and the location of the plurality of quadrupoles maintain the .beta, functions of less than about 5.5 m at the exit of the third dipole.

18. A gantry as defined in claim 2, wherein the plurality of quadrupoles comprises eight quadrupoles, wherein four quadrupoles are positioned along the axis of rotation before the first dipole magnet, two are positioned between the first and the second dipole and two are positioned between the second and the third dipole to achieve the achromatic conditions and to satisfy the condition R_x=R_y.

19. A gantry as defined in claim 18, wherein the strength and the location of the plurality of quadrupoles is determined by the achromaticity condition R₁₆=0 and R₂₆=0, the mirror symmetry of the particle beam, which requires that R₁₁=R₂₂ and R₃₃⁼R₄₄, and the decoupling condition R_x=R_y.

20. A method for delivering an unconstrained particle beam to a patient through a gantry comprising the steps of:

bending the unconstrained particle beam with a plurality of fixed field dipole magnets sequentially arranged along a beam tube of the gantry for the particle beam traveling in said beam tube;

maintaining the achromatic and uncoupled conditions of the particle beam from the gantry exit to the isocenter of the particle beam path by a plurality of quadrupole magnets;

wherein the size and shape of the particle beam is independent of the angle of gantry rotation for the particle beam unconstrained at the gantry entrance,

wherein the gantry can be rotated by any angle between 0 and 360 with respect to a fixed incoming beam line and wherein the plurality of quadrupoles comprises six quadrupoles arranged in three quadrupole pairs with each quadrupole pair symmetrically arranged about the center between each pair of dipole magnets adjacent to the three quadrupole pairs.

21. A method as defined in claim 20, wherein a plurality of dipole magnets comprises three dipole magnets positioned sequentially from the gantry entrance that bend the particle beam along the defined particle beam path by angles that provide a translation of the beam in the direction of the isocenter.

22. A method as defined in claim 21, wherein each quadrupole pair is excited at the same strength to achieve the achromatic conditions and the decoupling condition R_x=R_y.

23. A method as defined in claim 22, wherein the plurality of quadrupoles comprises six quadrupoles arranged in pairs about the center between the first and second dipole and six quadrupoles arranged in pairs about the center between the second and the third dipole.

24. A method as defined in claim 23, comprises a quadrupole magnet placed in the center between the first and the second dipole magnet to provide additional control on the .beta, functions.

25. A method as defined in claim 23, comprises a quadrupole magnet placed in the center between the second and the third dipole magnet to provide additional control on the .beta, functions.

26. A method as defined in claim 23, comprises a quadrupole magnet placed in the center between the first and the second dipole magnet and the second and the third dipole magnet to provide additional control on the .beta, functions.

27. A method as defined in claim 22, wherein the strength and the location of the plurality of quadrupoles maintain the .beta, functions of less than about 30 m between each set of dipoles and maintains the .beta, functions of less than about 5.5 m at the exit of the third dipole.