Programmable Particle Scatterer for Radiation Therapy Beam Formation

• US 20100308235A1
• Filed: 05/06/2010
• Published: 12/09/2010
• Est. Priority Date: 07/21/2004
• Status: Abandoned Application

• Current Assignee: Mevion Medical Systems Incorporated
• Original Assignee: Still River Systems Incorporated
• Inventors: Gall, Kenneth, Sliski, Alan
• Application Number:
  US12/775,007
• Publication Number:
  US 20100308235A1
• Time in Patent Office: Days
• US Class Current: 250/492.3
• CPC Class Codes: A61N 2005/1087 Ions; Protons
• CPC Class Codes: A61N 2005/1095 Elements inserted into the radiation path within the system, e.g. filters or wedges
• CPC Class Codes: A61N 5/1077 Beam delivery systems
• CPC Class Codes: G21K 1/08 Deviation, concentration or focusing of the beam by electric or magnetic means electron-optical arrangements in electric discharge tubes H01J29/46; details, e.g. electric or magnetic deviating means for direct voltage accelerators or in accelerators using single pulses H05H5/02; arrangements for injecting particles into orbits H05H7/08; arrangements for ejecting particles from orbits H05H7/10
• CPC Class Codes: G21K 5/04 with beam-forming means
• CPC Class Codes: H05H 7/00 Details of devices of the types covered by groups H05H9/00, H05H11/00, H05H13/00

Abstract

Interposing a programmable path length of one or more materials into a particle beam modulates scattering angle and beam range in a predetermined manner to create a predetermined spread out Bragg peak at a predetermined range. Materials can be “low Z” and “high Z” materials that include fluids. A charged particle beam scatterer/range modulator can comprise a fluid reservoir having opposing walls in a particle beam path and a drive to adjust the distance between the walls of the fluid reservoir under control by a programmable controller. A “high Z” and, independently, a “low Z” reservoir, arranged in series, can be used. When used for radiation treatment, the beam can be monitored by measuring beam intensity, and the programmable controller can adjust the distance between the opposing walls of the “high Z” reservoir and, independently, the distance between the opposing walls of the “low Z” reservoir according to a predetermined relationship to integral beam intensity. Beam scattering and modulation can be done continuously and dynamically during a treatment in order to deposit dose in a target volume in a predetermined three dimensional distribution.

Claims

1-32. -32. (canceled)

33. An apparatus for scattering and/or modulating a range of a charged particle beam, the apparatus comprising:

high Z material having a path length in a path of a charged particle beam;

low Z material having a path length in the path of the charged particle beam, at least one of the high Z and low Z materials including a liquid; and

a controller configured to adjust the path lengths of the high Z and low Z materials during exposure of a target to the charged particle beam.

34. The apparatus of claim 33 wherein the path lengths of the high Z and low Z materials are independently adjustable.

35. The apparatus of claim 33 wherein the path length of the low Z material and, independently, the path length of the high Z material are continuously adjustable.

36. The apparatus of claim 33 wherein the controller is programmable.

37. The apparatus of claim 33 wherein the charged particle beam includes protons.

38. The apparatus of claim 33 further including:

a source of charged particles that provides the charged particle beam.

39. The apparatus of claim 38 wherein the source is a cyclotron.

40. The apparatus of claim 39 wherein the cyclotron is a synchrocyclotron.

41. The apparatus of claim 40 wherein the low Z and high Z materials are in an extraction channel of the synchrocyclotron.

42. The apparatus of claim 39 further including:

a beam monitor configured to measure intensity of the charged particle beam, the beam monitor communicating the intensity to the controller, the controller adjusting the low Z and, independently, the high Z path lengths according to integral intensity.

43. The apparatus of claim 42 wherein the controller is configured to adjust the path length of the low Z material and, independently, the path length of the high Z material continuously and dynamically.

44. A method of scattering and/or modulating a range of a charged particle beam, comprising:

directing the charged particle beam through a high Z material having a path length in a charged particle beam path;

directing the charged particle beam through a low Z material having a path length in the charged particle beam path, at least one of the high Z and low Z materials including a liquid; and

adjusting the path lengths of the high Z and low Z materials during exposure of a target to the charged particle beam.

45. The method of claim 44 wherein adjusting the path lengths of the high Z and low Z materials includes adjusting the path lengths independently.

46. The method of claim 44 wherein the path length of the low Z material and, independently, the path length of the high Z material are continuously adjustable.

47. The method of claim 44 further including:

measuring intensity of the charged particle beam; and

wherein adjusting the path lengths of the high Z and low Z materials includes adjusting the path lengths according to the intensity.

48. The method of claim 47 wherein adjusting the path lengths of the high Z and low Z materials includes adjusting the path lengths continuously and dynamically.

49. The apparatus of claim 44 wherein the charged particle beam includes protons.

50. The method of claim 49 further including:

producing the charged particle beam.

51. The method of claim 50 wherein the charged particle beam is produced by a cyclotron.

52. The method of claim 51 wherein the cyclotron is a synchrocyclotron.

53. The method of claim 52 wherein the low Z and high Z materials are in an extraction channel of the synchrocyclotron.

54. The method of claim 44 wherein the target is within a patient.