Abstract:
A particle therapy system includes a particle accelerator to output a particle beam; and a scanning system for the particle accelerator to scan the particle beam across at least part of an irradiation target. The scanning system is configured to scan the particle beam in two dimensions that are at an angle relative to a direction of the particle beam. A structure defines an edge. The structure is controllable to move in the two dimensions relative to the irradiation target such that at least part of the structure is between at least part of the particle beam and the irradiation target. The structure includes a material that inhibits transmission of the particle beam.
Abstract:
In an example, a synchrocyclotron includes a particle source to provide pulses of ionized plasma to a cavity; a voltage source to provide a radio frequency (RF) voltage to the cavity to accelerate particles from the plasma column outwardly; and an extraction channel to receive a beam of particles from the cavity for output from the particle accelerator. The particle source is configured to control pulse widths of the ionized plasma in order to control an intensity of the beam of particles. This example synchrocyclotron may include one or more of the following features, either alone or in combination.
Abstract:
A particle therapy system includes a particle accelerator to output a particle beam; and a scanning system for the particle accelerator to scan the particle beam across at least part of an irradiation target. The scanning system is configured to scan the particle beam in two dimensions that are at an angle relative to a direction of the particle beam. A structure defines an edge. The structure is controllable to move in the two dimensions relative to the irradiation target such that at least part of the structure is between at least part of the particle beam and the irradiation target. The structure includes a material that inhibits transmission of the particle beam.
Abstract:
Systems and methods are provided to perform efficient, automatic adjustment of cyclotron beam currents within a wide range for multiple treatment layers within the same patient and treatment session; and to perform efficient, automatic cyclotron initialization, and calibration. In an embodiment, efficient adjustment is achieved by using beam current attenuation by an electrostatic vertical deflector installed in the inner center of the cyclotron. The beam current may, for example, be adjusted by the high voltage applied to the electrostatic vertical deflector, in front of each treatment the attenuation curve of the vertical deflector is recorded. Based on this attenuation curve, the vertical deflector voltage for the needed beam current of each irradiation layer is interpolated. In another embodiment, a process is provided that allows the automation of the initialization of a cyclotron after overnight or maintenance imposed shutdown. In one embodiment, five independent cyclotron system states are defined and the transition between one state to another may be automated, e.g., by the control system of the cyclotron.
Abstract:
Systems and methods are provided to perform efficient, automatic adjustment of cyclotron beam currents within a wide range for multiple treatment layers within the same patient and treatment session; and to perform efficient, automatic cyclotron initialization, and calibration. In an embodiment, efficient adjustment is achieved by using beam current attenuation by an electrostatic vertical deflector installed in the inner center of the cyclotron. The beam current may, for example, be adjusted by the high voltage applied to the electrostatic vertical deflector, in front of each treatment the attenuation curve of the vertical deflector is recorded. Based on this attenuation curve, the vertical deflector voltage for the needed beam current of each irradiation layer is interpolated. In another embodiment, a process is provided that allows the automation of the initialization of a cyclotron after overnight or maintenance imposed shutdown. In one embodiment, five independent cyclotron system states are defined and the transition between one state to another may be automated, e.g., by the control system of the cyclotron.
Abstract:
A linear particle accelerating structure is provided for accelerating protons using radio frequency, RF, radiation, the structure comprising at least two coupled resonant cavity units. Each resonant cavity unit comprising a corresponding resonant cavity with an input port and an output port for a beam of protons; and an RF input to receive an RF signal; an RF phase shifter to control the phase of the RF signal. The particle accelerating structure further comprises at least one RF phase shifter to adjust, in one or more of the respective cavities, a phase of the RF signal to expose the protons to an accelerating portion of the electric field for a first duration and to expose the protons to a decelerating portion of the electric field for a second duration, wherein the first duration is greater than the second duration and greater than zero and wherein the second duration is greater than or equal to zero.
Abstract:
Radio-frequency (RF) electrode for a cyclotron. The RF electrode includes a hollowed dee having first and second surfaces that oppose each other and define a gap therebetween. The hollowed dee is configured to be electrically controlled to direct a beam of charged particles through the gap and along an orbit plane of the cyclotron. The orbit plane extends parallel to the first and second surfaces through the gap. The RF electrode also includes a bridge structure that is coupled to and extends away from the hollowed dee. The bridge structure includes a side wall that defines an interior cavity of the bridge structure. The side wall has a particle opening therethrough that coincides with or is proximate to the orbit plane such that the particle opening receives neutral particles from an orbit of the charged particles.
Abstract:
A system for focusing and accelerating a beam of electrically charged particles, for example protons. The system comprises: a beam generator; a charge pulse generator;and a focusing and accelerating device comprising a body with a core. The body defines a charge path extending along the body and beam generator directs a beam of electrically charged particles through the core. The charge pulse generator simultaneously delivers charge pulses to the charge path. The charge path may be helical in shape. Movement of the charge pulse along the path creates an electric field that simultaneously accelerates and focuses the beam.
Abstract:
Die Erfindung betrifft einen Teilchenbeschleuniger (100) zum Beschleunigen eines helixförmigen Strahls (150) geladener Teilchen (151), die sich jeweils mit einer vorgegebenen Geschwindigkeit (v 1 ) gradlinig entlang einer vorgegebenen Achse (101) bewegen, umfassend: - eine kreiszylinderförmige HF-Kavität (110) mit einem ringförmigen Eintrittsspalt (113) und einem dem Eintrittsspalt (113) gegenüber liegenden ringförmigen Austrittsspalt (115) für den helixförmigen Teilchenstrahl (150), und - eine HF-Generatoreinrichtung (120) zum Erzeugen einer zirkular polarisierten elektromagnetischen Welle (160) innerhalb der HF-Kavität (110), wobei die zirkulär polarisierte elektromagnetische Welle ein in Richtung der Achse (101) orientiertes und synchron mit der Eintrittsstelle des helixförmigen Teilchenstrahls (150) in die HF-Kavität (110) um die Achse (101) rotierendes elektrisches Feld (161) umfasst. Ferner betrifft die Erfindung eine Beschleunigeranordnung sowie ein Verfahren zum Beschleunigen eines helixförmigen Strahls (150) geladener Teilchen (151).