A high-intensity external ion injector can includes (a) an ion source defining a plasma chamber and including an aperture through which ions can escape the plasma chamber, (b) a microwave source configured to generate microwave radiation and direct the microwave radiation into the plasma chamber, (c) a gas source filled with a plasma-forming gas and configured to supply the plasma-forming gas to the plasma chamber, (d) a voltage source configured to apply a voltage to the plasma chamber, (e) an einzel triplet lens, (f) an ion focus positioned and configured to focus an ion beam exiting the aperture of the ion source through the einzel triplet lens, and (g) a periodic focusing structure positioned and configured to receive an ion beam exiting the einzel triplet lens.

A gantry-less particle therapy system is provided. Charged particles are extracted from an ion source and accelerated in a beam transport system having an annular portion extending in a first plane and that circumscribes a volume, an arcuate portion extending in a second plane, and a transition portion that connects the annular portion and the arcuate portion. The arcuate portion terminates at a beam nozzle extending radially inward from the annular portion to deliver an ion beam to a treatment area contained in the volume circumscribed by the annular portion.

A low-erosion radio frequency ion source is disclosed having a hollow body with conductive interior walls that define a cylindrical cavity, with a gas supply inlet for plasma-forming gases and a power supply inlet for injecting radio frequency energy into the cavity; an expansion chamber connected to the cavity by means of a plasma outlet hole; an ion-extraction aperture in contact with the expansion chamber; coaxial conductor disposed in the cavity, parallel to the longitudinal axis thereof, one or both ends of the coaxial conductor being in contact with a circular interior wall of the body, forming a coaxial resonant cavity; the coaxial conductor having a conductive protuberance opposite the plasma outlet hole and which extends radially into the cavity. It substantially reduces the erosion of the conductive materials.

A device for guiding charge carriers and uses of the device are proposed, wherein the charge carriers are guided by means of a magnetic field along a curved or angled main path in a two-dimensional electron gas or in a thin superconducting layer, so that a different presence density is produced at electrical connections.

An accelerator includes: a plurality of ion sources 221, 222, and 233 that generate a plurality of different types of ions; an electromagnet 11 that generates a magnetic field; and a high frequency cavity 21 that generates a high frequency electric field. The center of an orbit of the ion is eccentric with acceleration, the magnetic field generated by the electromagnet 11 is a magnetic field distribution that decreases outward in a radial direction of the orbit, the high frequency cavity 21 accelerates the ion up to a predetermined energy by the high frequency electric field adjusted to an orbital frequency in response to a nuclide of the incident ion, and a frequency of the high frequency electric field changes following an energy of the ion. Accordingly, it is possible to provide an accelerator and a particle therapy system capable shortening an irradiation time with a small size.

In a circular accelerator that applies a radiofrequency wave in a main magnetic field to accelerate charged particle beam while increasing an orbit radius, another radiofrequency wave with a frequency different from the radiofrequency wave used for acceleration is applied to the charged particle beam in order to extract the charged particle beam. Thereby, in the circular accelerator that accelerates charged particle beam while increasing an orbit radius by applying a radiofrequency wave in a main magnetic field, the high precision control on extraction of the charged particle beam from the circular accelerator is achieved.

An acceleration radiofrequency acceleration system capable of frequency modulation and feeding an acceleration radiofrequency wave for accelerating a beam, a radiofrequency kicker 70 feeding an extraction radiofrequency wave different in frequency, from the acceleration radiofrequency wave for extracting a beam, a peeler magnetic field region 44 and a regenerator magnetic field region 45 for forming a disturbance magnetic field region including a high-order magnetic field that includes a magnetic field component having a number of poles of two poles or more and that includes at least a quadrupole magnetic field component, a shim of a magnetic material, and a septum magnet 43, 43A, 43B having an inner peripheral side septum coil conductor 5, an outer peripheral side septum coil conductor 6, a coil conductor connecting portion 7, and a coil lead-out portion 8 are provided.

A linear accelerator comprises a plurality of cyclotrons arranged axially in a cyclotron stack, each cyclotron having a set of dees and a central aperture passing through the set of dees. Each central aperture is axially aligned with one another in the stack, forming a central channel having an inlet and an outlet that passes through the stack. Magnets are positioned so as to generate a magnetic field perpendicular to the set of dees. A power supply applies an oscillating voltage to each set of dees of the stack. In operation, subatomic particles are ejected radially outwardly of the stack, creating a dead zone within the central channel that is void of particles and electromagnetic fields. A mass or light beam is accelerated as it passes through the central channel's dead zone, due to the absence of frictional forces acting on the mass or light within the dead zone.

The invention comprises a method and apparatus for scanning charged particles in a cancer therapy system, comprising the steps of: (1) providing a first and second dipole magnet system and a gap, the gap comprising a common gap length, along a path of the charged particles, within both the first and second dipole magnet systems, the gap comprising a progressively increasing x/y-plane cross-section area from an entrance area of the charged particles into the double dipole magnet system to an exit area of the double dipole magnet system, the x/y-plane perpendicular to a z-axis from a center of the entrance area to a center of the exit area; (2) scanning the positively charged particles along a first axis of the x/y-plane using the first dipole magnet system; and (3) scanning the positively charged particles along a second axis of the x/y-plane using the second dipole magnet system.

In a magnetic device 1, on faces opposite to a middle plane 2 between an upper magnetic pole 8 and a lower magnetic pole 9, recesses 21a, 21b, 21c, and 21d and projections 22a, 22b, 22c, and 22d are alternately placed along a beam circling direction. In the projections 22a, 22b, 22c, and 22d, angle widths θ of the projections 22a, 22b, 22c, and 22d when viewed from the center O1 of a beam closed orbit is narrowed as beam energy is increased. On the outer circumferential region of the recess 21a on the upper magnetic pole 8 and the lower magnetic pole 9, the inlet of an extraction channel 1019 that extracts a beam accelerated to a predetermined energy to outside an accelerator 1004 is provided.