H05H7/00

Charge stripping film for ion beam

A charge stripping method includes irradiating a charge stripping film with an ion beam. The charge stripping film includes a single layer body of a graphitic film having a carbon component of at least 96 at % and a thermal conductivity in a film surface direction at 25 C. of at least 800 W/mK, or a laminated body of the graphitic film. The charge stripping film has a thickness of not less than 100 nm and less than 10 m, a tensile strength in a film surface direction of at least 5 MPa, a coefficient of thermal expansion in the film surface direction of not more than 110.sup.5/K, and an area of at least 4 cm.sup.2.

Self-shielding accelerator and pet plastic bottle production line utilizing same

A self-shielding accelerator is provided, which includes an accelerator assembly, a high-frequency electrode plate, a rectification and voltage multiplication assembly, a solenoid-type transformer assembly, a cooling system assembly and a shielding steel cylinder. The self-shielding accelerator further includes a steel cylinder base connected to the shielding steel cylinder. The accelerator assembly is horizontally fixed to the steel cylinder base. The rectification and voltage multiplication assembly is fixed to the steel cylinder base by a support plate. The high-frequency electrode plate and the solenoid-type transformer assembly are connected to the steel cylinder base through multiple horizontally arranged support columns. The cooling system assembly is fixed to the shielding steel cylinder. The self-shielding accelerator adopts a fully horizontal self-shielding structure, and can be seamlessly joined to the filling production line, which makes online radiation processing possible. A PET plastic bottle production line utilizing the accelerator is also provided.

Self-shielding accelerator and pet plastic bottle production line utilizing same

A self-shielding accelerator is provided, which includes an accelerator assembly, a high-frequency electrode plate, a rectification and voltage multiplication assembly, a solenoid-type transformer assembly, a cooling system assembly and a shielding steel cylinder. The self-shielding accelerator further includes a steel cylinder base connected to the shielding steel cylinder. The accelerator assembly is horizontally fixed to the steel cylinder base. The rectification and voltage multiplication assembly is fixed to the steel cylinder base by a support plate. The high-frequency electrode plate and the solenoid-type transformer assembly are connected to the steel cylinder base through multiple horizontally arranged support columns. The cooling system assembly is fixed to the shielding steel cylinder. The self-shielding accelerator adopts a fully horizontal self-shielding structure, and can be seamlessly joined to the filling production line, which makes online radiation processing possible. A PET plastic bottle production line utilizing the accelerator is also provided.

NON-ACHROMATIC COMPACT GANTRY
20200306561 · 2020-10-01 ·

Embodiments of the present invention provide a compact gantry designed to provide particle therapy using a particle beam. A gantry for providing the particle therapy comprises a first dipole magnet operable to bend a particle beam received from a cyclotron by a first degree amount. The gantry further comprises a plurality of quadrupole magnets configured to condition the beam asymmetrically to produce an asymmetric beam, wherein a configuration of the quadrupole magnets is determined using a dispersion function of a second dipole magnet. Further, the second dipole magnet is operable to receive the asymmetric beam and bend the asymmetric beam by a second degree amount, and wherein the second dipole magnet disperses the asymmetric beam to produce a symmetric beam shape at a treatment isocenter or at any other reference point.

Neutron beam source generator and filter

A neutron beam source generator is provided, which includes an accelerator connecting to a beryllium target through a channel, a filter and a collimator. The beryllium target is disposed at an end of the channel and adjacent to the filter. The filter is disposed between the beryllium target and the collimator. The channel and the beryllium target have an angle therebetween, and the angle is between 0 and 90. The channel and the direction normal to the surface of the filter have an angle therebetween, and the angle is between 0 and 90. The cross-section of the channel is not circular.

LIQUID TARGET DEVICE
20200305268 · 2020-09-24 ·

A liquid target device includes a liquid accommodation portion in which a target liquid is accommodated, a beam passage through which a charged particle beam emitted from a particle accelerator passes to reach the liquid accommodation portion, a target foil that separates the beam passage and the liquid accommodation portion from each other, and a vacuum foil that separates a vacuum region provided upstream of the beam passage and the beam passage from each other. The beam passage is provided with a first gas chamber into which a cooling gas is supplied at a position on the vacuum foil side and a second gas chamber into which a cooling gas is supplied at a position closer to the target foil side than the first gas chamber and the first gas chamber and the second gas chamber are separated from each other by an intermediate foil.

Electron stripper foils and particle accelerators having the same

System includes a particle accelerator configured to direct a particle beam of charged particles along a designated path. The system also includes an extraction device positioned downstream from the particle accelerator. The extraction device includes a stripper foil and a foil holder that holds the stripper foil. The foil holder is configured to position the stripper foil across the designated path of the particle beam such that the particle beam is incident thereon. The stripper foil is configured to remove electrons from the charged particles, wherein the stripper foil includes a backing layer and a conductive layer stacked with respect to one another. The backing layer includes synthetic diamond.

Scalable continuous-wave ion linac PET radioisotope system
10714225 · 2020-07-14 · ·

A continuous wave ion linear accelerator PET radioisotope system is disclosed. The system includes a high brightness H.sup. ion source, a continuous wave RF quadrupole structure, and continuous wave RF interdigital structures to accelerate the ion beam to about 14 MeV. A high energy beam transport system is also described that includes a photo-detachment beam splitter and a magnet lattice for forming the proton beam into a beam having a Waterbag beam profile. The system also includes one or more targets upon which the proton beam is incident. The targets are either a high power metallic target oriented at about 10 degrees or a low thermal conductivity target oriented at about 35 degrees. The invention includes a method of producing PET isotopes by use of the systems described.

SYSTEM AND METHOD FOR GANTRY-LESS PARTICLE THERAPY
20200196429 · 2020-06-18 ·

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.

Energy degrader enabling high-speed energy switching

An example particle therapy system may include: a synchrocyclotron to produce a particle beam; a scanner to move the particle beam in one or more dimensions relative to an irradiation target; and an energy degrader that is between the scanner and the irradiation target. The energy degrader may include multiple plates that are movable relative to a path of the particle beam, with the multiple plates each being controllable to move while in the path of the particle beam and during movement of the particle beam. An aperture may be between the energy degrader and the irradiation target. The aperture being may be to trim the particle beam prior to the particle beam reaching the irradiation target.