A wafer-based charged particle accelerator includes a charged particle source and at least one RF charged particle accelerator wafer sub-assembly and a power supply coupled to the at least one RF charged particle accelerator wafer sub-assembly. The wafer-based charged particle accelerator may further include a beam current-sensor. The wafer-based charged particle accelerator may further include at least a second RF charged particle accelerator wafer sub-assembly and at least one ESQ charged particle focusing wafer. Fabrication methods are disclosed for RF charged particle accelerator wafer sub-assemblies, ESQ charged particle focusing wafers, and the wafer-based charged particle accelerator.

The present application provides a method for obtaining strong focusing of an isochronous accelerator by varying the magnetic field gradient in a large radial range. The method is characterized by the main magnet of the isochronous accelerator providing not only a bending effect but also a focusing effect, equivalent to the effects of quadrupole, sextupole, and octupole magnets used in a synchrotron accelerator.

A particle accelerator system including a particle accelerator that accelerates charged particles, a signal source that outputs high frequency power for accelerating the charged particles in the particle accelerator, an amplifying unit that amplifies the high frequency power from the signal source, and supplies the high frequency power to the particle accelerator, the amplifying unit including a plurality of semiconductor amplifiers using a semiconductor, and a control unit that controls an operation of the amplifying unit. The control unit controls output of at least one of the plurality of semiconductor amplifiers.

Disclosed is an adjustable transmission device for measuring transverse parameters of beams, including: a CCD transmission support assembly, an external transmission rod, the CCD transmission support assembly is connected with a support block, and the support block is provided with the slotted set screw with flat point, and is connected with a limit block via a first fastener; a snap ring is arranged in the rear of the external transmission and is matched with a base; the base is connected with the CCD fixed plate via a second fastener. The external transmission rod is provided with a second groove for mounting the first retaining ring, and a side of the first retaining ring is sequentially provided with a vacuum observation window, a second retaining ring, a head assembly, a retaining sleeve and a screwing mechanism.

A compact rare-earth superconducting cyclotron includes a magnetic yoke, a pair of superconducting coils, and a pair of rare-earth poles. The magnetic yoke defines a chamber contained within the magnetic yoke. The superconducting coils are contained in the chamber defined in the magnetic yoke and are positioned on opposite sides of a median acceleration plane in the chamber. Each rare-earth pole includes a rare-earth metal and is contained in the chamber defined in the magnetic yoke on opposite sides of the median acceleration plane. Each of the rare-earth poles also extends inward toward a central axis from one of the superconducting coils, is physically separated from the magnetic yoke, and is separated by at least 5 cm from the other rare-earth pole.

A proton therapy system based on a compact superconducting cyclotron, including: a superconducting cyclotron system, an energy selection system, a beam transport system, a fixed therapy room subsystem and a rotating frame therapy subsystem; a fixed-energy proton beam extracted from a superconducting cyclotron of the superconducting cyclotron system is adjusted into a continuous and adjustable proton beam of 70 MeV to 200 MeV by the energy selection system, thus realizing a longitudinal adjustment for a proton range during treating a tumor, and the continuous and adjustable proton beam is respectively transmitted to the fixed therapy room subsystem and the rotating frame therapy subsystem by the beam transport system. The cooperative control of the superconducting cyclotron system, the energy selection system, the beam transport system and the therapy head realizes the transverse expansion of proton beams, thus realizing intensity modulated radiation therapy for the tumor.

The invention relates to a container (100, 901, 902, 903, 904, 905, 906, 907, 908, 909, 910) for the production of radioisotopes by irradiation of a precursor material formed by a one-piece metal casing, the wall of said casing including one thin portion (130) having a thickness of between 5 and 100 m, the remainder having a thickness greater than 100 m. The invention also relates to a method for obtaining the container and to a target assembly using same.

An irradiation target positioning device and method for creating radioisotopes utilizing linear particle beam accelerators or cyclotron accelerators. The device positions a target proximate to a liquid reservoir and vapor expansion chamber. The target may be in a solid phase. Heat produced within the target during irradiation can be absorbed by the liquid. The liquid may be heated to its vaporization temperature and vapor emitted into the vapor chamber. The vapor chamber may utilize a cooling mechanism, allowing the vapor to condense (second phase change). The radioactive product may diffuse into the liquid, thereby allowing the irradiated product to be conveyed out of the target structure in a liquid, solution or slurry. Multiple radioisotopes may be produced simultaneously out of the target material and liquid and separated later. The target material and irradiated product may be removed from the target surface by acid.

An electronic system includes an external jacket; a wall of an internal cavity that is to be cooled; at least one fixed connection fixing the external wall of the internal cavity that is to be cooled to the external jacket; a heat-transport fluid cooling circuit comprising grooves on the external surface of the wall of the internal cavity and a sleeve comprising a flexible portion positioned flush with the external surface of the external wall of the internal cavity, thereby forming mini-canals with said grooves; a radial extension of the wall of the internal cavity creating connecting points intended to hold the sleeve in place; and a space between the external jacket and the sleeve at the flexible portion of the sleeve.

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.