Provided is a klynac including: a klystron input cell configured to form a first resonant circuit; a klystron output cell; and a plurality of linac cells configured to form a second resonant circuit with the klystron output cell.

Provided is a klynac including: a klystron input cell configured to form a first resonant circuit; a klystron output cell; and a plurality of linac cells configured to form a second resonant circuit with the klystron output cell.

Embodiments of systems, devices, and methods relating to a beam system. An example method of detecting beam misalignment a beam system includes detecting beam misalignment in an injector system of the beam system. The example method further includes detecting beam misalignment in an accelerator system of the beam system.

Embodiments of systems, devices, and methods relating to a beam system. An example method of detecting beam misalignment a beam system includes detecting beam misalignment in an injector system of the beam system. The example method further includes detecting beam misalignment in an accelerator system of the beam system.

A technique for outputting heterologous ions having the same per-nucleon energy at different timings by using one ion source is provided. An ion generation device includes: an ion generation energy setter that causes first ions and second ions generated by ionization in a vacuum chamber to be emitted in a mixed state from an opening; an electric-field voltage adjuster that imparts a same predetermined per-nucleon energy to each of the first and second ions by applying electric potential formed between the opening and extraction electrodes while switching the electric potential between first and second electric-field voltages; and an excitation current adjuster that causes the first and second ions to be outputted at different timings by supplying a coil of a separation electromagnet with an excitation current while switching the excitation current between first and second excitation currents.

A technique for outputting heterologous ions having the same per-nucleon energy at different timings by using one ion source is provided. An ion generation device includes: an ion generation energy setter that causes first ions and second ions generated by ionization in a vacuum chamber to be emitted in a mixed state from an opening; an electric-field voltage adjuster that imparts a same predetermined per-nucleon energy to each of the first and second ions by applying electric potential formed between the opening and extraction electrodes while switching the electric potential between first and second electric-field voltages; and an excitation current adjuster that causes the first and second ions to be outputted at different timings by supplying a coil of a separation electromagnet with an excitation current while switching the excitation current between first and second excitation currents.

An accelerator 4 includes a circular vacuum container including circular return yokes 5A, 5B. An injection electrode 18 is disposed closer to an inlet of a beam extraction path 20 in the return yoke 5B than a central axis C of the vacuum container. Magnetic poles 7A to 7F are radially disposed from the injection electrode 18 at the periphery of the injection electrode 18 in the return yoke 5B. Recessions 29A to 29F are disposed alternately with the magnetic poles 7A to 7F in the circumferential direction of the return yoke 5B. In the vacuum container, a concentric trajectory region, in which multiple beam turning trajectories centered around the injection electrode 18 are present, is formed, and an eccentric trajectory region, in which multiple beam turning trajectories eccentric from the injection electrode 18 are present, is formed around the region.

An accelerator 4 includes a circular vacuum container including circular return yokes 5A, 5B. An injection electrode 18 is disposed closer to an inlet of a beam extraction path 20 in the return yoke 5B than a central axis C of the vacuum container. Magnetic poles 7A to 7F are radially disposed from the injection electrode 18 at the periphery of the injection electrode 18 in the return yoke 5B. Recessions 29A to 29F are disposed alternately with the magnetic poles 7A to 7F in the circumferential direction of the return yoke 5B. In the vacuum container, a concentric trajectory region, in which multiple beam turning trajectories centered around the injection electrode 18 are present, is formed, and an eccentric trajectory region, in which multiple beam turning trajectories eccentric from the injection electrode 18 are present, is formed around the region.

Embodiments of the present invention disclose methods and systems for performing particle acceleration using a cyclotron RF resonator with an asymmetrical fixed tuner. A cyclotron RF resonator includes a single shorting plate tuner inside and a fixed short stem, and does not require top-bottom mirror symmetry. Small movements in relation to the wavelengths of the maximum acceleration voltage is bound by the capacitance of the accelerating surfaces. As such, the resonator may perform particle acceleration using asymmetrical tuning to reduce design complexity, cost of maintenance, fabrication and installation complexity, failure rate, and software complexity (e.g., control software), for example.

Embodiments of the present invention disclose methods and systems for performing particle acceleration using a cyclotron RF resonator with an asymmetrical fixed tuner. A cyclotron RF resonator includes a single shorting plate tuner inside and a fixed short stem, and does not require top-bottom mirror symmetry. Small movements in relation to the wavelengths of the maximum acceleration voltage is bound by the capacitance of the accelerating surfaces. As such, the resonator may perform particle acceleration using asymmetrical tuning to reduce design complexity, cost of maintenance, fabrication and installation complexity, failure rate, and software complexity (e.g., control software), for example.