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.

A linac-based X-ray system for cargo scanning and imaging applications uses linac design, RF power control, beam current control, and beam current pulse duration control to provide stable sequences of pulses having different energy levels or different doses.

A linac-based X-ray system for cargo scanning and imaging applications uses linac design, RF power control, beam current control, and beam current pulse duration control to provide stable sequences of pulses having different energy levels or different doses.

A particle accelerator for creation of a bunched particle beam and a method for the operation of such a particle accelerator are provided, wherein the particle accelerator includes an HF source and a directional coupler for splitting HF power of the HF source of an HF side into at least a first and a second HF power coupler of a cavity side for coupling in the HF power into at least one accelerator cavity. A. non-reciprocal phase shifter is inserted on the cavity side between the directional coupler and the second HF power coupler, and an HF load is connected on the HF side to the directional coupler, where the non-reciprocal phase shifter is configured to pass a reflected HF wave of the second HF power coupler with phase delay in the direction of the directional coupler in such a way that a destructive interference of the reflected HF waves of the first and second power couplets occurs in the directional coupler in the direction of the source on the HF side.

A particle accelerator for creation of a bunched particle beam and a method for the operation of such a particle accelerator are provided, wherein the particle accelerator includes an HF source and a directional coupler for splitting HF power of the HF source of an HF side into at least a first and a second HF power coupler of a cavity side for coupling in the HF power into at least one accelerator cavity. A. non-reciprocal phase shifter is inserted on the cavity side between the directional coupler and the second HF power coupler, and an HF load is connected on the HF side to the directional coupler, where the non-reciprocal phase shifter is configured to pass a reflected HF wave of the second HF power coupler with phase delay in the direction of the directional coupler in such a way that a destructive interference of the reflected HF waves of the first and second power couplets occurs in the directional coupler in the direction of the source on the HF side.

A method, system, and apparatus for vector control of radio frequency signals in narrow band devices such as Super-conducting Radio Frequency (SRF) cavities driven by injection locked magnetrons using carrier amplitude modulation by spectral energy spreading via phase modulation comprises coupling a magnetron to a cavity associated with a particle accelerator and injection locking the magnetron. A modulated amplitude and modulated phase of a drive signal is provided to the magnetron powering the cavity associated with the particle accelerator by removing power from a carrier according to a modulation scheme and providing vector control of the cavity radio frequency vector.

A method, system, and apparatus for vector control of radio frequency signals in narrow band devices such as Super-conducting Radio Frequency (SRF) cavities driven by injection locked magnetrons using carrier amplitude modulation by spectral energy spreading via phase modulation comprises coupling a magnetron to a cavity associated with a particle accelerator and injection locking the magnetron. A modulated amplitude and modulated phase of a drive signal is provided to the magnetron powering the cavity associated with the particle accelerator by removing power from a carrier according to a modulation scheme and providing vector control of the cavity radio frequency vector.

A system and method of operating a magnetron power source can achieve a broad range of output power control by operating a magnetron with its cathode voltage lower than that needed for free running oscillations (e.g., below the Kapitsa critical voltage or equivalently below the Hartree voltage) A sufficiently strong injection-locking signal enables the output power to be coherently generated and to be controlled over a broad power range by small changes in the cathode voltage. In one embodiment, the present system and method is used for a practical, single, frequency-locked 2-magnetron system design.

Methods and apparatus are provided for generating an amplified pulsed radio frequency (RF) signal used by a particle accelerator. The particle accelerator can generate an attenuation profile. The particle accelerator can determine a waveform and a duration for a pulsed RF signal based on the attenuation profile. The particle accelerator can generate the pulsed RF signal having the waveform and the duration. The particle accelerator can generate an amplified pulsed RF signal using one or more amplifiers of the particle accelerator. The amplifiers can include a pulse forming network (PFN), where the PFN can include a plurality of stages and a plurality of PFN switches, and where PFN stage can include one or more capacitors and inductors. The PFN switches can control the PFN stages. The duration of the amplified pulsed RF signal can be based on settings of the plurality of PFN switches.

A radiation treatment apparatus includes an accelerator that emits a charged particle beam, a time measurement unit that measures an emission time of the charged particle beam of the accelerator, a first control unit that controls the accelerator based on the emission time measured by the time measurement unit, and an emission determination unit that determines whether or not the accelerator is emitting the charged particle beam while the first control unit is controlling the accelerator. The time measurement unit adds a time, for which a result of a determination performed by the emission determination unit is that the accelerator is emitting the charged particle beam, to the emission time and does not add a time, for which the result of the determination performed by the emission determination unit is that the accelerator is not emitting the charged particle beam, to the emission time.