Electromagnetic waves for an accelerating structure of the radiation delivery system are generated by a microwave source. The electromagnetic waves generated by the microwave source are adjusted by an energy adjuster to an imaging energy level. A kilovolt (kV) imaging beam is generated by the accelerating structure based on the imaging energy level. The electromagnetic waves generated by the magnetic source are adjusted by the energy adjuster to a treatment energy level. A megavolt (MV) treatment beam is generated by the accelerating structure based on the treatment energy level.

A method of generating electromagnetic fields comprises the step of using the interaction between a laser source and an appropriate target, as the source for generating high-intensity electromagnetic fields. A strong positive charge is generated in the target hit by the laser. The target has a structure consisting of at least two different elements. The method can be used to obtain the acceleration, deceleration, deflection, focusing or selection of moving charges. Such charges have been previously accelerated by a completely separate process, and therefore the two processes of pre-acceleration and subsequent processing of the beam of particles are completely separate and therefore separately tunable and optimizable Such electromagnetic fields can be used in other fields than those previously indicated, such as—merely by way of example—medicine, biology, studies on materials, electromagnetic compatibility, and generation of terahertz radiation.

A method of generating electromagnetic fields comprises the step of using the interaction between a laser source and an appropriate target, as the source for generating high-intensity electromagnetic fields. A strong positive charge is generated in the target hit by the laser. The target has a structure consisting of at least two different elements. The method can be used to obtain the acceleration, deceleration, deflection, focusing or selection of moving charges. Such charges have been previously accelerated by a completely separate process, and therefore the two processes of pre-acceleration and subsequent processing of the beam of particles are completely separate and therefore separately tunable and optimizable Such electromagnetic fields can be used in other fields than those previously indicated, such as—merely by way of example—medicine, biology, studies on materials, electromagnetic compatibility, and generation of terahertz radiation.

Proton beams are a promising alternative to X-rays for therapeutic purposes because they may also destroy cancer cells, but with a greatly reduced damage to healthy tissue. The energy dose in tissue may be concentrated at the tumor site by configuring the beam to position the Bragg Peak proximate the tumor. The longitudinal range of a proton beam in tissue is generally dependent upon the energy of the beam. However, after switching energies, the proton-beam system requires some time for the beam energy to stabilize before it may be used for therapy. A proton linear accelerator system is provided for irradiating tissue with an improved beam energy control, configured to provide RF energy from a first RF energy source during the on-time of the proton beam operating cycle for changing the energy of the proton beam, and to provide RF energy from a second distinct RF energy source during the off-time of the proton beam operating cycle for increasing or maintaining the temperature of the cavity. Each RF source is operated independently, allowing higher RF pulse rates to reach the cavity, supporting a smaller time between proton beam energy pulses. In addition, the peak power requirements for the second RF energy source may, in general, be less than for the second RF energy source, allowing a less costly type to be used for the second source. The use of a first and second RF source may reduce the cavity settling time from minutes to less than 10 seconds.

There is described a device for generating electromagnetic field oscillation in a RF device or cavity. The device generally has a photo-diode configured for receiving a laser pulse train and emitting a first electrical signal based thereon, the first electrical signal having a plurality of frequencies; and a harmonics selector configured to output a second electrical signal having one or more frequency of the first electrical signal, the one or more frequency being selected in a manner for the output to generate the electromagnetic field oscillation in the RF device or cavity.

There is described a device for generating electromagnetic field oscillation in a RF device or cavity. The device generally has a photo-diode configured for receiving a laser pulse train and emitting a first electrical signal based thereon, the first electrical signal having a plurality of frequencies; and a harmonics selector configured to output a second electrical signal having one or more frequency of the first electrical signal, the one or more frequency being selected in a manner for the output to generate the electromagnetic field oscillation in the RF device or cavity.

An apparatus may include a drift tube assembly, the drift tube assembly defining a triple gap configuration, and arranged to accelerate and transmit an ion beam along abeam path. The apparatus may include a resonator, to output an RF signal to the drift tube assembly, and an RF quadrupole triplet, connected to the drift tube assembly, and arranged circumferentially around the beam path.

An apparatus may include a drift tube assembly, the drift tube assembly defining a triple gap configuration, and arranged to accelerate and transmit an ion beam along abeam path. The apparatus may include a resonator, to output an RF signal to the drift tube assembly, and an RF quadrupole triplet, connected to the drift tube assembly, and arranged circumferentially around the beam path.

Methods, devices and systems for ultra-high dose radiotherapy are disclosed. The described techniques rely in-part on active switching control of a photoconductive switch during the time the accelerator is accelerating charged particles to produce the output radiation at the desired dose rates. One radiotherapy system includes a particle accelerator configured to receive charged particles from a pulsed source. The particle accelerator includes a pipe configured to allow the charged particles to pass through as a beam, a magnetic core positioned proximate to the pipe and coupled to the pulsed source, and at least one multilayer insulator positioned adjacent to the pipe and the magnetic core. The system also includes a photoconductive switch coupled to the particle accelerator and configured to supply the particle accelerator with a plurality of voltage pulses.

A quality assurance device for a medical accelerator includes a housing having an inner radioluminescent layer adapted to provide a visual indication when contacted with invisible radiation generated by the medical accelerator. In addition, the quality assurance device includes one or more cameras located within the housing and adapted to image the inner radioluminescent layer of the housing including the visual indication.