Abstract: One or more example embodiments of the present invention relates to a radiofrequency source for a linear accelerator system, to the linear accelerator system, to a method for operating a radiofrequency source, and to an associated computer program product.

Abstract: A method is for closed-loop control of an X-ray pulse chain generated via a linear accelerator system. In an embodiment, the method includes modulating a first electron beam within a first radio-frequency pulse duration, wherein the first multiple amplitude X-ray pulse is produced on modulating the first electron beam; measuring time-resolved actual values of the first multiple amplitude X-ray pulse; adjusting at least one pulse parameter as a function of a comparison of the specified multiple amplitude X-ray pulse profile and the measured time-resolved actual values; and modulating a second electron beam within a second radio-frequency pulse duration as a function of the at least one adjusted pulse parameter for production of the second multiple amplitude X-ray pulse, so the X-ray pulse chain is controlled.

Abstract: A method is for closed-loop control of an X-ray pulse chain generated via a linear accelerator system. In an embodiment, the method includes modulating a first electron beam within a first radio-frequency pulse duration, wherein the first multiple amplitude X-ray pulse is produced on modulating the first electron beam; measuring time-resolved actual values of the first multiple amplitude X-ray pulse; adjusting at least one pulse parameter as a function of a comparison of the specified multiple amplitude X-ray pulse profile and the measured time-resolved actual values; and modulating a second electron beam within a second radio-frequency pulse duration as a function of the at least one adjusted pulse parameter for production of the second multiple amplitude X-ray pulse, so the X-ray pulse chain is controlled.

Abstract: A linear accelerator system according to an embodiment is for generating an MeV electron beam. The linear accelerator system includes a linear accelerator cavity having an enclosure, wherein the enclosure is open at one end to provide an exit port for the MeV electron beam; and a switchable magnet unit designed to, in a deflection mode, generate a magnetic field within the linear accelerator cavity to enable at least one electron, emitted within the linear accelerator cavity, to interact with the enclosure due to deflection away from the exit port caused by the magnetic field. Accordingly, in an embodiment, in the deflection mode, an intensity of the MeV electron beam passing through the exit port is relatively lower than an intensity of the MeV electron beam passing through the exit port in a beam generation mode of the switchable magnet unit.

Abstract: A target is for generating X-ray radiation by way of loading with a particle stream containing charged particles. In an embodiment, the target includes a layer structure including at least two metallic layers. A target surface, loadable by the particle stream, is formed by a first layer of the at least two metallic layers of the layer structure including a material including a first metallic element. A second layer of the at least two metallic layers of the layer structure includes a material including a second metallic element. Finally, an ordinal number of the first metallic element is less than an ordinal number of the second metallic element.

Abstract: An x-ray device is for creation of high-energy x-ray radiation. In an embodiment, the x-ray device includes a linear accelerator. The linear accelerator, for creation of x-ray radiation, is embodied so as to create an electron beam directed onto a target, of which the kinetic energy per electron amounts to at least 1 MeV. In an embodiment, the x-ray device further includes a beam limiting device, arranged in the beam path of the electron beam between linear accelerator and the target, including an edge region surrounding a beam limiting device opening. A material thickness of the edge region, in a propagation direction of the accelerated electron beam emerging from the linear accelerator, amounting to less than 10% of the average reach of electrons of the created kinetic energy in the material of the edge region.

Abstract: A high-voltage generator provides a high-voltage pulse including a plurality of energy storage cells, each including two input and two output terminals and a capacitor. A controllable switching element is connected to the input terminals and plus terminals and minus terminals are electrically connected to one another via a respective diode. The high-voltage generator further includes a series connection comprising the energy storage cells, a pulse transformer, and a charging terminal for charging the capacitors. In an embodiment, the high-voltage generator is developed so that a greater pulse rate can be achieved. In an embodiment, at least a respective one of the energy storage cells includes an electrical resistance, connected in series with the diode connecting the plus terminals of the respective energy storage cell.

Abstract: A high-voltage generator provides a high-voltage pulse including a plurality of energy storage cells, each including two input and two output terminals and a capacitor. A controllable switching element is connected to the input terminals and plus terminals and minus terminals are electrically connected to one another via a respective diode. The high-voltage generator further includes a series connection comprising the energy storage cells, a pulse transformer, and a charging terminal for charging the capacitors. In an embodiment, the high-voltage generator is developed so that a greater pulse rate can be achieved. In an embodiment, at least a respective one of the energy storage cells includes an electrical resistance, connected in series with the diode connecting the plus terminals of the respective energy storage cell.

Abstract: A target is for generating X-ray radiation by way of loading with a particle stream containing charged particles. In an embodiment, the target includes a layer structure including at least two metallic layers. A target surface, loadable by the particle stream, is formed by a first layer of the at least two metallic layers of the layer structure including a material including a first metallic element. A second layer of the at least two metallic layers of the layer structure includes a material including a second metallic element. Finally, an ordinal number of the first metallic element is less than an ordinal number of the second metallic element.

Abstract: An x-ray device is for creation of high-energy x-ray radiation. In an embodiment, the x-ray device includes a linear accelerator. The linear accelerator, for creation of x-ray radiation, is embodied so as to create an electron beam directed onto a target, of which the kinetic energy per electron amounts to at least 1 MeV. In an embodiment, the x-ray device further includes a beam limiting device, arranged in the beam path of the electron beam between linear accelerator and the target, including an edge region surrounding a beam limiting device opening. A material thickness of the edge region, in a propagation direction of the accelerated electron beam emerging from the linear accelerator, amounting to less than 10% of the average reach of electrons of the created kinetic energy in the material of the edge region.

Abstract: A linear accelerator is operated by emitting charged particles from a particle source and accelerating the particles in an accelerator by wayof a high-frequency alternating field in such a way that pulses of charged particles are generated. A high-frequency power is periodically supplied by way of high-frequency pulses to the accelerator in order to generate the high-frequency alternating field. A particle stream emitted by the particle source is varied during a HF pulse length of the high-frequency pulse in such a way that the pulse formed during the HF pulse length has at least two sub-pulses with different mean energies per particle. There is also described a linear accelerator that carries out the method and a material-discriminating radioscopy device with a linear accelerator of this kind.

Abstract: A radiation unit for generating bremsstrahlung includes an electron accelerator producing the bremsstrahlung, a supply unit disposed in a main unit, and at least one supply line connecting the supply unit and the electron accelerator. The at least one supply line is a waveguide. The at least one supply line has a first longitudinal section running from the supply unit to a terminal disposed on the main unit. The electron accelerator is disposed outside the main unit and is connected to the terminal via a second longitudinal section of the at least one supply line.

Abstract: The invention relates to a method for producing a partly hollow component (36) from a fiber composite material. In this case, a fusible core (4) is applied to a supporting core (6) by injection molding or casting. A reinforcing fiber (10) is then applied to the core (2). In the process, a fiber structure (14) is produced. The fiber structure (14) is impregnated with a resin. The fiber structure (14), together with the core (2), is put into a conveyor oven (18). During a continuous temperature process, first of all the resin is cured in order that the fiber structure (14) reaches a dimensionally stable state, and then the fusible core material is melted out of the core (2). The supporting core (6) is then removed from the component (36).

Abstract: A structural element made from fibre-reinforced plastic which has a multilayer structure comprising different types of fibre and different fibre orientations. The structural element includes at least one inner layer, which surrounds a substantially hollow core, an intermediate layer having at least one preferred fibre orientation in the direction of a load axis of the structural element, and an outer layer having electrically insulating fibres.