Abstract:
A beam guiding apparatus includes a vacuum chamber that includes a target region arranged to receive a target material for generating EUV radiation. The vacuum chamber includes a first and second opening for receiving into the vacuum chamber a first and second laser beam, respectively. The first and second laser beam have different wavelengths. The beam guiding apparatus further includes a superposition apparatus arranged to superpose the first and second laser beams entering into the vacuum chamber through the first and second openings, respectively, for common beam guidance in the direction of the target region. The superposition apparatus comprises a first optical element configured to seal the first opening of the vacuum chamber in a gas-tight manner and transmit the first laser beam, or a second optical element configured to seal off the second opening of the vacuum chamber in a gas-tight manner and transmit the second laser beam.
Abstract:
The invention relates to a drift tube accelerator (1) for the acceleration of ion packets in ion beam acceleration systems, wherein a housing (2) consists of a longitudinally divided three-part vacuum tank (3) having a central unit (4) and a lower half-shell (3) comprising a structured lower steel block (15) and an upper half-shell (6) comprising a structured upper steel block (19). (The cavity arranged between the central unit (4) and the structured steel blocks (15, 19) has at least two acceleration regions (24, 25), between which there is arranged a magnetic focussing device (17), which focuses the ion beam from one region (24) to the next region (25).) The drift tube accelerator (1) according to the invention has such a stable and massive structure that it requires no external supporting aids of any kind in order to obtain alignment, which is reliable and accurate to a few micrometers, of the acceleration components within the drift tube accelerator (1) with respect to the longitudinal axis (7) of ion beam guidance of the central unit (4). The massive structure of the drift tube accelerator (1) according to the invention can be used in general for any linear accelerator.
Abstract:
A wall structure comprising a first surface defining the commencement of a thickness of a metal or ceramic sheet, and a second surface defining the end of said thickness of said sheet said second surface also defining the commencement of a thickness of a three dimensional network defining a multiplicity of interconnecting free cells and a third surface defining the end of said thickness of said three dimensional network.
Abstract:
A system has a linear accelerator, ion pump and a compensating magnet. The ion pump includes an ion pump magnet position, an ion pump magnet shape, an ion pump magnet orientation, and an ion pump magnet magnetic field profile. The compensating magnet has a position, a shape, an orientation, and a magnetic field profile, where at least one of the position, shape, orientation, and magnetic field profile of the compensating magnet reduce at least one component of a magnetic field in the linear accelerator resulting from the ion pump magnet.
Abstract:
An isochronous cyclotron includes at least two superconducting coils, a magnetic yoke surrounding the coils and containing at least a portion of a beam chamber, a plurality of superconducting flutter coils on each side of the median acceleration plane, a non-magnetic reinforcement structure filling the valleys between the superconducting flutter coils so as to maintain the positioning of the superconducting flutter coils, internal reinforcement structures mounted inside the superconducting flutter coils, and a cryogenic refrigerator thermally coupled with the superconducting coils and with the magnetic yoke.
Abstract:
The invention concerns a damping adapter (3) insertable in a suction duct between a service chamber (2) and a vacuum pump (1). The adapter (3) consists of a tubular duct wall (6) in the form of a flexible bellows surrounded by a damping sleeve (7) supported on two end flanges (4, 5). The flexible bellows' plys (6a, 6b) receive a passive damping elastomer (8a) on their outer faces, engaged between the successive plys (6a, 6b). This considerably reduces the transmitting of vibrations from the vacuum pump (1) to the service chamber (2), enabling applications in the microscopy field in particular.
Abstract:
Synchrotron radiation is generated when a base of charged particles is bent by a bending magnet. The synchrotron radiation passes down a lead-out duct as the total number of pumps is limited by the size of the apparatus and many pumps are needed in order to achieve a good vacuum. An ion pump has a main magnetic field, normally generated by a magnet of the ion pump which controls the behavior of the electrons in the ion pump. However, the leakage magnetic field of the bending magnet affects the ion pump, and therefore the ion pump is arranged so that its main magnetic field is aligned with the leakage magnetic field at the ion pump, or at least with a main component thereof. In this way, the effect of the leakage magnetic field on the ion pump is reduced. Indeed, it is possible to use the leakage magnetic field as the main magnetic field of the ion pump.
Abstract:
A vacuum chamber for containing a charged particle beam in a rapidly changing magnetic environment comprises a ceramic pipe with conducting strips oriented along the longitudinal axis of the pipe and with circumferential conducting bands oriented perpendicular to the longitudinal axis but joined with a single longitudinal electrical connection. When both strips and bands are on the outside of the ceramic pipe, insulated from each other, a high-resistance conductive layer, such as nickel can be coated on the inside of the pipe.
Abstract:
This disclosure provides systems, methods, and apparatus related to deposition techniques using laser ablation. In one aspect, an optical fiber and target of a material to be deposited on a first region of an interior surface of a hollow component are positioned in the hollow component. A first end of the optical fiber is coupled to a laser system. A second end of the optical fiber is proximate the target. The material is deposited on the first region of the interior surface of the hollow component by directing a first laser pulse from the laser system through the optical fiber to impinge on the target.