Abstract:
In the preferred application for preionizing TE lasers, in particular excimer lasers, the plasma X-ray tube (ER), which can also be referred to as single-chamber ion tube, has an elongated, box-shaped housing (G) including in its inside an also elongated cylindrical cathode (K) of generally U-shaped cross-section, the open end of which faces the X-ray target in the form of a gastight film. An elongated wire-shaped initiating electrode (11) is arranged between X-ray target (1) and cylindrical cathode (K). An electrical field is generated around the initiating electrode (11) by applying thereto a positive voltage or voltage pulse. The field thus generated forces the electrons which are present because of the ambient radiation to form long spiral paths, thus ionising gas atoms. Electron avalanches develop and initiate the wire discharge. Ions (i+) are extracted from the low-pressure plasma (3) by applying to the cylindrical cathode (K) a beam potential of typically between 60 kV and a maximum of 120 kV, and accelerated against the cylindrical cathode (K). On impact of the ions from the cylindrical cathode (K), secondary electrons are emitted and accelerated in the opposite direction, thus forming the electron beam (E), which on striking the X-ray target (1) creates the X-ray bremsstrahlung (X). Said plasma X-ray tube is also basically suitable as an electron gun: for this application, the film used as an electron window covering the window opening in the target holding wall need only be designed so as to be accordingly radiolucent to electron beams.
Abstract:
The device disclosed generates high-voltage pulses for the laser in a pulse-generating network comprising a first, larger charging capacitor (C1) connected in series with a magnetic switch (M1 = saturable inductor) and a second, smaller changing capacitor (C2) connected in parallel with the series circuit (C1-M1) and with the laser electrode section. A series circuit comprising a high-voltage switch (Thy) and a choke (LS1) is connected in parallel with the laser electrode section. The high-voltage switch (Thy) acts as a trigger which initiates the charge reversal process in the first and second charging capacitors (C1, C2), which are charged by a battery charger (LG) to approximately twice the conducting voltage of the laser (LK). The invention also concerns a process for generating high-voltage pulses with said device. Excimer lasers are the preferred field of application.
Abstract:
The invention relates to a slab laser, especially a CO2 slab laser, comprising an optical imaging system for shaping a laser beam (LS) leaving a resonator (4). The divergence of said beam is smaller in a first direction (14) which is perpendicular to the direction of propagation than in a second direction (16) which is perpendicular to the first direction and to the direction of perpendicular. According to the invention the optical imaging system comprises a first optical imaging element (24) for focusing the laser beam (LS) in the first direction (14) and collimating the laser beam (LS) in the second direction (16), as well as a second optical imaging element (26) for collimating the focused laser beam (LS) in the first direction (14).
Abstract:
Described is a laser system with compensated optics, the invention calling for the system to be fitted with at least one optical element (4) which is thermally linked to a heat source (8) to provide thermal compensation for the distortion, caused by the laser beam, of the optical elements located in the laser beam path.
Abstract:
An excitation circuit for partial-discharge gas lasers produces a uniform high-pressure glow discharge in the gas cavity of a laser chamber between the laser electrodes. The high-speed high-voltage switch of the pulse-generating network is designed as a multichannel pseudo-spark switch (VIP switch S) and is preferably incorporated in the laser. It consists of a plurality of single pseudo-spark sections (P-switches 11) connected in parallel. The anode of each P-switch (11) is insulated in particular from all other anodes (12) and can therefore be controlled individually. The cathode (13), on the other hand, is common to all individual P-switches (11). The separate metallic anodes (12) are lodged in a common insulator, the anode holder (14). Slits (15) are arranged between the metallic anode inserts in the anode holder. The anode holder (14) is separated from the cathode (13) by an insulator, the main insulator (16), which maintains the anode holder (14) at a distance (d) from the cathode (13). The entire VIP switch (S) is filled with an ionizable low-pressure gas at pressure (p). A voltage is applied to the anode (12) and the cathode (13) so that the resultant gas discharge is located on the left-hand branch of the Paschen curve. The VIP switch of the excitation cicuit can also be used as a separate component for triggering an electrical high-voltage pulse circuit, as well as for so-called flat laser arrangements.
Abstract:
The device disclosed is connected to the pulse-generating network of an excitation circuit for gas lasers. The primary winding (W1) of a high-voltage pulse transformer (PT) is incorporated in the pulse-generating network between a storage capacitance (C1) and a high-voltage switch (S). Pre-ionization pulses for a pre-ionization device (VE), in particular an X-ray tube (RR), which precipitate the ignition of the laser glow discharge, are emitted at the secondary winding of the pulse transformer (PT). For this purpose, the pulse transformer is designed as a saturable magnetic inductor with at least one secondary winding (W2). When the high-voltage switch (S) is closed, the primary winding of the unsaturated pulse transformer (PT) attains its maximal inductance, at which point a high-voltage pulse is emitted at the secondary winding in accordance with the law of inductance. After a predetermined delay time of, for example, 50-100 ns, the inductance (Lp) of the primary winding drops sharply and the total current flows in the inversion circuit. As a result, the total high voltage required to ignite the glow discharge builds up at the laser electrodes (E1, E2).