Lambda Physik Gesellschaft Zur Herstellung Von Lasern Mbh

Lambda Physik Ag

Jurgen Kleinschmidt

Uwe Stamm

Peter Heist

Klaus Wolfgang Vogler

Peter Lokai

Dirk Basting

Hans-Stephan Albrecht

Vadim Berger

Wolfgang Zschoke

A wavelength calibration system determines an absolute wavelength of a narrowed spectral emission band of an excimer or molecular laser system. The system includes a module including an element which optically interacts with a component of an output beam of the laser within the tunable range of the laser system around the narrowed band. An inter-level resonance is detected by monitoring changes in voltage within the module, or photo-absorption is detected by photodetecting equipment. The absolute wavelength of the narrowed band is precisely determinable when the optical transitions occur and are detected. When the system specifically includes an ArF-excimer laser chamber, the module is preferably a galvatron containing an element that photo-absorbs around 193 nm and the element is preferably a gas or vapor selected from the group consisting of arsenic, carbon, oxygen, iron, gaseous hydrocarbons, halogenized hydrocarbons, carbon-contaminated inert gases, germanium and platinum vapor. When the system specifically includes F.sub.2 -laser chamber, the module is preferably a galvatron containing an element that photo-absorbs around 157 nm and the element is preferably a gas or vapor selected from the group consisting of selenium, bromine and silicon. The module is alternatively a purge chamber configurable for purging with a photo-absorbing gas.

Method and apparatus for wavelength calibration

An excimer laser system having a precisely calibratable absolute emission wavelength is provided wherein at least one source of reference light is used. The reference light may be a laser such as a HeNe laser or a cathode lamp such as a hollow Pt, As, C, or Fe cathode lamp. The reference light and the excimer laser beam are directed along substantially the same optical path. The beams are broadened and recollimated by beam expanding optics. The broadened beams impinge upon a dispersive element, preferably an echelle grating, and various orders for each incident wavelength are dispersed. The beams are refocused onto a position sensitive detector such as a CCD camera. Different orders of one or more lines of known wavelength of the reference light and a line from the excimer laser emission are also incident at the detector simultaneously. An absolute wavelength calibration of the excimer laser emission is precisely determinable based on a position of said excimer laser emission relative to positions of the one or more lines of the reference light at the detector. The grating constant of the preferred grating and the detector are such that calibration of the central wavelength of the narrowed excimer laser emission is performable when the central wavelength is anywhere within the broadband emission spectrum of the excimer laser. A processor calculates the absolute wavelength of the excimer laser emission. Embodiments are provided for refractive optic, catadioptric, and reflective imaging systems.

Wavelength calibration tool for narrow band excimer lasers

A laser, especially an excimer laser, is designed to generate narrow-band radiation and comprises a laser resonator, including two reflecting elements (12, 14) between which there is disposed a laser active medium (10), and further comprises a group of several refractive dispersive elements (32, 34) arranged in the laser beam path and each deflecting, incident light at an angle (.gamma..sub.a, .gamma..sub.b) which is specific of the wavelength of the incident light. It is provided to reduce variations of the emission wavelength which are temperature responsive and time dependent during burst operation by giving at least one of the refractive dispersive elements (32) a refractive index which increases as the temperature goes up and at least one of these elements (34) a refractive index which drops as the temperature rises.

Laser for generating narrow-band radiation

A narrow-band laser apparatus comprises an optical resonator including first and second reflectors for reflecting radiation, a laser medium for amplifying radiation in said resonator and an etalon for selecting a given wavelength component from said radiation. A polarizing beam splitter is provided for linearly polarizing said radiation and also for acting as an output coupler. In order to obtain very narrow bandwidth radiation of high intensity, a Faraday rotator is provided for rotating the plane of polarization while maintaining the linear polarization thereby allowing a second wavelength selection element (such as a grating) to be efficiently employed to further narrow the output of the laser.

Narrow-band laser apparatus

A pulsed laser comprises an oscillator (10), a laser medium (14), a wavelength selective member (12) for tuning the wavelength of a beam pulse (18) emitted by the oscillator, and means for pulsed excitation of the laser medium (14). The laser medium (14) is excited at least twice at consecutive times to generate a single beam pulse (18).

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Weissenfels, Germany

Jurgen Kleinschmidt