Matsushita Electric Industrial Co., Ltd.

Naoya Horiuchi

Takuhiro Ono

Takeo Miyata

Nobuaki Furuya

Keiichiro Yamanaka

Reiji Sano

Kenichi Takahata

Hitoshi Hongu

Takashi Iwabuchi

Takafumi Ohhara

Keiichro Yamanaka

A discharge-pumped gas laser, typically a discharge-pumped excimer laser, includes a main discharge circuit for producing an electric discharge in a laser gas to excite the laser gas for laser emission. The main discharge circuit comprises a first electric circuit having a thyratron, a charging circuit including a charging capacitor for storing an electric energy to operate the thyratron, and a discharging circuit including a pair of main discharge electrodes and a peaking capacitor for storing an electric energy to cause a main discharge in the laser gas between the main discharge electrodes. The laser gas is preionized by preionizers having a plurality of preionizing electrodes which produce an electric discharge to preionize the laser gas. The preionizing electrodes are connected in a second circuit which has a plurality of distributing capacitors for storing an electric energy to enable the preionizing electrodes to preionize the laser gas and supply substantially uniform electric currents to the preionizing electrodes. The distributing capacitors have substantially the same capacitances. The first and second electric circuits are substantially independent of each other.

Discharge-pumped gas laser with independent preionizing circuit

A discharge-pumped gas laser has a pressure container filled with a laser gas under pressure and a pair of elongate main discharge electrodes. The main discharge electrodes are disposed in the pressure container in confronting relationship to each other for producing an electric discharge in the laser gas in a main discharge region defined therebetween to excite the laser gas for laser emission. The laser gas is circulated to flow through the main discharge region in a direction perpendicular to the main discharge electrodes. The laser gas in the main discharge region is preionized by an UV preionizer disposed either upstream or downstream of the main discharge region with respect to the direction of flow of the laser beam. The pressure container houses a baffle partition for controlling the laser gas to flow past one of the main discharge electrodes and the preionizer while blocking the laser gas from directly flowing to the other of the main discharge electrodes and the preionizer.

Discharge-pumped gas laser with baffle partition for controlled laser

A gas laser apparatus includes an insulating material layer covering the outside of a pair of metal electrodes disposed on the outer peripheral surface of a dielectric discharge tube. The insulating material layer thus provided electrically separates the metal electrodes and prevents a dielectric tube which would otherwise occur through an air gap between adjacent portions of the metal electrodes when a high-frequency voltage is applied across the metal electrodes.

Gas laser apparatus

A laser apparatus comprises an optical resonator including first and second mirrors, and laser medium. An wavelength selection element is provided in the resonator for narrowing band-width. A polarizing conversion element for changing ratio of S to P components and polarizing beam splitter are provided for amplifying laser beam to output after wavelength selection and for reducing light load of the wavelength selection element. The polarizing conversion element is provided in the resonator light path. In another embodiment, the polarizing conversion element is provided in a branch light path formed by a second polarizing conversion element and a third mirror, where the second polarizing conversion element reflects and transmits P component at a given ratio and reflects S component. The wavelength selection element comprises a Fabry-Perot etalon, grating, or prism. The polarizing conversion element comprises a quarter-wave plate or a phase retarder mirror. The polarizing beam splitting element comprises a polarizing beam splitter or polarizing beam splitting prism. Such laser apparatus is suited for an exposure light source for photolithography.

Narrow-band laser apparatus

A laser beam generated between a total reflector and an output coupler is turned back by plural reflectors which are mounted in a discharge region along two main electrodes at 45.degree., and the discharge region is divided into plural divided discharge regions, thus, a diameter of an output laser beam is reduced to a diameter of the divided discharge regions.

Laser apparatus

A laser apparatus comprises an optical resonator including first and second mirrors, and lasing medium. An wavelength selection element is provided in the resonator for narrowing band-width. A polarizing conversion element for changing ratio of S to P components and polarizing beam splitter are provided for amplifying laser beam to output after wavelength selection and for reducing light load of the wavelength selection element. The polarizing conversion element is provided in the resonator light path. In another embodiment, the polarizing conversion element is provided in a branch light path formed by a second polarizing conversion element and a third mirror, where the second polarizing conversion element reflects and transmits P component at a given ratio and reflects S component. The wavelength selection element comprises a Fabry-Perot etalon, grating, or prism. The polarizing conversion element comprises a quarter-wave plate or a phase retarder mirror. The polarizing beam splitting element comprises a polarizing beam splitter or polarizing beam splitting prism. The polarizing beam splitter and phase retarder prism may have a fine adjusting mechanism to adjust its optical axis to obtain desired characteristic. Such laser apparatus is suited for an exposure light source for photolithography.

In a gas laser in which a mixture of gases is excited under the influence of an electric field, a first constituent gas of the mixture is introduced into a laser tube to allow a discharge to occur in the introduced gas at predetermined partial pressure. A second constituent gas of the mixture is then introduced into the laser tube until the combined gases reach the normally operating pressure of the mixture to allow a discharge to occur in the later introduced gas.

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Kawasaki, Japan

Naoya Horiuchi