Abstract: The invention relates to a parametric oscillator (1) for generating ultra-short pulses. The system (1) comprises a resonator (10) having an optical axis (11), an amplifier crystal (9) arranged in the resonator (10), and a pump laser system (4) for generating pump laser radiation (5) comprising pump photons, said pump laser radiation being directed onto the amplifier crystal (9). The invention is characterized in that the amplifier crystal (9) is an optically non-linear crystal configured for generating a signal photon and an idler photon from a pump photon by means of an optical-parametric process, wherein the resonator (10) is arranged in such a way that a signal pulse formed from the signal photons leaves the amplifier crystal (9) along the optical axis (11) of the resonator (10), and wherein dispersion compensation members for at least partially compensating the dispersion of the radiation circulating in the resonator (10) are provided.

Abstract: The invention relates to a parametric oscillator (1) for generating ultra-short pulses. The system (1) comprises a resonator (10) having an optical axis (11), an amplifier crystal (9) arranged in the resonator (10), and a pump laser system (4) for generating pump laser radiation (5) comprising pump photons, said pump laser radiation being directed onto the amplifier crystal (9). The invention is characterized in that the amplifier crystal (9) is an optically non-linear crystal configured for generating a signal photon and an idler photon from a pump photon by means of an optical-parametric process, wherein the resonator (10) is arranged in such a way that a signal pulse formed from the signal photons leaves the amplifier crystal (9) along the optical axis (11) of the resonator (10), and wherein dispersion compensation members for at least partially compensating the dispersion of the radiation circulating in the resonator (10) are provided.

Abstract: A high-repetition laser system for generating ultra-short pulses according to the principle of pulse decoupling is described. This is achieved by the use of an amplifying laser medium, a laser resonator with at least one resonator mirror and at least one pulse decoupling component, a saturable absorber mirror, and a pump source for pumping the laser medium wherein the pulse decoupling component is an electro-optical modulator.

Abstract: A high-repetition laser system for generating ultra-short pulses according to the principle of pulse decoupling is described. This is achieved by the use of an amplifying laser medium, a laser resonator with at least one resonator mirror and at least one pulse decoupling component, a saturable absorber mirror, and a pump source for pumping the laser medium wherein the pulse decoupling component is an electro-optical modulator.

Abstract: The invention relates to a high-repetition laser system for generating ultra-short pulses according to the principle of pulse decoupling according to the precharacterizing clause of claim 1 and a use of the laser system.

Abstract: A laser with a decoupling device for emitting a laser output depending on at least one influenceable parameter and a mode-coupling device for coupling a plurality of the laserable modes of the resonator. A detector is provided for detecting a value related to the emitted laser output and a parameter varying means for varying the at least one parameter in response to the detected value.

Abstract: The invention relates to a laser with a decoupling means for emitting a laser output depending on at least one influenceable parameter and a mode-coupling means for coupling a plurality of the laserable modes of the resonator. According to the invention, a detection means is provided for detecting a value related to the emitted laser output and a parameter varying means for varying the at least one parameter in response to the detected value.

Abstract: A mirror system for use in generating a short duration laser pulse is disclosed. The system includes first and second double-chirped mirrors disposed along an optical path within a cavity, where the second double-chirped mirror includes an additional phase-shifting layer as compared to the first double-chirped mirror. The additional phase-shifting layer causes the mirror system during use to produce a laser pulse that is characterized by oscillations in group delay substantially reduced in amplitude in comparison to oscillations in group delay for a pulse produced by the same system without the additional phase-shifting layer.