Titlebook: High-Power Lasers and Applications; Proceedings of the F Karl Ludwig Kompa,Herbert Walther Conference proceedings 1978 Springer-Verlag Berl

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Dominant Formation and Quenching Processes in E-Beam Pumped ArF* and KrF* Lasersnd Ar/Kr/F. mixtures with a 5A/cm., 150 keV E-beam. A steady state analysis is valid since the reaction times are short compared to the 300 nsec beam pulse length. The quenching of ArF* by F. and Ar has been measured by analyzing the ArF* (B.Σ. → X.Σ.) fluorescence as a function of the F. and Ar par

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New Visible Laser Transitions in the Mercury Halidescally, 12 J/liter with a 10% intrinsic efficiency has been obtained from KrF* by pure e-beam pumping and 10 J/liter with a 9.5% intrinsic efficiency from e-beam controlled discharge pumping. Recently another class of visible lasers, the mercury halides, has been discovered. These molecules, like the

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High Repetition Rate XeF Laser with Gas Recyclingbeen operated at very low pulse repetition rates, however, which has limited their average power and general utility. In this study we have investigated problems associated with high-repetition-rate operation of a rare gas halide device and have successfully constructed a discharge-excited XeF laser

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Long Pulse Electron Beam Excited XeF Laseriolet and visible laser generation .1., .2. , .3., .4. . The Laser-Plasma Laboratory of Marseille Fluid Mechanics Institute has developed a program on such high power, high efficiency, electronic lasers with particular focus on long pulse or possible c.w. emission. The type of excitation used is med

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Electronic Transition Laserschniques employed as well as of some representative laser systems. This paper is organized in such a way as to provide a historical perspective of research in this area and to provide suggestions for future research.

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CW Laser Emission at 3.8μm and 10.6μm Based Upon the Chemical Generation of Chlorine Atoms at 10.6μm may also be obtained by transfer from DF. or HCl. to CO.. The DF laser system has received the most attention recently because of the greater ease in producing large flows of vibrationally excited DF. The straight chain reaction between D. and F. proceeds rapidly at room temperature throu

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