Titlebook: Laser-Induced Processes in Molecules; Physics and Chemistr Karl Ludwig Kompa,Stanley Desmond Smith Conference proceedings 1979 Springer-Ver

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Laser-Induced Intermolecular and Intramolecular Energy Transfer Processesmprove dye lasers efficiency and to extend their spectral region of operation. Nitrogen laser pumped dye lasers are limited to dyes which absorb the nitrogen laser light (at 337.1 nm) or to pumping schemes where the excitation energy is transferred from an absorbing donor (D) to an acceptor (A) (the

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A New Method for Exposing Mammalian Cells to Intense Laser Radiation Using the Evanescent Fields Creer of attached cells covering a wide area on the waveguide surface is exposed to the evanescent tail produced by the propagating waveguide mode. The optical radiation-cell interaction is limited to involve only the high power density and intense electric field strength associated with the evanescent

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Low-Temperature Performance of Roto-Vibrational Molecular Lasersbased on the selective vibrational excitation of molecules. The laser-pumped roto-vibrational molecular lasers (OPML’s) operate in the mid-infrared and are capable of generating the high intensities required for many photochemical studies. Recent experimental results have demonstrated that by operat

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Tunable Infrared Generation from Four-Wave Mixing in Room-Temperature Germanium = .υ. - υ., υ. = .υ. - υ. Two efficient and powerful gas lasers (CO., NH.), operating between 900 and 1100 cm. (υ.) and near 780 cm. (υ.) respectively, enable combination frequencies to be generated in the photochemically important regions 1420 - 1020 cm. (υ.) and 660 - 460 cm. (υ.). Such mixing ca

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High-Resolution Double-Resonance Spectroscopy of SF6es. In the present work we have performed a double-resonance (DR) measurement by using a Q-switched CO. laser to saturate a variety of υ.-mode transitions in a small volume of SF. gas at low pressure, and probing that volume using the output of a tunable lead-salt diode laser. Our intent was to yiel

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Photophysics of Gaseous UF6 in the UV: Energy Balance Through Quantum Efficiency Measurementsral features of this fluorescence are now well established. The visible fluorescence spreads from 400 to 460 nm with a maximum around 420 nm: the shape of the spectrum is independent of pressure or of wavelength of excitation [4, 6]. The Stern-Volmer plot has a saturation like behaviour for the high

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Optical Dephasing in Molecular Iodinedemonstrated that atomic collisions can broaden spectral lines. Some 55 years later, similar time-dependent interactions were pursued in more sophisticated and detailed ways by pulsed nuclear magnetic resonance—the difference being that the measurements were carried out more directly in the time dom