LIFETIME-MEDIATED POLARIZATION EFFECTS IN NONLINEAR SPECTROSCOPY: DEGENERATE FOUR-WAVE MIXING STUDIES OF PREDISSOCIATED $S_{2}O$ IN A SLIT-JET EXPANSION

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1998

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Ohio State University

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Transient S2O molecules were entrained in a pulsed slit-jet expansion (Trot<10K) and interrogated through use of sub-Doppler Degenerate Four-Wave Mixing (DFWM) spectroscopy. High-resolution scans have been acquired for the 2ov(ν=3−10) vibronic bands of the intense C~1AX~1A(ππ) absorption system, where increasing excitation of the v2SS stretching mode is known to promote predissociation of the C~ state. For bands involving moderately-predissociated states (e.g., 204 where τ∗∗∗63ps), the recorded pattern of rovibronic line intensities exhibits a pronounced dependence upon DFWM polarization geometry, a situation not encountered in analogous studies performed for features terminating on long-lived levels of the C~ manifold (e.g., 203 where τ∗∗∗≃22ns). This behavior can be reproduced quantitatively through detailed weak-field analyses of the resonant DFWM response, however, a qualitative understanding follows from the selective dissipation of optically-induced transient gratings as incurred by unimolecular relaxation pathways. In strongly-predissociated members of the 20v progression (i.e., v≥5), additional polarization specificity is introduced by the presence of strong depopulation pumping processes which lead to the creation of net orientation and/or alignment of the molecular ensemble on a timescale commensurate with that of the pulsed four-wave mixing experiment Owing to its absorption-based response and laser-limited spectral resolution, DFWM is often applied to target species where rapid nonraditive relaxation channels preclude successful exploitation of detection techniques based upon secondary matter-field interactions (e.g., fluorescence or ionization). Therefore, a detailed understanding of the role which molecular lifetime plays as a mediator for resonant nonlinear response is of central importance for the quantitative application of this optical scheme.

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a Permanent address: High Magnetic Field Laboratory, CNRS, BP 166, 38042 Grenoble, Cedex 9 (France) b Present address: G.R. Harrison spectroscopy Laboratory, MIT, Cambridge, MA 02139


Author Institution: Department of Chemistry, Yale University

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