99 research outputs found

    VIBRATIONAL ANHARMONICITY OF SF6SF_{6} IN CRYOGENIC SOLUTION

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    1^{1} V.V. Bertsev, T.D. Kolomiitseva, and N.M. Tsyganenko, Opt. Spectrosc. 37, 263 (1974). 2^{2} S.R.J. Brueck, to be published. Experimental work supported by the Department of the Air Force.Author Institution:The infrared spectrum of SF6SF_{6} has been recorded in liquid oxygen1oxygen^{1} and liquid argon2argon^{2} solutions. The suppression of rotational structure and the elimination of hot bands at low temperature give estimates of band origins that could only be achieved in the gas phase by detailed high-resolution analyses of each hand. A normal coordinate anharmonic force field has been fitted directly to fundamental, overtone and combination bands of the cryogenic solution spectra. It will be shown that at least for ν3\nu_{3} the derived anharmonic constants are in good agreement with those obtained from gas phase data (and force fields based upon gas phase data), despite appreciable shifts in the fundamentals from gas to cryogenic solution

    HIGH-RESOLUTION STIMULATED RAMAN SPECTROSCOPY OF THE ν1\nu_{1} BAND OF SiH4SiH_{4}

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    1. A Owyoung, C. W. Patterson, and R. S. McDowell, Chem. Phys. Lett. 59, 156 (1978). 2. R. S. McDowell, C. W. Patterson, and A. Owyoung, J. Chem. Phys., in press. 3. A. Cabana, D. L. Gray, A. G. Robiette, and G. Pierre, Mo1. Phys. 36, 1503 (1978)Author Institution:A Doppler-limited isotropic Raman spectrum of the symmetric stretching fundamental (ν1)(\nu_{1}) of 28SiH4^{28}SiH_{4} has been recorded using high-sensitivity “quasi-cw” inverse Raman spectroscopy. Unlike the corresponding fundamentals of 12CH4^{12}CH_{4} (1) and 13CH4^{13}CH_{4} (2), this band exhibits compact non-overlapping J manifolds that extend over about 5cm15 cm^{-1}. Since ν1\nu_{1} and the infrared-active stretch ν3\nu_{3} reported by Cabana et al. (3) and the Raman frequencies of ν1\nu_{1} Q (0) through Q(14). The results confirm the infrared analysis (3), in which several perturbation-allowed ν1\nu_{1} transitions were identified in absorption, but the molecular constants are much better determined by the inclusion of the Raman data. Significant intensity perturbations occur at higher J due to a break down of the selection rule Δ=0\Delta=0 (N is the index distinguishing between levels of the same J and rovibrational symmetry), and have been quantitatively accounted for

    LINE ASSIGNMENTS AND INTENSITIES FOR THE ν2+ν4\nu_{2} + \nu_{4} BAND OF METHANE

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    Author Institution: Jet Propulsion Laboratory; Department of Physics, Florida State University; Department of Chemistry, The University, Whiteknights, ReadingThe forbidden transitions have been identified and allowed transitions assignments extended for the ν2+ν4\nu_{2} + \nu_{4} band of CH4CH_{4} using spectra recorded at 0.023cm10.023\, cm^{-1} resolution with the four-pass grating spectrometer at Florida State University. The assignment process has been greatly aided by the measurement of individual line strengths at different temperatures to obtain experimental values for the ground state energy levels of the transitions. Corresponding allowed transitions of ν2+ν4\nu_{2} + \nu_{4} of 13CH4^{13}CH_{4} have been identified

    INFRARED ABSORPTION LINE ASSIGNMENTS AND STRENGTHS FOR THE 2ν22\nu_{2} BAND OF METHANE

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    Author Institution:A 0.02cm10.02 cm^{-1} resolution study of the absorption line strengths of methane in the 3.3 μm\mu m region at both room and reduced temperatures reveals over 200 lines with strengths between 1×1021 \times 10^{-2} and 5×105cm2atm15 \times 10^{-5} cm^{-2} atm^{-1} at 296 K which belong to the 2ν22\nu_{2} band. Most of these lines can be assigned with the aid of combination differences, experimental values for EE^{\prime\prime} and a preliminary energy level calculation
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