Raman scattering has been observed from both the external and internal motions of the molecules in each of the four condensed phases of oxygen. The stretching vibration gives rise to a sharp band at 1552.5 cm−1 in each phase. Weak wings occur at the base of this band in the γ and liquid phases. Librational lattice modes are observed at 44 and 79 cm−1 in the α phase and at ∼ 50 cm−1 in the β phase. The intensities of these bands relative to that of the internal fundamental are in reasonable agreement with those expected from the oriented gas model. In γ- and liquid oxygen, the external motion gives rise to strong wings on the Rayleigh line. Estimates of the mean-square torsional amplitude and the torque acting on the molecule have been made from the observed low-frequency spectra, and indicate that the torsional motion is highly hindered in each phase. The root-mean-square torsional amplitude increases from an average of 9° in the α phase to 18° in the liquid.
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Cahill et al. (1969) studied this question.
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