The far infra-red absorption spectrum of the compressed gas ethylene has been measured in the region 10–200 cm −1 at pressures from 14.7 to 55.7 bar at 296 K. The origin of the broad bands observed is a bimolecular collision induced absorption as indicated by the dependence of the total integrated intensity on the square of the molecular number density. The quantum theory [6] of resonant, multipole induction, giving rise to sets of rotational transitions is an inadequate description of the observed broad continua, the peaks of which shift from 125 cm −1 to 150 cm −1 over the pressure range investigated. However, they are matched satisfactorily by a spectral function c(ω), generated from an approximation to its related classical autocorrelation function c(t), containing two equilibrium averages K o(o) and K l(l) (which are related to the coefficients in the Maclaurin expansion of c(t)); and a width parameter γ. All three phenomenological parameters vary with pressure, contrary to the quantum prediction of their constancy, and go through a smooth minimum at ca . 30 bar, where the correlation time τ is longest.
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