Intensity. From the absorption spectra in Figs. 1 and 2, qualitative differences between O2−O2 and O2−N2 collision-induced absorp- tion become apparent. The O2−O2 contributions are typically more intense, significantly broader in frequency, and decay less rapidly respectively. These profiles are compared to the results of the full calculations in Fig. 3, using realistic parameters a = 7a0 and = 3a −1. The analytical model reproduces the typical translational profiles, supporting the length-scale argument presented above.
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Intensity. From the absorption spectra in Figs. 1 and 2, qualitative differences between O2−O2 and O2−N2 collision-induced absorp- tion become apparent. The O2−O2 contributions are typically more intense, significantly broader in frequency, and decay less rapidly respectively. These profiles are compared to the results of the full calculations in Fig. 3, using realistic parameters a = 7a0 and μ = 3a −1. The analytical model reproduces the typical translational profiles, supporting the length-scale argument presented above.
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Samples: repository.ubn.ru.nl