Figure 4
From: On the importance of full-dimensionality in low-energy molecular scattering calculations
Cross sections for the CO excitation (jCO = 0 → 1) due to normal-H2(
) as functions of the collision energy.
The experimental data (filled circles) are from ref. 10, where full details about the measurements can be found. The theoretical curves of Figs 1 and 2 have been convolved with the experimental collision energy spread and assuming 25% relative population of para-H2(
) and 75% of ortho-H2(
).
