4.4 Basic Features of Atom–Diatom Reactions
141
Fig. 4.14 Minimum Energy Path of the Li + FH → LiF + H reaction
Fig. 4.15 J = 0 adiabats of the Li + FH reaction plotted as a function of ρ
In particular, the dense grid of resonances shown by the probabilities of Fig. 4.16
for J = 0 can be associated with the bound states supported by the wells formed by
the adiabats as ρ varies. Particularly interesting is the fact that, as can be clearly seen
141
Fig. 4.14 Minimum Energy Path of the Li + FH → LiF + H reaction
Fig. 4.15 J = 0 adiabats of the Li + FH reaction plotted as a function of ρ
In particular, the dense grid of resonances shown by the probabilities of Fig. 4.16
for J = 0 can be associated with the bound states supported by the wells formed by
the adiabats as ρ varies. Particularly interesting is the fact that, as can be clearly seen