The optical-potential method (OPM) developed in the previous paper is applied to the calculation of a large manifold of transitions of the type v--1, j, mj -->v' = O, j', mj in Li + N~ collisions. Trends related to the dependence of the cross section av,Lmj~v'J',raj on the states j, j' and m t are observed and analysed in terms of the physical effects involved. An information-theoretic model of the cross sections is tested as a means for a simple parametric representation of the results.
I. INTRODUCTIONSeveral sophisticated theoretical methods were introduced in recent years for the calculation of rib-rotational transition rates in atom-molecule collisions [1]. Applications of these methods, the most notable of which is the coupled-state approximation [2], were, however, confined to systems in which the molecular collision partner is a very light diatomic (e.g. cases such as He + H~, He + D 2, Li+H 2 [I]). This limitation is a consequence of the great computational difficulty for systems involving heavier molecules where the dense rotational energy spacings give rise to a large number of rotational states that play a role in the process, hence to scattering equations of enormous dimensionality [3]. The difficulty can be overcome by two approaches suggested recently in the literature. One of these schemes is an analytical model for rib-rotational transitions, applicable to systems with a potential surface of a certain type [4]. The second approach is an optical-potential method (OPM) described in reference [5] (referred to below as paper I). Tests on the He+H~ system have shown the above methods to be of good accuracy [4,5], and the loss of precision that these schemes entail is compensated by a much increased range of applicability. In the OPM approach the effect of the large manifold of open rotational channels on a rib-rotational transition of interest is incorporated through optical (absorptive) potentials. In this way the effort required to calculate a single rib-rotational cross section is virtually independent of the number of open rotational channels, and a drastic simplification of the computational effort ensues.