We
review the quantum nonadiabatic dynamics of atom + diatom collisions
due to the Renner–Teller (RT) effect, i.e., to the Hamiltonian operators that contain the total spinless electronic
angular momentum L̂. As is well-known, this
rovibronic effect is large near collinear geometries when at least
one of the interacting states is doubly degenerate. In general, this
occurs in insertion reactions and at short-range, where the potential
wells exhibit deep minima and support metastable complexes. Initial-state-resolved
reaction probabilities, integral cross sections, and thermal rate
constants are calculated via the real wavepacket method, solving the
equation of motion with an approximated or with an exact spinless
RT Hamiltonian. We present the dynamics of 10 single-channel or multichannel
reactions showing how RT effects depend on the product channels and
comparing with the Born–Oppenheimer (BO) approximation or coexisting
conical-intersection (CI) interactions. RT effects not only can significantly
modify the adiabatic dynamics or correct purely CI results, but also
they can be very important in opening collision channels which are
closed at the BO or CI level, as in electronic-quenching reactions.
In the OH(A2Σ+) + Kr electronic quenching,
where both nonadiabatic effects (CI and RT) coexist, they are in competition
because CI dominates the reactivity but RT couplings reduce the large
CI cross section and open a CI-forbidden evolution toward products,
so that CI + RT quantum results are in good agreement with experimental
or semiclassical findings. The different roles of these couplings
are due to the unlike nuclear geometries where they are large: rather
far from or near to linearity for CI or RT, respectively. The OH(A2Σ+) + Kr electronic quenching was investigated
with the exact RT Hamiltonian, validating the approximated one, which
was employed for all other collisions.