“…To carry out an exact calculation of the S matrix elements the nuclear Hamiltonian Ĥ N is applied to the Λ component of the time dependent partial wave Ψ JΛ (R,r,Θ,t) (or similarly to the time independent analogue Ψ JΛ (R,r,Θ) ). Most often, in order to evaluate cross sections and rate coefficients use is made of classical (cl) methods, which approximate the stateto-state probability as the fraction of the trajectories starting from state vj and ending in state ′ v ′ j , after all, trajectory calculations fully exploit the characteristic features of the High Throughput Computing technologies of EGI including the low level bridging of HTC with HPC [21]. This has allowed a straightforward use of the basic GEMS scheme because, as specified below in more detail, related PESs are also formulated as empirical functional forms fitted to ab initio data [22].…”