“…For example, under scanning tunneling microscopy study, the barrier for the double jump of a Pt adatom is 0.89 eV, which is slightly higher than 0.81 eV for the single jump in the missing row on the ͑1 ϫ 2͒ reconstructed Pt ͑110͒ substrate. 25,70 However, the activation energy of a long jump is the same as that of the associated single atomic-spacing jump, which limits the availability of the energetics approach to the study of long-jump diffusion. In order to calculate the exact diffusion rate of a long jump, we should consider the aforementioned prefactor and the energy barrier together in the context of nonadiabatic coupling of adatom and substrate excitation, which is beyond the current scope.…”