“…For hyperthermal energy, the initial sticking probability, S 0 , scales with translational energy, E i , and it is nearly independent of surface temperature, T, for both surfaces. At thermal energy the picture is, however, more complex since S 0 decreases significantly with T for T > 150 K on Cu(1 1 0) [5] and on sputtered Cu(1 0 0) [8], while it increases on flat Cu(1 0 0) [6]. This phenomenon was explained by the presence of a physisorbed precursor in the first two cases and in terms of phonon assisted adsorption for flat Cu(1 0 0).…”