Electronic and geometric structure ofC60on Al(111) and Al(110)

Abstract
Two new ordered monolayer phases of C60 on Al surfaces have been studied using electron spectroscopies and low-energy electron diffraction (LEED). On Al(111), in addition to the previously reported (6×6) phase formed by evaporating with Tsample=620 K, a metastable (23×23)R30° phase can be produced with Tsample=300 K. This phase exhibits the first LEED pattern reported for an unannealed C60 overlayer. On Al(110), when evaporations are also made with Tsample=620 K, LEED shows the presence of a monolayer with a pseudo-c(4×4) structure. Al 2p photoemission for C60/Al(110) and for (23×23)R30° C60/Al(111) reveals no evidence of strong substrate reconstruction. The perturbation of the geometric and electronic structure of the C60 molecule due to the bonding interaction with the Al surface increases in the order C60/Al(110), (23×23)R30° C60/Al(111), (6×6) C60/Al(111), as demonstrated using element-specific probing of the valence band with x-ray absorption and C 1s shakeup. The bond has covalent character in all three cases. Symmetry-induced splitting in the 5hu-derived level is observed using valence photoemission, and is particularly clear for C60/Al(110). The stability of the equilibrium structures can be qualitatively understood from considerations of the energetics of the overlayer compression and the chemical bond between adsorbate and substrate. Work-function measurements for these and other C60 overlayer systems cannot, in general, be understood within a simple description involving the addition of a dipole to the surface potential.