The interaction of C60 with Ag(111) was studied using UHV-STM, LEED, A
ES, and TOF-SIMS and compared with previous results for Au(111). On bo
th surfaces, C60 grows in a layer-by-layer manner with nucleation occu
rring at steps separating narrow terraces followed by growth from the
steps onto larger terraces. However, differences in C60 growth on the
two surfaces due to the Au(111) surface reconstruction were observed.
Also, on Ag(111), C60 was found to form a 2 square-root 3 X 2 square-r
oot 3 R30-degrees structure while on Au(111) a 38 X 38 in-phase struct
ure was also observed indicating a stronger driving force for adsorpti
on into specific sites on Ag(111). Adsorbed C60 molecules were found t
o rotate faster on Au(111) than on Ag(111) also indicating a stronger
interaction between C60 and Ag. Annealing studies, however, showed tha
t C60 desorbs from both Au(111) and Ag(111) at approximately 500-degre
es-C indicating that differences in interaction strength between the t
wo surfaces cannot be large. The mobility of first and second layer mo
lecules was also studied using STM. The results indicated that individ
ual adsorbed molecules are sufficiently mobile for thermodynamic consi
derations to be important in determining nucleation and growth on both
surfaces. It was also found that small second layer islands rearrange
over the time-scale of minutes, but that concerted motion and rearran
gement of large first layer domains is not likely at room temperature
on both surfaces.