We have studied the growth of Cu islands on rutile TiO2(110)-(1 x 1) using
scanning tunneling microscopy for Cu coverages of 0.03-1.25 monolayers (ML)
. The formation of three-dimensional islands at all the coverages reflects
the relatively high mobility of Cu atoms on TiO2 at room temperature (diffu
sion constant greater than or equal to 4 x 10(-10) cm(2)/s) and the weak in
teraction between Cu and TiO2 compared with Cu-Cu bonding. At low coverages
(< 0.5 ML)I the Cu islands exhibit self-limiting growth: with increasing c
overage, the average island size remains almost constant, and the island de
nsity increases. At higher coverages (>0.5 ML), the average island size sca
les with coverage, but this increase in island size is primarily due to an
increase in height, not diameter. Although larger islands can be formed by
annealing, the average size of the islands is nearly independent of coverag
e for any given annealing temperature. We propose two general schemes that
can simultaneously explain the increase in island density with increasing c
overage and the narrow island size distribution. In the first scheme, the r
ate at which adatoms attach to existing islands drops rapidly as the island
size increases. This could be due to the existence of strain fields that a
ccommodate the lattice mismatch at the interface between the Cu islands and
the TiO2 substrate. Adatoms rejected by the islands are then available for
nucleation of new islands. In the second scheme, the rate at which adatoms
reach existing islands drops rapidly as the Cu coverage increases. This co
uld be related to continued nucleation of islands at defects in the TiO2 su
rface. (C) 2000 Elsevier Science B.V. All rights reserved.