A model which describes self-diffusion, island nucleation and film gro
wth on fee (001) metal substrates is presented. The parameters of the
model are optimized to describe Cu diffusion on Cu(001) by comparing a
ctivation energy barriers to a full set of barriers obtained from semi
-empirical potentials via the embedded-atom method. It is found that t
his model (model I), with only three parameters, provides a very good
description of the full landscape of hopping-energy barriers. These en
ergy barriers are grouped in foils main peaks. A reduced model (model
II) with only two parameters is also presented. in which each peak is
collapsed into a single energy value. From the results of our simulati
ons, we find that this model still maintains the essential features of
diffusion and growth oil this model surface. We Iind that hopping rat
es along island edges are much higher than for isolated atoms (giving
rise to compact island shapes), and that vacancy mobility is higher th
an adatom mobility. We observe substantial dimer mobility (comparable
to the single-atom mobility) as well as some mobility of trimers. The
mobility of small islands affects the scaling of island density IV ver
sus deposition rate F (N approximate to F-v) as well as the island siz
e distribution. In the asymptotic limit of slow deposition. scaling ar
guments and rate equations show that gamma=i/(2i+1), where i* is the
size of the largest mobile island. Our Monte Carlo results, obtained f
or a range of experimentally relevant conditions, show gamma=0.32 +/-
0.01 for the EAM barrier, 0.33 +/- 0.01 for the model I barrier and 0.
31+/-0.01 For the model II barrier. These results are loa rr than the
anticipated value of gamma greater than or equal to 0.4 due to dimer (
and trimer) mobility. (C) 1998 Elsevier Science B.V.