The growth of magnetic films with ferromagnetic interactions between neares
t-neighbor spins is studied in (d+1)-dimensional rectangular geometries for
d=1,2. Magnetic films are grown irreversibly by adding spins at the bounda
ries of the growing interface. The orientation of the added spins depends o
n both the energetic interaction with already deposited spins and the tempe
rature through a Boltzmann factor. At low temperatures thin films, of thick
ness L, are constituted by a sequence of well ordered magnetic domains. Spi
ns belonging to each domain, of average length l(D)> >L, have mostly the sa
me orientation, but consecutive domains have opposite magnetization. This k
ind of "spontaneous magnetization reversal" during the growth process has a
short characteristic length l(R), such that l(D)> >l(R)similar toL. At hig
her temperatures, a transition between ordered and disordered states is als
o observed. The emerging behavior is compared to that of the equilibrium Is
ing model. (C) 2001 American Institute of Physics.