We address the problem of MBE growth in one horizontal and one vertica
l direction in the presence of Schwoebel barriers. The time-independen
t growth equation introduced previously is shown to be identical to th
at for a classical particle in a potential well. We solve this equatio
n using periodic boundary conditions and find time-independent solutio
ns consisting of a periodic array of mounds. We derive the ''dispersio
n relation'', i.e. the amplitude as a function of wavelength for these
mounds. The equation of motion is derivable from a free energy indica
ting that there is a most stable ground state, which is independent of
the initial conditions. The mounds are marginally unstable and there
is a minimum wavelength below which no mounds exist. The wavelength of
the mounds coarsens slowly in time according to LAMBDA approximately
t(alpha), with alpha almost-equal-to 1/4.