We explore the layer-by-layer (Frank-van der Merwe) growth regime within th
e context of a discrete solid-on-solid kinetic Monte Carlo model. Our resul
ts demonstrate a nontrivial scaling of the lattice step edge density, a qua
ntity that oscillates about a nominally constant value prior to the onset o
f kinetic roughening. This value varies with the ratio of the surface diffu
sivity to the deposition flux, R=D/F, as a nearly perfect power law over a
wide range of R. This ''intermediate'' scaling regime extends in coverage f
rom one to at least a few tens of monolayers, which is exactly the regime o
f most importance to the growth of device-quality semiconductor quantum het
erostructures. Comparison with lowest-order linear theories for height fluc
tuations demonstrates the validity of the Wolf-Villain mean-field theory fo
r the description of lattice step density and "in-plane" structure for all
coverages down to the first monolayer of growth. However, the mean-field th
eory does not fully account for the surface width in this regime and conseq
uently does not quantitatively predict the observed step density scaling.