Simulated kinematic antiphase RHEED and HRLEED profiles are calculated
along with the surface structure factor for a model of Fe/Fe(100) dep
osition in order to clarify the interpretation of diffraction profiles
in recent experiments on Fe/Fe(100) growth. Similar calculations are
also presented for a self-affine surface. While self-affine surfaces d
o not exhibit a characteristic RHEED peak, in the case of surfaces wit
h a typical length scale the simulated RHEED profile exhibits a peak c
orresponding to the typical feature size, in agreement with recent exp
eriments. The existence of this peak appears to be due to the large am
ount of shadowing present in low-angle RHEED, which limits the amount
of destructive interference between layers. In contrast, simulated ant
iphase HRLEED patterns appear to approach an invariant profile for bot
h self-affine and mound-like surface morphologies. For the case of sma
ll mounds, our results predict a HRLEED profile with a weak peak corre
sponding to the average terrace size which moves outward with increasi
ng coverage, and eventually reaches an invariant form due to angle sel
ection. The disappearance of the HRLEED peak for surfaces which have l
arge mound structures is explained in terms of the antiphase condition
and the range of variation of terrace sizes and provides an alternati
ve explanation for the HRLEED results observed in Ref. [10].