We have calculated the local magnetic moments and magnetic order for a
Fe(Cr) monolayer adsorbed on a stepped Cr(Fe)(107) substrate. The ele
ctronic structure at T=0 K has been self-consistently determined withi
n the unrestricted Hartree-Fock approximation of the Hubbard Hamiltoni
an in the framework of a real-space tight-binding method. In the Cr/Fe
(107) system, two magnetic arrangements have been obtained, the more s
table being the less frustrated as obtained in the case of V overlayer
s on vicinal substrates of Fe. An analysis of both solutions in terms
of the total energy calculation and the different degree of frustratio
n is presented. For Fe/Cr(107), a two-step periodicity is obtained. Th
e sign of the magnetization at the Fe overlayer changes from step to s
tep. This spin-flop transition is consistent with the two-layer period
oscillation recently observed in Fe/Cr/Fe wedge structures, and with
the total magnetization determined from in situ magnetometer measureme
nts during growth of ultrathin Fe films on Cr(001).