The electronic structure and the magnetism of an Fe monolayer on Mo(110) [1
Fe/Mo(110)] were investigated by means of the all-electron full-potential l
inearized augmented plane-wave (FLAPW) method, based on the local density a
pproximation (LDA), with a single slab approach to simulate the system. For
an unrelaxed clean 1Fe/Mo(110)(assuming the Fe-Mo interlayer spacing to be
the average value of the bulk Fe and the Mo interlayer spacings), we found
the magnetic moment of the Fe to be 2.21 mu(B), which was almost the same
as the calculated value (2.22 mu(B)) of the Fe bulk. For a relaxed clean on
e determined from the total energy calculations, we found the magnetic mome
nt of the Fe to be 2.15 mu(B) which was a little bit smaller than the calcu
lated value (2.18 mu(B)) of Fe in a relaxed 1Fe/W(110) system. The total co
ntact hyperfine field and the work function for relaxed (unrelaxed) 1Fe/Mo(
110) were calculated to be -158 kG (-168 kG) and 4.60 eV (4.59 eV), respect
ively. The charge and the spin densities, as well as the layer projected de
nsity of states, are presented to discuss the effects of band hybridization
between the Fe and the Mo atoms on the magnetism of Fe.