The geometric structure,
electronic states, and surface spin polarization
of a (H, NO)-coadsorbed Fe3O4(100) surface have
been studied using density functional theory calculations. H atoms
saturate the surface dangling bonds through bonding with the O atom
(O1) without a tetrahedral Fe neighbor (Fe(A)), inducing a deeper
level shift of the spin-up surface state bands and a widening of the
spin-up band gap between the Fermi level (E
F) and the valence band maximum. NO molecules are adsorbed on surface
octahedral Fe atoms (Fe(B)). The adsorbate/substrate and molecule–molecule
interactions cause considerable filling and broadening of the spin-down
2π* states of the adsorbed NO molecule. A −100% spin
polarization is obtained over the energy range of −0.8 eV to E
F for the (H, NO)-coadsorbed Fe3O4(100) surface, indicating that this system has greater potential
for application in spintronic devices than either the solely H-adsorbed
or NO-adsorbed surfaces. Furthermore, the adsorbed NO molecule can
provide a considerable density of −100% spin-polarized states.
Both of these findings are significant for the application and design
of spintronic devices.