Abstract

We investigate three superstructures c(2×2), c(3×1) and c(1×1) of oxygen atom adsorption on Fe(110) surface by using first-principles density functional theory. The former two superstructures have been found by experiments at low oxygen exposures. The oxygen adsorption results in some electron transfer from surface Fe atom to O atom due to the strong electronegativity of oxygen atom, which also causes a positive work function change. For all three superstructures, the calculated surface spin density at Fermi level is positive, unlike that on a clean Fe(110) surface. The adsorbate–substrate hybridization is mainly from the interaction between O 2p and Fe 3d orbitals, and O 2p state exhibits obvious exchange spin–split induced by the Fe–O magnetic interaction. The adsorbate O 2p bands of c(2×2) and c(3×1) superstructures exhibit a weaker dispersion, whereas those bands of c(1×1) structure show larger dispersion due to the O–O interaction. Through the band structure calculation, we also calculate the exchange splitting energy of O 2px orbital for c(3×1) structure in k space and compare them with experimental results.

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