We determined the surface structure of RuO2(100) formed on Ru(1010) by empl
oying the techniques of low-energy electron diffraction (LEED) and density
functional theory (DFT) calculations. The RuO2(100) film grows lattice-matc
hed with its [010] direction along the [0001] direction of Ru(1010) (4.5% c
ompressively strained), while it grows incommensurately with the [001] dire
ction of RuO2(100) along the [1.210] direction of Ru(1010). The RuO2(100) s
urface is terminated by bridging O atoms, which are attached to the coordin
atively unsaturated Ru (cus-Ru) atoms with a bond length pf 2.01 Angstrom.
The other Ru-O bond lengths are in the range of 1.90-2.05 Angstrom, typical
for bulk RuO2. Due to the presence of cus-Ru atoms on RuO2(100), CO molecu
les adsorb quite strongly as evidenced by a desorption state at 300-400 K.
The activity of the RuO2(100) surface for the CO oxidation reaction is simi
lar to that of RuO2(110). The surface energies of RuO2(110) and RuO2(100) a
re 71 and 87 meV/Angstrom (2), respectively.