Driving force for the WO3(001) surface relaxation

• DOI: 10.1016/j.susc.2007.01.013
• Publication Date: 2007-01-19T12:18:45Z
• Authors: I.N. Yakovkin; M. Gutowski
• Keywords: 02 engineering and technology; 0210 nano-technology

Abstract The optimized structure of the WO 3 (0 0 1) surface with various types of termination ((1 × 1)O, (1 × 1)WO 2 , and c(2 × 2)O) has been simulated using density functional theory with the Perdew–Wang 91 gradient corrected exchange–correlation functional. While the energy of bulk WO 3 depends weakly on the distortions and tilting of the WO 6 octahedra, relaxation of the (0 0 1) surface results in a significant decrease of surface energy (from 10.2 × 10 −2 eV/A 2 for the cubic ReO 3 -like, c(2 × 2)O-terminated surface to 2.2 × 10 −2 eV/A 2 for the relaxed surface). This feature illustrates a potential role of surface relaxation in formation of crystalline nano-size clusters of WO 3 . The surface relaxation is accompanied by a dramatic redistribution of the density of states near the Fermi level, in particular a transformation of surface electronic states. This redistribution is responsible for the decrease of electronic energy and therefore is suggested to be the driving force for surface relaxation of the WO 3 (0 0 1) surface and, presumably, similar surfaces of other transition metal oxides.