N doping of rutile TiO2 (110) surface. A theoretical DFT study


Por: Graciani J., Álvarez L.J., Rodriguez J.A., Sanz J.F.

Publicada: 1 ene 2008
Resumen:
A realistic model, consisting of six-layer slabs, and density-functional calculations were used to perform a detailed analysis of the structural and electronic properties of N doped TiO2(110). All the positions examined for adsorption of atomic N are unstable regarding the formation and further escape of N2(g). The adsorption of atomic N could take place only when having isolated adatoms. In this case, N prefers to bond to O centers located either on the surface or in the interstitial channels of the oxide lattice. These N adatoms probably give rise to the peak seen at ?400 eV in N 1s XPS spectra. The coexistence of N with O vacancies and surface reconstructions are explained in terms of cooperative behaviors and the special electronic structure of the TiNxO2-2x(110) system. Here, electrons move from the O vacancies to implanted N to fill up its electronic shell. Such electron transfer yields the normal oxidation state of nitrogen, N3-, and explains a number of things: the easiness to form O vacancies when implanted N is present, the easiness to implant N when O vacancies are present, and the difficulty for the implanted N to escape. It is not likely that N-doping will improve the photocatalytic behavior of TiO 2-x(110) surfaces. For these compounds the band gap will be always equal or larger than that of pure stoichiometric TiO2. © 2008 American Chemical Society.

Filiaciones:
Departamento de Química Física, Facultad de Química, Universidad de Sevilla, E-41012, Sevilla, Spain
Instituto de Matemáticas, Unidad Cuernavaca, Universidad Nacional Autónoma de México, 62170 Cuernavaca, Morelos, Mexico
Chemistry Department, Brookhaven National Laboratory, Upton, NY 11973, United States
ISSN: 19327447
Editorial
AMER CHEMICAL SOC, 1155 16TH ST, NW, WASHINGTON, DC 20036 USA, Estados Unidos America
Tipo de documento: Article
Volumen: 112 Número: 7
Páginas: 2624-2631
WOS Id: 000253222200059

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