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O deficiency in the rutile TiO 2 (110) surface: Ab initio quantum chemical investigation of the electronic properties
Author(s) -
Von Oertzen G. U.,
Gerson A. R.
Publication year - 2006
Publication title -
international journal of quantum chemistry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.484
H-Index - 105
eISSN - 1097-461X
pISSN - 0020-7608
DOI - 10.1002/qua.21007
Subject(s) - castep , density functional theory , rutile , atomic orbital , chemistry , ab initio , fermi level , vacancy defect , electronic structure , band gap , stoichiometry , electron , condensed matter physics , atomic physics , molecular physics , crystallography , computational chemistry , physics , organic chemistry , quantum mechanics
The (110) surface of rutile TiO 2 (110) has been modeled using a density functional theory (DFT) plane‐wave pseudo‐potential method (CASTEP). In this study, 6 and 9 atomic‐layer slabs have been examined. The stoichiometric surface converges to a low‐spin solution in both cases with a density of states (DOS) similar to that for the bulk. O deficiencies are introduced by the removal of neutral O atoms thus leaving a neutral model with a surfeit of 2 e − per vacancy. This results in the partial filling of the Ti t 2g conduction band orbitals and a compensatory shift in the Fermi level. The reduced surface converges to a high‐spin solution in all cases, with the excess spin located within the previously unoccupied Ti t 2g orbitals. Removal of the bridging surface O atoms results in an excess spin of 2 electrons per unit cell with approximately one‐half that for removal of in‐plane surface O atoms and subsurface O atoms. The removal of O atoms from the surface leads to an increase of the band gap, with the largest increase due to the removal of in‐plane 3‐fold coordinated surface O atoms, and the smallest one due to the removal of subsurface O atoms. © 2006 Wiley Periodicals, Inc. Int J Quantum Chem, 2006