Dipartimento di Scienza dei Materiali, Università di Milano-Bicocca, Via R. Cozzi 53, 20125 Milano, Italy.
Phys Chem Chem Phys. 2011 Oct 21;13(39):17667-75. doi: 10.1039/c1cp21987a. Epub 2011 Sep 7.
It has been experimentally observed that Ti doping of bulk ZrO(2) induces a large red-shift of the optical absorption edge of the material from 5.3 to 4.0 eV [Livraghi et al., J. Phys. Chem. C, 2010, 114, 18553-18558]. In this work, density functional calculations based on the hybrid functional B3LYP show that Ti dopants in the substitutional position to Zr in the tetragonal lattice cause the formation of an empty Ti 3d band about 0.5 eV below the bottom of the conduction band. The optical transition level ε(opt)(0/-1) from the topmost valence state to the lowest empty Ti impurity state is found at 4.9 eV in a direct band gap of 5.7 eV. The calculated shift is consistent with the experimental observation. The presence of Ti(3+) species in Ti-doped ZrO(2), probed by means of electron paramagnetic resonance (EPR), is rationalized as the result of electron transfers from intrinsic defect states, such as oxygen vacancies, to substitutional Ti(4+) centers.
实验观察到,Ti 掺杂体相 ZrO(2)会使材料的光吸收边从 5.3 eV 红移到 4.0 eV[Livraghi 等人,J. Phys. Chem. C,2010,114,18553-18558]。在这项工作中,基于杂化泛函 B3LYP 的密度泛函计算表明,在四方晶格中取代 Zr 的 Ti 掺杂剂会导致导带底部以下约 0.5 eV 处形成一个空的 Ti 3d 带。从最高价态到最低空 Ti 杂质态的光学跃迁能级 ε(opt)(0/-1)在 5.7 eV 的直接带隙中位于 4.9 eV。计算出的位移与实验观察结果一致。通过电子顺磁共振 (EPR) 探测到的 Ti 掺杂 ZrO(2)中 Ti(3+)物种可以通过从本征缺陷态(如氧空位)到取代 Ti(4+)中心的电子转移来解释。