Many competing ceria (110) oxygen vacancy structures: From small to large supercells

被引:47
|
作者
Kullgren, Jolla [1 ]
Hermansson, Kersti [1 ,2 ]
Castleton, Christopher [3 ]
机构
[1] Uppsala Univ, Dept Chem, Angstrom Lab, S-75121 Uppsala, Sweden
[2] Royal Inst Technol KTH, Dept Theoret Chem, S-10691 Stockholm, Sweden
[3] Nottingham Trent Univ, Sch Sci & Technol, Nottingham NG11 8NS, England
来源
JOURNAL OF CHEMICAL PHYSICS | 2012年 / 137卷 / 04期
基金
瑞典研究理事会;
关键词
LOW-INDEX SURFACES; ELECTRONIC-STRUCTURE; POLARON MOTION; MICROSCOPIC OBSERVATIONS; CEO2(111) SURFACES; CEO2; SURFACES; REDUCED CEO2; DYNAMICS; METAL; TRANSITION;
D O I
10.1063/1.4723867
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We present periodic "DFT+U" studies of single oxygen vacancies on the CeO2(110) surface using a number of different supercells, finding a range of different local minimum structures for the vacancy and its two accompanying Ce(III) ions. We find three different geometrical structures in combination with a variety of different Ce(III) localization patterns, several of which have not been studied before. The desired trapping of electrons was achieved in a two-stage optimization procedure. We find that the surface oxygen nearest to the vacancy either moves within the plane towards the vacancy, or rises out of the surface into either a symmetric or an unsymmetric bridge structure. Results are shown in seven slab geometry supercells, p(2 x 1), p(2 x 2), p(2 x 3), p(3 x 2), p(2 x 4), p(4 x 2), and p(3 x 3), and indicate that the choice of supercell can affect the results qualitatively and quantitatively. An unsymmetric bridge structure with one nearest and one next-nearest neighbour Ce(III) ion (a combination of localizations not previously found) is the ground state in all (but one) of the supercells studied here, and the relative stability of other structures depends strongly on supercell size. Within any one supercell the formation energies of the different vacancy structures differ by up to 0.5 eV, but the same structure can vary by up to similar to 1 eV between supercells. Furthermore, finite size scaling suggests that the remaining errors (compared to still larger supercells) can also be similar to 1 eV for some vacancy structures. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4723867]
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