TY - JOUR
T1 - Theoretical study of the (110) surface of Sn1 - XTi xO2 solid solutions with different distribution and content of Ti
AU - Hahn, Konstanze R.
AU - Tricoli, Antonio
AU - Santarossa, Gianluca
AU - Vargas, Angelo
AU - Baiker, Alfons
PY - 2011/8
Y1 - 2011/8
N2 - The composition and thermodynamic stability of the (110) surface of Sn 1 - xTixO2 rutile solid solutions was investigated as a function of Ti-distribution and content up to the formation of a full TiO2 surface monolayer. The bulk and (110) surface properties of Sn1 - xTixO2 were compared to that of the pure SnO2 and TiO2 crystal. A large supercell of 720 atoms and a localized basis set based on the Gaussian and plane wave scheme allowed the investigation of very low Ti-content and symmetry. For the bulk, optimization of the crystal structure confirmed that up to a Ti-content of 3.3 at.%, the lattice parameters (a, c) of SnO2 do not change. Increasing further the Ti-content decreased both lattice parameters down to those of TiO2. The surface energy of these solid solutions did not change for Ti-substitution in the bulk of up to 20 at.%. In contrast, substitution in the surface layer rapidly decreased the surface energy from 0.99 to 0.74 J/m 2 with increasing Ti-content from 0 to 20 at.%. As a result, systems with Ti atoms distributed in the surface (surface enrichment) had always lower energies and thus were thermodynamically more favorable than those with Ti homogeneously distributed in the bulk. This was attributed to the lower energy necessary to break the TiO bonds than SnO bonds in the surface layer. In fact, distributing the Ti atoms homogeneously or segregated in the (110) surface led to the same surface energy indicating that restructuring of the surface bond lengths has minimal impact on thermodynamic stability of these rutile systems. As a result, a first theoretical prediction of the composition of Sn 1 - xTixO2 solid solutions is proposed.
AB - The composition and thermodynamic stability of the (110) surface of Sn 1 - xTixO2 rutile solid solutions was investigated as a function of Ti-distribution and content up to the formation of a full TiO2 surface monolayer. The bulk and (110) surface properties of Sn1 - xTixO2 were compared to that of the pure SnO2 and TiO2 crystal. A large supercell of 720 atoms and a localized basis set based on the Gaussian and plane wave scheme allowed the investigation of very low Ti-content and symmetry. For the bulk, optimization of the crystal structure confirmed that up to a Ti-content of 3.3 at.%, the lattice parameters (a, c) of SnO2 do not change. Increasing further the Ti-content decreased both lattice parameters down to those of TiO2. The surface energy of these solid solutions did not change for Ti-substitution in the bulk of up to 20 at.%. In contrast, substitution in the surface layer rapidly decreased the surface energy from 0.99 to 0.74 J/m 2 with increasing Ti-content from 0 to 20 at.%. As a result, systems with Ti atoms distributed in the surface (surface enrichment) had always lower energies and thus were thermodynamically more favorable than those with Ti homogeneously distributed in the bulk. This was attributed to the lower energy necessary to break the TiO bonds than SnO bonds in the surface layer. In fact, distributing the Ti atoms homogeneously or segregated in the (110) surface led to the same surface energy indicating that restructuring of the surface bond lengths has minimal impact on thermodynamic stability of these rutile systems. As a result, a first theoretical prediction of the composition of Sn 1 - xTixO2 solid solutions is proposed.
KW - Density functional calculations
KW - Low index single crystal surfaces
KW - Semiconducting surfaces
KW - Surface energy
KW - Surface relaxation and reconstruction
KW - Surface structure morphology
KW - Tin oxides
KW - Titanium oxide
UR - http://www.scopus.com/inward/record.url?scp=79959830448&partnerID=8YFLogxK
U2 - 10.1016/j.susc.2011.05.016
DO - 10.1016/j.susc.2011.05.016
M3 - Article
SN - 0039-6028
VL - 605
SP - 1476
EP - 1482
JO - Surface Science
JF - Surface Science
IS - 15-16
ER -