TY - JOUR
T1 - Origin of the Diverse Behavior of Oxygen Vacancies in ABO3 Perovskites: A Symmetry Based Analysis
AU - Yin, Wan Jian
AU - Wei, Su Huai
AU - Al-Jassim, Mowafak M.
AU - Yan, Yanfa
PY - 2012/5/14
Y1 - 2012/5/14
N2 - Using band symmetry analysis and density functional theory calculations, we reveal the origin of why oxygen vacancy (V O) energy levels are shallow in some ABO 3 perovskites, such as SrTiO 3, but are deep in some others, such as LaAlO 3. We show that this diverse behavior can be explained by the symmetry of the perovskite structure and the location (A or B site) of the metal atoms with low d orbital energies, such as Ti and La atoms. When the conduction band minimum (CBM) is an antibonding Γ 12 state, which is usually associated with the metal atom with low d orbital energies at the A site (e.g., LaAlO 3), then the V O energy levels are deep inside the gap. Otherwise, if the CBM is the nonbonding Γ25 ′ state, which is usually associated with metal atoms with low d orbital energies at the B site (e.g., SrTiO 3), then the V O energy levels are shallow and often above the CBM. The V O energy level is also deep for some uncommon ABO 3 perovskite materials that possess a low s orbital, or large-size cations, and an antibonding Γ 1 state CBM, such as ZnTiO 3. Our results, therefore, provide guidelines for designing ABO 3 perovskite materials with desired functional behaviors.
AB - Using band symmetry analysis and density functional theory calculations, we reveal the origin of why oxygen vacancy (V O) energy levels are shallow in some ABO 3 perovskites, such as SrTiO 3, but are deep in some others, such as LaAlO 3. We show that this diverse behavior can be explained by the symmetry of the perovskite structure and the location (A or B site) of the metal atoms with low d orbital energies, such as Ti and La atoms. When the conduction band minimum (CBM) is an antibonding Γ 12 state, which is usually associated with the metal atom with low d orbital energies at the A site (e.g., LaAlO 3), then the V O energy levels are deep inside the gap. Otherwise, if the CBM is the nonbonding Γ25 ′ state, which is usually associated with metal atoms with low d orbital energies at the B site (e.g., SrTiO 3), then the V O energy levels are shallow and often above the CBM. The V O energy level is also deep for some uncommon ABO 3 perovskite materials that possess a low s orbital, or large-size cations, and an antibonding Γ 1 state CBM, such as ZnTiO 3. Our results, therefore, provide guidelines for designing ABO 3 perovskite materials with desired functional behaviors.
UR - http://www.scopus.com/inward/record.url?scp=84861534040&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.85.201201
DO - 10.1103/PhysRevB.85.201201
M3 - Article
AN - SCOPUS:84861534040
SN - 1098-0121
VL - 85
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 20
M1 - Article No. 201201(R)
ER -