International Journal of Modern Physics B · 2014 · 107 citations · 132 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsInorganic ChemistryMaterials ChemistryAb Initio MethodsCrystal ChemistryPerovskite MaterialsSurface Chemistry Of SolidsSurface EnergeticsSurface PhysicsAb Initio CalculationsAb Initio Few-body CalculationsAb Initio Potential Energy SurfacesHalide PerovskitesOrganic-inorganic Hybrid PerovskitesOxide PerovskitesPerovskite Crystal StructureTerminations
In this paper, the review of recent results of calculations of surface relaxations, energetics, and bonding properties for ABO 3 perovskite (001), (011) and (111) surfaces using mostly a hybrid description of exchange and correlation is presented. Both AO and BO 2 -terminations of the nonpolar (001) surface and A , BO , and O terminations of the polar (011) surface, as well as B and AO 3 -terminations of the polar (111) surface were considered. On the AO -terminated (001) surface, all upper-layer A atoms relax inwards, while all second layer atoms relax outwards. For the BO 2 -terminated (001) surface, in most cases, the largest relaxations are on the second-layer metal atoms. For almost all ABO 3 perovskites, the surface rumpling is much larger for the AO -terminated than for the BO 2 -terminated (001) surface, but their surface energies are always quite similar. In contrast, different terminations of the (011) ABO 3 surface lead to very different surface energies for the O -terminated, A -terminated, and BO -terminated (011) surface, respectively. A considerable increase in the Ti – O or Zr – O , respectively, chemical bond covalency near the (011) surface as compared both to the bulk and to the (001) surface in ABO 3 perovskites were predicted. According to the results of ab initio calculations for Nb doped SrTiO 3 , Nb is a shallow donor; six nearest O ions are slightly displaced outwards from the Nb ion. The F center in ABO 3 perovskites resembles electron defects in the partially-covalent SiO 2 crystal rather than usual F centers in ionic crystals like MgO and alkali halides. The results of calculations for several perovskite KNb x Ta 1-x O 3 (KTN) solid solutions, as well as hole and electron polarons in ABO 3 perovskites are analyzed.
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Density-functional thermochemistry. III. The role of exact exchange
Axel D. Becke · The Journal of Chemical Physics · 1993 · 102.8K citations
Natural Sciences, Chemistry, Physics +13
Origin of ferroelectricity in perovskite oxides
R. E. Cohen · Nature · 1992 · 3.1K citations