SBO In Silico Materials B/10784/*

Increasing the Al concentration in Al-doped ZnO (AZO) is one way of improving the conductivity of this transparent conductive oxide (TCO). Beyond a certain concentration, an unwanted secondary phase develops with a low conductivity. Its stoichiometry is Zn3Al2O6, and its crystal structure has not yet been convincingly determined. By applying unbiased ab initio structure prediction tools, we predict the crystal structure of Zn3Al2O6 to be monoclinic with space group Pm. It can be described as a nanofabric, with one-dimensional Al2O3 wires penetrating a ZnO matrix. This crystal has a formation energy that is lower than any structure proposed before, and is consistent with all available experimental information. Knowledge of the nature of this phase can help to avoid its formation and therefore to engineer AZO crystals with an increased level of Al-doping and associated increased conductivity.

We present an experimental lattice location study of Ga atoms in Ge after ion implantation at elevated temperature (250 degrees C). Using extended x-ray absorption fine structure (EXAFS) experiments and a dedicated sample preparation method, we have studied the lattice location of Ga atoms in Ge with a concentration ranging from 0.5 at. % down to 0.005 at. %. At Ga concentrations http://dx.doi.org/10.1063/1.4773185]

We present electronic band structures of transparent oxides calculated using the Tran–Blaha modified Becke–Johnson (TB-mBJ) potential. We studied the basic n-type conducting binary oxides In2O3, ZnO, CdO and SnO2 along with the p-type conducting ternary oxides delafossite CuXO2 (X=Al, Ga, In) and spinel ZnX2O4 (X=Co, Rh, Ir). The results are presented for calculated band gaps and effective electron masses. We discuss the improvements in the band gap determination using TB-mBJ compared to the standard generalized gradient approximation (GGA) in density functional theory (DFT) and also compare the electronic band structure with available results from the quasiparticle GW method. It is shown that the calculated band gaps compare well with the experimental and GW results, although the electron effective mass is generally overestimated.