The electronic band structure of polar polymorph α/β-BaTeMo2O9 phases
Creators
- 1. Center of Excellence Geopolymer and Green Technology, School of Material Engineering, University Malaysia Perlis, 01007 Kangar, Perlis (Malaysia)
- 2. New Technologies – Research Centre, University of West Bohemia, Univerzitni 8, 306 14 Pilsen (Czech Republic)
Description
Based on the reported experimental geometrical structure, a comprehensive theoretical calculations were performed to investigate the electronic band structure, the angular momentum projected density of states, the electronic charge density distribution and the chemical bonding characters of α-BaTeMo2O9 and β-BaTeMo2O9. Calculation reveals that in both phases the conduction band minimum (CBM) is located at Γ point of first Brillouin zone (BZ) whereas the valence band maximum (VBM) of β-BaTeMo2O9 phase is situated in the mid way between Z and Γ points of BZ, while it is located at Z point for α-BaTeMo2O9 phase, resulting in an indirect band gap of about 2.93 eV (β) and 3.12 eV (α) in good agreement with the measured values 2.95 eV (β) and 3.12 eV (α). It has been noticed that the VBM is mainly formed by O-p states while the CBM is controlled by Mo-d state. The valence band's electronic charge density distribution reveals that β-BaTeMo2O9 phase show there exists a strong covalent bonding between Mo and O also between Te and O atoms, while Ba atom forms mostly ionic and partially covalent bonding with O atom. The phase transition from β → α cause to perturb the interaction between Mo and O atoms, Te and O atoms and Ba and O atoms which is attributed to the different arrangement between the atoms of the two phases, where the asymmetric unit of β-phase have a formula BaTeMo2O9 while for α-phase the asymmetric unit have the formula Ba2Te2Mo4O18. Due to the electro-negativity difference between the atoms we can see a charge transfer towards O atoms as indicated by the blue color around O atoms. The calculated bond lengths and angles show good agreement with the experimental values. The good agreement with experimental data in the matter of lattice parameters, energy gap values, the bond lengths and angles reveals the accuracy of the selected exchange correlation potentials used here. - Highlights: • β-BaTeMo2O9 and α-BaTeMo2O9 phases show indirect band gap. • The valence band's electronic charge density distribution were calculated. • Asymmetric unit of β-phase have formula BaTeMo2O9 while α-phase it has Ba2Te2Mo4O18.
Availability note (English)
Available from http://dx.doi.org/10.1016/j.jallcom.2015.08.142Additional details
Identifiers
- DOI
- 10.1016/j.jallcom.2015.08.142;
- PII
- S0925-8388(15)30838-0;
Publishing Information
- Journal Title
- Journal of Alloys and Compounds
- Journal Volume
- 651
- Journal Page Range
- p. 308-315
- ISSN
- 0925-8388
- CODEN
- JALCEU
INIS
- Country of Publication
- Netherlands
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 49048710
- Subject category
- S36: MATERIALS SCIENCE;
- Resource subtype / Literary indicator
- Numerical Data
- Descriptors DEI
- ATOMS; BOND LENGTHS; BONDING; BRILLOUIN ZONES; CHARGE DENSITY; CHEMICAL BONDS; ENERGY GAP; EXPERIMENTAL DATA; LATTICE PARAMETERS; PHASE TRANSFORMATIONS
- Descriptors DEC
- DATA; DIMENSIONS; FABRICATION; INFORMATION; JOINING; LENGTH; NUMERICAL DATA; ZONES
Optional Information
- Copyright
- Copyright (c) 2015 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.