Abstract
Until recently, tight-binding has been applied to either covalent or metallic solid state systems, or charge transfer treated in a simple point charge framework. We present a self-consistent tight-binding model which, for the first time, includes electrostatic ion polarisability and crystal field splitting. The tight-binding eigenvectors are used to construct multipole moments of the ionic charges which are used to obtain angular momentum components of the electrostatic potential in structure constant expansions. Our first test of the model is to study the phase stability in zirconia; in particular the instability of the fluorite phase to a spontaneous symmetry breaking, and its interpretation in terms of band effects and ion polarisability. This new formalism opens up the way to apply the tight-binding approximation to problems in which polarisation of atomic charges is important, for example oxides and other ceramic materials and surfaces of metals.
Original language | English |
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Pages (from-to) | 265-274 |
Journal | Materials Research Society Symposium Proceedings |
Volume | 491 |
Publication status | Published - 1998 |
Event | Symposium on Materials Science of the Cell at the 1997 MRS Fall Meeting - BOSTON Duration: 1 Dec 1997 → 4 Dec 1997 |
Keywords
- Ions
- Metals
- Mathematical models
- Ceramic materials
- Zirconia, Crystal field splitting
- Self consistent tight binding approximation, Materials science
- Stability
- Electrostatic ion polarisability
- Polarisable ions
- Fluorine compounds
- Eigenvalues and eigenfunctions
- Surfaces
- Approximation theory
- Oxides