Density Functional Theory
An apparent failure of density functional theory (DFT) with the local
density approximation (LDA) or generalized gradient approximations (GGA)
is the overestimation of the electronic static dielectric constant
compared to experiment. Since the dielectric constant is determined by
the second derivative of the ground-state energy with respect to an
applied electric field, it is a ground state property and can in
principle be calculated exactly within DFT. However, for medium- and
small-band-gap materials, the dielectric constant is overestimated by at
least 10% in LDA-based calculations. A slight reduction occurs in the
case of silicon using GGA rather than LDA. The discrepancy between
experiment and LDA- or GGA-based calculations of the dielectric constant
indicates a principal failure inherent to both approximations.
This failure can be traced back to the neglect of the
exchange-correlation energy's polarization dependence in LDA and GGA.
The talk and the paper quantify the relevance of the neglect of
polarization dependence for medium- and wide-gap semiconductors.
To cite this page:
Density Polarization Functional Theory
<http://www.physics.ohio-state.edu/~aulbur/dpft/dpft.html>