Macroscopic Polarization from Electronic Wavefunctions
Abstract
The dipole moment of any finite and neutral system, having a square-integrable wavefunction, is a well defined quantity. The same quantity is ill-defined for an extended system, whose wavefunction invariably obeys periodic (Born-von Karman) boundary conditions. Despite this fact, macroscopic polarization is a theoretically accessible quantity, for either uncorrelated or correlated many-electron systems: in both cases, polarization is a rather "exotic" observable. For an uncorrelated-either Hartree-Fock or Kohn-Sham-crystalline solid, polarization has been expressed and computed as a Berry phase of the Bloch orbitals (since 1993). The case of a correlated and/or disordered system received a definitive solution only very recently (1998): this latest development allows us present here the whole theory from a novel, and very general, viewpoint. The modern theory of polarization is even relevant to the foundations of density functional theory in extended systems.
Cite
@article{arxiv.cond-mat/9903216,
title = {Macroscopic Polarization from Electronic Wavefunctions},
author = {Raffaele Resta},
journal= {arXiv preprint arXiv:cond-mat/9903216},
year = {2007}
}
Comments
14 pages with 2 figures. Presented at the Sanibel Symposium 1999