Abstract
An analysis of the symmetry of the electron wave functions as they evolve under the molecular-dynamics equation of motion is presented. It is found that symmetry in the initial conditions, corresponding to wave functions of two or more bands being partner functions, can prevent wave functions from converging to eigenfunctions of the Hamiltonian. This artificial symmetry is broken by the Gram-Schmidt orthogonalization procedure so any convenient initial conditions will lead to convergence to eigenstates of the Hamiltonian.
- Received 6 April 1987
DOI:https://doi.org/10.1103/PhysRevB.37.8138
©1988 American Physical Society