Characterization of BAND
- Formation energy with respect to isolated atoms that are computed with a
fully numerical Herman-Skillman type subprogram
- A choice of density functionals, including LDA (Local Density
Approximation) and GGA (Generalized Gradient Approximation) formulas
- Automatic geometry optimization has not yet been implemented
- Mulliken populations for basis functions, overlap populations between
atoms or between basis functions.
- Densities-of-States: DOS, PDOS and OPWDOS/COOP
- Form factors (X-ray structures)
- Charge analysis using Voronoi cells (yielding Voronoi Deformation Charges)
- Orbital plots
- One-electron energies and orbitals at the Brillouin Zone sample points
- Fragment orbitals and a Mulliken type population analysis in terms of the
fragment orbitals
- SCF convergence based on a Direct Inversion of Iterative Subspace (DIIS)
method
- The implementation is built upon a highly optimized numerical integration
scheme for the evaluation of matrix elements of the Hamiltonian, property
integrals involving the charge density, etc.
- The program has been parallelized and vectorized
- Basis functions are Slater-Type Orbitals (STOs) and/or Numerical Orbitals
(NOs) and/or Plane Waves (PWs).
- Fit functions are Slater-type exponential functions centered on the atoms
and are used to fit the deformation density, which is the difference between
the final density and the startup density. The deformation density has zero
charge and will in general be small. The fitted deformation density is used for
the calculation of the Coulomb potential and the derivatives of the total
density (needed for the gradient corrections in the exchange-correlation
functionals). In both cases the main part, due to the startup density, is
calculated accurately by a numerical procedure, and only the small part from
the deformation density is obtained via the fit.
- A frozen core facility is provided to allow efficient treatment of the
inner atomic shells.
- Space group symmetry is used to reduce the computational effort in the
integrals over the Brillouin zone.