Electrostatic corrections
For charged cells or for calculations of molecules and surfaces with a large dipole moment, the energy converges very slowly with respect to the size of the supercell. Using methods discussed in Ref. [55,56] VASP can correct for the leading errors, but one should stress, that in many details, we have taken a more general approach than the one outlined in Ref. [55].
For systems with a net dipole moment, the energy also converges slowly with respect to the size of the super cell. The dipole corrections (and quadrupole corrections for charged systems) fall off like . Both corrections, dipole and quadrupole for charged systems, will be calculated and added to the total energy if the IDIPOL flag is set.
Note: strictly speaking quadrupole corrections is not the proper wording. The relevant quantity is
The following flags control the behaviour of VASP.
- NELECT, total number of electrons
- EPSILON, dielectric constant
- IDIPOL, type of correction (monopole/dipole and quadrupole)
- DIPOL, center of the net charge of the cell
- LDIPOL and LMONO, enable dipole and/or monopole corrections
- EFIELD, applied electrostatic field
For the current implementation, there are several restrictions; please read carefully:
- Charged systems:
Quadrupole corrections are only correct for cubic supercells (this means that the calculated corrections are wrong for charged supercells if the supercell is non cubic). In addition, we have found empirically that for charged systems with excess electrons (NELECTNELECT ) more reliable results can be obtained if the energy after correction of the linear error () is plotted against to extrapolate results manually for . This is due to the uncertainties in extracting the quadrupole moment of systems with excess electrons. - Potential corrections are only possible for orthorhombic cells (at least the direction in which the potential is corrected must be orthogonal to the other two directions).
Related Tags and Sections
NELECT, EPSILON, DIPOL, IDIPOL, LDIPOL, LMONO, EFIELD