LDIPOL: Difference between revisions
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The biggest advantage of this mode is that leading errors in the forces are corrected and that the work function can be evaluated for asymmetric slabs. The disadvantage is that the convergence to the electronic ground state might slow down considerably, i.e., more electronic iterations might be required to obtain the required precision. | The biggest advantage of this mode is that leading errors in the forces are corrected and that the work function can be evaluated for asymmetric slabs. The disadvantage is that the convergence to the electronic ground state might slow down considerably, i.e., more electronic iterations might be required to obtain the required precision. | ||
{{NB|important|It is important to ensure convergence of the dipole correction, e.g., by increasing the number of elementary steps with {{TAG|NELM}} and tightening the energy convergence <code>{{TAG|EDIFF}} {{=}} 1E-6</code>. An unconverged dipole correction can lead to erroneous forces [[https://vasp.at/forum/viewtopic.php?t=20300]].}} | {{NB|important|It is important to ensure convergence of the dipole correction, e.g., by increasing the number of elementary steps with {{TAG|NELM}} and tightening the energy convergence <code>{{TAG|EDIFF}} {{=}} 1E-6</code>. Furthermore convergence can be often accelerated by setting AMIN to a smaller value, <code>{{TAG|AMIN}} {{=}} 0.01</code>. An unconverged dipole correction can lead to erroneous forces [[https://vasp.at/forum/viewtopic.php?t=20300]].}} | ||
{{NB|warning| For charged systems, the potential correction is currently only implemented for cubic supercells. VASP will stop if the supercell is not cubic and {{TAG|LDIPOL}} is used. }} | {{NB|warning| For charged systems, the potential correction is currently only implemented for cubic supercells. VASP will stop if the supercell is not cubic and {{TAG|LDIPOL}} is used. }} | ||
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Revision as of 10:06, 8 November 2025
LDIPOL = .TRUE. | .FALSE.
Default: LDIPOL = .FALSE.
Description: LDIPOL switches on corrections to the potential and forces. Can be applied for charged molecules and slabs with a net dipole moment.
The presence of a dipole in combination with periodic boundary conditions leads to a slow convergence of the total energy with the size of the supercell. Furthermore, finite-size errors affect the potential and the forces. This effect can be counterbalanced by setting LDIPOL=.TRUE. in the INCAR file. For LDIPOL=.TRUE., a linear correction, and for charged cells, a quadratic electrostatic potential is added to the local potential in order to correct the errors introduced by the periodic boundary conditions. When activating this tag the tag IDIPOL has to be specified, and optionally the tag DIPOL as well.
| Mind: This is in the spirit of Neugebauer et al. [1], though more general. Note that the total energy is correctly implemented, whereas Ref. [1] contains an erroneous factor 2 in the total energy. |
The biggest advantage of this mode is that leading errors in the forces are corrected and that the work function can be evaluated for asymmetric slabs. The disadvantage is that the convergence to the electronic ground state might slow down considerably, i.e., more electronic iterations might be required to obtain the required precision.
Important: It is important to ensure convergence of the dipole correction, e.g., by increasing the number of elementary steps with NELM and tightening the energy convergence EDIFF = 1E-6. Furthermore convergence can be often accelerated by setting AMIN to a smaller value, AMIN = 0.01. An unconverged dipole correction can lead to erroneous forces [[1]].
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| Warning: For charged systems, the potential correction is currently only implemented for cubic supercells. VASP will stop if the supercell is not cubic and LDIPOL is used. |
Related tags and articles
Monopole Dipole and Quadrupole corrections, NELECT, EPSILON, IDIPOL, DIPOL, LMONO, EFIELD