NGZF: Difference between revisions
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On this "fine" FFT mesh the localized augmentation charges are represented if ultrasoft pseudopotentials (USPPs) or the PAW method are used. In case USPPs are used, the local potentials (exchange-correlation, Hartree-potential, and ionic potentials) are also calculated on this "fine" FFT-mesh. | On this "fine" FFT mesh the localized augmentation charges are represented if ultrasoft pseudopotentials (USPPs) or the PAW method are used. In case USPPs are used, the local potentials (exchange-correlation, Hartree-potential, and ionic potentials) are also calculated on this "fine" FFT-mesh. | ||
By default {{TAG|NGZF}} is set in accordance with the requested "precision" | By default {{TAG|NGZF}} is set in accordance with the requested "precision" mode {{TAG|PREC}}, {{TAG|NGZ}}, and the plane wave kinetic energy cutoffs {{TAG|ENCUT}} and {{TAG|ENAUG}}: | ||
::{| cellpadding="5" cellspacing="0" border="1" | ::{| cellpadding="5" cellspacing="0" border="1" | ||
|{{TAG|PREC}} || {{TAG|NGZ}} || {{TAG|NGZF}} | |{{TAG|PREC}} ||align="center"| {{TAG|NGZ}} ||align="center"| {{TAG|NGZF}} | ||
|- | |- | ||
| Normal || 3/2× | | Normal ||align="center"| 3/2×<math>G_{\rm cut}</math> ||align="center"| 2×{{TAG|NGZ}} | ||
|- | |- | ||
| Single || 3/2× | | Single (VASP.5) ||align="center"| 3/2×<math>G_{\rm cut}</math> ||align="center"| {{TAG|NGZ}} | ||
|- | |- | ||
| | | Single (VASP.6) ||align="center"| 2×<math>G_{\rm cut}</math> ||align="center"| {{TAG|NGZ}} | ||
|- | |- | ||
| | | SingleN (VASP.6) ||align="center"| 3/2×<math>G_{\rm cut}</math> ||align="center"| {{TAG|NGZ}} | ||
|- | |- | ||
| | | Accurate ||align="center"| 2×<math>G_{\rm cut}</math> ||align="center"| 2×{{TAG|NGZ}} | ||
|- | |- | ||
| High || | | Low ||align="center"| 3/2×<math>G_{\rm cut}</math> ||align="center"| 3×<math>G_{\rm aug}</math> | ||
|- | |||
| Medium ||align="center"| 3/2×<math>G_{\rm cut}</math> ||align="center"| 4×<math>G_{\rm aug}</math> | |||
|- | |||
| High ||align="center"| 2×<math>G_{\rm cut}</math> ||align="center"| 16/3×<math>G_{\rm aug}</math> | |||
|} | |} | ||
where | where | ||
:<math>E_{\rm cut}=\frac{\hbar^2}{2m_e}G_{\rm cut}^2 \qquad E_{\rm aug}=\frac{\hbar^2}{2m_e}G_{\rm aug}^2</math> | :<math>E_{\rm cut}=\frac{\hbar^2}{2m_e}G_{\rm cut}^2 \qquad E_{\rm aug}=\frac{\hbar^2}{2m_e}G_{\rm aug}^2</math> | ||
with | with <math>E_{\rm cut}</math>={{TAG|ENCUT}} and <math>E_{\rm aug}</math>={{TAG|ENAUG}}. | ||
Alternatively, {{TAG|NGZF}} | Alternatively, {{TAG|NGZF}} can be set to a specific value in the {{FILE|INCAR}} file. | ||
== Related tags and articles == | == Related tags and articles == | ||
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{{TAG|PREC}}, | {{TAG|PREC}}, | ||
{{TAG|ENCUT}}, | {{TAG|ENCUT}}, | ||
{{TAG|ENAUG | {{TAG|ENAUG}} | ||
{{sc|NGZF|Examples|Examples that use this tag}} | {{sc|NGZF|Examples|Examples that use this tag}} | ||
[[Category:INCAR tag]][[Category: | [[Category:INCAR tag]][[Category:Projector-augmented-wave method]] |
Latest revision as of 11:57, 17 October 2024
NGZF = [integer]
Default: NGZF = set in accordance with PREC, NGZ, ENCUT and ENAUG
Description: NGZF sets the number of grid points in the "fine" FFT grid along the first lattice vector.
On this "fine" FFT mesh the localized augmentation charges are represented if ultrasoft pseudopotentials (USPPs) or the PAW method are used. In case USPPs are used, the local potentials (exchange-correlation, Hartree-potential, and ionic potentials) are also calculated on this "fine" FFT-mesh.
By default NGZF is set in accordance with the requested "precision" mode PREC, NGZ, and the plane wave kinetic energy cutoffs ENCUT and ENAUG:
where
Alternatively, NGZF can be set to a specific value in the INCAR file.