LNOAUGXC: Difference between revisions
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{{TAGDEF|LNOAUGXC|.TRUE. {{!}} .FALSE. |.FALSE.}} | {{TAGDEF|LNOAUGXC|.TRUE. {{!}} .FALSE. |.FALSE.}} | ||
Description: {{TAG|LNOAUGXC}} specifies if a | Description: {{TAG|LNOAUGXC}} specifies if a [[meta-GGA|meta-GGA functional]] is evaluated with a density that is augmented or not. | ||
---- | ---- | ||
The Kohn-Sham kinetic-energy density <math>\tau_{\sigma}</math> should in principle be larger than the von Weizsäcker kinetic-energy density <math>\tau_{\sigma}^{\textrm{W}}=\left\vert\nabla | The Kohn-Sham kinetic-energy density | ||
:<math>\tau_{\sigma}=\frac{1}{2}\sum_{i}\nabla\psi_{i\sigma}^{*}\cdot\nabla\psi_{i\sigma}</math> | |||
should, in principle, be larger than the von Weizsäcker kinetic-energy density{{cite|kurth:ijqc:1999}} | |||
:<math>\tau_{\sigma}^{\textrm{W}}=\frac{\left\vert\nabla n_{\sigma}\right\vert^{2}}{8 n_{\sigma}}.</math> | |||
However, this may not always be the case, particularly within the PAW spheres, when the pseudo density is augmented with the compensation charge. If {{TAG|LNOAUGXC}}=.TRUE. is set in the {{FILE|INCAR}} file, then the pseudo density is not augmented, which should alleviate the breaking of the condition <math>\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}</math>. | |||
A violation of <math>\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}</math> can make the calculations unstable, in particular with the TPSS family of functionals. | |||
{{NB|mind| | {{NB|mind| | ||
*This tag is available since VASP.6.5.0 and is a replacement of the compiler option [[Precompiler options#-DnoAugXCmeta|-DnoAugXCmeta]] that was available until VASP.6.4.3. | *This tag is available since VASP.6.5.0 and is a replacement of the compiler option [[Precompiler options#-DnoAugXCmeta|-DnoAugXCmeta]] that was available until VASP.6.4.3. | ||
*This option may negatively affect the results, therefore it should be used only for functionals, e.g. TPSS, for which the breaking of the condition <math>\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}</math> may lead to numerical problems.}} | *This option may negatively affect the results, therefore it should be used only for functionals, e.g., TPSS, for which the breaking of the condition <math>\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}</math> may lead to numerical problems.}} | ||
== Related tags and articles == | == Related tags and articles == | ||
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<references/> | <references/> | ||
[[Category:INCAR tag]][[Category:Exchange-correlation functionals]][[Category:meta-GGA]][[Category:Projector-augmented-wave method]] | |||
[[Category:INCAR tag]][[Category:Exchange-correlation functionals]][[Category:meta-GGA]] | |||
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Latest revision as of 11:02, 7 January 2025
LNOAUGXC = .TRUE. | .FALSE.
Default: LNOAUGXC = .FALSE.
Description: LNOAUGXC specifies if a meta-GGA functional is evaluated with a density that is augmented or not.
The Kohn-Sham kinetic-energy density
should, in principle, be larger than the von Weizsäcker kinetic-energy density[1]
However, this may not always be the case, particularly within the PAW spheres, when the pseudo density is augmented with the compensation charge. If LNOAUGXC=.TRUE. is set in the INCAR file, then the pseudo density is not augmented, which should alleviate the breaking of the condition .
A violation of can make the calculations unstable, in particular with the TPSS family of functionals.
Mind:
|