LNOAUGXC: Difference between revisions

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{{TAGDEF|LNOAUGXC|.TRUE. {{!}} .FALSE. |.FALSE.}}
{{TAGDEF|LNOAUGXC|.TRUE. {{!}} .FALSE. |.FALSE.}}


Description: {{TAG|LNOAUGXC}} specifies if the {{TAG|METAGGA}} exchange-correlation functionals are evaluated with a density that is augmented or not.
Description: {{TAG|LNOAUGXC}} specifies if a [[meta-GGA|meta-GGA functional]] is evaluated with a density that is augmented or not.
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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\rho_{\sigma}\right\vert^{2}/\left(8\rho_{\sigma}\right)</math>. However, this may not be always the case in particular within the PAW spheres when the pseudo density is augmented with the compensation charge. If {{TAG|LNOAUGXC}}=.TRUE. in {{FILE|INCAR}}, then the pseudo density is not augmented, which should alleviate the breaking of the condition <math>\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}</math>.
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>.


Not having <math>\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}</math> satisfied can make the calculations unstable, in particular with the functionals of the TPSS family.
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|
See {{TAG|LTBOUNDLIBXC}} for a related tag.
*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.}}


== Related tags and articles ==
== Related tags and articles ==
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<references/>
<references/>


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<!--
[[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]]
-->

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:
  • This tag is available since VASP.6.5.0 and is a replacement of the compiler option -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 may lead to numerical problems.

Related tags and articles

METAGGA, LTBOUNDLIBXC

Examples that use this tag

References