LNOAUGXC: Difference between revisions
No edit summary |
No edit summary |
||
Line 7: | Line 7: | ||
Not having <math>\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}</math> satisfied can make the calculations unstable, in particular with TPSS family of functionals. | Not having <math>\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}</math> satisfied can make the calculations unstable, in particular with TPSS family of functionals. | ||
{{NB|mind|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> leads to numerical problems.}} | {{NB|mind| | ||
*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> leads to numerical problems. | |||
*fefefe}} | |||
See {{TAG|LTBOUNDLIBXC}} for a related tag. | See {{TAG|LTBOUNDLIBXC}} for a related tag. |
Revision as of 06:58, 11 June 2024
LNOAUGXC = .TRUE. | .FALSE.
Default: LNOAUGXC = .FALSE.
Description: LNOAUGXC specifies if a METAGGA exchange-correlation 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 be always the case, in particular within the PAW spheres when the pseudo density is augmented with the compensation charge. If LNOAUGXC=.TRUE. in INCAR, then the pseudo density is not augmented, which should alleviate the breaking of the condition .
Not having satisfied can make the calculations unstable, in particular with TPSS family of functionals.
Mind:
|
See LTBOUNDLIBXC for a related tag.
Related tags and articles
References