LNOAUGXC: Difference between revisions
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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.}} | ||
Revision as of 16:16, 10 June 2024
LNOAUGXC = .TRUE. | .FALSE.
Default: LNOAUGXC = .FALSE.
Description: LNOAUGXC specifies if the METAGGA exchange-correlation functionals are 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: 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 leads to numerical problems. |
See LTBOUNDLIBXC for a related tag.
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