LNOAUGXC

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

\tau_{\sigma}=\frac{1}{2}\sum_{i}\nabla\psi_{i\sigma}^{*}\cdot\nabla\psi_{i\sigma}

should, in principle, be larger than the von Weizsäcker kinetic-energy density^[1]

\tau_{\sigma}^{\textrm{W}}=\frac{\left\vert\nabla n_{\sigma}\right\vert^{2}}{8 n_{\sigma}}.

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 $\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}$ .

A violation of $\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}$ 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 $\tau_{\sigma}^{\textrm{W}}<\tau_{\sigma}$ may lead to numerical problems.

References

↑ S. Kurth, J. P. Perdew, and P. Blaha, Molecular and solid-state tests of density functional approximations: LSD, GGAs, and meta-GGAs, Int. J. Quantum Chem. 75, 889 (1999).

[kurth:ijqc:1999-1] S. Kurth, J. P. Perdew, and P. Blaha, Molecular and solid-state tests of density functional approximations: LSD, GGAs, and meta-GGAs, Int. J. Quantum Chem. 75, 889 (1999).

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References