Category:DFT+U: Difference between revisions

The LDA and semilocal GGA functionals often fail to describe systems with localized (strongly correlated) ${\displaystyle d}$ or ${\displaystyle f}$ electrons (this manifests itself primarily in the form of unrealistic one-electron energies or too small magnetic moments in the case of systems with ${\displaystyle d}$ electrons). In some cases this can be remedied by introducing on the ${\displaystyle d}$ or ${\displaystyle f}$ atom a strong intra-atomic interaction in a simplified (screened) Hartree-Fock like manner (${\displaystyle E_{\text{HF}}(\hat{n})}$), as an on-site replacement of the semilocal functional (double-counting term ${\displaystyle E_{\text{dc}}(\hat{n})}$):

${\displaystyle E_{\text{xc}}^{\text{LDA/GGA}+U}(n,\hat{n}) = E_{\text{xc}}^{\text{LDA/GGA}}(n) + E_{\text{HF}}(\hat{n}) - E_{\text{dc}}(\hat{n})}$

where ${\displaystyle \hat{n}}$ is the on-site occupancy matrix of the ${\displaystyle d}$ or ${\displaystyle f}$ electrons. This approach is known as the DFT+U method (traditionally called LSDA+U^[1] ).

The first VASP DFT+U calculations, including some additional technical details on the VASP implementation, can be found in Ref. ^[2] (the original implementation was done by Olivier Bengone ^[3] and Georg Kresse).

More detail about the formalism of the DFT+U method can be found here.

How to

DFT+U can be switched on with the LDAU tag in the INCAR file, while the LDAUTYPE tag determines the DFT+U flavor that is used. The effective on-site Coulomb and exchange interactions (in eV) are set with the LDAUU and LDAUJ tags, respectively.

References