LDAU: Difference between revisions
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== Example Calculations using this Tag == | == Example Calculations using this Tag == | ||
{{TAG|NiO LSDA+U}} | {{TAG|Constraining the local magnetic moments}}, {{TAG|Determining the Magnetic Anisotropy}}, {{TAG|Estimation of J magnetic coupling}}, {{TAG|Including the Spin-Orbit Coupling}}, {{TAG|NiO GGA+U}}, {{TAG|NiO LSDA+U}} | ||
---- | ---- | ||
[[The_VASP_Manual|Contents]] | [[The_VASP_Manual|Contents]] | ||
[[Category:INCAR]][[Category:LDA+U]] | [[Category:INCAR]][[Category:LDA+U]] |
Revision as of 10:05, 24 February 2017
LDAU = .TRUE. | .FALSE.
Default: LDAU = .FALSE.
Description: LDAU=.TRUE. switches on the L(S)DA+U.
Note on bandstructure calculation: The CHGCAR file contains only information up to angular momentum quantum number L=LMAXMIX for the on-site PAW occupancy matrices. When the CHGCAR file is read and kept fixed in the course of the calculations (ICHARG=11), the results will be necessarily not identical to a selfconsistent run. The deviations are often large for L(S)DA+U calculations. For the calculation of band structures within the L(S)DA+U approach, it is hence strictly required to increase LMAXMIX to 4 (d elements) and 6 (f elements).
Related Tags and Sections
LDAUTYPE, LDAUL, LDAUU, LDAUJ, LDAUPRINT, LMAXMIX
Example Calculations using this Tag
Constraining the local magnetic moments, Determining the Magnetic Anisotropy, Estimation of J magnetic coupling, Including the Spin-Orbit Coupling, NiO GGA+U, NiO LSDA+U