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LVTOT-tag, and core level shifts

LVTOT = .TRUE. | .FALSE.

Default    
LVTOT = .FALSE.


This tag determines whether the total local potential (file LOCPOT ) is written. Note that in VASP.5.2.12, the default is to write the entire local potential, including the exchange correlation potential (see also Sec. 6.54, if LVHAR=.TRUE. only the ionic and Hartree potential are written to the file, recovering the behaviour of older VASP versions).

VASP also calculates the average electrostatic potential at each ion. This is done, by placing a test charge with the norm 1, at each ion and calculating

$\displaystyle \bar V_n = \int V({\bf r}) \rho_{\rm test} (\vert{\bf r}- {\bf R_n}\vert) d^3 {\bf r}
$

The spatial extend of the test charge is determined by ENAUG (see Sec. 6.10), so that calculations can be compared only if ENAUG is kept fixed. The change of the core level shift $ \Delta c$ between to models can be calculated by the simple formula

$\displaystyle \Delta c= \bar V^1_n - \epsilon_{\rm Fermi}^1 - ( \bar V^2_n - \epsilon_{\rm Fermi}^2 ),
$

where $ V^1_n$ and $ V^2_n$ are the electrostatic potentials at the core of an ion for the first and second calculations, respectively, and $ \epsilon_{\rm Fermi}^1$ and $ \epsilon_{\rm Fermi}^2$ are the Fermi levels in these calculations. Clearly, the core level shift is the same for all core electrons in this simple approximation. In addition, screening effects are not taken into account.


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Next: LVHAR-tag Up: The INCAR File Previous: LWAVE-tag, LCHARG-tag   Contents   Index
N.B. Requests for support are to be addressed to: vasp.materialphysik@univie.ac.at