In the DFT-D3 method of Grimme et al.[1], the following expression for the vdW-dispersion energy-correction term is used:

Unlike in the method DFT-D2, the dispersion coefficients
are geometry-dependent as they are adjusted on the basis of the local geometry (coordination number) around atoms
and
. In the zero-damping variant of the DFT-D3 method (DFT-D3(zero)), the damping function reads:

where
, the parameters
,
,
and
are fixed at values of 14, 16, 1, and 1, respectively, while
and
are adjustable parameters whose values depend on the choice of the exchange-correlation functional. The DFT-D3(zero) method is invoked by setting IVDW=11. Optionally, the following parameters can be user-defined (the given values are the default ones):
- VDW_RADIUS=50.2 : cutoff radius (in
) for pair interactions considered in the equation of 
- VDW_CNRADIUS=20.0 : cutoff radius (in
) for the calculation of the coordination numbers
- VDW_S8=[real] : damping function parameter

- VDW_SR=[real] : damping function parameter

Alternatively, the Becke-Johnson (BJ) damping can be used in the DFT-D3 method[2]:

with
and
,
, and
being adjustable parameters.
This variant of DFT-D3 method (DFT-D3(BJ)) is invoked by setting IVDW=12. As before, the parameters VDW_RADIUS and VDW_CNRADIUS can be used to change the default values for the cutoff radii. The parameters of the damping function can be controlled using the following tags:
Mind:
- The default values for the damping function parameters are available for several GGA (PBE, RPBE, revPBE and PBEsol), METAGGA (TPSS, M06L and SCAN) and hybrid (B3LYP and PBEh/PBE0) functionals, as well as Hartree-Fock. If another functional is used, the user has to define these parameters via the corresponding tags in the INCAR file. The up-to-date list of parametrized DFT functionals with recommended values of damping function parameters can be found on the webpage https://www.chemiebn.uni-bonn.de/pctc/mulliken-center/software/dft-d3/dft-d3.
- The DFT-D3 method has been implemented in VASP by Jonas Moellmann based on the dftd3 program written by Stefan Grimme, Stephan Ehrlich and Helge Krieg. If you make use of the DFT-D3 method, please cite reference [1]. When using DFT-D3(BJ) references [1] and [2] should also be cited.
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Related tags and articles
VDW_RADIUS,
VDW_CNRADIUS,
VDW_S8,
VDW_SR,
VDW_A1,
VDW_A2,
IVDW,
DFT-D2
References