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 calculated on the basis of the local geometry (coordination number) around atoms
and
. Two variants of DFT-D3, that differ in the damping functions
, are available.
DFT-D3(zero)
In the zero-damping variant of DFT-D3,[1] invoked by setting IVDW=11, 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.
Optionally, the following parameters can be defined in the INCAR file (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

DFT-D3(BJ)
In the Becke-Johnson (BJ) damping variant of DFT-D3,[2], invoked by setting IVDW=12, the damping function is given by

with
and
,
, and
being adjustable parameters. As before, the parameters VDW_RADIUS and VDW_CNRADIUS can be used to change the default values for the cutoff radii.
Optionally, the parameters of the damping function can be controlled using the following INCAR 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.chemie.uni-bonn.de/grimme/de/software/dft-d3/ and follow the link "List of parametrized functionals".
- 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. Also carefully check the more extensive list of references found on https://www.chemie.uni-bonn.de/grimme/de/software/dft-d3/.
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Related tags and articles
VDW_RADIUS,
VDW_CNRADIUS,
VDW_S8,
VDW_SR,
VDW_A1,
VDW_A2,
IVDW,
DFT-D2,
DFT-ulg,
DFT-D4
References