DFT-D3

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

$E_{\mathrm{disp}} = -\frac{1}{2} \sum_{i=1}^{N_{at}} \sum_{j=1}^{N_{at}} \sum_{\mathbf{L}}{}^\prime \left ( f_{d,6}(r_{ij,L})\,\frac{C_{6ij}}{r_{ij,{L}}^6} +f_{d,8}(r_{ij,L})\,\frac{C_{8ij}}{r_{ij,L}^8} \right ).$

Unlike in the method DFT-D2, the dispersion coefficients $C_{6ij}$ are geometry-dependent as they are adjusted on the basis of the local geometry (coordination number) around atoms $i$ and $j$. In the zero-damping variant of the DFT-D3 method (DFT-D3(zero)), the damping function reads:

$f_{d,n}(r_{ij}) = \frac{s_n}{1+6(r_{ij}/(s_{R,n}R_{0ij}))^{-\alpha_{n}}}$

where $R_{0ij} = \sqrt{\frac{C_{8ij}}{C_{6ij}}}$, the parameters $\alpha_6$, $\alpha_8$, $s_{R,8}$ and $s_{6}$ are fixed at values of 14, 16, 1, and 1, respectively, while $s_{8}$ and $s_{R,6}$ 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 values):

• VDW_RADIUS=50.2 : cutoff radius (in $\AA$) for pair interactions considered in the equation of $E_{\mathrm{disp}}$
• VDW_CNRADIUS=20.0 : cutoff radius (in $\AA$) for the calculation of the coordination numbers
• VDW_S8=[real] : damping function parameter $s_8$
• VDW_SR=[real] : damping function parameter $s_{R,6}$

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

$f_{d,n}(r_{ij}) = \frac{s_n\,r_{ij}^n}{r_{ij}^n + (a_1\,R_{0ij}+a_2)^n}$

with $s_6=1$ and $a_1$, $a_2$, and $s_8$ 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:

• VDW_S8=[real]
• VDW_A1=[real]
• VDW_A2=[real]

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Mind: 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 . When using DFT-D3(BJ) references and should also be cited.

Related tags and articles

IVDW, IALGO, DFT-D2, Tkatchenko-Scheffler method, Tkatchenko-Scheffler method with iterative Hirshfeld partitioning, Self-consistent screening in Tkatchenko-Scheffler method, Many-body dispersion energy, dDsC dispersion correction

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