DFT-D2: Difference between revisions

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{{TAG|Many-body dispersion energy}},
{{TAG|Many-body dispersion energy}},
{{TAG|dDsC dispersion correction}}
{{TAG|dDsC dispersion correction}}


== References ==
== References ==

Revision as of 12:59, 19 July 2022

In the DFT-D2 method of Grimme[1], the correction term takes the form:

where the first two summations are over all atoms in the unit cell and the third summation is over all translations of the unit cell where the prime indicates that for . denotes the dispersion coefficient for the atom pair , is the distance between atom located in the reference cell and atom in the cell and the term is a damping function whose role is to scale the force field such as to minimize the contributions from interactions within typical bonding distances. In practice, the terms in the equation for corresponding to interactions over distances longer than a certain suitably chosen cutoff radius (VDW_RADIUS, see below) contribute only negligibly to and can be ignored. Parameters and are computed using the following combination rules:

and

The values for and are tabulated for each element and are insensitive to the particular chemical situation (for instance, for carbon in methane takes exactly the same value as that for C in benzene within this approximation). In the DFT-D2 method, a Fermi-type damping function is used:

whereby the global scaling parameter has been optimized for several different DFT functionals such as PBE (), BLYP () or B3LYP (). The parameter is usually fixed at 1.00. The DFT-D2 method can be activated by setting IVDW=1|10 or by specifying LVDW=.TRUE. (this parameter is obsolete as of VASP.5.3.3). Optionally, the damping function and the vdW parameters can be controlled using the following flags (the default values are listed):

  • VDW_RADIUS=50.0 : cutoff radius (in ) for pair interactions
  • VDW_S6=0.75 : global scaling factor (available in VASP.5.3.4 and later)
  • VDW_SR=1.00 : scaling factor (available in VASP.5.3.4 and later)
  • VDW_SCALING=0.75 : the same as VDW_S6 (obsolete as of VASP.5.3.4)
  • VDW_D=20.0 : damping parameter
  • VDW_C6=[real array] : parameters () for each species defined in the POSCAR file
  • VDW_R0=[real array] : parameters () for each species defined in the POSCAR file
  • LVDW_EWALD=.FALSE. : decides whether the lattice summation in expression by means of Ewald's summation is computed (available in VASP.5.3.4 and later)

The performance of PBE-D2 method in optimization of various crystalline systems has been tested systematically in reference [2].


Important: It is recommended to use the more advanced and more accurate method DFT-D3.[3]


Mind: The defaults for VDW_C6 and VDW_R0 are defined only for elements in the first five rows of the periodic table (i.e. H-Xe). If the system contains other elements the user has to define these parameters in INCAR.
Mind: The defaults for parameters controlling the damping function (VDW_S6, VDW_SR, VDW_D) are available only for the PBE functional. If a functional other than PBE is used in a DFT-D2 calculation, the value of VDW_S6 (or VDW_SCALING in versions before VASP.5.3.4) has to be defined in INCAR.
Mind: As of VASP.5.3.4, the default value for VDW_RADIUS has been increased from 30 to 50 .
Mind: Ewald's summation in the calculation of calculation (controlled via LVDW_EWALD) is implemented according to reference [4] and is available as of VASP.5.3.4.

Related tags and articles

IVDW, DFT-D3, Tkatchenko-Scheffler method, Tkatchenko-Scheffler method with iterative Hirshfeld partitioning, Self-consistent screening in Tkatchenko-Scheffler method, Many-body dispersion energy, dDsC dispersion correction

References