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The Journal of Chemical Physics· 2019Q1

A generally applicable atomic-charge dependent London dispersion correction

Eike Caldeweyher, Sebastian Ehlert, Andreas Hansen, Hagen Neugebauer et al.

Short summary

The new D4 model improves London dispersion calculations in density functional theory (DFT) by scaling atomic polarizabilities based on partial charges, achieving a 3.8% mean relative deviation for molecular dispersion coefficients, outperforming the previous D3 model (4.7%).

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Key points

  • The D4 model introduces charge-dependent scaling of atomic polarizabilities for London dispersion calculations in DFT.
  • It achieves a 3.8% mean relative deviation for molecular dipole-dipole dispersion coefficients, surpassing the D3 model's 4.7%.
  • Efficient analytical derivatives for classical charges and numerical Casimir-Polder integration are used.
  • The model covers elements up to radon (Z=86) and includes dipole-dipole and dipole-quadrupole interactions, plus three-body effects.

AI-generated from the title and abstract; the full text is not read.

Abstract

The so-called D4 model is presented for the accurate computation of London dispersion interactions in density functional theory approximations (DFT-D4) and generally for atomistic modeling methods. In this successor to the DFT-D3 model, the atomic coordination-dependent dipole polarizabilities are scaled based on atomic partial charges which can be taken from various sources. For this purpose, a new charge-dependent parameter-economic scaling function is designed. Classical charges are obtained from an atomic electronegativity equilibration procedure for which efficient analytical derivatives with respect to nuclear positions are developed. A numerical Casimir-Polder integration of the atom-in-molecule dynamic polarizabilities then yields charge- and geometry-dependent dipole-dipole dispersion coefficients. Similar to the D3 model, the dynamic polarizabilities are precomputed by time-dependent DFT and all elements up to radon (Z = 86) are covered. The two-body dispersion energy expression has the usual sum-over-atom-pairs form and includes dipole-dipole as well as dipole-quadrupole interactions. For a benchmark set of 1225 molecular dipole-dipole dispersion coefficients, the D4 model achieves an unprecedented accuracy with a mean relative deviation of 3.8% compared to 4.7% for D3. In addition to the two-body part, three-body effects are described by an Axilrod-Teller-Muto term. A common many-body dispersion expansion was extensively tested, and an energy correction based on D4 polarizabilities is found to be advantageous for larger systems. Becke-Johnson-type damping parameters for DFT-D4 are determined for more than 60 common density functionals. For various standard energy benchmark sets, DFT-D4 slightly but consistently outperforms DFT-D3. Especially for metal containing systems, the introduced charge dependence of the dispersion coefficients improves thermochemical properties. We suggest (DFT-)D4 as a physically improved and more sophisticated dispersion model in place of DFT-D3 for DFT calculations as well as other low-cost approaches like semi-empirical models.

The authors' abstract, as published at the source. The Journal of Chemical Physics, 2019 · DOI ↗

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Field: Inorganic Chemistry

Inorganic ChemistryChemistry