The Journal of Chemical Physics· 2019Q1
A generally applicable atomic-charge dependent London dispersion correction
- 1,829citations
- Q1SCImago
- 2019year
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