Abstract
Herein, Grimme's popular DFT-D3 approach for the treatment of London-dispersion interactions is reviewed. Based on a molecular geometry as the only input, DFT-D3 provides corrections to the molecular total energy, energy gradient and frequencies that are added to the results obtained with nearly any conventional density-functional theory approximation and also some other common mean-field approaches. The main advantage of DFT-D3 is its computational efficiency and robustness across the periodic table, which makes this approach particularly valuable for the treatment of large systems. DFT-D3 has been published in three variations, which are all discussed herein. Extensions that allow the treatment of three-body dispersion effects, as well as the treatment of periodic systems, are also reviewed. This chapter concludes with a brief overview of DFT-D3's performance for noncovalent interaction energies, thermochemistry and geometry optimizations. This overview may serve as a guideline for readers that intend to use DFT-D3 in the future.
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
More From: Non-covalent Interactions in Quantum Chemistry and Physics
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.