Dispersion interactions are among the most significant non-covalent forces in chemistry and play an important role in the stability and behavior of a wide range of chemical systems. Although individually weak, these interactions are inherently additive and become increasingly important as the molecular size grows. This makes them essential for example in stabilizing van der Waals complexes, 2 forming molecular crystals and determining structure of large biomolecules. To accurately model dispersion interactions, Kohn-Sham density functional theory (DFT) with dispersion corrections has become an essential tool. While wave function based methods beyond Hartree-Fock can capture these long-range interactions via an ab initio treatment, they are usually computationally more expensive than the DFT approach. The critical drawback of DFT is that semilocal density functionals struggle with dispersion interactions due to their long-range nature, necessitating the development of dispersion corrections. Notable among these are Grimme's dispersion correction series (DFT-D2, -D3, and -D4 ), the Tkatchenko-Scheffler (TS) method, many-body dispersion (MBD) approaches and the exchange-hole dipole (XDM) method by Becke and Johnson. Additionally, explicitly non-local density functional approximations such as vdW-DF, vdW-DF2, VV9, and VV10 have gained popularity not only in molecular computational chemistry but also in the solid-state and condensed matter community.