London Dispersion Interactions Imitate Pressure for Molecular Crystals

The packing of molecular crystals, in which the constituent molecular units have no directional forces, is primarily controlled by weak London dispersion (LD) forces. These forces assist in stabilizing the system by bringing the molecular units into the proximity of each other. In this paper, the same effect is shown to be externally induced by pressure. The minimal pressure required to correctly describe the crystal structure without LD interactions (P_LD) provides a quantifiable measure for the weak intermolecular interactions. LD forces are shown to be essential for an accurate description of the pressure-induced phase transitions across examples of linear, trigonal-planar, square-planar, tetrahedral, trigonal bipyramidal, and octahedral molecules.