“…Variation in the electronic couplings between different pairs of neighbor cores (i.e., in different directions) results in the anisotropy of charge mobility in many crystalline organic semiconductors. In cases where the experimental crystal structure is available, it can be used to extract the representative nearest-neighbor dimers, compute their electronic couplings and construct the angular resolution mobility anisotropy curve. − A more sophisticated alternative, often referred to as the multiscale approach, takes into account the entire crystal structure and involves computing electronic and local electron–phonon couplings, running molecular dynamics simulations to access the energetic, configurational and dynamic disorder, and finally performing the diffusive charge dynamics simulation to evaluate the bulk mobility. − In the absence of experimental crystal structures, which is often the case for newly designed systems, the morphology of ordered systems is often approximated by scanning various dimer geometries, generated either manually by systematically varying their structural parameters ,, or in an automatized manner using, for instance, random search algorithms, and constructing two-dimensional maps of their electronic couplings; for disordered systems, molecular dynamics (MD) simulations are often employed to probe the morphologies . However, neither of these methods affords insights beyond the dimer level.…”