Given the morphological disorder of the HH-TT system, it is more appropriate to describe the charge transport herein either with a hopping model assuming the charges to be localized on discrete sites or by trapping and releasing from localized states into higher energy mobile states. It should be noted that the models mentioned above still rely heavily on assumptions limiting their applicability, especially when it comes to intermediate cases of charge transport, which do not adhere to the limiting regimes. The development of new methods that bridge the gap between these regimes to advance the understanding of charge transport in organic semiconducting materials is an ongoing field.