“…Luminescence of both free (F) and self-trapped (ST) excitons (henceforth they will be designated as dimeric excitons) have been observed in both α-pyrene and α-perylene crystals at low temperature (say, below 50 K). − In these crystals at room temperature, delocalized free excitons generated by photoexcitation are rapidly relaxed into ST excitons because of strong exciton–phonon interaction. ,− ST excitons are considered as excimers, which emit spectrally red-shifted, broadened excimer luminescence, which is a forbidden transition. − A two-step excimer formation mechanism has been proposed from the results of temperature-dependent fluorescence studies as well as ultrafast dynamics studies. ,,− However, only a few of these studies reported migration dynamics of excitons in these crystals, probably because of rapid relaxation of free excitons into excimers (within a few ps), which prevents excitons from being propagated even over a few nanometers. ,,,, In contrast to the concept that molecular excimers are trapped states and hence should be immobile, Pensack et al revealed that the excimer was diffusive and considered as a singlet exciton. ,,− However, it is now well understood that diffusivity of the dimeric excitons is much slower than that of the monomeric excitons because the resonance energy transfer process involving ST excitons must be accompanied by intermolecular structural changes that can cause the diffusion process to be thermally activated. ,,,, On the other hand, the monomeric excitons populated in the β-form of the crystals have larger mobility. ,, …”