In addition, we introduce highest (H), intermediate (H-1 and L+1), and lowest (L) monomers through sorting the FTDM diagonal, F H > F H-1 > F L+1 > F L , allowing one to judge on exciton localization on single geometry level (for excitons dominated by local excitations). We note that we calculate FTDM and derived quantities (IPR, LE, and CT) along surface hopping trajectories, i.e. these quantities depend on R(t). Finally, averaging over a swarm of trajectories (for a given system) is performed.