To calculate the total absorption spectrum for the full ensemble it would be straightforward to sum over the individual spectra of each member of the ensemble. Similarly, the densities of states (DOS) and densities of charge transfer (CT) character can be easily accessed. However, for a more detailed analysis it is of interest to deconvolve the properties of the average spectrum into the contributions of the individual electronic states. Examining the characters and contributions of individual states in each member of an ensemble is not straightforward because the electronic structure at each distorted geometry will differ. This is caused by a reordering of the excited electronic states or by a mixing of their characters. In other words, the electronic states of the distorted geometries are not going to be in 1:1 correspondence with the states at the optimized geometry. The physical origins of reordering and mixing of the excited states can be traced to the presence of conical intersections and the Herzberg-Teller effect, respectively.