ter between the original CT 1 and the L excitons (see Fig. and Fig. for the transition dipole matrix for the lowest 20 electronic states). The electron distribution is moderately affected moving from completely right-localized to mostly leftlocalized with some non-zero right-arm character. Additionally, both the hole and electron NTOs are reduced in magnitude due to the non-zero mixture of the cavity photon, which is most prominent for the electron.