The analysis of the TDM also yields a consistent picture. The lowest excited BSE@GW states have a dominant MLCT character. In contrast, the TDDFT results come with a stronger mixing. While TDDFT predicts numerous high-lying LLCT states, BSE@GW does not support this finding. For the triplet states, we observe that BSE@GW predicts a stabilizing effect for the MLCT states. It estimates that the low-lying MC states no longer form a continuous block, but MLCT states are found in between. One could conclude that this would eventually lead to longer MLCT lifetimes. Remarkably, our TDDFT computation does not show similar characteristics, which matches our previous findings of a better description of the excited states by BSE@GW over TDDFT. Given that this system contains twice the number of NHC units compared to 4 and further destabilizes the MC states beyond what is observed in 4, these findings regarding the BSE@GW electronic structure are also consistent with experimental observations. 60