“…enable fine-tuning of the optoelectronic properties both in solution and in the solid state. 90 -93 Bazan and colleagues have notably reported that the solid-state photoluminescence properties of a cationic CPE based on a poly((9,9dihexylfluorene)-alt-(4,7-(2 ′ ,1 ′ ,3 ′ -benzothiadiazole))) backbone (PFBT-X) (Scheme 4) can be manipulated by changing the size of the counterion: larger anions lead to increased interchain distance and thereby increased emission quantum yields. 94 The same authors also showed that replacing the bromide counterion with the larger tetrakis(1-imidazolyl)borate (BIm 4 − ) anion in a cationic narrow bandgap CPE (Scheme 4) derived from the poly((2,6-(4,4bis(2-ethylhexyl)cyclopenta-[2,1-b;3,4-b ′ ]-dithiophene))-alt-(4,7-(2 ′ ,1 ′ ,3 ′ -benzothiadiazole))) (PCPDTBT) framework (Scheme 3) not only modified the HOMO and LUMO energy levels, but also its semiconducting character (p-type for Br − and n-type for BIm 4 − ).…”