“… [6, 7] This limitation can be commonly overcome in two different ways: i) introducing sterically bulky substituents in the molecular design, typically at the chromophore's core, [8, 9–11] or ii) including chromophores with various freely‐rotating groups that undergo restriction in intramolecular rotation (RIR) upon aggregation (Scheme 1). [12, 13] While the former strategy often induces a J‐type aggregation process with red‐shifted absorption and emission, [11, 14, 15] the latter approach leads to a turn‐on or a dramatic amplification of the emission compared to the monomer species via aggregation‐induced emission (AIE) [12, 16] . Thus, self‐assembly of π‐conjugated building blocks generally results in significant changes in the original photophysical properties of the system.…”