“…The obtained morphologies are driven by (1) the entropy of mixing of the two blocks, described by the Flory-Huggins solution theory 15,16 , and (2) their corresponding volume fractions 17 , taking into account that, in presence of NPs, there is a significant decrease in the copolymers' conformational entropy coming from particle sequestration 10 . Although very promising in many situations, the diblock copolymer approach shows important limitations: (1) a constrained size ratio between the two blocks to access lamellar assemblies (generally comprised between 0.4 and 0.6 volume fraction with random coil polymers), (2) in presence of NPs, an imprecise control of their localization (as it is governed by entropy) and (3) in solution, a strong dependence to experimental conditions (concentration, temperature, presence of cosolvent, etc.) 10,15,16 .…”