“…where λ is the wavelength in air, n is the average cholesteric refractive index and θ is the incidence angle to m. Cholesteric Bragg reflection can be seen in the strikingly coloured and circularly polarised reflections from cuticles of certain beetles 3,4 , and even from some fruits 5,6 , revealing their helical arrangement of fibres of chitin and cellulose, respectively. In fact, cholesteric helical self-assembly can be found across a large range of biomaterials 7 , providing advantages beyond optics for, e.g., optimised packing of DNA/RNA [8][9][10] and spectacular mechanical properties of composites built around collagen 11,12 , amyloid 13 , chitin 14,15 or cellulose 16,17 . Attempts to mimic this structuring via self-assembly in cholesteric colloidal nanorod suspensions, for instance by drying cholesteric suspensions of cellulose nanocrystals (CNCs) 18 , often yield non-uniform films reflecting a range of colours with imperfect circular polarisation, and reproducibility and tunability are challenging 1,[19][20][21][22][23][24] .…”