“…In contrast, if the droplet is placed on a surface with a structured morphology in the Cassie–Baxter wetting regime, air will be trapped below the water droplet, thereby minimizing the contact area between the surfaces of the substrate and water droplet. The air trapped in the surface cavities is a poor thermal conductor and, together with the reduction of the contact area, will considerably hinder the heat transfer between the substrate and the liquid, significantly delaying the freezing time of the droplet. − The low hysteresis CA (7°) along the high CA (160°) displayed by the PFPE-modified rough aluminum reveals that the droplet on this surface is in the Cassie–Baxter wetting regime, preventing the water penetration between the surface topography features and trapped air pockets and delaying the frost formation process. Despite the heterogeneous ice nucleation theory, which establishes that a critical radius of ice nuclei smaller than the size of the surface features allows spontaneous ice growth, and an ice nucleus radius of 4.5 nm calculated at −10 °C, significantly smaller than the size of the surface features on the rough aluminum (see Figures , S2 and Table S1), the substantial increase in the freezing delay time observed on the PFPE-modified rough aluminum, is attributed to the surface topography and to the small solid–liquid contact area and air pockets entrapped on the hierarchical micro/nanostructure (hindering the heat transfer), providing a low rate for ice nucleation and growth as was previously described in refs and .…”