impact on these surfaces can save a large part of initial energy in the pancake liquid film at maximum spread, [10][11][12] then go through a fast retraction [13][14] and bounce away from surfaces. This ability of repelling impacting droplets greatly shortens the contact time with surfaces [15][16][17][18] and allows droplets bounce away before freezing. [19][20] Since Mishchenko et al. first proposed to realize ice-free nanostructured surfaces by repelling impacting water droplets, [21] droplets impact and freezing on cold surfaces have been widely investigated. Compared with room temperature, the influence of supercooled surface on droplet impact mainly includes the droplet physical properties and droplet deposition behavior below bounce transition temperature. [22][23][24] Maitra et al. found that viscosity dissipation at low temperature reduces the droplet maximum spread, and the meniscus penetrates into surface texture results in a decrease of retraction velocity. [25] Zhang et al. suggested that it is the ice nucleation that causes droplet adhesion rather than viscosity, the contact of droplet with surface texture will result in a higher nucleation rate. [26] Kanta et al. developed total internal reflection technology and observed the solidification of droplets propagates continuously from the impact center to the edge of the liquid film on cold surfaces. [27] Zhu et al. summarized the four frozen droplet morphologies of different elliptical caps and rings on cold-inclined hydrophilic surfaces. [28] Although some progress has been achieved, the boundary between droplet bounce and deposition on superhydrophobic surface is not clear. Since nucleation in supercooled water droplets is a stochastic process and affected by temperature and local surface morphology, [29][30][31] single droplet behavior cannot get a stable result statistically.Moreover, most of the studies about droplet impact on cold surfaces are carried out under dry environment, [32][33] which are significantly different from freezing rain environment (0 to −5 °C, >50 RH%). Actually, the frosting and droplet impact freezing in freezing rain should not be studied separately. For example, condensation and desublimation from vapor changes the surface wettability and affects droplet impact dynamics, [34] while the freezing of supercooled droplets leads to the formation of ice bridge or frost halo and further promotes solidification propagating within the frost layer. [35][36] The lack of clear criterion for bionic superhydrophobic surface repelling impact Icephobic material is of great importance in power transportation, communication, aerospace, and so on. Bionic lotus superhydrophobic surfaces show good application prospects in anti-icing by repelling impacting droplets. However, the boundary (criterion) between droplet bounce and deposition on superhydrophobic surface under cold freezing rain is unclear. Here, from the view of statistics, the boundary and internal heat transfer mechanism of the droplet bounce, pinning, and three kinds of depositio...