achieving high performance dry adhesion compared to ordinary cylindrical micropillars or those having other shapes of contact elements. [11][12][13][14][15] The physical mechanism underlying the superior adhesion demonstrated by the mushroomshaped micropillars has been interpreted from different perspectives, e.g., increased contact area due to the protruding portion of the tip, [16,17] the structure compliance and effective material property, [18] the strong adaptability for cracks near the tip edge, [19] the energy release condition, [20,21] the vacuum suction effect, [6,9,22] the interfacial contact state, [23,24] and stress distributions, [25] as well as their corresponding detachment behaviors. [26,27] These potential mechanisms could give us better insight into the mushroom-shaped dry adhesives and why they make the dry adhesion technique so valuable for application in technology and our daily life. However, the friction contribution is seldom discussed.As has been widely investigated in biological [28][29][30][31] and artificial [32][33][34] adhesive systems that usually feature asymmetrical tips (e.g., spatulae) and slant fibers, friction force has been demonstrated to be much higher than the adhesive force in some special circumstances. For example, Autumn et al. [28] measured the maximum friction force of a single seta from the feet of a gecko to be about 200 µN, as much as ten times the adhesive force of about 20 µN. Tian et al. [29] also demonstrated that the friction force plays an equally important role in gecko motions associated with frequent attachment and detachment behaviors. However, the friction contribution to normal adhesive properties of artificial surfaces with vertical and symmetric structures, especially the mushroom-shaped micropillars, is often overlooked. This is because the classic detachment mode of direct separation is less likely to cause any slippage or slippage trend that is essential for the generation of friction force. This is potentially not true for mushroom-shaped micropillars, especially for those of optimal size, since the detachment process, as presented theoretically modeled by Carbone et al. [25] and further demonstrated experimentally by Heepe et al. [26] through a direct observation of the interface behavior, is by the crack nucleation somewhere in the middle of the contact region, followed by propagation until complete separation. One of the very significant findings of these works is clearly breaking the ultrafast interface variation down to three coherent phases, in which the pull-off force reaches its maximum value as the crack Bioinspired mushroom-shaped micropillar recently has attracted considerable interest from researchers on adhesion-functionalized artificial surface due to its prominent dry adhesive property. Understanding the interface behavior and further exploring the physical mechanism are of significance for properly designing the structure dimension with enhanced performance. However, the friction contribution to such type of adhesive structures is...