with liquid droplets. [15] However, because of liquid hydrodynamics, the contact time on an SHB surface is usually restricted by the theoretical limit of the inertia-capillary time scale. [16,17] With advances in micro/nanofabrication technology, the inertia-capillary limit is breakable; a contact time lower than this theoretical limit can be achieved on SHB surfaces through axial symmetry breaking, [18] asymmetric bouncing, [19] and pancake bouncing [20] at room temperature. Nevertheless, coating materials used to create an SHB surface may be damaged at high temperatures, [21] preventing the reduction of t c on SHB surfaces at high temperatures. Moreover, when the temperature is higher than the Leidenfrost point (LFP), a stable vapor cushion forms on SHB surfaces, insulating the liquid droplet and the solid surface. [22,23] Consequently, the t c reduction ability of SHB surfaces is lost in the Leidenfrost (LF) state. Furthermore, the vapor cushion inhibits heat and mass transfer between the solid surface and liquid droplet in the LF state and causes extensive thermal resistance that requires elaborate thermal management. [24][25][26] Generally, the LFP decreases with surface hydrophobicity. [27] Hence, SHB surfaces usually exhibit a very low LFP. [28] Although studies have achieved t c reduction at elevated temperatures on hydrophilic (HP) surfaces, [13,29,30] the range of such temperatures was limited to 200-400 °C because of the strong liquid-solid interaction on HP surfaces. [13,29,30] The strong liquid-solid interaction on HP surfaces at high temperatures also causes a fouling effect and may damage thermal devices. Therefore, a hydrophobic (HB) surface for minimizing liquid-solid interactions, suppressing the LF effect, and reducing t c at high temperatures is required. To realize such a surface, we developed a double-reentrant groove (DRG) array surface (hereafter referred to as DRG surface) with an overhanging structure composed of nanoscale vertical and horizontal overhangs situated on top of the microgrooves. This structure provided an upward surface tension force to prevent droplets from penetrating the microgrooves at room temperature. [5,31] The measured contact angle on the DRG surface was ≈141°. Despite its HB property, the DRG surface's specific topography could suppress the LF effect. The LFP of the DRG surface was 530 °C, which is the highest reported LFP for an HB surface. The smallest t c value of the surface, which was ≈13.3 ms, was obtained at 477 °C; this value is lower than the theoretical inertia-capillary limit of ≈15 ms. According to our review of the literature, the DRG surface is Reducing the contact time (t c ) of a droplet impacting a solid surface is crucial in various fields. Superhydrophobic (SHB) surfaces are used to reduce t c at room temperature. However, at high temperatures, SHB surfaces cannot achieve t c reduction because of the failure of the coating materials or the Leidenfrost (LF) effect. Therefore, a surface that can suppress the LF effect and reduce t c at high temper...