]/ns at 400 K (Figure ). The stretched exponent β decreased linearly from ∼ 1.25 at 298 K to ∼ 0.12 at 400 K. The relaxation times t 0 of the water nanodroplet increase with temperature, mainly due to the increase in instantaneous rates of droplet disintegration and formation relative to the droplet at 298 K. The average lifetime of the droplet, τ , obtained using equa-tion 1 decreases from around 1004.73 ns at 298 K to around 441.2 ns at 400 K (Figure B), using the first order decay formulation. Similarly, using the stretched exponential formulation (equation 2), τ ′ is obtained to be 837.84 ns at 298 K and 150.55 ns at 400 K, clearly demonstrating the effect of temperature on droplet disintegration, with higher temperatures leading to significantly shorter nonodroplet disintegration times (Figure . In future studies, we will investigate whether the relaxation of water nanodroplets under various physicochemical conditions follows a stretched exponential trend and assess the universality of this relaxation behavior.