Figures and) show that the effective diffusivities of emulsions produced in the aqueous phase exhibit a wide range of 𝐷/𝐷 𝑒 values that, in general, increase with 𝜎 𝐴 2 . Had the diffusion of droplets been governed entirely by usual thermal noise, 𝐷/𝐷 𝑒 would be close to unity. There are only few cases, which present this type of value [Table ], for which 𝜎 𝐴 2 values were undetectably small that they could not be potted along with the other data in Figure . However, in most cases 𝐷 is several orders of magnitude higher then 𝐷 𝑒 . The fact that 𝐷≫𝐷 𝑒 indicates that the droplets acquire certain amount of additional kinetic energy as soon as they were formed in the aqueous phase below the interface. We conjectured such a possibility previously; however, the current studies clearly suggest that such a fast diffusion could be controlled by the non-thermal fluctuations that result from the explosive events reported in Figure and).