“…A remarkable feature of the random structure is that glass microscopically lacks the long-range order and is similar to liquid in terms of density–density correlations [ 1 , 2 , 3 , 4 , 5 , 6 ]. As a precursor to the random structure of glass, supercooled liquids show heterogeneity over space and time [ 1 , 2 , 3 , 4 , 5 , 6 , 7 , 8 , 9 , 10 , 11 ]. The dynamical heterogeneity and facilitation [ 4 , 7 , 8 , 9 , 10 , 11 , 12 , 13 , 14 ] emerges on approaching the dynamical transition temperature ( ), accompanied by the crossover from relaxational to activated dynamics.…”