Figure 3
From: Interference between the glass, gel, and gas-liquid transitions
(a) Numerical results for the inverse localization length λ−1(Tf) (empty circles) and the inverse latency distance dl−1(Tf) (solid circles) as a function of Tf, along the isochore ϕ = 0.2. As discussed in ref.20, the crossover from exponential to power-law divergence of λ−1(Tf) occurs at T0(ϕ) (vertical solid line). As explained in the SM, the same procedure can be applied to dl−1(Tf), yielding ν = 1.25, and an alternative determination of T0(ϕ). (b) Crossover temperature T0(ϕ) obtained from λ(Tf) (empty circles) and from dl(Tf) (solid circles), represented on the non-Equilibrium phase diagram of Fig. 1(a). Regions I, II, and III correspond, respectively, to full gas-liquid phase separation, to gel formation, and to the formation of porous glasses.
