Fig. 4: Emergence of an optimal scale to observe temperature chaos.
From: Temperature chaos is present in off-equilibrium spin-glass dynamics
The difference 1 − X(F, T1, T2, ξ, r) [recall that X(F, T1, T2, ξ, r) is the inverse of the distribution function] as a function of the cubic root \({N}_{r}^{1/3}\) of the number of spins in the spheres, as computed for different values of the probability level F, the temperatures T1 and T2, and the coherence length ξ. In this representation, the optimal size of the spheres for the observation of chaos (for given parameters F, T1, T2 and ξ) appears as the maximum of the curves. Continuous lines are fits to a smooth interpolating function, further details can be found in Supplementary Note 2. Error bars represent one standard deviation.
