“…For a fixed number of colors q, in high enough dimensions (d ≥ Cq 10 log 2 q suffices), the situation is similar to that of 3-colorings in that the measures obtained from fixed-color boundary conditions are not translation-invariant, but they are invariant to parity-preserving automorphisms [26]. On the other hand, in any given dimension, when the number of colors is large (q > 4d suffices), there is a unique Gibbs measure, the finite-volume measures (with any boundary conditions) converge to this measure, and this measure is translation-invariant and satisfies strong spatial mixing (this all follows from Dobrushin's uniqueness condition; see, for example, [27]). Consequently, this measure is Bernoulli, and in fact, also a finitary factor of an i.i.d.…”