Codina Cotar (University College of London)

It is a famous result of statistical mechanics that, at low enough temperature, the random field Ising model is disorder relevant for d<=2, i.e. the phase transition between uniqueness/non-uniqueness of Gibbs measures disappears,  and disorder irrelevant otherwise (Aizenman-Wehr 1990). Generally speaking, adding disorder to a model tends to destroy the non-uniqueness of Gibbs measures.

In this talk we consider – in non-convex potential regime – a random gradient