On the free energy of vector spin glasses with non-convex interactions
Hong-Bin Chen, Jean-Christophe Mourrat
TL;DR
This work extends the rigorous understanding of mean-field vector spin glasses to non-convex interactions by linking the limit free energy to a Hamilton–Jacobi functional. Assuming the limit exists, the authors prove that the limit value is realized as a critical value of an explicit Parisi-type functional, with the associated overlap law corresponding to a critical point. They develop a robust framework based on continuous Poisson–Dirichlet cascades, cavity methods, and Ghirlanda–Guerra identities to analyze the overlap structure and to connect the limit to a Hamilton–Jacobi equation, recovering the replica-method intuition in a rigorous setting. The results provide a principled variational and dynamic description of non-convex vector spin glasses, highlighting the role of characteristic lines in the solution structure and offering a pathway toward a full characterization of the limit free energy beyond convex settings.
Abstract
The limit free energy of spin-glass models with convex interactions can be represented as a variational problem involving an explicit functional. Models with non-convex interactions are much less well-understood, and simple variational formulas involving the same functional are known to be invalid in general. We show here that a slightly weaker property of the limit free energy does extend to non-convex models. Indeed, under the assumption that the limit free energy exists, we show that this limit can always be represented as a critical value of the said functional. Up to a small perturbation of the parameters defining the model, we also show that any subsequential limit of the law of the overlap matrix is a critical point of this functional. We believe that these results capture the fundamental conclusions of the non-rigorous replica method.
