We develop a quenched thermodynamic formalism for a wide class of random maps with non-uniform expansion, where no Markov structure, no uniformly bounded degree or the existence of some expanding dynamics is required. We prove that every measurable and fibered C 1 -potential at high temperature admits a unique equilibrium state which satisfies a weak Gibbs property, and has exponential decay of correlations. The arguments combine a functional analytic approach for the decay of correlations (using Birkhoff cone methods) and Carathéodory-type structures to decribe the relative pressure of not necessary compact invariant sets in random dynamical systems. We establish also a variational principle for the relative pressure of random dynamical systems.
Contents7. Hyperbolic potentials and high temperature 27 7.1. Hyperbolic potentials 27 7.2. Entropy of the set of points with no expansion 27 7.3. Proof of Theorem D 30 8. Existence and uniqueness of equilibrium states for hyperbolic potentials 30 9.