using a new set of ideas that combines dynamical systems techniques with control theory and viscosity solutions methods. In (1), H(p, x) : R → R is a smooth Hamiltonian, strictly convex, i.e., D vvL(x, v) > γ > 0 uniformly (this is also called uniformly convex by some authors), and coercive in p (lim|p|→∞ H(p,x) |p| = ∞), and Z n periodic in x (H(p, x + k) = H(p, x) for k ∈ Z). Since R is the u...