“…Despite the great success of the theory of Floer, the question remained how far the original approach by Rabinowitz, Conley, and Zehnder can be generalized to manifolds different from the torus. In [10] we started addressing this question by showing that, for a Hamiltonian H : T × T * M → R with quadratic growth at infinity, the Hamiltonian action A H : M 1−s → R, s ∈ (1/2, 1), (1.2) satisfies the Palais-Smale condition, M 1−s being the Hilbert bundle over the Hilbert manifold of loops H s (T, M ), s ∈ (1/2, 1), whose typical fibre is given by the space of H 1−s -sections of the pull-back bundle c * (T * M ), where c : T → M is any smooth loop. Roughly speaking, instead of considering loops with Sobolev regularity 1/2, one considers loops in T * M whose projection to the base has regularity larger than 1/2 (but strictly less than 1), thus making them continuous in the base direction, and whose projection to the fiber has regularity smaller than 1/2 (but strictly larger than L 2 -regularity) in such a way that the mean regularity is 1/2.…”