is a completely integrable system with phase space L2(S1). Although the
Hamiltonian ℋ(q) :=∫S1dx is defined only on the dense
subspace H1(S1), we prove that the frequencies ωj= can be defined on the
whole space L2(S1), where (Jj)j≥1 denote the action variables which are
globally defined on L2(S1). These frequencies are real analytic functionals
and can be used to analyze Bourgain’s weak solutions of KdV with initial
data in L2(S1). The same method can be used for any equation in the
KdV −hierarchy.