Singular KAM theory for convex Hamiltonian systems

In this note, we briefly discuss how singular KAM Theory - which was worked out in a previous work by L.B. and L.C. for the mechanical case $\frac{1}{2}\mathrm{\mid }y{\mathrm{\mid }}^2+\epsilon f(x)$ - can be extended to convex real analytic nearly integrable Hamiltonian systems with Hamiltonian in action-angle variables given by $h(y)+\epsilon f(x)$ with $h$ convex and generic $f$.