“…More precisely, the authors in [32][33][34] defined the so-called scattering map which accounts for the outer dynamics along homoclinic orbits, and overcame the large gap problem by incorporating in the transition chain new invariant objects, like secondary tori and the stable and unstable manifolds of lower dimensional tori; in [73], the author geometrically defined the so-called separatrix map near the NHIC, then he showed in [74] the existence of diffusion by making full use of the dynamics of this map, and even estimated the optimal diffusion speed of order ε/|log ε| (see also [8]). Moreover, for the case of a priori unstable Hamiltonians with higher degrees of freedom, similar results have also been obtained by variational or geometric methods in [3,25,36,37,46,59,75].…”