“…The similarity between second-order Hamiltonian systems and the corresponding first-order gradient flows is wellknown in mechanical control systems [19], in dynamic optimization [20], [21], [22], and also in transient stability studies [23], [24], [25], but we are not aware of any result as general as Theorem III.1. In [23], [24], [25], statements 1) and 2) are proved under the more stringent assumptions that H λ has a finite number of isolated and hyperbolic equilibria.…”