“…The appearance and/or the destruction of Anderson localization in linear and nonlinear disordered systems, as well as the properties of energy propagation in such models, have attracted extensive attention in theory, numerical simulations and experiments, especially in recent years . a e-mail: snybob001@myuct.ac.za b e-mail: haris.skokos@uct.ac.za Studies of disordered versions of two basic, nonlinear Hamiltonian lattice models, namely the Klein-Gordon (KG) oscillator lattice and the discrete nonlinear Schrödinger equation (DNLS), revealed the existence of various dynamical behaviors, the so-called 'weak' and 'strong chaos' spreading regimes, as well as the 'selftrapping' regime and determined the statistical characteristics of energy propagation and chaos in these systems [12,13,15,33,[17][18][19]23,24,26,30,32]. One basic outcome of these studies is that energy propagation in disordered lattices is a chaotic process which, in general, results in the destruction of Anderson localization.…”