Re-localization due to finite response times in a nonlinear Anderson chain

Abstract

We study a disordered nonlinear Schrödinger equation with an additional relaxation process having a finite response time $\tau$. Without the relaxation term, $\tau =0$, this model has been widely studied in the past and numerical simulations showed subdiffusive spreading of initially localized excitations. However, recently Caetano et al.\ (EPJ. B \textbf{80}, 2011) found that by introducing a response time $\tau >0$, spreading is suppressed and any initially localized excitation will remain localized. Here, we explain the lack of subdiffusive spreading for $\tau >0$ by numerically analyzing the energy evolution. We find that in the presence of a relaxation process the energy drifts towards the band edge, which enforces the population of fewer and fewer localized modes and hence leads to re-localization. The explanation presented here is based on previous findings by the authors et al.\ (PRE \textbf{80}, 2009) on the energy dependence of thermalized states.

3 pages, 4 figures

References in corpus (9)

• Destruction of Anderson localization by a weak nonlinearity
• Universal spreading of wavepackets in disordered nonlinear systems
• Delocalization of a disordered bosonic system by repulsive interactions
• Absence of Wavepacket Diffusion in Disordered Nonlinear Systems
• Odeint - Solving ordinary differential equations in C++
• Weak chaos in the disordered nonlinear Schroedinger chain: destruction of Anderson localization by Arnold diffusion
• Strong and weak chaos in weakly nonintegrable many-body Hamiltonian systems
• Scaling of energy spreading in strongly nonlinear disordered lattices
• Spreading in Disordered Lattices with Different Nonlinearities