Re-localization due to finite response times in a nonlinear Anderson chain
arXiv:1112.3838 · doi:10.1140/epjb/e2012-21040-5
Abstract
We study a disordered nonlinear Schrödinger equation with an additional relaxation process having a finite response time . Without the relaxation term, , 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 , spreading is suppressed and any initially localized excitation will remain localized. Here, we explain the lack of subdiffusive spreading for 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 (7)
- Destruction of Anderson localization by a weak nonlinearity
- Universal spreading of wavepackets in disordered nonlinear systems
- Absence of Wavepacket Diffusion in Disordered Nonlinear Systems
- Odeint - Solving ordinary differential equations in C++
- 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