Slow relaxation and sensitivity to disorder in trapped lattice fermions after a quench
arXiv:1609.06640 · doi:10.1103/PhysRevA.94.063643
Abstract
We consider a system of non-interacting fermions in one dimension subject to a single-particle potential consisting of (a) a strong optical lattice, (b) a harmonic trap, and (c) uncorrelated on-site disorder. After a quench, in which the center of the harmonic trap is displaced, we study the occupation function of the fermions and the time-evolution of experimental observables. Specifically, we present numerical and analytical results for the post-quench occupation function of the fermions, and analyse the time-evolution of the real-space density profile. Unsurprisingly for a non-interacting (and therefore integrable) system, the infinite-time limit of the density profile is non-thermal. However, due to Bragg-localization of the higher-energy single-particle states, the approach to even this non-thermal state is extremely slow. We quantify this statement, and show that it implies a sensitivity to disorder parametrically stronger than that expected from Anderson localization.
15 pages, 11 figures
References in corpus (11)
- Thermalization and its mechanism for generic isolated quantum systems
- Many body localization and thermalization in quantum statistical mechanics
- Direct observation of Anderson localization of matter-waves in a controlled disorder
- Phenomenology of fully many-body-localized systems
- Many-body localization in periodically driven systems
- Anomalous diffusion and Griffiths effects near the many-body localization transition
- Generalized Thermalization in an Integrable Lattice System
- Correlations after quantum quenches in the XXZ spin chain: Failure of the Generalized Gibbs Ensemble
- Strongly interacting bosons in a disordered optical lattice
- Generalized Gibbs Ensembles for Quantum Field Theories
- Single-atom density of states of an optical lattice