Abstract

We consider the evolution of an initially localized wave packet after a sudden change in the Hamiltonian, i.e. a quench. When both bound and scattering eigenstates exist in the post-quench Hamiltonian, one might expect partial delocalization of the wave packet to ensue. Here we show that if the quench consists of a sudden switching-off of short-range inter-particle interactions, then Tanʼs universal relations guarantee delocalization through the high-momentum tail of the momentum distribution. Furthermore, we consider the influence of the range of the interaction and show how a finite range alters the coupling to highly excited states. We illustrate our results using numerical simulations of externally trapped particles in one dimension. If the external potential is both disordered and correlated, then the interaction quench leads to transport via delocalized states, showing that localization in disordered systems is sensitive to non-adiabatic changes in the interactions between particles.

Highlights

  • We show that as long as some scattering states exist and the interparticle interactions have zero range, the quench leads to partial delocalization, and we characterize this delocalization quantitatively for certain specific systems

  • We show how the range of the interactions influences the coupling to highly excited states, as expected from the high-momentum tail of the momentum distribution (1)

  • An interaction quench leads to transport through delocalized states in disordered systems, provided they exist

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Summary

13 January 2015

Received 9 October 2014, revised 27 October 2014 Accepted for publication 30 October 2014 Published 24 November 2014 New Journal of Physics 16 (2014) 113051 doi:10.1088/1367-2630/16/11/113051

Introduction
Quench-induced delocalization
Methods
Finite well
The long-time limit
Pair correlations
Finite-range interactions
Anderson localization
Numerical results
Conclusions
Full Text
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