Periodically driven integrable systems with long-range pair potentials
arXiv:1709.08897 · doi:10.1088/1751-8121/aaced6
Abstract
We study periodically driven closed systems with a long-ranged Hamiltonian by considering a generalized Kitaev chain with pairing terms which decay with distance as a power law characterized by exponent . Starting from an initial unentangled state, we show that all local quantities relax to well-defined steady state values in the thermodynamic limit and after drive cycles for any and driving frequency . We introduce a distance measure, , that characterizes the approach of the reduced density matrix of a subsystem of sites to its final steady state. We chart out the dependence of and identify a critical value below which they generically decay to zero as . For , in contrast, for with at least one intermediate dynamical transition. We also study the mutual information propagation to understand the nature of the entanglement spreading in space with increasing for such systems. We point out existence of qualitatively new features in the space-time dependence of mutual information for , where is the largest critical frequency for the dynamical transition for a given . One such feature is the presence of {\it multiple} light cone-like structures which persists even when is large. We also show that the nature of space-time dependence of the mutual information of long-ranged Hamiltonians with differs qualitatively from their short-ranged counterparts with for any drive frequency and relate this difference to the behavior of the Floquet group velocity of such driven system.
v2; two-column format, 19 pages, 16 figures (Shortened abstract due to character limit for arXiv submission; see main text); slightly modified version submitted for review
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