Abstract

Shaking optical lattices in a resonant manner offers an efficient and versatile method to devise artificial gauge fields and topological band structures for ultracold atomic gases. This was recently demonstrated through the experimental realization of the Harper–Hofstadter model, which combined optical superlattices and resonant time-modulations. Adding inter-particle interactions to these engineered band systems is expected to lead to strongly-correlated states with topological features, such as fractional Chern insulators. However, the interplay between interactions and external time-periodic drives typically triggers violent instabilities and uncontrollable heating, hence potentially ruling out the possibility of accessing such intriguing states of matter in experiments. In this work, we study the early-stage parametric instabilities that occur in systems of resonantly-driven Bose–Einstein condensates in optical lattices. We apply and extend an approach based on Bogoliubov theory (Lellouch et al 2017 Phys. Rev. X 7 021015) to a variety of resonantly-driven band models, from a simple shaken Wannier–Stark ladder to the more intriguing driven-induced Harper–Hofstadter model. In particular, we provide ab initio numerical and analytical predictions for the stability properties of these topical models. This work sheds light on general features that could guide current experiments to stable regimes of operation.

Highlights

  • Driving quantum systems periodically in time has been proposed as a versatile tool to generate unusual quantum phases of matter [1,2,3,4,5,6]

  • In the context of ultracold quantum gases, it was shown that subjecting neutral atoms to an external time-periodic drive could be used to design artificial gauge fields in these systems [6,7,8,9,10], opening promising perspectives in the quantum simulation of topological states of matter [11,12,13] and quantum magnetism [10, 14, 15]; see the recent work [16] on the control of magnetic correlations in driven cold gases

  • The absolute maximum is reached for q = 0 in the upper branch, which precisely corresponds to the most unstable mode identified in our numerics: to the previous model discussed in section 3, we find that the onset of parametric instability is governed by the mode of highest time-averaged Bogoliubov energy, which is consistent with the fact that this mode will be the first one to resonate [Eav (q = 0) = w] as one increases the interaction strength g [40]

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Summary

Introduction

Driving quantum systems periodically in time has been proposed as a versatile tool to generate unusual quantum phases of matter [1,2,3,4,5,6]. A interesting class of periodically-driven setups is that featuring resonant time-modulations [23,24,25,26,27,28], in which the driving frequency ω resonates with an energy separation Δ ≈ ÿω that is inherent to the underlying static system Such schemes can be exploited to finely control the tunneling matrix elements connecting neighboring sites of a lattice, and can be implemented by resonantly modulating a superlattice or a Wannier–Stark ladder; see [29, 30] for experimental realizations and [10] for a review.

General method
Linear stability analysis
A first example: the resonantly-shaken Wannier–Stark ladder
Numerical results
Moving lattices with a space-dependent phase: the 1D case
The model We consider a 1D model described by the Hamiltonian
The driven-induced Harper–Hofstadter model
Conclusion
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