Abstract

We develop and utilize the SU(3) truncated Wigner approximation (TWA) in order to analyze far-from-equilibrium quantum dynamics of strongly interacting Bose gases in an optical lattice. Specifically, we explicitly represent the corresponding Bose-Hubbard model at an arbitrary filling factor with restricted local Hilbert spaces in terms of SU(3) matrices. Moreover, we introduce a discrete Wigner sampling technique for the SU(3) TWA and examine its performance as well as that of the SU(3) TWA with the Gaussian approximation for the continuous Wigner function. We directly compare outputs of these two approaches with exact computations regarding dynamics of the Bose-Hubbard model at unit filling with a small size and that of a fully connected spin-1 model with a large size. We show that both approaches can quantitatively capture quantum dynamics on a timescale of $\ensuremath{\hbar}/(Jz)$, where $J$ and $z$ denote the hopping energy and the coordination number. We apply the two kinds of SU(3) TWA to dynamical spreading of a two-point correlation function of the Bose-Hubbard model on a square lattice with a large system size, which has been measured in recent experiments. Noticeable deviations between the theories and experiments indicate that proper inclusion of effects of the spatial inhomogeneity, which is not straightforward in our formulation of the SU(3) TWA, may be necessary.

Highlights

  • Quantum simulators built with synthetic quantum platforms that are highly controllable have been applied for studying quantum many-body physics in and out of equilibrium

  • We demonstrated that the SU(3)discrete TWA (DTWA) is nearly as accurate as the Gaussian SU(3)truncated Wigner approximation (TWA) in simulating time evolution after sudden quantum quenches

  • V), we have applied the SU(3)TWA to sudden quench dynamics of a strongly interacting Bose gas in the 2D optical lattice

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Summary

INTRODUCTION

Quantum simulators built with synthetic quantum platforms that are highly controllable have been applied for studying quantum many-body physics in and out of equilibrium. [11], the Gross-Pitaevskii truncated-Wigner approximation (GPTWA), which is a semiclassical phasespace method on the basis of the GP mean-field theory [12,13], has been directly compared with experimental data regarding dynamics of the 3D Bose-Hubbard model in a weakly interacting regime after a quantum quench. We expect that the SU(3)TWA may simulate the dynamics in the strongly interacting regime of the experiment [15], beyond the capability of the GPTWA, and the SU(2)TWA In their original work, the performance of the SU(3)TWA was tested by applying it to a fully connected spin-1 model, which has an all-to-all spin-exchange (or hopping) term and can be numerically diagonalized even at a large size. VI, we conclude this paper and present outlooks for future studies

MODELS
MONTE CARLO INTEGRATIONS
Gaussian approximation
Fully connected spin-1 model
APPLICATION TO THE 2D BOSE-HUBBARD SYSTEM
Experimental setup
Small-size case
Comparison to the experimental results
Discussions
CONCLUSIONS AND OUTLOOKS
Full Text
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