Abstract

Dicke-like models can describe a variety of physical systems, such as atoms in a cavity or vibrating ion chains. In equilibrium these systems often feature a radical change in their behavior when switching from weak to strong spin-boson interaction. This usually manifests in a transition from a "dark" to a "superradiant" phase. However, understanding the out-of-equilibrium physics of these models is extremely challenging, and even more so for strong spin-boson coupling. Here we show that the nonequilibrium strongly interacting multimode Dicke model can mimic some fundamental properties of an associative memory-a system which permits the recognition of patterns, such as letters of an alphabet. Patterns are encoded in the couplings between spins and bosons, and we discuss the dynamics of the spins from the perspective of pattern retrieval in associative memory models. We identify two phases, a "paramagnetic" and a "ferromagnetic" one, and a crossover behavior between these regimes. The "ferromagnetic" phase is reminiscent of pattern retrieval. We highlight similarities and differences with the thermal dynamics of a Hopfield associative memory and show that indeed elements of "machine learning behavior" emerge in the strongly coupled multimode Dicke model.

Highlights

  • Cavity, circuit [1] and waveguide quantum electrodynamics (QED) [2], as well as trapped ions [3, 4] provide controllable platforms for quantum simulation

  • We show that the non-equilibrium strongly interacting multi-mode Dicke model can mimic some fundamental properties of an associative memory - a system which permits the recognition of patterns, such as letters of an alphabet

  • Patterns are encoded in the couplings between spins and bosons, and we discuss the dynamics of the spins from the perspective of pattern retrieval in associative memory models

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Summary

Introduction

Circuit [1] and waveguide quantum electrodynamics (QED) [2], as well as trapped ions [3, 4] provide controllable platforms for quantum simulation. Patterns are encoded in the couplings between spins and bosons, and we discuss the dynamics of the spins from the perspective of pattern retrieval in associative memory models. Phase diagram of the overlap mμ = (Gμ ⋅ σ⃗stat) N between the classical, stationary spin configuration and the pattern as a function of the parameter η = (γ − κ) ω (for details see text).

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