Abstract

Critical phenomena involve structural changes in the correlations of its constituents. Such changes can be reproduced and characterized in quantum simulators able to tackle medium-to-large-size systems. We demonstrate these concepts by engineering the ground state of a three-spin Ising ring by using a pair of entangled photons. The effect of a simulated magnetic field, leading to a critical modification of the correlations within the ring, is analysed by studying two- and three-spin entanglement. In particular, we connect the violation of a multipartite Bell inequality with the amount of tripartite entanglement in our ring.

Highlights

  • Critical phenomena involve structural changes in the correlations of its constituents

  • We show that the Svetlichny function evaluated using the simulated ground state of the Ising chain violates the Nparty local-realistic bound that, even for a short chain, is very close to the quantum critical point defined in the thermodynamic limit N R ‘

  • The bipartite non-locality (Fig. 2 a), which is null for b R 0 and b R 2‘, reaches a non-zero value close to the point of structural changes b^{1, which would correspond to the critical point for N At the same time, the tripartite non-locality witnessed by

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Summary

Introduction

Critical phenomena involve structural changes in the correlations of its constituents. Anyonic statistics[13] and frustration in a Heisenberg chain[14] have been studied in analog photonic quantum simulators, while special topologically protected bound states predicted by models of condensed-matter physics have been emulated[15,16]. One can take the approach of constructing multi-photon states enjoying the same symmetries as the ground states by using continuously tuneable quantum gates realized by means of pre-available entangled pairs of particles and measurement-induced interactions, when necessary[14,16] This approach is relevant when obtaining statistical information by classical computation might be challenging, e.g. the spin correlation function of a one-dimensional antiferromagnetic Heisenberg model[17,18]. In this paper we follow such an approach to demonstrate the nonlocal properties of the ground state of a paradigmatic many-body system: the transverse Ising model

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