Abstract

Quantum entanglement is a form of correlation between quantum particles that cannot be increased via local operations and classical communication. It has therefore been proposed that an increment of quantum entanglement between probes that are interacting solely via a mediator implies non-classicality of the mediator. Indeed, under certain assumptions regarding the initial state, entanglement gain between the probes indicates quantum coherence in the mediator. Going beyond such assumptions, there exist other initial states which produce entanglement between the probes via only local interactions with a classical mediator. In this process the initial entanglement between any probe and the rest of the system "flows through" the classical mediator and gets localised between the probes. Here we theoretically characterise maximal entanglement gain via classical mediator and experimentally demonstrate, using liquid-state NMR spectroscopy, the optimal growth of quantum correlations between two nuclear spin qubits interacting through a mediator qubit in a classical state. We additionally monitor, i.e., dephase, the mediator in order to emphasise its classical character. Our results indicate the necessity of verifying features of the initial state if entanglement gain between the probes is used as a figure of merit for witnessing non-classical mediator. Such methods were proposed to have exemplary applications in quantum optomechanics, quantum biology and quantum gravity.

Highlights

  • Quantum entanglement is widely recognised as a resource “as real as energy” [13]

  • It is understood that entanglement gain in these schemes is not bounded by the communicated entanglement, but rather by communicated quantum discord [8, 31,32,33,34, 41], a form of quantum correlation that persists in many disentangled states [11, 24, 27]

  • From the experimentally measured three-qubit deviation density matrices we compute various quantum correlations such as discord between the two probes and mediator, DAB|M, quantum entanglement between the probes, as measured by the negativity EA:B, as well as the negativity EB:AM

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Summary

Introduction

Quantum entanglement is widely recognised as a resource “as real as energy” [13]. Yet, limits on establishing entanglement between remote particles were systematically studied only recently and with surprising results. It is understood that entanglement gain in these schemes is not bounded by the communicated entanglement, but rather by communicated quantum discord [8, 31,32,33,34, 41], a form of quantum correlation that persists in many disentangled states [11, 24, 27] In another route to producing remote entanglement, the exchange of quantum particles is replaced by continuous interactions of distant systems (probes) with a third object, a mediator. In this scenario the theory predicts that the probes can get entangled without ever entangling the mediator [9], and that they can even get entangled in the absence of any quantum discord between the probes and the mediator [17]. This lack of discord is a strong notion of classicality which means that the mediator can be measured

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