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Multipartite entanglement for continuous variables

Peter van Loock, Samuel L. Braunstein

Published Jun 6, 1999• 0 citations
OpenAlex

Abstract

It is known that even a single one-mode squeezed state incident on a beamsplitter is sufficient to produce bipartite (pure-state) entanglement with respect to the field quadratures. We show that such entanglement enables quantum teleportation with a fidelity better than could be achieved in any classical scheme. Furthermore, using a continuous-variable teleportation protocol involving more than two parties, we show that a single one-mode squeezed state and linear optics is sufficient to produce a truly N-partite entangled state for arbitrarily many parties, provided that a minimal amount of squeezing is available. This multipartite entanglement may be made arbitrarily good using more and stronger one-mode squeezed states.

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It is known that even a single one-mode squeezed state incident on a beamsplitter is sufficient to produce bipartite (pure-state) entanglement with respect to the field quadratures. We show that such entanglement enables quantum teleportation with a fidelity better than could be achieved in any classical scheme. Furthermore, using a continuous-variable teleportation protocol involving more than two parties, we show that a single one-mode squeezed state and linear optics is sufficient to produce a truly N-partite entangled state for arbitrarily many parties, provided that a minimal amount of squeezing is available. This multipartite entanglement may be made arbitrarily good using more and stronger one-mode squeezed states.
We show that one single-mode squeezed state distributed among N parties using linear optics suffices to produce a truly N-partite entangled state for any nonzero squeezing and arbitrarily many parties. From this N-partite entangled state, via quadrature measurements of N-2 modes, bipartite entanglement between any two of the N parties can be "distilled," which enables quantum teleportation with an experimentally determinable fidelity better than could be achieved in any classical scheme.
First, we show how the quantum circuits for generating and measuring multi-party entanglement of qubits can be translated to continuous quantum variables. We derive sufficient inseparability criteria for NNN-party continuous-variable states and discuss their applicability. Then, we consider a family of multipartite entangled states (multi-party multi-mode states with one mode per party) described by continuous quantum variables and analyze their properties. These states can be efficiently generated using squeezed light and linear optics.
In this work we point out how the continuous variable teleportation protocol takes advantage of the quadrature entanglement in different ways, depending on the preparation of the entangled state. For a given amount of the entanglement resource, we describe the best production scheme for a two-mode Gaussian state, which enables quantum teleportation with optimal fidelity. We extend this study to multiparty entangled Gaussian states and define an operative measure of multipartite entanglement related to the optimal fidelity in a quantum teleportation network experiment. This optimal fidelity is shown to be equivalent to the entanglement of formation for the standard two-user protocol, and to the multipartite localizable entanglement for the multiuser protocol.
Traditional continuous-variable teleportation can only approach unit fidelity in the limit of an infinite (and unphysical) amount of squeezing. We describe a new method for continuous-variable teleportation that approaches unit fidelity with finite resources. The protocol is not based on squeezed states as in traditional teleportation but on an ensemble of single photon entangled states. We characterize the teleportation scheme with coherent states, mesoscopic superposition states, and two-mode squeezed states and we find several situations in which near-unity teleportation fidelity can be obtained with modest resources.