No-local-broadcasting theorem for quantum correlations

TL;DR

This paper establishes a no-local-broadcasting theorem that characterizes quantum correlations in multipartite states, showing that local sharing of correlations reveals their quantumness, and introduces measures for quantumness of correlations.

Contribution

The paper proves a no-local-broadcasting theorem for quantum correlations, linking local broadcasting feasibility to the classicality of correlations, and develops an operational approach to quantify quantumness.

Findings

Local broadcasting is possible only for classical correlations.

Unentangled states can exhibit quantum correlations.

The theorem implies the standard no-broadcasting theorem for single systems.

Abstract

We prove that the correlations present in a multipartite quantum state have an \emph{operational} quantum character as soon as the state does not simply encode a multipartite classical probability distribution, i.e. does not describe the joint state of many classical registers. Even unentangled states may exhibit such \emph{quantumness}, that is pointed out by the new task of \emph{local broadcasting}, i.e. of locally sharing pre-established correlations: this task is feasible if and only if correlations are classical and derive a no-local-broadcasting theorem for quantum correlations. Thus, local broadcasting is able to point out the quantumness of correlations, as standard broadcasting points out the quantum character of single system states. Further, we argue that our theorem implies the standard no-broadcasting theorem for single systems, and that our operative approach leads in a natural way to the definition of measures for quantumness of correlations.