Genuine -partite entanglement without -partite correlation functions
arXiv:1704.03385 · doi:10.1103/PhysRevA.95.062331
Abstract
A genuinely -partite entangled state may display vanishing -partite correlations measured for arbitrary local observables. In such states the genuine entanglement is noticeable solely in correlations between subsets of particles. A straightforward way to obtain such states for odd is to design an `anti-state' in which all correlations between an odd number of observers are exactly opposite. Evenly mixing a state with its anti-state then produces a mixed state with no -partite correlations, with many of them genuinely multiparty entangled. Intriguingly, all known examples of `entanglement without correlations' involve an \emph{odd} number of particles. Here we further develop the idea of anti-states, thereby shedding light on the different properties of even and odd particle systems. We conjecture that there is no anti-state to any pure even--party entangled state making the simple construction scheme unfeasable. However, as we prove by construction, higher-rank examples of `entanglement without correlations' for arbitrary even indeed exist. These classes of states exhibit genuine entanglement and even violate an -partite Bell inequality, clearly demonstrating the non-classical features of these states as well as showing their applicability for quantum communication complexity tasks.
arXiv comment8 pages
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Cited by in corpus (11)
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- Higher dimensional entanglement without correlations
- A Moment for Random Measurements
- Genuinely entangled symmetric states with no -partite correlations
- Valid and efficient entanglement verification with finite copies of a quantum state
- Unmasking the Polygamous Nature of Quantum Nonlocality
- Cooperation and dependencies in multipartite systems