Localizing genuine multimode entanglement: Asymmetric gains via non-Gaussianity

Measurement-based quantum correlation mimics several characteristics of multipartite quantum correlations and at the same time, it reduces the parent system to a smaller subsystem. On the other hand, genuine multipartite entanglement measures can capture certain features of a multisite composite sys...

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Bibliographic Details
Published inarXiv.org
Main Authors Banerjee, Ratul, Roy, Saptarshi, Das, Tamoghna, Aditi Sen De
Format Paper
LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 18.03.2021
Subjects
Continuity (mathematics)
Correlation analysis
Entanglement
Permutations
Subsystems
Subtraction
Symmetry
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Summary:Measurement-based quantum correlation mimics several characteristics of multipartite quantum correlations and at the same time, it reduces the parent system to a smaller subsystem. On the other hand, genuine multipartite entanglement measures can capture certain features of a multisite composite system that are inaccessible via bipartite quantum correlation quantifiers. We merge these two concepts by introducing localizable genuine multimode entanglement for continuous variable systems, both for Gaussian and non-Gaussian multimode parent states. We report a compact form of localizable generalized geometric measure for multimode Gaussian states when Gaussian measurements are performed in some of the modes. We show that non-Gaussian measurements can concentrate more genuine multimode entanglement compared to the Gaussian ones. For non-Gaussian states with non-Gaussian measurements, we find that although four-mode squeezed vacuum state has permutation symmetry with respect to the exchange of first and third modes as well as the second and the fourth modes, the symmetry can be broken by performing measurements in one of the modes in case of addition while for subtraction, such symmetry is preserved, thereby providing a method for distinguishing multimode photon-added and -subtracted states via localizations.
ISSN:2331-8422