Extending Hudson’s theorem to mixed quantum states

dc.contributor.authorMandilara, Aikaterini
dc.contributor.authorKarpov, E.
dc.contributor.authorCerf, N. J.
dc.date.accessioned2016-02-04T10:03:45Z
dc.date.available2016-02-04T10:03:45Z
dc.date.issued2009
dc.description.abstractAccording to Hudson’s theorem, any pure quantum state with a positive Wigner function is necessarily a Gaussian state. Here, we make a step toward the extension of this theorem to mixed quantum states by finding upper and lower bounds on the degree of non-Gaussianity of states with positive Wigner functions. The bounds are expressed in the form of parametric functions relating the degree of non-Gaussianity of a state, its purity, and the purity of the Gaussian state characterized by the same covariance matrix. Although our bounds are not tight, they permit us to visualize the set of states with positive Wigner functions
dc.identifier.citationMandilara, A., Karpov, E., & Cerf, N. (2009). Extending Hudson’s theorem to mixed quantum states. Physical Review A—Atomic, Molecular, and Optical Physics, 79(6), 062302.
dc.identifier.doihttps://doi.org/10.1103/PhysRevA.79.062302
dc.identifier.urihttp://nur.nu.edu.kz/handle/123456789/1141
dc.language.isoen
dc.rightsMetadata only
dc.sourcePhysical Review A—Atomic, Molecular, and Optical Physics, 79(6).
dc.subjectPhysics
dc.subjectHudson’s theorem
dc.titleExtending Hudson’s theorem to mixed quantum states
dc.typeArticle

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