2016
DOI: 10.1103/physreva.94.013807
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Interplay of nonclassicality and entanglement of two-mode Gaussian fields generated in optical parametric processes

Abstract: The behavior of general nonclassical two-mode Gaussian states at a beam splitter is investigated. Single-mode nonclassicality as well as two-mode entanglement of both input and output states are analyzed suggesting their suitable quantifiers. These quantifiers are derived from local and global invariants of linear unitary two-mode transformations such that the sum of input (or output) local nonclassicality measures and entanglement measure gives a global invariant. This invariant quantifies the global nonclass… Show more

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Cited by 28 publications
(27 citation statements)
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“…[47] and their nonclassicality invariant describing the behavior of their entanglement on a beam-splitter has been discussed in Refs. [48,49].…”
Section: Nonclassicality Criteria Based On the Elements Of Photocmentioning
confidence: 99%
“…[47] and their nonclassicality invariant describing the behavior of their entanglement on a beam-splitter has been discussed in Refs. [48,49].…”
Section: Nonclassicality Criteria Based On the Elements Of Photocmentioning
confidence: 99%
“…On the other hand, the balanced beam splitter with T = 1/2 is optimal for the generation of squeezed light in both output ports. [28][29][30] In general, an arbitrary beam splitter has the potential to generate states that may exhibit both local non-classicality and entanglement.…”
Section: Identification Of Non-classicality Of Two-mode States Beyondmentioning
confidence: 99%
“…Here, we would like to stress that when analyzing below NWs R k and M for the Gaussian states under consideration, we will compare those NWs with genuine nonclassicality identifiers for the two-mode Gaussian states derived in Refs. [30,31]. Namely, those genuine nonclassicality identifiers comprise the local nonclassicality identifiers (LNIs) I…”
Section: B Beam Splitter Transformationmentioning
confidence: 99%
“…To include noise in the system, we utilize the model of the superposition of the quantum signal and noise [29], meaning that only the vacuum fluctuations B 1 of the signal field need to be modified in the covariance matrix, i.e., B 1 = B sq + B n , where B n is the mean thermal noise photon number, and all other quantities in the covariance matrix A N are left unchanged [31].…”
Section: A Spontaneous Second Subharmonic Emissionmentioning
confidence: 99%
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