2010
DOI: 10.1103/physreva.81.042107
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Analytical proof of Gisin’s theorem for three qubits

Abstract: Gisin's theorem assures that for any pure bipartite entangled state, there is violation of Bell-CHSH inequality revealing its contradiction with local realistic model. Whether, similar result holds for three-qubit pure entangled states, remained unresolved. We show analytically that all three-qubit pure entangled states violate a Bell-type inequality, derived on the basis of local realism, by exploiting the Hardy's non-locality argument.

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Cited by 30 publications
(35 citation statements)
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“…An important approach to characterize entanglement is Bell inequality [3][4][5][6][7][8]. For instance, N. Gisin has proved that all two-qubit pure entangled states violate the CHSH inequality [4].…”
Section: Introductionmentioning
confidence: 99%
“…An important approach to characterize entanglement is Bell inequality [3][4][5][6][7][8]. For instance, N. Gisin has proved that all two-qubit pure entangled states violate the CHSH inequality [4].…”
Section: Introductionmentioning
confidence: 99%
“…Hardy's paradox, with post-selections taken into consideration, therefore stands out among the others, since (i) it applies to the two-party scenario; (ii) it can be generalized to multi-party and high-dimensional scenar-ios [14] (hereafter we would like to call Cereceda's version of n-qubit Hardy's paradox/inequality as the standard Hardy's paradox/inequality, to distinguish them from the most general ones that we shall present in this paper); and (iii) inequalities constructed based on it allow to detect more entangled states and provide a key element to prove Gisin's theorem [31,32] -which states that any entangled pure state violates Bell's inequality [33]. The GHZ paradox does not share most of these merits (see also the Mermin-Ardehali-Belinskii-Klyshko inequality [34][35][36], which was also a kind of generalization of CHSH inequality to n qubits, but was not violated by all pure entangled states, even not by all the generalized GHZ states).…”
mentioning
confidence: 99%
“…(20) we have used the fact that the maximum of x cos θ + y sin θ taking over all θ is x 2 + y 2 . Formulas (14) and (15) can be similarly proven.…”
Section: The Maximal Violations For the Bell Inequalitiesmentioning
confidence: 82%
“…Due to their significance, Bell inequalities have been generalized from the two-qubit case, such as the Clauser-Horne-Shimony-Holt (CHSH) inequality [10] to the N -qubit case, such as the Mermin-Ardehali-Belinskii-Klyshko (MABK) inequality [11,12], and to arbitrary d-dimensional (qudit) systems such as the Collins-Gisin-Linden-Masser-Popescu inequality [13]. However, except for some special cases such as bipartite pure states [2,3,6], three-qubit pure states [5,14], and general two-qubit quantum states [15], there are no Bell inequalities yet that can be violated by all the entangled quantum states, although it is shown recently that any entangled multipartite pure states should violate a Bell inequality [7]. Thus it is of great importance to find more effective Bell-type inequalities to detect the quantum entanglement.…”
Section: Introductionmentioning
confidence: 99%