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Entanglement is often verified by a violation of an inequality like a Bell inequality or an entanglement witness.
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M. Ardehali, Phys. Rev. A 46
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For an overview of the different approaches, see C. Amsler et al
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Indeed, with the given choice of observables the operators ℬ M \mathcal{B}_{\rm M} and ℬ A \mathcal{B}_{\rm A} are identical within quantum mechanics. However, the use of A A and B B within the Ardehali inequality results in a more restrictive test for LHV models
Cited in the paper.
This is also important, as for nearly perfect GHZ states, some count numbers n k l n_{kl} will be close to zero. Then, the interpretation of the statistical error as a confidence interval may be questioned
Cited in the paper.
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O. Gühne and G. Tóth, Phys. Reports 474
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M. Lewenstein et al
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In Ref. [ 10 ] the second term, − ⟨ ℳ ⟩ / n tot -\langle{\mathcal{M}}\rangle/n_{\rm tot} , is omitted, leading to a systematic overestimation of the standard deviation. Such an overestimation is problematic, if the claim is that certain state properties (e.g. having a negative partial transpose) are not significant. This can occur, e.g. in the analysis of bound entanglement, see A. Elias and M. Bourennane, Nature Phys. 5
2009
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H.F. Hofmann, Phys. Rev. Lett. 94
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