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arXiv:0801.1572

Preliminary analysis of a recent experiment by F. A. Bovino

Emilio Santos

Published Jan 10, 2008• 0 citations
arXivHTMLPDF

Abstract

An analysis is made of the results of a recent polarization correlation experiment by Bovino (unpublished) where about 60,000 data have been obtained. I assume that the state of the photon pairs produced in the source (a non-linear crystal) are in a (slightly)non-maximally entangled state and the most relevant non-idealities of the set-up are taken into account. A comparison is made between the predictions of quantum mechanics and a simple family of local hidden varaibles models with the result that the former is violated by more than 4 standard deviations whislt the data are compatible with the family of local models.

DOI
10.48550/arxiv.0801.1572

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An analysis is made of the results of a recent polarization correlation experiment by Bovino (unpublished) where about 60,000 data have been obtained. I assume that the state of the photon pairs produced in the source (a non-linear crystal) are in a (slightly)non-maximally entangled state and the most relevant non-idealities of the set-up are taken into account. A comparison is made between the predictions of quantum mechanics and a simple family of local hidden varaibles models with the result that the former is violated by more than 4 standard deviations whislt the data are compatible with the family of local models.
We analyze anomalies in data to test the violation of Bell's inequality for the EPR-Bohm experiment. We found that the experimental correlations for photon polarization have an intriguing property. In the experimental data there are visible non-negligible deviations of probabilities $P_{++}^{\rm{exp}}(α, β), P_{+-}^{\rm{exp}}(α, β), P_{-+}^{\rm{exp}}(α, β), P_{--}^{\rm{exp}}(α, β) $ from the predictions of quantum mechanics, namely, P++(α,β)=P−−(α,β)=1/2cos⁡2(α−β)P_{++}(α, β)=P_{--}(α, β)= {1/2}\cos^2(α-β)P++​(α,β)=P−−​(α,β)=1/2cos2(α−β) and P+−=P−+(α,β)=1/2sin⁡2(α−β).P_{+-}=P_{-+}(α, β)={1/2}\sin^2(α-β).P+−​=P−+​(α,β)=1/2sin2(α−β). However, in some mysterious way those deviations compensate each other and finally the correlation Eexp(α,β)=P++exp(α,β)−P+−exp(α,β)−P−+exp(α,β)+P−−exp(α,β)E^{\rm{exp}}(α, β)= P_{++}^{\rm{exp}}(α, β)- P_{+-}^{\rm{exp}}(α, β)- P_{-+}^{\rm{exp}}(α, β)+ P_{--}^{\rm{exp}}(α, β)Eexp(α,β)=P++exp​(α,β)−P+−exp​(α,β)−P−+exp​(α,β)+P−−exp​(α,β) is in the complete agreement with the QM-prediction, namely, E(α,β)=P++(α,β)−P+−(α,β)−P−+(α,β)+P−−(α,β)=cos⁡2(α−β).E(α, β)= P_{++}(α, β)- P_{+-}(α, β)- P_{-+}(α, β)+ P_{--}(α, β)= \cos 2(α-β).E(α,β)=P++​(α,β)−P+−​(α,β)−P−+​(α,β)+P−−​(α,β)=cos2(α−β). Therefore such anomalies play no role in the Bell's inequality framework. Nevertheless, other linear combinations of experimental probabilities do not have such a compensation property. There can be found non-negligible deviations from predictions of quantum mechanics. Thus neither classical nor quantum model can pass the whole family of statistical tests given by all possible linear combinations of the EPR-Bohm probabilities. Does it mean that both models are wrong?
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The launch of a satellite capable of distributing entanglement through long distances and the first loophole-free violation of Bell inequalities are milestones indicating a clear path for the establishment of quantum networks. However, nonlocality in networks with independent entanglement sources has only been experimentally verified in simple tripartite networks, via the violation of bilocality inequalities. Here, by using a scalable photonic platform, we implement star-shaped quantum networks consisting of up to five distant nodes and four independent entanglement sources. We exploit this platform to violate the chained n-locality inequality and thus witness, in a device-independent way, the emergence of nonlocal correlations among the nodes of the implemented networks. These results open new perspectives for quantum information processing applications in the relevant regime where the observed correlations are compatible with standard local hidden variable models but are non-classical if the independence of the sources is taken into account.