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Please use this identifier to cite or link to this item: http://hdl.handle.net/2289/4378
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dc.contributor.authorMartin, A.-
dc.contributor.authorAlibart, O.-
dc.contributor.authorFlesch, J.C.-
dc.contributor.authorSamuel, J.-
dc.contributor.authorSinha, Supurna-
dc.contributor.authorTanzilli, S.-
dc.contributor.authorKastberg, Anders-
dc.date.accessioned2012-04-11T08:28:27Z-
dc.date.available2012-04-11T08:28:27Z-
dc.date.issued2012-01-
dc.identifier.citationEurophysics Letters, 2012, Vol.97, p.10003en
dc.identifier.issn0295-5075-
dc.identifier.issn1286-4854(online)-
dc.identifier.urihttp://hdl.handle.net/2289/4378-
dc.descriptionRestricted Access. An open-access version is available at arXiv.org (one of the alternative locations)en
dc.description.abstractWe report the experimental observation of the non-local geometric phase in Hanbury Brown-Twiss polarized intensity interferometry. The experiment involves two independent, polarized, incoherent sources, illuminating two polarized detectors. Varying the relative polarization angle between the detectors introduces a geometric phase equal to half the solid angle on the Poincaré sphere traced out by a pair of single photons. Local measurements at either detector do not reveal the effect of the geometric phase, which appears only in the coincidence counts between the two detectors, showing a genuinely non-local effect. We show experimentally that coincidence rates of photon arrival times at separated detectors can be controlled by the two-photon geometric phase. This effect can be used for manipulating and controlling photonic entanglement.en
dc.language.isoenen
dc.publisherEPL Associationen
dc.relation.urihttp://arxiv.org/abs/1110.0416en
dc.relation.urihttp://dx.doi.org/10.1209/0295-5075/97/10003en
dc.relation.urihttp://adsabs.harvard.edu/abs/2012EL.....9710003Men
dc.rights2012, EPLAen
dc.titleNon-local geometric phase in two-photon interferometryen
dc.typeArticleen
Appears in Collections:Research Papers (TP)

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