Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4174
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dc.contributor.authorSUDHEER KUMAR, C Sen_US
dc.date.accessioned2019-11-01T03:45:37Z
dc.date.available2019-11-01T03:45:37Z
dc.date.issued2019-11en_US
dc.identifier.citationPramana, 93(5).en_US
dc.identifier.issn0304-4289en_US
dc.identifier.issn0973-7111en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/4174
dc.identifier.urihttp://dx.doi.org/10.1007/s12043-019-1830-3en_US
dc.description.abstractHHere we show that if we insert context-dependent local unitary evolutions into the spatial (i.e. normal) Bell–Clauser–Horne–Shimony–Holt (Bell-CHSH) test, then it is possible to violate the space–time Bell-CHSH inequality maximally (i.e. up to 4). The correct context dependency can be achieved via post-selection. However, this does not contradict the Tsirelson quantum bound (22–√), because the latter has been derived without taking into consideration the context-dependent unitary evolutions and / or post-selection. As an important application, this leads to a more efficient (in terms of resource (singlets) and classical communication) and more sensitive (to eavesdropping) quantum key distribution (QKD) protocol, compared to Ekert’s and Wigner’s QKD protocols.en_US
dc.language.isoenen_US
dc.publisherIndian Academy of Sciencesen_US
dc.subjectSpace time Bellen_US
dc.subjectClauser Horne Shimonyen_US
dc.subjectHolt test quantumen_US
dc.subjectKey distribution unitary evolutionen_US
dc.subjectPost-selectionen_US
dc.subjectTOC-OCT-2019en_US
dc.subject2019en_US
dc.titleViolation of space-time Bell-CHSH inequality beyond the Tsirelson bound and quantum cryptographyen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePramanaen_US
dc.publication.originofpublisherIndianen_US
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