Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/2733
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dc.contributor.authorMantri, Atul-
dc.date.accessioned2020-12-07T07:09:10Z-
dc.date.available2020-12-07T07:09:10Z-
dc.date.issued2013-
dc.identifier.citationPhysical Review Letters, 111(23).en_US
dc.identifier.otherhttps://doi.org/10.1103/PhysRevLett.111.230502-
dc.identifier.urihttps://journals.aps.org/prl/abstract/10.1103/PhysRevLett.111.230502-
dc.identifier.urihttp://hdl.handle.net/123456789/2733-
dc.descriptionOnly IISERM authors are available in the record.-
dc.description.abstractBlind quantum computation allows a client with limited quantum capabilities to interact with a remote quantum computer to perform an arbitrary quantum computation, while keeping the description of that computation hidden from the remote quantum computer. While a number of protocols have been proposed in recent years, little is currently understood about the resources necessary to accomplish the task. Here, we present general techniques for upper and lower bounding the quantum communication necessary to perform blind quantum computation, and use these techniques to establish concrete bounds for common choices of the client’s quantum capabilities. Our results show that the universal blind quantum computation protocol of Broadbent, Fitzsimons, and Kashefi, comes within a factor of 8 3 of optimal when the client is restricted to preparing single qubits. However, we describe a generalization of this protocol which requires exponentially less quantum communication when the client has a more sophisticated device.en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectCapabilitiesen_US
dc.subjectQuantum computationen_US
dc.subjectClienten_US
dc.subjectComputationen_US
dc.titleOptimal Blind Quantum Computationen_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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