Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/2572
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dc.contributor.authorSingh, Mandip-
dc.date.accessioned2020-12-03T09:00:02Z-
dc.date.available2020-12-03T09:00:02Z-
dc.date.issued2017-
dc.identifier.citationPhysical Review A, 95 (4)en_US
dc.identifier.other10.1103/PhysRevA.95.043620-
dc.identifier.urihttps://journals.aps.org/pra/abstract/10.1103/PhysRevA.95.043620-
dc.identifier.urihttp://hdl.handle.net/123456789/2572-
dc.description.abstractIn this paper, a quantum Stern-Gerlach thought experiment is introduced where, in addition to the intrinsic angular momentum of an atom, the magnetic field is considered to be a quantum mechanical field. A free falling spin polarized Bose-Einstein condensate passes close to a flux qubit and interacts with the quantum superimposed magnetic field of the flux qubit. Such an interaction results a macroscopic quantum entanglement of the path of a Bose-Einstein condensate with the magnetic flux quantum state of the flux qubit. In this paper, three regimes of coupling between the flux qubit and a free falling Bose-Einstein condensate are discussed. This paper also explains how to produce a path entangled Bose-Einstein condensate where the condensate can be located at physically distinct locations simultaneously. This paper highlights new insights about the foundations of the quantum Stern-Gerlach experiment.en_US
dc.language.isoen_USen_US
dc.publisherAPSen_US
dc.subjectquantum Stern-Gerlachen_US
dc.subjectatomen_US
dc.subjectBose-Einstein condensateen_US
dc.titleQuantum Stern-Gerlach experiment and path entanglement of a Bose-Einstein condensateen_US
dc.typeArticleen_US
Appears in Collections:Research Articles

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