Superposition states at finite temperature

dc.contributor.authorHuyet, Guillaume
dc.contributor.authorFranke-Arnold, Sonja
dc.contributor.authorBarnett, Stephen M.
dc.date.accessioned2017-08-29T09:04:00Z
dc.date.available2017-08-29T09:04:00Z
dc.date.issued2001
dc.description.abstractWe describe a method to create superposition states from a mixed state of a harmonic oscillator. If the initial state is described by a thermal state, then the resulting superposition state will be a "hot'' superposition state. Such a state can be distinguished from a statistical mixture by its coherence properties. Here we suggest how to demonstrate the coherence of the superposition state by observing interference fringes when the two parts of the wave packet are overlapped. In the case of the mixed superposition state, a partial overlap may not be sufficient to observe the presence of fringes. We introduce therefore the idea of a coherence length for the wave packet and demonstrate its relevance for interferometry of mixed states. We illustrate our ideas with the example of superposition states for the motion of a single trapped ion.en
dc.description.statusPeer revieweden
dc.description.versionPublished Versionen
dc.format.mimetypeapplication/pdfen
dc.identifier.articleid43812
dc.identifier.citationHuyet, G., Franke-Arnold, S. and Barnett, S. M. (2001) 'Superposition states at finite temperature', Physical Review A, 63(4), 043812 (7pp). doi: 10.1103/PhysRevA.63.043812en
dc.identifier.doi10.1103/PhysRevA.63.043812
dc.identifier.issn1050-2947
dc.identifier.issued4
dc.identifier.journaltitlePhysical Review Aen
dc.identifier.urihttps://hdl.handle.net/10468/4562
dc.identifier.volume63
dc.language.isoenen
dc.publisherAmerican Physical Societyen
dc.relation.urihttps://journals.aps.org/pra/abstract/10.1103/PhysRevA.63.043812
dc.rights© 2001, American Physical Societyen
dc.subjectQuantum jumpsen
dc.subjectThermal noiseen
dc.subjectTrapped atomen
dc.titleSuperposition states at finite temperatureen
dc.typeArticle (peer-reviewed)en
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