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EIT-assisted atomic squeezing

dc.contributor.authorDantan, A.en_US
dc.contributor.authorPinard, M.en_US
dc.contributor.authorBerman, P. R.en_US
dc.date.accessioned2006-09-11T14:03:45Z
dc.date.available2006-09-11T14:03:45Z
dc.date.issued2003-11en_US
dc.identifier.citationDantan, A.; Pinard, M.; Berman, P. R.; (2003). "EIT-assisted atomic squeezing." The European Physical Journal D 27(2): 193-199. <http://hdl.handle.net/2027.42/43944>en_US
dc.identifier.issn1434-6060en_US
dc.identifier.issn1434-6079en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/43944
dc.description.abstractThe interaction of classical and quantized electromagnetic fields with an ensemble of atoms in an optical cavity is considered. Four fields drive a double- level scheme in the atoms, consisting of a pair of systems sharing the same set of lower levels. Two of the fields produce maximum coherence, , between the ground state sublevels 1 and 2. This pumping scheme involves equal intensity fields that are resonant with both the one- and two-photon transitions of the system. There is no steady-state absorption of these fields, implying that the fields induce a type Electromagnetically-Induced Transparency (EIT) in the medium. An additional pair of fields interacting with the second system, combined with the EIT fields, leads to squeezing of the atom spin associated with the ground state sublevels. Our method involves a new mechanism for creating steady-state spin squeezing using an optical cavity. As the cooperativity parameter C is increased, the optimal squeezing varies as C -1/3 . For experimentally accessible values of C , squeezing as large as 90% can be achieved.en_US
dc.format.extent214957 bytes
dc.format.extent3115 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.language.isoen_US
dc.publisherSpringer-Verlag; EDP Sciences, Società Italiana di Fisica, Springer-Verlagen_US
dc.subject.otherPhysicsen_US
dc.titleEIT-assisted atomic squeezingen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelMathematicsen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumMichigan Center for Theoretical Physics, FOCUS Center, ; Physics Department, University of Michigan, 48109-1120, Ann Arbor, Michigan, USA,en_US
dc.contributor.affiliationotherLaboratoire Kastler Brossel, Case 74, 4 place Jussieu, 75252, Paris Cedex 05, France,en_US
dc.contributor.affiliationotherLaboratoire Kastler Brossel, Case 74, 4 place Jussieu, 75252, Paris Cedex 05, France,en_US
dc.contributor.affiliationumcampusAnn Arboren_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/43944/1/10053_2003_Article_253.pdfen_US
dc.identifier.doihttp://dx.doi.org/10.1140/epjd/e2003-00253-yen_US
dc.identifier.sourceThe European Physical Journal Den_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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