Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/3046
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dc.contributor.authorDilip, A-
dc.contributor.authorDas, B. P-
dc.contributor.authorPerger, W. F-
dc.contributor.authorSamal, M. K-
dc.contributor.authorGeetha, K. P-
dc.date.accessioned2008-08-06T05:52:20Z-
dc.date.available2008-08-06T05:52:20Z-
dc.date.issued2001-08-
dc.identifier.citationJournal of Physics B: Atomic, Molecular, and Optical Physics, Vol. 34, No. 15, pp. 3089 - 3106en
dc.identifier.issn0953-4075-
dc.identifier.urihttp://hdl.handle.net/2248/3046-
dc.descriptionRestricted Access-
dc.description.abstractThe existence of the permanent electric dipole moment (EDM) of an atom implies the simultaneous violation of parity and time-reversal symmetries. Two experiments based on laser cooling have been proposed to search for the EDM of atomic ytterbium. We propose three different relativistic many-body approaches to calculate the EDM of atoms with strongly interacting configurations. Two of them are based on the configuration-interaction method and the third is an algebraic many-body perturbation theory that explicitly uses configuration state functions. We use these three approaches to calculate the EDM of atomic ytterbium arising from an electron-nucleus tensor-pseudotensor interaction. The results of these calculations are in excellent agreement with each other.en
dc.format.extent3894 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherInstitute of Physicsen
dc.relation.urihttp://www.iop.org/EJ/abstract/0953-4075/34/15/314/en
dc.subjectElectric Dipole Moment (Edm)en
dc.subjectLaser Coolingen
dc.subjectAtomic Ytterbiumen
dc.subjectRelativisticen
dc.subjectElectron-Nucleus Tensor-Pseudotensor Interactionen
dc.titleMany-body theory of the electric dipole moment of atomic ytterbiumen
dc.typeArticleen
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