Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/5726
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dc.contributor.authorGopakumar, G-
dc.contributor.authorSur, C-
dc.contributor.authorDas, B. P-
dc.contributor.authorChaudhuri, R. K-
dc.contributor.authorMukherjee, D-
dc.contributor.authorHirao, K-
dc.date.accessioned2012-03-07T14:05:29Z-
dc.date.available2012-03-07T14:05:29Z-
dc.date.issued2006-
dc.identifier.citationJournal of Theoretical and Computational Chemistry, Vol. 5, No. 4, pp. 945-956en
dc.identifier.urihttp://hdl.handle.net/2248/5726-
dc.descriptionRestricted Accessen
dc.description.abstractThe connections between the Random Phase Approximation (RPA) and Many-Body Perturbation Theory (MBPT) and its all order generalization, the Coupled-Cluster Theory (CCT), have been explored. Explicit expressions have been derived for the electric dipole amplitudes for allowed and forbidden transitions induced by the parity non-conserving neutral weak interaction. The Goldstone diagrams associated with the RPA terms in both cases are shown to arise in MBPT and CCT, and the numerical verification of this relationship is made for the allowed electric dipole transitions.en
dc.language.isoenen
dc.publisherWorld Scientific Publishing Coen
dc.relation.urihttp://dx.doi.org/10.1142/S0219633606002611en
dc.rights© World Scientific Publishingen
dc.subjectRandom Phase Approximationen
dc.subjectMany-Body Perturbation Theoryen
dc.subjectCoupled-Cluster Theoryen
dc.titleRandom phase approximation for allowed and parity non-conserving electric dipole transition amplitudes and its connection with many-body perturbation theory and coupled-cluster theoryen
dc.typeArticleen
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