Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/3507
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dc.contributor.authorChaudhuri, R. K-
dc.contributor.authorFreed, K. F-
dc.date.accessioned2008-09-09T11:06:27Z-
dc.date.available2008-09-09T11:06:27Z-
dc.date.issued2005-04-
dc.identifier.citationJournal of Chemical Physics, Vol. 122, No. 15, pp. 154310en
dc.identifier.issn0021-9606-
dc.identifier.urihttp://hdl.handle.net/2248/3507-
dc.description.abstractCalculations of the ground and excited state potential energy curves of C2 using the third-order effective valence Hamiltonian (H/Sup-3rd(v) ) method are benchmarked against full configuration interaction and other correlated single-reference perturbative and nonperturbative theories. The large nonparallelity errors (NPEs) exhibited even by state-of-art coupled cluster calculations through perturbative triples indicate a serious deficiency of these single-reference theories. The Hv method, on the other hand, produces a much reduced NPE, rendering it a viable approximate many-body method for accurately determining global ground and excited state potential energy curves/surfaces.en
dc.language.isoenen
dc.publisherAmerican Institute of Physicsen
dc.relation.urihttp://link.aip.org/link/?JCPSA6/122/154310/1en
dc.relation.urihttp://dx.doi.org/10.1063/1.1879812en
dc.subjectGround Statesen
dc.subjectExcited Statesen
dc.subjectPotential Energy Surfacesen
dc.subjectCarbonen
dc.subjectConfiguration Interactionsen
dc.subjectPerturbation Theoryen
dc.subjectCoupled Cluster Calculationsen
dc.titleGeneration of potential energy curves for the X-1Sigma (+) g, B-1 Delta (+) (g), and B' (1) states of C-2 using the effective valence shell Hamiltonian methoden
dc.typeArticleen
Appears in Collections:IIAP Publications

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