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dc.contributor.authorCamacho, Cristopheren_US
dc.contributor.authorWitek, Henryk A.en_US
dc.contributor.authorCimiraglia, Renzoen_US
dc.date.accessioned2014-12-08T15:06:42Z-
dc.date.available2014-12-08T15:06:42Z-
dc.date.issued2010-06-28en_US
dc.identifier.issn0021-9606en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.3442374en_US
dc.identifier.urihttp://hdl.handle.net/11536/5247-
dc.description.abstractA systematic investigation of low-lying states of Sc(2) using multireference perturbation theory (NEVPT2 and NEVPT3) indicates that the ground state of this system is 5 Sigma(u) with r(e)= 2.611 angstrom, w(e)= 241.8 cm(-1), and De= 1.78 eV. This state is closely followed by other low-lying states of Sc(2): (3)Sigma(u)-, (5)Delta(u), (3)Pi(g), (1)Pi(g), and (1)Sigma(u)-. Our energy ordering of the (5)Sigma(u)- and (3)Sigma(u)- states confirms the recent MRCI results of Kalemos et al. [J. Chem. Phys. 132, 024309 (2010)] and is at variance with the earlier diffusion Monte Carlo predictions of Matxain et al. [J. Chem. Phys. 128, 194315 (2008)]. An excellent agreement between the second-and third-order NEVPT results and between the computed and experimental values of omega(e) (241.8 versus 238.9 cm(-1)) for the (5)Sigma(u)- state suggests high accuracy of our predictions. (C) 2010 American Institute of Physics. [doi: 10.1063/1.3442374]en_US
dc.language.isoen_USen_US
dc.titleThe low-lying states of the scandium dimeren_US
dc.typeArticleen_US
dc.identifier.doi10.1063/1.3442374en_US
dc.identifier.journalJOURNAL OF CHEMICAL PHYSICSen_US
dc.citation.volume132en_US
dc.citation.issue24en_US
dc.citation.epageen_US
dc.contributor.department應用化學系zh_TW
dc.contributor.department應用化學系分子科學碩博班zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.contributor.departmentInstitute of Molecular scienceen_US
dc.identifier.wosnumberWOS:000279740200023-
dc.citation.woscount20-
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