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Calculations of Configurations of Doubly Ionized Copper (Cu III)

The energy levels belonging to the configurations 3d(7)4s(2) and 3d(8)nℓ (nℓ = 4s, 5s, 4p 5p, 4d 5d 4f, and 5g) have been calculated. The radial energy integrals were treated as parameters and adjusted to give a least-squares fit to the observed levels. Two- and three-body effective electrostatic in...

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Detalles Bibliográficos
Autores principales: Sugar, J., Martin, W. C.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: [Gaithersburg, MD] : U.S. Dept. of Commerce, National Institute of Standards and Technology 1976
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5293353/
https://www.ncbi.nlm.nih.gov/pubmed/32196274
http://dx.doi.org/10.6028/jres.080A.052
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author Sugar, J.
Martin, W. C.
author_facet Sugar, J.
Martin, W. C.
author_sort Sugar, J.
collection PubMed
description The energy levels belonging to the configurations 3d(7)4s(2) and 3d(8)nℓ (nℓ = 4s, 5s, 4p 5p, 4d 5d 4f, and 5g) have been calculated. The radial energy integrals were treated as parameters and adjusted to give a least-squares fit to the observed levels. Two- and three-body effective electrostatic interactions for equivalent electrons were included, as well as two-body effective interactions for inequivalent electrons. Strong configuration interaction between 3d(7)4s(2) and 3d(8)4d was taken into account. Values of the parameters are given for all the above configurations, and the calculated levels are given for all except 3d(8)4s and 3d(8)4p (for which essentially equivalent results have been published). Leading eigenvector percentages are given in appropriate coupling schemes.
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spelling pubmed-52933532020-03-18 Calculations of Configurations of Doubly Ionized Copper (Cu III) Sugar, J. Martin, W. C. J Res Natl Bur Stand A Phys Chem Article The energy levels belonging to the configurations 3d(7)4s(2) and 3d(8)nℓ (nℓ = 4s, 5s, 4p 5p, 4d 5d 4f, and 5g) have been calculated. The radial energy integrals were treated as parameters and adjusted to give a least-squares fit to the observed levels. Two- and three-body effective electrostatic interactions for equivalent electrons were included, as well as two-body effective interactions for inequivalent electrons. Strong configuration interaction between 3d(7)4s(2) and 3d(8)4d was taken into account. Values of the parameters are given for all the above configurations, and the calculated levels are given for all except 3d(8)4s and 3d(8)4p (for which essentially equivalent results have been published). Leading eigenvector percentages are given in appropriate coupling schemes. [Gaithersburg, MD] : U.S. Dept. of Commerce, National Institute of Standards and Technology 1976 1976-06-01 /pmc/articles/PMC5293353/ /pubmed/32196274 http://dx.doi.org/10.6028/jres.080A.052 Text en https://creativecommons.org/publicdomain/zero/1.0/ The Journal of Research of the National Bureau of Standards Section A is a publication of the U.S. Government. The papers are in the public domain and are not subject to copyright in the United States. Articles from J Res may contain photographs or illustrations copyrighted by other commercial organizations or individuals that may not be used without obtaining prior approval from the holder of the copyright.
spellingShingle Article
Sugar, J.
Martin, W. C.
Calculations of Configurations of Doubly Ionized Copper (Cu III)
title Calculations of Configurations of Doubly Ionized Copper (Cu III)
title_full Calculations of Configurations of Doubly Ionized Copper (Cu III)
title_fullStr Calculations of Configurations of Doubly Ionized Copper (Cu III)
title_full_unstemmed Calculations of Configurations of Doubly Ionized Copper (Cu III)
title_short Calculations of Configurations of Doubly Ionized Copper (Cu III)
title_sort calculations of configurations of doubly ionized copper (cu iii)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5293353/
https://www.ncbi.nlm.nih.gov/pubmed/32196274
http://dx.doi.org/10.6028/jres.080A.052
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