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Low Even Configurations in the First Spectrum of Ruthenium (Ru I), part 2

A published calculation for the 4d(8), 4d (7)5s, and 4d(6) 5s(2) configurations of Ru I (R. E. Trees, J. Opt. Soc. Am. 49, 838 (1959).) is repeated in steps. Displacements produced by configuration interaction are evaluated, and departures of term positions from familiar expectations in the absence...

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Autor principal: Trees, R. E.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: [Gaithersburg, MD] : U.S. Dept. of Commerce, National Institute of Standards and Technology 1959
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5287037/
https://www.ncbi.nlm.nih.gov/pubmed/31216133
http://dx.doi.org/10.6028/jres.063A.019
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author Trees, R. E.
author_facet Trees, R. E.
author_sort Trees, R. E.
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description A published calculation for the 4d(8), 4d (7)5s, and 4d(6) 5s(2) configurations of Ru I (R. E. Trees, J. Opt. Soc. Am. 49, 838 (1959).) is repeated in steps. Displacements produced by configuration interaction are evaluated, and departures of term positions from familiar expectations in the absence of configuration interaction are explained. The weaker perturbations produced by second-order effects of the spin-orbit interaction are then determined. It is shown that the neglect of these effects in published hand computations has obscured the remarkably good agreement between theory and observation that is obtainable in spectra of the second long period. The eigenvectors are based on “third-order eigenfunctions” which describe the levels simply, and show the degree of LS-coupling in a more quantitative manner.
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spelling pubmed-52870372019-06-18 Low Even Configurations in the First Spectrum of Ruthenium (Ru I), part 2 Trees, R. E. J Res Natl Bur Stand A Phys Chem Article A published calculation for the 4d(8), 4d (7)5s, and 4d(6) 5s(2) configurations of Ru I (R. E. Trees, J. Opt. Soc. Am. 49, 838 (1959).) is repeated in steps. Displacements produced by configuration interaction are evaluated, and departures of term positions from familiar expectations in the absence of configuration interaction are explained. The weaker perturbations produced by second-order effects of the spin-orbit interaction are then determined. It is shown that the neglect of these effects in published hand computations has obscured the remarkably good agreement between theory and observation that is obtainable in spectra of the second long period. The eigenvectors are based on “third-order eigenfunctions” which describe the levels simply, and show the degree of LS-coupling in a more quantitative manner. [Gaithersburg, MD] : U.S. Dept. of Commerce, National Institute of Standards and Technology 1959 1959-12-01 /pmc/articles/PMC5287037/ /pubmed/31216133 http://dx.doi.org/10.6028/jres.063A.019 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
Trees, R. E.
Low Even Configurations in the First Spectrum of Ruthenium (Ru I), part 2
title Low Even Configurations in the First Spectrum of Ruthenium (Ru I), part 2
title_full Low Even Configurations in the First Spectrum of Ruthenium (Ru I), part 2
title_fullStr Low Even Configurations in the First Spectrum of Ruthenium (Ru I), part 2
title_full_unstemmed Low Even Configurations in the First Spectrum of Ruthenium (Ru I), part 2
title_short Low Even Configurations in the First Spectrum of Ruthenium (Ru I), part 2
title_sort low even configurations in the first spectrum of ruthenium (ru i), part 2
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5287037/
https://www.ncbi.nlm.nih.gov/pubmed/31216133
http://dx.doi.org/10.6028/jres.063A.019
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