Definition and utilization of atomic partial screening constants
Identifieur interne : 003B41 ( Istex/Corpus ); précédent : 003B40; suivant : 003B42Definition and utilization of atomic partial screening constants
Auteurs : Tran Huu Loi ; Michel Remy ; Michel Gantois ; Claude ZellerSource :
- Zeitschrift für Physik A Atoms and Nuclei [ 0939-7922 ] ; 1976-03-01.
English descriptors
- Teeft :
- Atomic levels, Correct order, Cristallographie universit6, Different formulae, Energy values, Experimental values, Hartree fock, Heavy atoms, Laboratoire, Light elements, Mathematical methods, Michel gantois laboratoire, Outer shells, Partial screening, Partial screening constants, Periodic chart, Physical meaning, Screening, Screening constants, Screening effect, Variational method.
Abstract
Abstract: The screening constant can be decomposed into a sum of different terms over the different atomic shells. This decomposition visualizes the electron distribution. The energy levels which are calculated by means of these constants agree well with the experimental values for the inner-shells. Our method is therefore complementary to Slater's used for the outer shells.
Url:
DOI: 10.1007/BF01409084
Links to Exploration step
ISTEX:F7E93B261DBD2343A25EA33E3D7B1F79AB33F454Le document en format XML
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DisplayOrder="Western"><GivenName>Tran</GivenName><GivenName>Huu</GivenName><FamilyName>Loi</FamilyName></AuthorName></Author><Author AffiliationIDS="Aff3"><AuthorName DisplayOrder="Western"><GivenName>Michel</GivenName><FamilyName>Remy</FamilyName></AuthorName></Author><Author AffiliationIDS="Aff2"><AuthorName DisplayOrder="Western"><GivenName>Michel</GivenName><FamilyName>Gantois</FamilyName></AuthorName></Author><Author AffiliationIDS="Aff4"><AuthorName DisplayOrder="Western"><GivenName>Claude</GivenName><FamilyName>Zeller</FamilyName></AuthorName></Author><Affiliation ID="Aff1"><OrgDivision>Laboratoire de Minéralogie et Cristallographie</OrgDivision><OrgName>Université de Nancy I</OrgName><OrgAddress><City>Nancy</City><Country>France</Country></OrgAddress></Affiliation><Affiliation ID="Aff3"><OrgDivision>Laboratoire de Physique des Milieux Ionisés</OrgDivision><OrgName>Université de Nancy I</OrgName><OrgAddress><Country>France</Country></OrgAddress></Affiliation><Affiliation ID="Aff2"><OrgName>Laboratoire de Génie Métallurgique-Ecole des Mines de Nancy</OrgName><OrgAddress><Postcode>54042</Postcode><City>Nancy Cedex</City><Country>France</Country></OrgAddress></Affiliation><Affiliation ID="Aff4"><OrgDivision>Laboratoire de Minéralogie et Cristallographie</OrgDivision><OrgName>Université de Nancy I</OrgName><OrgAddress><Country>France</Country></OrgAddress></Affiliation></AuthorGroup><Abstract ID="Abs1" Language="En"><Heading>Abstract</Heading><Para>The screening constant can be decomposed into a sum of different terms over the different atomic shells. This decomposition visualizes the electron distribution. The energy levels which are calculated by means of these constants agree well with the experimental values for the inner-shells. Our method is therefore complementary to Slater's used for the outer shells.</Para></Abstract></ArticleHeader><NoBody></NoBody></Article></Issue></Volume></Journal></Publisher></istex:document></istex:metadataXml><mods version="3.6"><titleInfo lang="en"><title>Definition and utilization of atomic partial screening constants</title></titleInfo><titleInfo type="alternative" contentType="CDATA"><title>Definition and utilization of atomic partial screening constants</title></titleInfo><name type="personal"><namePart type="given">Tran</namePart><namePart type="given">Huu</namePart><namePart type="family">Loi</namePart><affiliation>Laboratoire de Minéralogie et Cristallographie, Université de Nancy I, Nancy, France</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">Michel</namePart><namePart type="family">Remy</namePart><affiliation>Laboratoire de Physique des Milieux Ionisés, Université de Nancy I, France</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">Michel</namePart><namePart type="family">Gantois</namePart><affiliation>Laboratoire de Génie Métallurgique-Ecole des Mines de Nancy, 54042, Nancy Cedex, France</affiliation><role><roleTerm type="text">author</roleTerm></role></name><name type="personal"><namePart type="given">Claude</namePart><namePart type="family">Zeller</namePart><affiliation>Laboratoire de Minéralogie et Cristallographie, Université de Nancy I, France</affiliation><role><roleTerm type="text">author</roleTerm></role></name><typeOfResource>text</typeOfResource><genre type="research-article" displayLabel="OriginalPaper" authority="ISTEX" authorityURI="https://content-type.data.istex.fr" valueURI="https://content-type.data.istex.fr/ark:/67375/XTP-1JC4F85T-7">research-article</genre><originInfo><publisher>Springer-Verlag</publisher><place><placeTerm type="text">Berlin/Heidelberg</placeTerm></place><dateIssued encoding="w3cdtf">1976-03-01</dateIssued><copyrightDate encoding="w3cdtf">1976</copyrightDate></originInfo><language><languageTerm type="code" authority="rfc3066">en</languageTerm><languageTerm type="code" authority="iso639-2b">eng</languageTerm></language><abstract lang="en">Abstract: The screening constant can be decomposed into a sum of different terms over the different atomic shells. 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