J/A+A/426/717ivo://CDS.VizieR/J/A+A/426/717doi:10.26093/cds/vizier.34260717CDSTayal S.S.2004-12-26T21:23:51Z2004-12-26T22:23:43ZCDS support team

CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France

cds-question@unistra.fratomic-physicsNon-orthogonal orbitals technique in the multiconfiguration Hartree-Fock approach is used to calculate oscillator strengths and transition probabilities for allowed and intercombination lines in Cl II. The relativistic corrections are included through the Breit-Pauli Hamiltonian. The Cl II wave functions show strong term dependence. The non-orthogonal orbitals are used to describe the term dependence of radial functions. Large sets of spectroscopic and correlation functions are chosen to describe adequately strong interactions in the 3s^2^ 3p^3^nl ^3^P^o^, ^1^P^o^ and ^3^D^o^ Rydberg series and to properly account for the important correlation and relaxation effects. The length and velocity forms of oscillator strength show good agreement for most transitions.2004A&A...426..717Thttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/426/717CatalogResearchIsServedByTAP VizieR generic servicerelated-toJ/A+A/418/363 : Effective collision strengths for Cl II (Tayal+, 2004)https://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/A+A/426/717https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/A+A/426/717http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/A+A/426/717https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/A+A/426/717https://vizier.iucaa.in/viz-bin/votable?-source=J/A+A/426/717http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/A+A/426/717GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/A+A/426/717/table1Comparison of calculated excitation energies (au) with measured valuesrecnoRecord number assigned by the VizieR team. Should Not be used for identification.intTransTransitionJJ valueintEexcPPresent value of excitation energyRydoubleEexcM? Measured value of excitation energyRydoublenullableDiff? Difference between present and measured valuesRyfloatnullableJ/A+A/426/717/table2The length and velocity values of oscillator strengths and length value of transition probability for allowed transitionsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.intTransTransitionJJ levelintJ'J' levelintlambdaWavelength0.1nmdoublefLospresent length value of oscillator strengthdoublefVospresent velocity value of oscillator strengthdoubleALPresent length value of transition probabilitys**-1doublefLosD? Length oscillator strength of Deb et al. (2003)doublenullablefVosD? Velocity oscillator strength of Deb et al. (2003)doublenullableJ/A+A/426/717/table3The length and velocity values of oscillator strengths and length value of transition probability for allowed transitionsTransTransitionrecnoRecord number assigned by the VizieR team. Should Not be used for identification.intJJ levelintJ'J' levelintlambdaWavelength0.1nmdoublefLospresent length value of oscillator strengthdoublefVospresent velocity value of oscillator strengthdoubleALPresent length value of transition probabilitys**-1doublefLosD? Length oscillator strength of Deb et al. (2003)doublenullablefVosD? Velocity oscillator strength of Deb et al. (2003)doublenullableJ/A+A/426/717/table4The length and velocity values of oscillator strengths and length value of transition probability for intercombination transitionsJJ levelintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.intTransTransitionJ'J' levelintlambda? Wavelength0.1nmdoublenullablefLospresent length value of oscillator strengthdoublefVospresent velocity value of oscillator strengthdoubleALPresent length value of transition probabilitys**-1double