J/A+AS/144/141ivo://CDS.VizieR/J/A+AS/144/141CDSNahar S.N.Delahaye F.Pradhan A.K.Zeippen C.J.2000-09-23T22:31:35Z2000-09-23T22:31:27ZCDS support team

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

cds-question@unistra.fratomic-physicsAn extensive set of dipole-allowed, intercombination, and forbidden transition probabilities for Fe V is presented. The Breit-Pauli R-matrix (BPRM) method is used to calculate 1.46x10^6^ oscillator strengths for the allowed and intercombination E1 transitions among 3865 fine-structure levels dominated by configuration complexes with n<=10 and l<=9. These data are complemented by an atomic structure configuration interaction (CI) calculation using the SUPERSTRUCTURE program for 362 relativistic quadrupole (E2) and magnetic dipole (M1) transitions among 65 low-lying levels dominated by the 3d^4^ and 3d^3^ 4s configurations. Procedures have been developed for the identification of the large number of fine-structure levels and transitions obtained through the BPRM calculations. The target ion Fe VI is represented by an eigenfunction expansion of 19 fine-structure levels of 3d^3^ and a set of correlation configurations. Fe V bound levels are obtained with angular and spin symmetries SL{pi} and J{pi} of the (e + Fe VI) system such that 2S+1=5, 3, 1, L<=10, J<=8 of even and odd parities. The completeness of the calculated dataset is verified in terms of all possible bound levels belonging to relevant LS terms and transitions in correspondence with the LS terms. The fine-structure averaged relativistic values are compared with previous Opacity Project LS coupling data and other works. The 362 forbidden transition probabilities considerably extend the available data for the E2 and M1 transitions, and are in good agreement with those computed by Garstang for the 3d^4^ transitions.2000A&AS..144..141Nhttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+AS/144/141CatalogResearchIsServedByTAP VizieR generic servicerelated-toJ/A+AS/103/273 : IRON Project II IR collision strengths of C-like ionsJ/A+A/283/319 : IRON Project III B-like ionsJ/A+AS/108/1 : IRON Project V Collision strengths of O-like ionsJ/A+A/293/953 : IRON Project VI Fe II collision strengthsJ/A+A/293/967 : IRON Project VII Fe II radiative transitionsJ/A+AS/109/193 : IRON Project VIII Electron excitation of Ti-like ionsJ/A+AS/119/509 : IRON Project XVII Radiative transition in Fe IIIJ/A+AS/119/523 : IRON Project XVIII Electron impact for Fe IIIJ/A+AS/120/361 : IRON Project XIX Fe II radiative transitionsJ/A+AS/123/159 : IRON Project XXII C and O radiative ratesJ/A+AS/123/575 : IRON Project XXIII Fe XXII excitation rate coefficientsJ/A+AS/126/373 : IRON Project XXVII Fe IV collision strengthsJ/A+AS/131/499 : IRON Project XXIX Boron isoelectronic sequenceJ/A+AS/131/153 : IRON Project XXXI Fe XII electron excitationJ/A+AS/135/347 : IRON Project XXXV Fe XXIV & Fe XXV oscillator strengthsJ/A+AS/136/395 : IRON Project XXXVII Fe VI collision strengthsJ/A+AS/137/165 : IRON Project XXXVIII Fe XV fine-structure transitionsJ/A+AS/143/483 : IRON Project XLII Fe XXI electron impact excitationJ/A+AS/147/111 : IRON Project XLIV Fe VI trans. prob. & line ratioJ/A+AS/147/253 : IRON Project XLV Ar XIII, Fe XXI trans. probabilitiesJ/A+A/365/268 : IRON Project XLVII Ni III electron impact excitationJ/A+A/372/1078 : IRON Project XLIX Fe XX electron impact excitationJ/A+A/372/1083 : IRON Project L Fe XIX electron impact excitationJ/A+A/394/753 : IRON Project LI Fe IX electron impact excitationJ/A+A/408/789 : IRON Project LIII Fe XVII transition probabilitiesJ/A+A/413/779 : IRON Project LIV Fe XX transition probabilitiesJ/A+A/420/763 : IRON Project LV Ni II electron impact excitationJ/A+A/437/345 : IRON Project LIX Fe IV transition probabilitiJ/A+A/448/779 : IRON Project LXI Fe IV radiative transitionsJ/A+A/457/721 : IRON Project LXII Fe XVIII allowed and forbidden trans.J/A+A/466/763 : IRON Project LXIII Fe^19+^ electron impact excitationhttps://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/A+AS/144/141https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/A+AS/144/141http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/A+AS/144/141https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/A+AS/144/141https://vizier.iucaa.in/viz-bin/votable?-source=J/A+AS/144/141http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/A+AS/144/141GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/A+AS/144/141/table1aIdentified fine-structure energy levels of Fe Vii levelphys.atmol.levelintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintNlvTotal number of symmetry J{pi} (1)phys.atmol.levelintJPJ value (o: odd, e: even)phys.atmol.qncharCtt configuration (2)phys.atmol.configurationcharStLtPtt core level (2)phys.atmol.configurationcharJtJ value at t (2)phys.atmol.qncharnlPrincipal and orbital quantum numbers of the outer electronphys.atmol.qncharJJ valuephys.atmol.qnintEEnergyRyphys.energy;phys.atmol.leveldoubleEQN? Effective Quantum Number (3)phys.atmol.qnfloatnullableTermsPossible LS terms of the energy levelphys.atmol.qncharJ/A+AS/144/141/table5aTable of oscillator strengths where observed energies are usedff valuephys.atmol.leveldoublerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintCiInitial configuration (1)phys.atmol.configurationcharCjFinal configurationphys.atmol.configurationcharSiLiPiInitial core levelphys.atmol.configurationcharSjLjPjFinal core levelphys.atmol.configurationchar2Ji+12Ji+1 valuephys.atmol.qnintIi? Energy level index of 2Ji+1phys.atmol.qnintnullable2Jj+12Jj+1 valuephys.atmol.qnintIj? Energy level index of 2Jj+1phys.atmol.qnintnullableEiInitial energyRyphys.energy;phys.atmol.levelfloatEjFinal energyRyphys.energy;phys.atmol.levelfloatAA values**-1phys.atmol.transProbdoubleJ/A+AS/144/141/table5bTable of oscillator strengths from table5a.dat, but ordered in energy and grouped according to components of LS multipletsrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintCiInitial configuration (1)phys.atmol.configurationcharCjFinal configurationphys.atmol.configurationcharSiLiPiInitial core levelphys.atmol.configurationcharSjLjPjFinal core levelphys.atmol.configurationchar2Ji+12Ji+1 valuephys.atmol.qnintIi? Energy level index of 2Ji+1phys.atmol.qnintnullable2Jj+12Jj+1 valuephys.atmol.qnintIj? Energy level index of 2Jj+1phys.atmol.qnintnullableEiInitial energyRyphys.energy;phys.atmol.levelfloatEjFinal energyRyphys.energy;phys.atmol.levelfloatff valuephys.atmol.leveldoubleAA values**-1phys.atmol.transProbdoubleJ/A+AS/144/141/table7The Complete dataset of forbidden transition probabilities (M1 and E2) for Fe V among the levels of 3d^4^ and 3d^3^4srecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintCiInitial configurationphys.atmol.configurationcharCjFinal configurationphys.atmol.configurationcharSiLiPiInitial core levelphys.atmol.configurationcharSjLjPjFinal core levelphys.atmol.configurationcharJiInitial J valuephys.atmol.qnintJjFinal J valuephys.atmol.qnintLvacWavelength in vacuum0.1nmem.wl;phys.atmol.transitiondoubleEiInitial energycm**-1phys.energy;phys.atmol.leveldoubleEjFinal energycm**-1phys.energy;phys.atmol.leveldoubleAM1jiForbidden M1 transition probabilitys**-1phys.atmol.transProbdoubleAE2jiForbidden E2 transition probabilitys**-1phys.atmol.transProbdouble