J/ApJS/207/20ivo://CDS.VizieR/J/ApJS/207/20doi:10.26093/cds/vizier.22070020CDSRuffoni M.P.Pickering J.C.2017-07-11T13:08:57Z2013-09-25T09:35:08ZCDS support team

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

cds-question@unistra.fratomic-physicsspectroscopyWe report a comprehensive list of accurate Ritz wavelengths for parity-forbidden [Co II] and [V II] lines obtained from the analysis of energy levels measured in the laboratory with Fourier transform emission spectroscopy. Such lines, particularly those in the infrared, are in demand for the analysis of low-density astrophysical plasmas in and around objects such as planetary nebulae, star-forming regions, and active galactic nuclei. Transitions between all known metastable levels of Co II and V II are included in our analysis, producing wavelengths for 1477 [V II] lines and 782 [Co II] lines. Of these, 170 [V II] lines and 171 [Co II] lines arise from transitions with calculated transition probabilities greater than 1x10^-2^/s and upper level excitations of less than 5 eV, and thus are likely to be observed in astrophysical spectra.2013ApJS..207...20Rhttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJS/207/20CatalogResearchIsServedByTAP VizieR generic servicerelated-toJ/ApJS/207/13 : The spectrum and term analysis of V II (Thorne+, 2013)J/A+AS/130/541 : Co II oscillator strengths (Raassen+ 1998)J/A+AS/129/147 : Co II radiative transition probabilities (Quinet 1998)https://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/ApJS/207/20https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/ApJS/207/20http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/ApJS/207/20https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/ApJS/207/20https://vizier.iucaa.in/viz-bin/votable?-source=J/ApJS/207/20http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/ApJS/207/20GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapOpticaldefaultJ/ApJS/207/20/V-IICombined table from original tablessigma[4/44200] Wavenumbercm**-1em.freqdoublerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintExSimbad column added by the CDSmeta.notechare_sigmaUncertainty in sigmacm**-1stat.errorfloatsig.0Vacuum wavelength; Angstroms0.1nmem.freqdoublee_sig.0Uncertainty in sig.00.1nmstat.errordoublesig.1Air wavelength; Angstroms (1)0.1nmem.freqdoubleTr0Lower level transitionphys.atmol.transitionTr1Upper level transitionphys.atmol.transitionE0Lower level energy (2)cm**-1phys.energy;phys.atmol.levelintE1Upper level energy (2)cm**-1phys.energy;phys.atmol.levelintA? Transition probability (3)s**-1phys.atmol.transProbdoublenullableTypeTransition type (E1, E2, M1) (5)meta.notecharJ/ApJS/207/20/CoIICombined table from original tablesrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintExSimbad column added by the CDSmeta.notecharsigma[4/44200] Wavenumbercm**-1em.freqdoublee_sigmaUncertainty in sigmacm**-1stat.errorfloatsig.0Vacuum wavelength; Angstroms0.1nmem.freqdoublee_sig.0Uncertainty in sig.00.1nmstat.errordoublesig.1Air wavelength; Angstroms (1)0.1nmem.freqdoubleTr0Lower level transitionphys.atmol.transitionTr1Upper level transitionphys.atmol.transitionE0Lower level energy (2)cm**-1phys.energy;phys.atmol.levelintE1Upper level energy (2)cm**-1phys.energy;phys.atmol.levelintA? Transition probability (3)s**-1phys.atmol.transProbdoublenullablef_AFlag on A (4)meta.codecharTypeTransition type (E1, E2, M1) (5)meta.notechar