VI/136ivo://CDS.VizieR/VI/136CDSSochi T.Storey P.J.2014-02-23T12:53:41Z2013-08-06T07:59:17ZCDS support team

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

cds-question@unistra.fratomic-physicsA computed list of transition lines for the atomic ion C^+^ is generated using R-matrix [1], Autostructure [2] and Emissivity [3] codes. These lines are produced by dielectronic recombination and subsequent cascade decays of the low-lying autoionizing states above the threshold of C^2+1^S^e^ with a principal quantum number n<5 for the captured electron. The line list contains 6187 optically-allowed transitions which include many C II lines observed in the astronomical spectra [4]. Beside the transition lines, the data also include level energies for the bound and resonance states, radiative transition probabilities, recombination rate coefficients, and oscillator strengths. A 26-term C^2+^ atomic target was used within an intermediate coupling scheme in the production of these data. The theoretical results for energy and fine structure splitting agree very well with the available experimental data for both resonances and bound states. The data were also validated by comparison to theoretical data previously reported in the literature which include radiative transition probabilities, effective dielectronic recombination rate coefficients and autoionization probabilities.2013yCat.6136....0Shttps://cdsarc.cds.unistra.fr/viz-bin/cat/VI/136CatalogResearchIsServedByTAP VizieR generic servicerelated-toVI/119 : High accuracy computed water line list - BT2 (Barber+, 2006)VI/130 : High accuracy computed H2D+ line list - ST1 (Sochi+, 2010)https://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=VI/136https://vizier.iucaa.in/viz-bin/VizieR-2?-source=VI/136http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=VI/136https://vizier.cds.unistra.fr/viz-bin/votable?-source=VI/136https://vizier.iucaa.in/viz-bin/votable?-source=VI/136http://vizieridia.saao.ac.za/viz-bin/votable?-source=VI/136GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultVI/136/transRecombination coefficientsConf1Lower level Configuration termphys.atmol.configurationcharRC3.9Recombination coefficient at logT=3.9m**3.s**-1arith.rate;phys.atmol.transitiondoublerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintIndex[1/6187] Indexmeta.idintStatStatus (FF, FB or BB transition where "F" stands for Free and "B" for Bound)instr.setupcharExp[00/11] Experimental state of the energy data of the upper and lower levels ('0' for theoretical data and '1' for experimental: 00, 01, 10 or 11)phys.energyint2J1[1/11] Lower level 2J valuephys.atmol.qnintP1[0/1] Lower level parityphys.atmol.parity;phys.atmol.levelintConf2Upper level Config Term 2J termphys.atmol.term;phys.atmol.levelchar2J2[1/11] Upper level 2J valuephys.atmol.qnintP2[0/1] Upper level parityphys.atmol.parity;phys.atmol.levelintlam.v[450/5.4e+7] Wavelength in vacuum0.1nmem.wl;phys.atmol.transitiondoublelam.a[2000/5.4e+7]? Wavelength in air (only for {lambda}>200nm)0.1nmem.wl;phys.atmol.transitiondoublenullableGammaRadiative transition probability, Gamma^r^_ul_s**-1phys.atmol.transProbdoubleRC2.0Recombination coefficient at logT=2.0m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.1Recombination coefficient at logT=2.1m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.2Recombination coefficient at logT=2.2m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.3Recombination coefficient at logT=2.3m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.4Recombination coefficient at logT=2.4m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.5Recombination coefficient at logT=2.5m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.6Recombination coefficient at logT=2.6m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.7Recombination coefficient at logT=2.7m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.8Recombination coefficient at logT=2.8m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC2.9Recombination coefficient at logT=2.9m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.0Recombination coefficient at logT=3.0m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.1Recombination coefficient at logT=3.1m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.2Recombination coefficient at logT=3.2m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.3Recombination coefficient at logT=3.3m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.4Recombination coefficient at logT=3.4m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.5Recombination coefficient at logT=3.5m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.6Recombination coefficient at logT=3.6m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.7Recombination coefficient at logT=3.7m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC3.8Recombination coefficient at logT=3.8m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC4.0Recombination coefficient at logT=4.0m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC4.1Recombination coefficient at logT=4.1m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC4.2Recombination coefficient at logT=4.2m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC4.3Recombination coefficient at logT=4.3m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC4.4Recombination coefficient at logT=4.4m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC4.5Recombination coefficient at logT=4.5m**3.s**-1arith.rate;phys.atmol.transitiondoubleRC4.6Recombination coefficient at logT=4.6m**3.s**-1arith.rate;phys.atmol.transitiondouble