J/MNRAS/462/1203ivo://CDS.VizieR/J/MNRAS/462/1203doi:10.26093/cds/vizier.74621203CDSShen X.Liu J.Zhou F.2024-08-16T20:18:06Z2016-11-02T08:50:56ZCDS support team

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

cds-question@unistra.fratomic-physicsWavefunctions were determined using the Multi-Configuration Dirac-Hartree-Fock (MCDHF) method. The core-core, core-valence, valence correlation, Breit interaction and quantum electrodynamics (QED) effects, as well as some higher order correlation effects, were considered to obtain accurate wavelengths (lambda), oscillator strengths (gf) and transition rates (A) of 2s^2^2p^2^-2s2p^3^, 2s2p^3^-2s^2^2pnl (n>=3) and 2s2p^3^-2s2p^2^3s E1 transitions.2016MNRAS.462.1203Shttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/MNRAS/462/1203CatalogResearchIsServedByTAP VizieR generic servicehttps://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/MNRAS/462/1203https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/MNRAS/462/1203http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/MNRAS/462/1203https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/MNRAS/462/1203https://vizier.iucaa.in/viz-bin/votable?-source=J/MNRAS/462/1203http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/MNRAS/462/1203GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/MNRAS/462/1203/tablea1Wavelengths, line strengths, oscillator strengths and transition rates of 2s^2^2p^2^-2s2p^3^, 2s2p^3^-2s^2^2pnl (n>=3) and 2s2p^3^-2s2p^2^3s E1 transitions in N^+^SLine strengthspect.line.intensitydoublerecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTransTransitionmeta.id;phys.atmol.transitionLowerLower statemeta.id;phys.atmol.transitionUpperUpper statemeta.id;phys.atmol.transitionlambdaCCalculated wavelength0.1nmem.wl;phys.atmol.transitiondoublelambdaOObserved wavelength0.1nmem.wl;phys.atmol.transitiondoublexsiPercentage uncertainty on lambdaC and lambdaO%stat.errorfloatType[E1] Transition (E1)meta.id;phys.atmol.transitionchargfOscillator strengthphys.atmol.oscStrengthdoubleATransition rates in this works**-1phys.atmol.transProb;phys.atmol.transitiondoubleAa? Transition rates cited from Fischer & Tachiev (2004, At. Data Nucl. Data Tables, 87, 1)s**-1phys.atmol.transProb;phys.atmol.transitiondoublenullableAb? Transition rates cited from Bell et al. (1995, Phys. Scr., 52, 240)s**-1phys.atmol.transProb;phys.atmol.transitiondoublenullableAc? Transition rates cited from Jonsson & Bieron (2010, At. Mol. Opt. Phys., 43, 074023)s**-1phys.atmol.transProb;phys.atmol.transitiondoublenullableAd? Transition rates cited from Mar et al. (2000A&AS..144..509M)s**-1phys.atmol.transProb;phys.atmol.transitiondoublenullableJ/MNRAS/462/1203/tablea2Adjusted transition rates by NIST wavelengthsxsiPercentage uncertainty on lambdaC and lambdaO%stat.errorfloatrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTransTransitionmeta.id;phys.atmol.transitionLowerLower statesmeta.id;phys.atmol.transitionUpperUpper statesmeta.id;phys.atmol.transitionlambdaCCalculated wavelength0.1nmem.wl;phys.atmol.transitiondoublelambdaOObserved wavelength0.1nmem.wl;phys.atmol.transitiondoubleType[E1] Transition (E1)meta.id;phys.atmol.transitioncharATransition rate in this workarith.rate;phys.atmol.transProb;phys.atmol.transitiondoubleAdjAdjusted transition rates**-1phys.atmol.transProbdoubleAa? Transition rate cited from Fischer & Tachievs**-1phys.atmol.transProbdoublenullableAb? Transition rate cited from Bell et al. (1995, Phys. Scr., 52, 240)s**-1phys.atmol.transProbdoublenullableAc? Transition rate cited from Mar et al. (2000A&AS..144..509M)s**-1phys.atmol.transProbdoublenullable