J/A+A/618/A141ivo://CDS.VizieR/J/A+A/618/A141doi:10.26093/cds/vizier.36180141CDSEzzeddine R.Merle T.Plez B.Gebran M.Thevenin F.Van der Swaelmen M.2018-11-05T10:52:51Z2018-10-22T07:45:36ZCDS support team

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

cds-question@unistra.fratomic-physicsDetermination of high-precision abundances of late-type stars has been and always will be an important goal of spectroscopic studies, which requires accurate modeling of their stellar spectra with non-local thermodynamic equilibrium (NLTE) radiative transfer methods. This entails using up-to-date atomic data of the elements under study, which are still subject to large uncertainties. We investigate the role of hydrogen collisions in NLTE spectral line synthesis, and introduce a new general empirical recipe to determine inelastic charge transfer (CT) and bound-bound hydrogen collisional rates. This recipe is based on fitting the energy functional dependence of published quantum collisional rate coefficients of several neutral elements (BeI, NaI, MgI, AlI, SiI and CaI) using simple polynomial equations. We perform thorough NLTE abundance calculation tests using our method for four different atoms, Na, Mg, Al and Si, for a broad range of stellar parameters. We then compare the results to calculations computed using the published quantum rates for all the corresponding elements. We also compare to results computed using excitation collisional rates via the commonly used Drawin equation for different fudge factors, SH, applied. We demonstrate that our proposed method is able to reproduce the NLTE abundance corrections performed with the quantum rates for different spectral types and metallicities for representative NaI and AlI lines to within 0.05dex and 0.03dex, respectively. For MgI and SiI lines, the method performs better for the cool giants and dwarfs, while larger discrepancies up to 0.20dex could be obtained for some lines for the subgiants and warm dwarfs. We obtained larger NLTE correction differences between models incorporating Drawin rates relative to the quantum models by up to 0.40dex. These large discrepancies are potentially due to ignoring either or both CT and ionization collisional processes by hydrogen in our Drawin models.Our general empirical fitting method (EFM) for estimating hydrogen collision rates performs well in its ability to reproduce, within narrow uncertainties, the abundance corrections computed with models incorporating quantum collisional rates. It performs generally best for the cool and warm dwarfs, with slightly larger discrepancies obtained for the giants and subgiants. It could possibly be extended in the future to transitions of the same elements for which quantum calculations do not exist, or, in the absence of published quantum calculations, to other elements as well.2018A&A...618A.141Ehttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/A+A/618/A141CatalogResearchIsServedByTAP VizieR generic servicehttps://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/A+A/618/A141https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/A+A/618/A141http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/A+A/618/A141https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/A+A/618/A141https://vizier.iucaa.in/viz-bin/votable?-source=J/A+A/618/A141http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/A+A/618/A141GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/A+A/618/A141/tablea1NLTE corrections obtained for NaI, MgI, AlI and SiI at [Fe/H]=+0.0 and [Fe/H]=-1.0 for Teff=4500 and logg=2.5, logg=3.5 and logg=4.5recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTeffEffective TemperatureKphys.temperature.effectiveintloggSurface Gravitylog(cm.s**-2)phys.gravityfloat[Fe/H]Metallicityphys.abund.ZfloatElElemental Speciesphys.atmol.elementcharlamWavelengthnmem.wldoubleDel(QM)NLTE abundance correction using QMarith.factorfloatDel(EFM)NLTE abundance correction using EFMarith.factorfloatDel(DRW-0.1)NLTE abundance correction using DRW,SH=0.1arith.factorfloatDel(DRW-1.0)NLTE abundance correction using DRW,SH=1.0arith.factorfloatDel(DRW-0.002)? NLTE abundance correction using DRW,SH=0.002arith.factorfloatnullableJ/A+A/618/A141/tablea2NLTE corrections obtained for NaI, MgI, AlI and SiI at [Fe/H]=+0.0 and [Fe/H]=-1.0 for Teff=5500 and logg=3.5 and logg=4.5 and for Teff=6500 and logg=4.5recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTeffEffective TemperatureKphys.temperature.effectiveintloggSurface Gravitylog(cm.s**-2)phys.gravityfloat[Fe/H]Metallicityphys.abund.ZfloatElElemental Speciesphys.atmol.elementcharlamWavelengthnmem.wldoubleDel(QM)NLTE abundance correction using QMarith.factorfloatDel(EFM)NLTE abundance correction using EFMarith.factorfloatDel(DRW-0.1)NLTE abundance correction using DRW,SH=0.1arith.factorfloatDel(DRW-1.0)NLTE abundance correction using DRW,SH=1.0arith.factorfloatDel(DRW-0.002)? NLTE abundance correction using DRW,SH=0.002arith.factorfloatnullableJ/A+A/618/A141/tablea3NLTE corrections obtained for NaI, MgI, AlI and SiI at [Fe/H]=-2.0 and [Fe/H]=-3.0 for Teff=4500 and logg=2.5, logg=3.5 and logg=4.5recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTeffEffective TemperatureKphys.temperature.effectiveintloggSurface Gravitylog(cm.s**-2)phys.gravityfloat[Fe/H]Metallicityphys.abund.ZfloatElElemental Speciesphys.atmol.elementcharlamWavelengthnmem.wldoubleDel(QM)NLTE abundance correction using QMarith.factorfloatDel(EFM)NLTE abundance correction using EFMarith.factorfloatDel(DRW-0.1)NLTE abundance correction using DRW,SH=0.1arith.factorfloatDel(DRW-1.0)NLTE abundance correction using DRW,SH=1.0arith.factorfloatDel(DRW-0.002)? NLTE abundance correction using DRW,SH=0.002arith.factorfloatnullableJ/A+A/618/A141/tablea4NLTE corrections obtained for NaI, MgI, AlI and SiI at [Fe/H]=-2.0 and [Fe/H]=-3.0 for Teff=5500 and logg=3.5 and logg=4.5 and for Teff=6500 and logg=4.5recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintTeffEffective TemperatureKphys.temperature.effectiveintloggSurface Gravitylog(cm.s**-2)phys.gravityfloat[Fe/H]Metallicityphys.abund.ZfloatElElemental Speciesphys.atmol.elementcharlamWavelengthnmem.wldoubleDel(QM)NLTE abundance correction using QMarith.factorfloatDel(EFM)NLTE abundance correction using EFMarith.factorfloatDel(DRW-0.1)NLTE abundance correction using DRW,SH=0.1arith.factorfloatDel(DRW-1.0)NLTE abundance correction using DRW,SH=1.0arith.factorfloatDel(DRW-0.002)? NLTE abundance correction using DRW,SH=0.002arith.factorfloatnullable