J/ApJ/855/21ivo://CDS.VizieR/J/ApJ/855/21doi:10.26093/cds/vizier.18550021CDSHodges J.N.Bittner D.M.Bernath P.F.2020-03-26T14:17:48Z2019-01-04T07:23:24ZCDS support team

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

cds-question@unistra.fratomic-physicsmolecular-physicsMolecular ions are key reaction intermediates in the interstellar medium. OH+ plays a central role in the formation of more complex chemical species and for estimating the cosmic ray ionization rate in astrophysical environments. Here, we use a recent analysis of a laboratory spectrum in conjunction with ab initio methods to calculate infrared and ultraviolet oscillator strengths. These new oscillator strengths include branch dependent intensity corrections, arising from the Herman-Wallis effect, that have not been included before. We estimate 10% total uncertainty in the UV and 6% total uncertainty in the IR for the oscillator strengths.2018ApJ...855...21Hhttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJ/855/21CatalogResearchIsServedByTAP VizieR generic servicerelated-toJ/ApJS/216/22 : 3060-3700{AA} spectra analysis of early-type starsJ/ApJ/840/81 : A^3^{Pi}-X^3^{Sigma}^-^ transitions of OH+ (Hodges+, 2017)https://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/ApJ/855/21https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/ApJ/855/21http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/ApJ/855/21https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/ApJ/855/21https://vizier.iucaa.in/viz-bin/votable?-source=J/ApJ/855/21http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/ApJ/855/21GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/ApJ/855/21/table2Dipole moments for the X-X and A-X transitions as a function of bond lengthrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintLength[0.7/2.2] Bond length in Angstrom0.1nmphys.atmolfloatXXDipole[1.6/5.3] Dipole moment for X-X transitions in DebyeDphys.mol.dipolefloatAXDipole[-0.6/0.08]? Dipole moment for A-X transitions in DebyeDphys.mol.dipolefloatnullableJ/ApJ/855/21/table3A portion of the linelist with positions, oscillator strengths, lower state energy, and Einstein A coefficentsEta0[X] Lower electronic statephys.energy;phys.atmol.levelcharv0Lower vibrational quantum number ("v=0" to "v=4")phys.mol.qncharJ0[0/30] Lower J quantum numberinstr.det.qe;stat.minintN0[0/31] Lower N quantum numberphys.atmol.qnintrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintEta1[AX] Upper electronic statephys.energy;phys.atmol.levelcharv1Upper vibrational quantum number ("v=0" to "v=4")phys.mol.qncharJ1[0/30] Upper J quantum numberinstr.det.qe;stat.maxintN1[0/31] Upper N quantum numberphys.atmol.qnintFn1e/fUpper F quantum number and parityphys.atmol.qncharFn0e/fLower F quantum number and parityphys.atmol.qncharBranchRovibrational branch labelmeta.id;phys.atmol.transitioncharWaveNum[9.5/30373.3] Line position in wavenumbercm**-1em.freqdoublelambda[3291.4/1.1e+07] Line position in wavelength (1)0.1nmem.wl;phys.atmol.transitiondoublef[1.6e-18/0.0011] Oscillator strengthphys.atmol.oscStrengthdoubleElo[-0.05/22862] Lower state energycm**-1phys.energy;phys.atmol.leveldoubleAEinstein A coefficients**-1phys.atmol.transProbchar