Atomic transition probabilities of MnJ/ApJS/194/35ivo://CDS.VizieR/J/ApJS/194/35doi:10.26093/cds/vizier.21940035CDSDen Hartog E.A.Lawler J.E.Sobeck J.S.Sneden C.Cowan J.J.2011-10-15T17:49:23Z2011-09-22T11:28:50ZCDS support team
CDS, Observatoire de Strasbourg, 11 rue de l'Universite, F-67000 Strasbourg, France
cds-question@unistra.fratomic-physicsThe goal of the present work is to produce transition probabilities with very low uncertainties for a selected set of multiplets of MnI and MnII. Multiplets are chosen based upon their suitability for stellar abundance analysis. We report on new radiative lifetime measurements for 22 levels of MnI from the e^8^D, z^6^P, z^6^D, z^4^F, e^8^S, and e^6^S terms and six levels of MnII from the z^5^P and z^7^P terms using time-resolved laser-induced fluorescence on a slow atom/ion beam. New branching fractions for transitions from these levels, measured using a Fourier-transform spectrometer, are reported.2011ApJS..194...35Dhttps://cdsarc.cds.unistra.fr/viz-bin/cat/J/ApJS/194/35CatalogResearchIsServedByTAP VizieR generic servicerelated-toVI/34 : A Multiplet Table for MnI (Adelman+, 1989)J/A+AS/125/539 : Mn III transition probabilities (Uylings+ 1997)https://cds.unistra.fr/vizier-org/licences_vizier.htmlhttps://vizier.cds.unistra.fr/viz-bin/VizieR-2?-source=J/ApJS/194/35https://vizier.iucaa.in/viz-bin/VizieR-2?-source=J/ApJS/194/35http://vizieridia.saao.ac.za/viz-bin/VizieR-2?-source=J/ApJS/194/35https://vizier.cds.unistra.fr/viz-bin/votable?-source=J/ApJS/194/35https://vizier.iucaa.in/viz-bin/votable?-source=J/ApJS/194/35http://vizieridia.saao.ac.za/viz-bin/votable?-source=J/ApJS/194/35GETtext/xml+votablehttps://tapvizier.cds.unistra.fr/TAPVizieR/tapdefaultJ/ApJS/194/35/table3Recommended Atomic transition probabilities for Mn I (half integral J) & Mn II (integral J) organized by increasing wavelength in airJ0Lower level J valuephys.atmol.qnfloatrecnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintlamAirWavelength in air in Angstroms0.1nmem.wlfloatE1Upper level energycm**-1phys.energy;phys.atmol.leveldoubleP1Upper level parityphys.atmol.parity;phys.atmol.levelcharJ1Upper level J valuephys.atmol.qnfloatE0Lower level energycm**-1phys.energy;phys.atmol.leveldoubleP0Lower level parityphys.atmol.paritycharTranPTransition probability; recommended1e+06s**-1phys.atmol.transProbfloate_TranPTotal uncertainty in TranP1e+06s**-1stat.errorfloatlog(gf)Recommended log of the degeneracy times the oscillator strengthphys.atmol.oscStrengthfloatBWlog(gf)? Log of the degeneracy times the oscillator strength; Blackwell-Whitehead et al. 2005ApJS..157..402Bphys.atmol.oscStrengthfloatnullablee_BWlog(gf)? Total uncertainty in BWlog(gf)stat.errorfloatnullableTElog(gf)Log of the degeneracy times the oscillator strength; this experimentphys.atmol.oscStrengthfloate_TElog(gf)Total uncertainty in TElog(gf)stat.errorfloat
J/ApJS/194/35/table4*Hyperfine structure line component patterns for ^55^MnI (integral F) & ^55^MnII (half integral F)recnoRecord number assigned by the VizieR team. Should Not be used for identification.meta.recordintsigmaCenter-of-Gravity Wavenumber {sigma}cm**-1em.wavenumberdoublelamAirCenter-of-Gravity Air Wavelength in Angstroms0.1nmem.wldoubleF1Component upper level F or total angular momentumphys.atmol.qnfloatF0Component lower level F or total angular momentumphys.atmol.qnfloatdsigmaComponent offset Wavenumber with respect to Center-of-gravity Wavenumbercm**-1stat.fit.omc;phys.energydoubledlamComponent offset Wavelength with respect to Center-of-gravity Wavelength0.1nmem.wl;arith.diffdoubleStrComponent strength (1)spect.line.widthdouble