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WWeesstteerrnn UUnniivveerrssiittyy SScchhoollaarrsshhiipp@@WWeesstteerrnn Electronic Thesis and Dissertation Repository 10-21-2015 12:00 AM NNiittrrooggeenn AAbbuunnddaanncceess iinn EEaarrllyy--TTyyppee BBee SSttaarrss Ahmed Ahmed, The University of Western Ontario Supervisor: Dr. T.A.A. Sigut, The University of Western Ontario A thesis submitted in partial fulfillment of the requirements for the Doctor of Philosophy degree in Astronomy © Ahmed Ahmed 2015 Follow this and additional works at: https://ir.lib.uwo.ca/etd Part of the Stars, Interstellar Medium and the Galaxy Commons RReeccoommmmeennddeedd CCiittaattiioonn Ahmed, Ahmed, "Nitrogen Abundances in Early-Type Be Stars" (2015). Electronic Thesis and Dissertation Repository. 3354. https://ir.lib.uwo.ca/etd/3354 This Dissertation/Thesis is brought to you for free and open access by Scholarship@Western. It has been accepted for inclusion in Electronic Thesis and Dissertation Repository by an authorized administrator of Scholarship@Western. For more information, please contact [email protected]. NITROGEN ABUNDANCES IN EARLY-TYPE BE STARS (Thesis format: Monograph) by Ahmed Ahmed Graduate Program in Astronomy A thesis submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy The School of Graduate and Postdoctoral Studies The University of Western Ontario London, Ontario, Canada (cid:13)c Ahmed M. H. Ahmed 2015 Abstract A sample of 26 Be stars from the Magnetism in Massive Stars (MiMeS) spectroscopic surveyareanalyzedfortheirphotosphericnitrogenabundancesinanefforttodetectrotational mixing in the Be stars. Be stars are massive stars, between 3 and 20 times the mass of the Sun, that are surrounded by a thin, equatorial disk of gas that produces emission lines in their optical and near-infrared spectra. Be stars are the most rapidly-rotating stellar population on the main sequence, where stars produce energy by core hydrogen burning. New, non-LTE line transfer calculations are performed for the Nii ion, the dominant ionization stage in the photospheres of the B stars, and an extensive error analysis is performed via Monte Carlo simulation to determine the achievable accuracy of nitrogen abundances among these stars. To analyze the measured Nii equivalent widths from the MiMeS survey, the effects of both gravitational darkening, due to the rapid rotation of the central B star, and the veiling effect of emission from the Be star circumstellar disk are considered. Both of these effects are found to be small for the sample population, affecting the final nitrogen abundances at the level ≈ ±0.1 dex. The final, average nitrogen abundance for the MiMeS sample, AMiMeS = 7.78, N hasavalueingoodagreementwiththesolarabundance, A◦ = 7.83,andrecent,high-precision N abundancemeasurementsformainsequenceBstars. Nevertheless,theMiMeSsamplestandard deviation is over a factor of two larger than that of the observed nitrogen abundances in the atmospheres of B stars in the solar neighbourhood, with many low abundance objects and a few high abundance objects. No discernible trend of the nitrogen abundance can be seen with stellar gravity, logg (as a proxy for stellar age), or stellar equatorial velocity in the MiMeS survey. It is suggested that possible disk emission in the Nii line transitions may explain the lowerabundanceobjects,andthiswillbethesubjectoffuturework. Keywords: stars: abundances-stars: atmospheres-stars: rotation-radiativetransfer-line: formation ii Acknowlegements IwouldtolikeexpressmysinceregratitudetomysupervisorAaronSigutforhisexpertiseand patience. Also,IwouldliketothankmyadvisorycommitteemembersMartinHoudeandJohn D. Landstreet for their continuous support and suggestions. Finally, I would like to thank my examiners for their helpful comments and suggestions, Drs Gregg Wade, Jan Cami, John D. Landstreet,andPaulRagogna. iii Contents Abstract ii Acknowlegements iii ListofFigures vii ListofTables xii ListofAppendices xv 1 IntroductionandOverview 1 2 Early-TypeStars 5 2.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 5 2.2 PhysicalCharacteristicsofMassiveStars . . . . . . . . . . . . . . . . . . . . . 6 2.3 SurfaceAbundancesofB-typestars . . . . . . . . . . . . . . . . . . . . . . . 6 2.4 EvolutionofMassiveStarsonTheMainSequence . . . . . . . . . . . . . . . 9 2.4.1 EffectsofRotationonMassiveStarEvolution ontheMain-Sequence . . 11 RotationalMixing . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 11 ModellingResults . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 2.4.2 ObservationalConstraintsonRotationalMixinginMassivestars . . . . 22 3 TheClassicalBestars 28 3.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28 3.2 SpectralfeaturesofBeStars . . . . . . . . . . . . . . . . . . . . . . . . . . . 30 3.3 PossibleFormation MechanismsofBeStarDisks . . . . . . . . . . . . . . . . 33 3.4 Diskstructure . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 34 3.5 BeStarsandRotational Mixing . . . . . . . . . . . . . . . . . . . . . . . . . . 36 4 TheNon-LTERadiativeTransferProblem 37 4.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37 4.2 TheRadiativeTransferEquation . . . . . . . . . . . . . . . . . . . . . . . . . 38 4.2.1 LocalThermodynamic Equilibrium . . . . . . . . . . . . . . . . . . . 41 4.2.2 non-LocalThermodynamic Equilibrium . . . . . . . . . . . . . . . . . 42 4.2.3 NumericalSolutionofTheNon-LTERadiativeTransferProblem . . . . 42 5 Non-LTEforCalculation N ii 45 iv 5.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45 5.2 PreviousWorks . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 46 5.3 NitrogenAtomicData . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 49 5.3.1 Nii . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 49 5.3.2 Niii andNiv . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 56 5.4 Calculations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 56 5.4.1 IonizationBalancesandDepartureCoefficients . . . . . . . . . . . . . 57 5.4.2 EquivalentWidths . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 61 5.5 Multi-multi Analysis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71 5.6 TheAccuracyofthePredictednon-LTEEquivalentWidths . . . . . . . . . . . 77 5.6.1 RandomErrors . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 77 5.6.2 SystematicErrors . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 81 6 Non-LTECalculation forHe i 87 6.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 87 6.2 Previousworks . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 88 6.3 HeiAtomic data . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 92 6.4 CalculationGridofHeiAtom . . . . . . . . . . . . . . . . . . . . . . . . . . 97 6.4.1 IonizationBalancesandDepartureCoefficients . . . . . . . . . . . . . 97 6.4.2 EquivalentWidths . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 99 6.5 TheAccuracyofthePredictednon-LTEEquivalentWidths . . . . . . . . . . . 106 7 Gravitational Darkening 108 7.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 108 7.2 Gravitational DarkeningAssumingSolidBodyRotation . . . . . . . . . . . . . 108 7.3 Gravitational DarkeningEffectsonSpectralLines . . . . . . . . . . . . . . . . 113 7.3.1 Gravitational DarkeningEffectsonNiiλ3995Å . . . . . . . . . . . . . 114 7.3.2 Gravitational DarkeningeffectsonHeiλ6678Å . . . . . . . . . . . . 117 7.3.3 Gravitational DarkeningeffectsonMgiiλ4481Å . . . . . . . . . . . . 118 7.3.4 Gravitational DarkeningEffectsonv siniMeasurements . . . . . . . . 119 8 NitrogenAbundancesforaSampleofBeStarsfromtheMiMeSSurvey 122 8.1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 122 8.2 TheBestarSample . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 123 8.2.1 SpectraNormalization . . . . . . . . . . . . . . . . . . . . . . . . . . 123 8.2.2 StellarParameters . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 134 8.2.3 EquivalentWidthMeasurements . . . . . . . . . . . . . . . . . . . . . 146 8.3 EstimationsofDiskParameters . . . . . . . . . . . . . . . . . . . . . . . . . . 151 8.4 NitrogenAbundances . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 159 8.4.1 Estimations of Nitrogen Abundances Based Solely on the Observed EquivalentWidths . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 159 8.4.2 Corrections for Circumstellar Disks Effects on the Measured Nitrogen Abundances . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 167 8.5 Discussion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 174 v 9 Conclusions 175 9.1 ResultsofNon-LTEcalculations . . . . . . . . . . . . . . . . . . . . . . . . . 175 9.2 Gravitational DarkeningEffects . . . . . . . . . . . . . . . . . . . . . . . . . . 176 9.3 ResultsoftheAbundanceAnalysis . . . . . . . . . . . . . . . . . . . . . . . . 177 9.4 FutureDirections . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 178 Bibliography 179 A ListofConstantsandAbbreviations 187 A.1 Constants . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 187 A.2 Abbreviations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 187 B multiResultsofSelectedNiilines 188 C MonteCarloResults 218 D HαFittingFigures 234 E NiiNormalizedSpectra 254 CurriculumVitae 276 vi List of Figures 2.1 Theevolution oftherotational profileofa9M star . . . . . . . . . . . . . . . 15 ⊙ 2.2 Theevolution oftheH,He,C,N,andOsurfaceabundancesofa9M star . . . 16 ⊙ 2.3 Theevolution ofarotating9M staronthemain-sequence . . . . . . . . . . . 17 ⊙ 2.4 Theevolutionarytrackwithandwithoutrotationforstarswithmassesbetween 9M and120M . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 18 ⊙ ⊙ 2.5 Evolutionary tracksoftheatmosphericnitrogenabundanceinmassivestars . . 19 2.6 Evolutionary tracks of the ratio of the carbon abundance to the nitrogen abun- danceinmassivestars. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 20 2.7 Ioschronesforrotating andnonrotating models . . . . . . . . . . . . . . . . . 21 2.8 Thechangeoftheratiooftheangularrotational velocitytothecriticalvalue . . 22 2.9 Theincreaseofnitrogenabundancewithstellarage . . . . . . . . . . . . . . . 24 2.10 The nitrogen abundances for a sample of MagellC B and Be stars (Dunstall et al.,2011) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 25 2.11 The change of the atmospheric nitrogen abundances with the change of the rotationalvelocity . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26 3.1 ThedependenceoftheobservedlineprofilesofBestarsonthestellarinclination 32 3.2 colour-colour diagramforanumberofBestars . . . . . . . . . . . . . . . . . 35 5.1 NiiGrotrian diagram . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 50 5.2 Quadratic stark width ratios of N ii lines versus the effective quantum number oftheupperlevel . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 54 5.3 Thefractionofsinglyionizednitrogenasafunctionoftheopticaldepth . . . . 57 5.4 RadiationtemperatureoftheionizingmeanintensityforthefirsttenlevelsofNii 58 5.5 Non-LTE departures coefficients for the first sixteen energy levels of Nii plus thegroundlevelofNiii . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 59 5.6 The predicted LTE (dashed lines) and non-LTE equivalent (solid lines) widths ofNiiλ3995Å andλ6482Å . . . . . . . . . . . . . . . . . . . . . . . . . . 64 5.7 ThelinesourcefunctionofN iiλ3995Å λ6482Å . . . . . . . . . . . . . . . 65 5.8 HydrogenopacityeffectsonthecomputedequivalentwidthsofNiiλ6482Å and λ3995Å . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 66 5.9 CurvesofgrowthforNiiλ6482Å andλ3995Å . . . . . . . . . . . . . . . . 67 5.10 ThesourcefunctionoftheN iiλ3995Å&λ6482Åfordifferentnitrogenabun- dances . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 71 5.11 The line source function of N ii λ 3995Å line from the results of the multi- multianalysis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 74 vii 5.12 The line source function of N ii λ 6482Å line from the results of the multi- multianalysis . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 75 5.13 The distribution of the equivalent widths results of the Monte-multi analysis forλ6482Å andλ3995Å . . . . . . . . . . . . . . . . . . . . . . . . . . . . 80 5.14 The uncertainties of the estimated nitrogen abundances due to inaccuracies in theatomicdata . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 82 5.15 Thechangeofthecomputedequivalentwidthsofλ3995Å andλ6482Å with thechangeofthesizeofthenitrogen atom . . . . . . . . . . . . . . . . . . . . 85 6.1 HeiGrotrian diagramshowingthesingletandtriplet spinsystems. . . . . . . . 92 6.2 ThestarkwidthratiosofHe ilinesversustheeffectivequantumnumberofthe upperLSstate . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 96 6.3 Theionization BalancesofHeiandHeii . . . . . . . . . . . . . . . . . . . . . 98 6.4 Theradiationtemperatureofthephotoionizingradiationatthethresholdwave- lengthforthelowest10LSstatesoftheHei . . . . . . . . . . . . . . . . . . . 99 6.5 Thenon-LTEdeparturecoefficientsofthepopulationnumbersofthelowest15 LSstatesofHeiplusthegroundlevelofHeii . . . . . . . . . . . . . . . . . . 100 6.6 ThecomputedequivalentwidthsofanumberofHei(I) . . . . . . . . . . . . . 102 6.7 ThecomputedequivalentwidthsofanumberofHeilines(II) . . . . . . . . . . 103 6.8 ThecomputedequivalentwidthsofanumberofHeiλ10830Å line. . . . . . . 104 7.1 TheDistribution oftheeffectivetemperatureoverthesurfaceofarotating star . 113 7.2 The gravitational darkening effects on the predicted equivalent widths of the N ii3995Å and6482Å lines. . . . . . . . . . . . . . . . . . . . . . . . . . . 115 7.3 Gravitationally darkening effects on the predicted equivalent widths of λ 3995 andλ6482Å Niilinesforv =0.85 . . . . . . . . . . . . . . . . . . . . . . 116 frac 7.4 Thegravitational darkeningeffectsontheequivalentwidthoftheHe iλ6678Å 117 7.5 The gravitational darkening effects on the predicted equivalent widths of the Mg iiλ4481Å . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 119 7.6 The gravitational darkening effects on the estimated v sini using measured equivalentwidthsoftheHeiλ6678Å andtheMg iiλ4481Å. . . . . . . . . . 120 8.1 Normalization processoftheHαlineprofileoftheBestarHD143275 . . . . . 126 8.2 NormalizedHαoftheBestarHD143275 . . . . . . . . . . . . . . . . . . . . 127 8.3 Normalization processoftheNiiλ3995.0Å lineoftheBestarHD143275 . . 128 8.4 Normalization processoftheNiiλ4447.0Å lineoftheBestarHD143275 . . 129 8.5 Normalization processoftheNiiλ5679.0Å lineoftheBestarHD143275 . . 130 8.6 NormalizedNiilinesoftheBestarHD143275 . . . . . . . . . . . . . . . . . 131 8.7 NormalizedNiilinesoftheBestarHD11415 . . . . . . . . . . . . . . . . . . 132 8.8 NormalizedNiilinesoftheBestarHD143275 . . . . . . . . . . . . . . . . . 133 8.9 Comparison of the T estimates of Levenhagen & Leister (2006) for 22 Be eff starsinthesamplewiththecorrespondingvaluesofFre´matetal.(2005) . . . . 137 8.10 Comparison of the T estimates of Catanzaro (2013) for seven Be stars in the eff samplewiththecorresponding valuesofFre´matetal.(2005) . . . . . . . . . . 138 8.11 vsinidistribution fortheBestarssample . . . . . . . . . . . . . . . . . . . . . 141 viii 8.12 FittingoftheobservedHeiλ4471Å,Mgiiλ4481Å andHeiλ6678Å lines withsyntheticnon-LTElineprofilesoftheBestarHD11415. . . . . . . . . . . 143 8.13 FittingoftheobservedHeiandMgiilineswithsyntheticnon-LTElineprofiles oftheBestarHD174237 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 143 8.14 FittingoftheobservedHeiandMgiilineswithsyntheticnon-LTElineprofiles oftheBestarHD65875 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 144 8.15 FittingoftheobservedHeiandMgiilineswithsyntheticnon-LTElineprofiles oftheBestarHD45725 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 144 8.16 FittingoftheobservedHeiandMgiilineswithsyntheticnon-LTElineprofiles oftheBestarHD203467 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 145 8.17 Comparisonofthecurrentestimatesofloggwiththeavailablevaluesinliterature145 8.18 MeasuringequivalentwidthsofobservedNiilinesinthespectraoftheBestar HD11415. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 147 8.19 Measured equivalent widths of observed Nii lines in the spectra of the Be star HD67698 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 148 8.20 Measured equivalent widths of observed Nii lines in the spectra of the Be star HD58343 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 149 8.21 NormalizedHαoftheBestarHD49567 . . . . . . . . . . . . . . . . . . . . . 152 8.22 HαlinefittingoftheBestarHD189687 . . . . . . . . . . . . . . . . . . . . . 154 8.23 HαlinefittingoftheBestarHD143275 . . . . . . . . . . . . . . . . . . . . . 154 8.24 HαlinefittingoftheBestarHD45725 . . . . . . . . . . . . . . . . . . . . . . 155 8.25 ComparisonofcurrentinclinationestimationswiththoseofFre´matetal.(2005) forthecommonobjects. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 157 8.26 ResultsofKStestresultforcurrentinclinationestimationsandthoseofFre´mat etal.(2005) . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 158 8.27 ResultsofKStestresultfortheentiresampleofFre´matetal.(2005) . . . . . . 159 8.28 TheestimationofthenitrogenabundanceoftheBestarHD56139basedonthe measuredequivalentwidth oftheNii3995Åline. . . . . . . . . . . . . . . . . 161 8.29 NitrogenabundanceestimationsofthesampleofBestarsversustheireffective temperatures . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 162 8.30 ResultsofKStestresultfortheestimatednitrogenabundancesofthesample. . 163 8.31 Comparisonoftheestimatednitrogenabundancesfromλ3995Å Niilinewith theresultsoftheabundanceanalysisincludingallobservedNiilines . . . . . . 165 8.32 RelationbetweentheestimatednitrogenabundancesoftheBestarssampleand theirgravities . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 166 8.33 Figure shows relation between the estimated nitrogen abundances of the Be starssampleandtheirequatorialrotational velocities . . . . . . . . . . . . . . 167 8.34 FigureshowsthediskcontaminationasfunctionofthewavelengthforB3-type Bestar . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 169 8.35 FigureshowsthediskcontaminationasfunctionofthewavelengthforB4-type Bestar . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 169 8.36 Correctionsofthemeasurednitrogenabundancesfordiskcontamination effect 172 8.37 HistogramsofmeasuredBandBestarnitrogenabundancesfromseveralsources173 D.1 HαlinefittingoftheBestarHD33328 . . . . . . . . . . . . . . . . . . . . . . 234 ix

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31000 K log(τ5000. ) log n(NIII) / n(N). (b). Figure 5.3: Panel (a) shows the fraction of singly ionized nitrogen as a function of the optical depth, τ5000, for several stellar effective temperatures and logg= 4.0 (ξt Morton, Donald C., Wu, Qixue, & Drake, G.W.F. 2006, Canadian Journal of Physi
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