88 CHAPTER 5: Probing AGB nucleosyn<strong>thesis</strong> via accurate Planetary Nebula abundancesFigure 5.6–. Carbon abundances and C/O ratios in PNe with low helium abundances (He/H≤ 0.13).Open symbols denote predictions of synthetic TP-AGB calculations for various choices of model parameters– specified in the legenda – corresponding to a stellar progenitor with (M i = 2.0M ⊙, Z i =0.019). See text and cases B-C-D-E of Table 5.4 for more details.Reproducing the extent of carbon enrichmentTo tackle the problem of carbon we consider a stellar model with 2 M ⊙ initial mass, a typicalmass of carbon stars in the Galactic disk (Groenewegen et al. 1995). Figure 5.6 shows a fewmodels of the predicted carbon abundance and corresponding PN values.As starting model we consider the one with the κ fix assumption. It is clearly located wellabove the observed points (diamond in left panel of Fig. 5.6).A first significant improvement is obtained acting on the opacity, that is adopting variablemolecular opacities during the TP-AGB calculations. We replace κ fix with κ var , whilekeeping the other model parameters fixed. In this model (starred symbol) the predicted C/His lowered because of a shorter C-star phase, hence a decrease in the number of dredge-upepisodes (see Marigo 2002, 2003).Additional cases are explored. <strong>The</strong> usual assumption of constant dredge-up efficiency λis replaced with the recent recipe by Karakas et al. (2002), who provide analytic relations– fitting the results of full AGB calculations – that express the evolution of λ as a functionof metallicity Z, stellar mass M, and progressive pulse number. For a given M and Z, λ isfound to increase from initially zero up to nearly constant maximum value, λ max . This latteralso varies depending on mass loss. Adopting λ max = 0.457 as suggested by Karakas et al.(2002) for the (M = 2 M ⊙ , Z = 0.02) combination, we end up with a somewhat lower C/H(triangle), compared to the case with (κ var , λ = 0.5). This reflects the smaller amount ofcarbon globally dredged-up with the λ var assumption.
5.6. Comparison between models and observations 89A further test is made with respect to the assumed initial oxygen abundance. We calculatethe TP-AGB evolution of the 2 M ⊙ model replacing the surface oxygen abundance at thefirst thermal pulse – as predicted by Girardi et al. (2000) evolutionary calculations, basedon Anders & Grevesse (1989) solar mixture (the O ⊙ High in Table 5.4) – by the recentlyrevised determination by Allende Prieto et al. (2001; the O ⊙ Low in Table 5.4).With the new lower oxygen abundance the solar C/O ratio increases from 0.48 to 0.78.This increment in the initial C/O ratio has important effects on the later TP-AGB evolutionand PN abundances: fewer dredge-up episodes are necessary to produce a carbon star andhence, on average, a lower C abundance is expected in the PN ejecta. This can be seen inFig. 5.6, by comparing the models labeled by triangle and circle symbols. We also noticethat the trend in the predicted values of C/H (left panel) or C/O (right panel) is reversed.<strong>The</strong> O ⊙ Low prescription leads to a reduced absolute carbon enrichment compared to theO ⊙ High case, while the final C/O ratio is larger in the former case. It should be remarkedthat using the recent carbon abundance by Allende Prieto et al. (2002) together with the newlower oxygen abundance the C/O ratio is 0.50, nearly equally to the ratio of Grevesse &Noels (1993), negating the above comment.At this point the results already appear better compared to the starting model, but inorder to carry the expected C/H point within the observational error bars, we change anotherfundamental model parameter, i.e. the dredge-up efficiency λ. A good fit of the PNe data isobtained by lowering λ max from 0.457 to 0.3, that simply means diminishing the amount ofdredged-up carbon.In summary, from these calculations we derive the following indications. Both the C/Hand the C/O ratios of the carbon-rich Galactic PNe – evolved from stars with typical massesof ∼ 2.0 M ⊙ – can be reproduced by assuming i) variable molecular opacities κ var , ii)an initial oxygen abundance as recently revised by Allende Prieto et al. (2001), and iii)a dredge-up efficiency λ ≈ 0.3 − 0.4. <strong>The</strong>se indications – in particular points i) and iii)– agree with the results recently obtained by Marigo (2002, 2003) in her analysis of theproperties of Galactic carbon stars in the disk. Variable molecular opacities and λ 0.5 arerequired to reproduce a number of observables of carbon stars, like their C/O ratios, effectivetemperatures, mass-loss rates, and near-infrared colours.<strong>The</strong>n, from the representative case of the 2.0 M ⊙ model, we consider a wider mass range,i.e. 1.1 − 5.0 M ⊙ , with initial metallicity Z = 0.019. Results of the C/H and C/O ratios asa function of He/H, expected in the corresponding PNe, are displayed in Figs. 5.7 and 5.8and are also summarized in the top-left panels of Figs. 5.11 and 5.12 (triangles connectedby solid line). <strong>The</strong>y show a satisfactory agreement with the observed data for He/H< 0.14,suggesting a mass interval for the stellar progenitors from about 1.0 to 4.0 M ⊙ .Synthetic TP-AGB calculations are carried out by adopting the κ var and O ⊙ Lowprescriptions, and assuming λ ≈ 0.3 − 0.5 for lower stellar masses (M 3.0 M ⊙ ), whileincreasing it up to λ ≈ 0.98 for the largest masses. This means that the third dredge-upshould become deeper in more massive stars, as indicated by full TP-AGB calculations
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RIJKSUNIVERSITEIT GRONINGENPhysics
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To my parents
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Contents1 Introduction 11.1 Evoluti
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CONTENTSvii5 Probing AGB nucleosynt
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1IntroductionPLANETARY NEBULAE are
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1.1. Evolution of low and intermedi
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1.2. Planetary Nebulae 5Flash−Dri
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1.3. Physics in PNe 7their whole li
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1.3. Physics in PNe 95.35 eVO IIIλ
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1.4. Studying PNe in the infrared 1
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2The ISO-SWS Spectrum ofPlanetary N
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2.3. Data reduction 15Table 2.1-. C
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2.4. Line flux discussion 17Table 2
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2.5. The visual and the ultraviolet
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2.6. Analysis 21Table 2.5-. Electro
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24 CHAPTER 2: The ISO-SWS Spectrum
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26 CHAPTER 2: The ISO-SWS Spectrum
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28 CHAPTER 2: The ISO-SWS Spectrum
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3An ISO and IUE study of PlanetaryN
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3.3. Corrections to line fluxes 33[
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3.4. Line fluxes 35Table 3.1-. Comp
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7Conclusions and future workTHE res
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141• PNe with He/H > 0.14. The st
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143HERSCHEL The launch of this sate
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Nederlandse SamenvattingSTERREN wor
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Nederlandse Samenvatting 147Figuur
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Nederlandse Samenvatting 149PHOTOIO
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Nederlandse Samenvatting 151Figuur
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Nederlandse Samenvatting 153infraro
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English SummarySTARS are born, live
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English Summary 157Figure 2-. Two e
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English Summary 159PHOTOIONIZATIONR
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English Summary 161Figure 5-. Spect
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English Summary 163all) stages of i
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BibliographyAcker A., Marcout J., O
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BIBLIOGRAPHY 167Henry R.B.C., Kwitt
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BIBLIOGRAPHY 169Pottasch S.R., Bern
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List of PublicationsPublications in
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AcknowledgementsI could easily writ
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Acknowledgements 175sense of humor,