82 CHAPTER 5: Probing AGB nucleosyn<strong>thesis</strong> via accurate Planetary Nebula abundances• <strong>The</strong> composition of the convective inter-shell (in terms of the elemental abundancesX csh,i ) developed at thermal pulses, i.e. of the dredged-up material. We essentiallyspecify the abundances of helium X csh ( 4 He), carbon X csh ( 12 C), and oxygenX csh ( 12 O) (see Table 5.4). We recall that detailed calculations of thermal pulsesindicate a typical inter-shell composition [X csh ( 4 He) ∼ 0.76; X csh ( 12 C) ∼ 0.22;X csh ( 16 O) ∼ 0.02] (see e.g. Boothroyd & Sackmann 1988a; Forestini & Charbonnel1997). However, these results may drastically change with the inclusion of extendedovershooting from convective boundaries (i.e. X csh ( 12 C) ∼ 0.50; X csh ( 16 O) ∼ 0.25according to Herwig et al. 1997), or in the most massive TP-AGB models with deepdredge-up penetration (i.e. Vassiliadis & Wood 1993; Frost et al. 1998). This latterpossibility, relevant to our analysis, is discussed in Sect. 5.6.4.In addition to 4 He, 12 C, and 16 O, we account for the possible production of 22 Ne,via the chain of reactions 14 N(α, γ) 18 F(β + , ν) 18 O(α, γ) 22 Ne (Iben & Renzini1983). <strong>The</strong>n a certain amount of 22 Ne may be burned via the neutron source reaction22 Ne(α, n) 25 Mg. <strong>The</strong> efficiency of this nuclear step strongly depends on the maximumtemperature achieved at the bottom of the inter-shell developed at thermal pulses,being marginal for T < 3 × 10 8 K (about 1 % of 22 Ne is converted into 25 Mg), whilebecoming more and more important at higher temperatures (Busso et al. 1999).In our study, we parameterize the Ne and Mg production assuming that the abundancesin the convective intershell are given by (see also Marigo et al. 1996):X csh ( 22 Ne) = X e ( 22 Ne) + F × 2214 × X Hsh( 14 N) (5.1)X csh ( 25 Mg) = X e ( 25 Mg) + (1 − F ) × 2514 × X Hsh( 14 N)where X e refers to the envelope abundance before the dredge-up, and F representsthe degree of efficiency of the 22 Ne production, that is clearly complementary to thatof 25 Mg (1 − F ). In most of our calculations we assume F = 0.99, that meansallowing the chain of α-capture reactions to proceed from 14 N to 22 Ne, with essentiallyno further production of 25 Mg. This point is discussed in Sect. 5.6.4.In the above equations X Hsh ( 14 N) denotes the nitrogen abundance left by the H-burning shell in the underlying inter-shell region, just before the occurrence of thepulse. It is estimated with[X Hsh ( 14 Xe ( 12 C)N) = 14 ×12X e ( 15 N)+ X e( 16 O)+ X e( 17 O)15 16 17+ X e( 13 C)13+ X e( 18 O)18+ X e( 14 N)+] 14,i.e. we assume that all CNO nuclei are converted in 14 N, which is a good approximationwhen the CNO-cycle operates under equilibrium conditions. In this way we accountfor the possible primary component of 14 N in the inter-shell, which is produced every
5.6. Comparison between models and observations 83time some freshly dredged-up 12 C in the envelope is engulfed by the H-burning shellduring the quiescent inter-pulse evolution.As a consequence, the resulting X csh ( 22 Ne), synthesized via the chain of Eq. (5.1),contains a primary component, which can also be injected into the surface chemicalcomposition through the dredge-up. We note that 22 Ne is expected to be purely secondaryin low-mass stars that do not experience the third dredge-up.<strong>The</strong> reader can find more details about model prescriptions in Table 5.4.5.6 Comparison between models and observationsWe will now perform an analysis of the observed PN elemental abundances with the aid ofthe TP-AGB models just described. <strong>The</strong> basic idea is to constrain the model parameters so asto reproduce the observed data, and hence derive indications on the evolution and nucleosyn<strong>thesis</strong>of AGB stellar progenitors. <strong>The</strong> chemical elements under consideration are He, C, N,O and Ne.5.6.1 <strong>The</strong> starting point: TP-AGB models with solar-scaled molecular opacitiesFirst “old” predictions of PN abundances (Marigo 2001) are considered; see Fig. 5.3. In thosemodels with an initially solar composition the dredge-up parameters (λ and Tbdred ) werecalibrated to reproduce the observed carbon star luminosity functions in both MagellanicClouds (Marigo et al. 1999). Moreover, envelope integrations were carried out using fixedsolar-scaled molecular opacities (κ fix ; see Sect. 5.5).By inspecting Fig. 5.3 we note that, though a general agreement is found between measuredand predicted abundances with respect to nitrogen and neon abundances, three maindiscrepancy points occur:1. A sizeable overproduction of carbon by models, up to a factor of 3-5;2. <strong>The</strong> lack of extremely He-rich models, with 0.15 < He/H ≤ 0.20;3. A general overabundance of oxygen in all models, amounting up to a factor of 3.While the first two aspects are probably related to the nucleosynthetic assumptions inthe TP-AGB models, the third one could also reflect our choice of oxygen abundance in thesolar mixture (Anders & Grevesse 1989), which has recently been subject of major revision(Allende Prieto et al. 2001). <strong>The</strong> aim of the following analysis is to single out the main causesof the disagreement and possibly to remove it by proper changes in the model assumptions.5.6.2 Sub-grouping of the ISO sample and comparison with other PNe dataBefore starting the interpretative analysis, it is worth noticing that the PNe data (see Fig. 5.3)seem to segregate in two different groups in the observational abundance plots – one atlower (He/H ≤ 0.14) and the other at higher helium content (He/H > 0.14) –, and theirchemical patterns for carbon and nitrogen already suggest likely different mass ranges forthe progenitors (i.e. low- and intermediate-mass stars respectively).
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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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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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6.11. General discussion 133Table 6
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6.11. General discussion 135Figure
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6.12. Summary and Conclusions 137su
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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,