78 CHAPTER 5: Probing AGB nucleosyn<strong>thesis</strong> via accurate Planetary Nebula abundancesstages of ionization are observed, in which case no error from the ICF is involved. <strong>The</strong>abundances have been obtained using the most recent results available for the collisionalstrengths (mainly from the IRON project) so that these uncertainties are much reduced. Aquantitative idea of the errors on the abundance can also be inferred by looking at the sulfurand argon abundances in Fig. 5.2. Sulfur and argon are not supposed to vary in the course ofevolution, and as can be seen from the figure, they are within 30%. This strongly suggeststhat the abundance error derived from the intensity of the lines is the main contributor to thetotal error. <strong>The</strong>refore 30% is a good estimate of the abundance error and has been assumedin this work for all nebulae except for the nitrogen abundance of NGC 6543 which has anerror 50%. This is because the main contribution to the nitrogen abundance comes from theN ++ whose ionic abundance is derived either with the 57.3 µm or 1750 Å lines. <strong>The</strong> formeris density dependent and the latter temperature dependent, increasing therefore the error (seechapter 4). <strong>The</strong> error in the helium abundance is around 5% except, again, for NGC 6543where it is 7-8%.5.3.2 Comparison with Solar abundances<strong>The</strong> PNe abundances (Table 5.3) are shown in Fig. 5.2 with respect to the solar. <strong>The</strong> typicalerror bar applies to all elements except helium for which the error is 6 times smaller. Thiscomparison is important because in principle one might expect that the progenitor stars ofthese PNe have evolved from a solar metallicity. <strong>The</strong>refore, primary elements that do notchange in the course of evolution should lie close to the solar line, elements that are destroyedor produced should lie below or above.An inspection of the figure leads to several conclusions. NGC 7662 shows low abundancesfor all elements. It is then suspected that the progenitor mass of this PNe was low andthat it did not experience much change in the course of evolution.All other PNe show a He enhancement, which should be expected as He is brought to thesurface in the different dredge-up episodes. Four PNe show a decrease in carbon, especiallyNGC 6302 and He 2-111. <strong>The</strong> remaining PNe show solar or enhanced carbon. All PNe(except NGC 7662) show an increase of nitrogen. <strong>The</strong> oxygen abundance is close to solar forall PNe except three. <strong>The</strong> exceptions are NGC 6302, NGC 6537 and He 2-111 which show aclear decrease. It should be noticed that the solar abundance adopted in this work is that ofAllende Prieto et al. (2001). If the value of Grevesse & Sauval (1998) had been adopted allPNe would lie below the solar value.Within the errors all neon abundances except that of NGC 7662 agree with solar. Of allelements neon is probably the best determined and it is likely that the error is somewhatsmaller than 30%. In this sense it is interesting to see how PNe with higher neon abundancesare clumped at around 0.15 and the three with lower values also have lower helium abundanceof the sample.<strong>The</strong> remaining elements, sulfur and argon, are supposed to remain unchanged in thecourse of evolution and therefore should be close to solar. <strong>The</strong> argon abundance is compatiblewith this but the sulfur abundance is lower than solar.
5.4. Nucleosyn<strong>thesis</strong> in low- and intermediate-mass stars 795.4 Nucleosyn<strong>thesis</strong> in low- and intermediate-mass starsWe will recall the main nucleosynthetic and convective mixing events that may possibly alterthe surface chemical composition of a low-/intermediate-mass star in the course of its evolution.According to the classical scenario 1 four processes are important (see e.g. Forestini &Charbonnel 1997 for a recent extended analysis), namely:<strong>The</strong> first dredge-up. At the base of the RGB the outer convective envelope reaches regionsof partial hydrogen burning (CN cycle). As a consequence, the surface abundance of 4 He isincreased (and that of H depleted), 14 N and 13 C are enhanced at the expense of 12 C, while16 O remains almost unchanged.<strong>The</strong> second dredge-up. This occurs in stars initially more massive than 3-5 M ⊙ (dependingon composition) during the early AGB phase. <strong>The</strong> convective envelope penetrates intothe helium core (the H-burning shell is extinguished) so that the surface abundances of 4 Heand 14 N increase, while those of 12 C, 13 C and 16 O decrease.<strong>The</strong> third dredge-up. This takes place during the TP-AGB evolution in stars more massivethan ≈ 1.5 M ⊙ for solar composition, starting at lower masses for lower metallicities (seeMarigo et al. 1999). It actually consists of several mixing episodes occurring at thermalpulses during which significant amounts of 4 He and 12 C, and smaller quantities of othernewly-synthesized products (e.g. 16 O, 22 Ne, 25 Mg, s-process elements) are convected to thesurface.Hot bottom burning. This occurs in the most massive and luminous AGB stars (with initialmasses M 4 − 4.5M ⊙ , depending on metallicity). <strong>The</strong> convective envelope penetratesdeeply into the hydrogen-burning shell, and the CN-cycle nucleosyn<strong>thesis</strong> actually occursin the deepest envelope layers of the star. As a consequence, besides the syn<strong>thesis</strong> of newhelium, 12 C is first converted into 13 C and then into 14 N. In the case of high temperaturesand after a sufficiently long time, the ON cycle can also be activated, so that 16 O is burnedinto 14 N.It should be remarked that the third dredge-up and hot-bottom burning are the processesthat are expected to produce the most significant changes in CNO and He surface abundances,being affected at the same time by the largest uncertainties in the theory of stellar evolution.This latter point motivates the adoption of free parameters (e.g. the dredge-up efficiency) todescribe these processes in synthetic TP-AGB models, that are discussed next.5.5 Synthetic TP-AGB calculationsIn order to interpret the abundance data reported in Sect. 5.3.1, synthetic evolutionary calculationsof the TP-AGB phase have been carried out with the aid of the model developed byMarigo et al. (1996, 1998, 1999), Marigo (1998, 2001, 2002), to whom we refer for all details.1 We do not consider here any additional extra-mixing process, such as the one invoked to explain the observedabundance anomalies in low-mass RGB stars (see e.g. Charbonnel 1995).
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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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6.10. Atomic, ionized and molecular
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6.10. Atomic, ionized and molecular
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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,