92 CHAPTER 5: Probing AGB nucleosyn<strong>thesis</strong> via accurate Planetary Nebula abundancesFigure 5.8–. <strong>The</strong> same as in Fig. 5.7, but expressing the abundance data with different combinationsof elemental ratios.would be flatter 2 than the present one (connected triangles in Fig. 5.11). But this casecould not be rejected either since corresponding predictions are still confined withinthe observed domain.5.6.4 PNe with extremely high He abundanceBelow we discuss the PNe exhibiting the largest enrichment in helium, i.e. with 0.14 He/H 0.20 (see e.g. Fig. 5.3). <strong>The</strong>se objects share other chemical properties, namely:• Marked carbon deficiency compared to the solar value;• Sizeable enhancement of nitrogen, but not exceeding the upper values observed in thePNe with lower He/H;• Significant depletion of oxygen, which makes these PNe appear as a distinct groupwith respect to the PNe with lower He/H abundances;• Possible, but still not compelling, hint of over-abundance of neon compared to the solarvalue.By looking at Fig. 5.5, we conclude that model predictions after the first and seconddredge-up processes cannot account for the extremely high He/H values of these PNe. <strong>The</strong>n,2 In any case Ne/H should keep a slightly increasing trend, not becoming exactly horizontal since, even if Ne=const., the hydrogen content H decreases as a consequence of dredge-up events.
5.6. Comparison between models and observations 93we are led to consider additional He contributions from the third dredge-up and HBB duringthe TP-AGB phase.Qualitatively, the enrichment in helium and nitrogen and the simultaneous deficiency incarbon would naturally point to HBB as a possible responsible process, via the CNO-cyclereactions. <strong>The</strong>refore, as a working hypo<strong>thesis</strong>, let us assume that the stellar progenitors ofthese extremely He-rich PNe are intermediate-mass stars (M 4.5 M ⊙ ), experiencing HBBduring their AGB evolution. We will now investigate under which conditions all elementalfeatures can be reproduced.To allow an easier understanding of the following analysis, Figs. 5.9 and 5.10 show thepredicted time evolution of He, C, N, O, and Ne elemental abundances in the envelope duringthe TP-AGB phase of models experiencing HBB. Different assumptions are explored.<strong>The</strong> observed PN abundances should be compared with the last starred point along the theoreticalcurves, which marks the last event of mass ejection, and it may be then consideredrepresentative of the expected PN abundances.Constraints from oxygen and sulfur abundancesAt this point additional information comes from the marked oxygen under-abundancecompared to solar (for both High and Low values), common to the extremely He-rich PNe.We recall that the oxygen abundance in the envelope remains essentially unchanged afterthe first and second dredge-up events. <strong>The</strong> third dredge-up may potentially increase oxygen,depending on the chemical composition of the convective inter-shell that forms at thermalpulses. In any case, no oxygen depletion is expected by any of these processes. A destructionof oxygen could be caused by a very efficient HBB, that is if the ON cycle is activated andoxygen starts being transformed into nitrogen.We have explored this possibility on a 5M ⊙ TP-AGB model with original solar metallicity.To analyse the effects of a larger HBB efficiency, the mixing-length parameter α MLhas been increased, and set equal to 1.68, 2.00, and 2.50. In fact, larger values of α MLcorrespond to higher temperatures at the base of the convective envelope. In none of thethree cases have we found any hint of oxygen destruction, as indicated by the flat behaviourof the abundance curves in the bottom-left panel of Fig. 5.9 (solid and long-dashed lines, forα = 1.68 and 2.50, respectively).At this point we decided to stop further increasing α – which would have likely ledto oxygen destruction at some point – since we run into a major discrepancy. In fact,increasing the efficiency of HBB causes a systematic over-enrichment in nitrogen, as shownby the model with α ML = 2.50 (short-dashed line). We also note that a significant nitrogenproduction is accompanied by a mirror-like destruction of carbon (upper-left panel ofFig. 5.9). This is not the case of the model with α ML = 1.68 (solid line), in which HBB isalmost inoperative.From these results we can expect that, even if a destruction of oxygen is obtained forlarger values of α ML , the problem of nitrogen over-production would become even more
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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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Table 3.3-. IUE intensities, fluxes
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3.5. Physical parameters 393.4.3 Op
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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,