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Published byAllen Holmes Modified over 9 years ago
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AIMS OF G ALACTIC C HEMICAL E VOLUTION STUDIES To check / constrain our understanding of stellar nucleosynthesis (i.e. stellar yields), either statistically (mean, dispersion) or in individual objects To establish a chronology of events in a given system e.g. when metallicity reached a given value, or when some stellar source (SNIa, AGB etc.) became important contributor to the abundance of a given isotope / element To infer how a system was formed (Star Formation Rate, large scale gas mouvements) e.g. slow infall of gas in case of solar neighborhood
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THE SOLAR NEIGHBORHOOD SLOW INFALL ( = 7 Gyr) to fix G-dwarf problem, SNIa to account for [Fe/O] evolution PREDICTIONS : D evolution, evolution of abundances (depends on yields) AGE-METALLICITY METALLICITY DISTRIBUTION
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Woosley and Weaver 1995, Overproduction factors of elements in massive stars
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ABUNDANCES AT SOLAR SYSTEM FORMATION (Massive stars: Woosley+Weaver 1995; Intermediate mass stars: van den Hoek+Gronewegen 1997; SNIa: Iwamoto et al. 2000)
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AGES OF GLOBULAR CLUSTERS AGES OF HALO STARS Marquez and Schuster 1994 Salaris and Weiss 2002
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Norris and Ryan 1991
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INFALL OUTFLOW
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AGE – METALLICITY IN THE GALACTIC HALO Note: Instantaneous mixing approximation probably invalid at early times Stars of mass M > 2 Mʘ (Lifetime < 1 Gyr) enriched the Galaxy during the halo phase
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NOTE: PRIMARIES VS SECONDARIES 1) CHEMICAL EVOLUTION (yield: IMF integrated or individual stars) PRIMARY: yield y P independent of Z SECONDARY: yield y S proportional to Z 2) STELLAR NUCLEOSYNTHESIS (yield from individual stars) PRIMARY: from H, He and their products (C,O) (yield not necessarily Z independent!) SECONDARY: from some metal at stellar formation (yield not necessarily proportional to Z!)
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NITROGEN PRODUCTION MASSIVE STARS ( 10 7 years): Secondary Non Rotating : INTERMEDIATE MASS ( 10 8 years): Primary LOW MASS STARS ( 10 9 years): Secondary Rotating: MASSIVE STARS ( 10 7 years): Secondary Stars INTERMEDIATE AND LOW MASS ( 10 8 years): Primary STELLAR CNO YIELDS
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C and N abundances always follow Fe PRIMARIES ? But: 2/3 of Fe in disk come late from SNIa ⇩ 2/3 of C and N in disk come from a late source (not operating in halo) Low mass stars ? Secondary N (but C?) Z-dependent yields from massive stars? No sign of secondary N in early halo: Which primary source? EVOLUTION OF CNO IN SOLAR NEIGHBORHOOD
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Stellar rotation has similar effect on yields of nitrogen (mostly from Intermediate mass stars) as Hot Bottom Burning Difficult to explain earliest primary Nitrogen (Massive star yields insufficient -even with rotation…) However: timescales at low [Fe/H] uncertain ! Secondary N production at late times matches Fe production from SNIa [N/Fe] 0 Not exactly the case for C…
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FRACTIONAL CONTRIBUTION TO NITROGEN-14 PRODUCTION FRACTIONAL CONTRIBUTION TO CARBON-12 PRODUCTION
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PRIMARY NITROGEN… WITH RESPECT TO WHAT ??? WW95 + VdHG97 MM02 No Rot MM02 + Rot PSEUDO-SECONDARY BEHAVIOUR WITH RESPECT TO OXYGEN
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Inside-Out formation and radially varying SFR efficiency required to reproduce observed SFR, gas and colour profiles (Scalelengths: R B 4 kpc, R K 2.6 kpc) (Boissier and Prantzos 1999) THE MILKY WAY DISK
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METALLICITY PROFILE OF MILKY WAY DISK Present day gradient : dlog(O/H)/dR ∼ - 0.07 dex/kpc Models predict (e.g. Hou et al. 2000 ) that abundance gradients were steeper in the past
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METALLICITY PROFILE OF MILKY WAY DISK Recent observations (Maciel et al 2002) of planetary nebulae of various ages support that prediction: The disk was formed inside-out “Observed” evolution of O gradient: d[dlog(O/H)/dR]/dt ∼ 0.004 dex/kpc/Gyr In broad agreement with theory
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ABUNDANCE GRADIENTS OF CNO IN MILKY WAY DISK O : dlog(O/H) / dR = - 0.07 dex/kpc But: Deharveng et al. (2001): -0.04 dex/kpc N: dlog(N/H) / dR = - 0.08 dex/kpc C : dlog(C/H) / dR = - 0.07 dex/kpc
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C and O not sensitive to different sets of yields (primaries) For N, stellar yields up to Z=3 Z ⊙ (not available at present) are required in order to model the inner disk ABUNDANCE GRADIENTS OF CNO IN MILKY WAY DISK
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