planetary nebulae and the chemical evolution of the galactic bulge

19
Roberto D.D. Costa André V. Escudero Walter J. Maciel (IAG/USP, Brazil) Planetary nebulae and the chemical evolution of the galactic bulge Work supported by FAPESP

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Planetary nebulae and the chemical evolution of the galactic bulge. Roberto D.D. Costa André V. Escudero Walter J. Maciel (IAG/USP, Brazil). Work supported by FAPESP. The idea. Spectrophotometric data for a sample of bulge PNe, representatives of its intermediate age population. - PowerPoint PPT Presentation

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Page 1: Planetary nebulae  and the chemical evolution  of the galactic bulge

Roberto D.D. Costa André V. Escudero Walter J. Maciel

(IAG/USP, Brazil)

Planetary nebulae and the chemical evolution of the galactic bulge

Work supported by FAPESP

Page 2: Planetary nebulae  and the chemical evolution  of the galactic bulge

The idea

• Spectrophotometric data for a sample of bulge PNe, representatives of its intermediate age population.

• Electron temperatures, densities, ionic and elemental abundances of helium, nitrogen, oxygen, argon, sulfur and neon were derived for the sample.

• Using these observational results as constraints, a model to the chemical evolution of the bulge was developed.

• Results indicate that the best fit for the measured chemical abundances is achieved using a double-infall model, where the first one is a fast collapse of primordial gas and the second is slower and enriched by material ejected by the bulge itself during the first episode.

Page 3: Planetary nebulae  and the chemical evolution  of the galactic bulge

Data

57 bulge PNe. Details of observations and data reduction in: Escudero & Costa 2001 (A&A 380, 300)

Escudero et al. 2004 (A&A 414, 211)

Observations: ESO 1.5 m (Chile)

LNA 1.6 m (Brazil)

Data reduction and analysis homogeneous for the whole sample The largest homogeneous sample on chemical abundances of bulge PNe in the literature. (~30% of the total)

Abundances derived empirically using ICFs

Page 4: Planetary nebulae  and the chemical evolution  of the galactic bulge

Distribution of chemical abundances

Helium

Literature data from Köppen et al. (1991), Samland et al. (1992), Cuisinier et al. (1996, 2000), Stasinska et al. (1998), Gorny et al. (2004)

Page 5: Planetary nebulae  and the chemical evolution  of the galactic bulge

Nitrogen

Page 6: Planetary nebulae  and the chemical evolution  of the galactic bulge

Oxygen

Page 7: Planetary nebulae  and the chemical evolution  of the galactic bulge

6,0 6,5 7,0 7,5 8,0 8,5 9,0 9,5 10,06,0

6,5

7,0

7,5

8,0

8,5

9,0

9,5

10,0

(N)

(O)

Nossos Dados LiteraturaOur sampleLiterature

0,00 0,05 0,10 0,15 0,20 0,25-2,0

-1,5

-1,0

-0,5

0,0

0,5

1,0

log

(N/O

)

He/H

Nossa Amostra LiteraturaOur sampleLiterature

Correlations between abundances

Old objects

Intermediate age objects Young objects

Page 8: Planetary nebulae  and the chemical evolution  of the galactic bulge

6,5 7,0 7,5 8,0 8,5 9,0 9,54,5

5,0

5,5

6,0

6,5

7,0

7,5

(Ar)

(O)

Nossos Dados Literatura

Our sampleLiterature

6,5 7,0 7,5 8,0 8,5 9,0 9,54,5

5,0

5,5

6,0

6,5

7,0

7,5

8,0

8,5

(S)

(O)

Nossa Amostra Literatura

Our sampleLiterature

Old objects

Young objects

Page 9: Planetary nebulae  and the chemical evolution  of the galactic bulge

Distribution

Latitude

-20 -15 -10 -5 0 5 10 15 207,0

7,5

8,0

8,5

9,0

9,5

10,0

(O)

latitude

Nossos Literatura

Longitude

-20 -15 -10 -5 0 5 10 15 207,0

7,5

8,0

8,5

9,0

9,5

10,0

(O)

longitude

Nossos Literatura

Page 10: Planetary nebulae  and the chemical evolution  of the galactic bulge

The model

Goal: Model the chemical evolution of the bulge using PNe as representatives of their intermediate age population

Compare model results with derived abundances for many elements

Page 11: Planetary nebulae  and the chemical evolution  of the galactic bulge

Basic equations

Infall: dM/dt = A exp[- t /], where dM = MT SFR = 2.5 10-10 g

k [M year-1 pc-2 ] (Kennicutt 1998)

IMF: Kroupa (2002)

Model 1 Simple infall during 1 Gyr with primordial abundance Outflow from 0 to 75% during 2 Gyr.

Model 21. First infall during 0.1 Gyr with primordial abundance. Salpeter’s IMF during the first 0.4 Gyr Outflow of 50% during 2 Gyr.2. Second infall during 2.0 Gyr, occuring 2.0 Gyr after the first one. No winds or

outflow

Model 31. Same as Model 2, but with second infall gas enriched by the first infall wind2. Multizone

Page 12: Planetary nebulae  and the chemical evolution  of the galactic bulge

Results

• Model 1 (simple infall) with different mass loss fractions, compared with observational results for two different elements. • Mass is ejected by SN II/Ia. It can be seen that the wind rate is crucial to reproduce the observational data. Windless models overestimate the oxygen abundances. • Recent models point to a great mass loss by SN II in the early bulge formation phases (Ferraras et al. 2003). Other alpha-element results are similar to oxygen.

Page 13: Planetary nebulae  and the chemical evolution  of the galactic bulge

6,0 6,5 7,0 7,5 8,0 8,5 9,0 9,5 10,00,00

0,05

0,10

0,15

0,20

0,25

0,30 Woosley & Weaver (1995) Tsujimoto et al. (1995)

N /

Nto

t

(O)

Results from model 2 (double infall) using two SN II yields compared with observational data derived from PNe.

Page 14: Planetary nebulae  and the chemical evolution  of the galactic bulge

5,0 5,5 6,0 6,5 7,0 7,5 8,0 8,5 9,0 9,50,00

0,05

0,10

0,15

0,20

0,25

0,30

0,35

Woosley & Weaver (1995) Tsujimoto et al. (1995)

N /

Nto

t

(Ne)

4,0 4,5 5,0 5,5 6,0 6,5 7,0 7,5 8,00,00

0,05

0,10

0,15

0,20

0,25

0,30

0,35

Woosley & Weaver (1995) Tsujimoto et al. (1995)

N /

Nto

t(Ar)

Page 15: Planetary nebulae  and the chemical evolution  of the galactic bulge

-1,0 -0,5 0,0 0,5 1,0-0,5

0,0

0,5

Pompeia et al. (2003)

[O/F

e]

[Fe/H]

• Model 2 results using two SN II yields (dotted: Woosley & Weaver 1995; solid: Tsujimoto et al. 1995) compared with observational data derived from stars. Red dots correspond to upper limits. • A less steeper IMF (Salpeter) is required during the first 0.4 Gyr, in order to reproduce the higher O/Fe ratio found in bulge stars with respect to disk objects.

Page 16: Planetary nebulae  and the chemical evolution  of the galactic bulge

Model 3 (multizone, double infall, second enriched)

40 %

~ 10 %

~ 10 - 25 %

Sketch of the multizone model, indicating the different mass fractions ejected by SN II/Ia. Each zone correspond to 1.5 kpc and has its own infall timescale and gas mass. Gas ejected by SN II/Ia is exchanged between zones.

Page 17: Planetary nebulae  and the chemical evolution  of the galactic bulge

• Solid lines represent the N/O ratio according to the multizone model with an interzone exchange between 10 to 25 %.

• Blue lines correspond to the center of the bulge (central zone in the sketch). Red lines correspond to the first ring.

• Dotted lines correspond to a model for which progenitors with masses smaller than 1 solar mass do not produce nitrogen, with interzone exchange of 10%. • Dashed red line corresponds to an intezone exchange of 25%.

• Objects produced by the second infall, previously enriched by SN II ejecta during the first infall.

• Variation of the SFR efficiency is not enough to account for the observed N/O ratios

Page 18: Planetary nebulae  and the chemical evolution  of the galactic bulge

• Correlation between N/O and He abundance. Blue lines correspond to the central zone and red lines correspond to the first ring (bulge-disk border)

• The N/O vs. He/H does not change critically from one zone to other

0,00 0,05 0,10 0,15 0,20 0,25-2,0

-1,5

-1,0

-0,5

0,0

0,5

1,0

log

(N/O

)

He/H

Nossa Amostra LiteraturaOur sampleLiterature

Page 19: Planetary nebulae  and the chemical evolution  of the galactic bulge

Main conclusions

• Fast initial collapse (0.1 Gyr)

• High SFR induces a high mass loss of material produced by SN II. This material goes to disk, halo and outside the Galaxy (2 Gyr)

• A second and slower infall (2 Gyr) of enriched material generated the disk.

Steps required to reproduce the PNe abundance distribution :