2000ApJ...542..308S


Query : 2000ApJ...542..308S

2000ApJ...542..308S - Astrophys. J., 542, 308-327 (2000/October-2)

Synthetic post-asymptotic giant branch evolution: basic models and applications to disk populations.

STANGHELLINI L. and RENZINI A.

Abstract (from CDS):

We explore the realm of post-asymptotic giant branch (post-AGB) stars from a theoretical viewpoint, by constructing a synthetic population of transition objects, proto-planetary nebulae, planetary nebula nuclei (PNNs), and post-planetary nebula objects. We use the Monte Carlo procedure to filter out the populations according to a given set of assumptions. We explore the parameter space by studying the effects of the initial mass function (IMF), the initial mass-final mass relation (IMFMR), the transition time (ttr), the envelope mass at the end of the envelope ejection (MRe), the planetary nebula (PN) lifetime tPN, and the hydrogen- and helium-burning phases of the central stars. The results are discussed on the basis of the H-R diagram distributions, the MV-t plane, and mass histograms. We found that (1) the dependence of the synthetic populations on the assumed IMF and IMFMR is generally mild; (2) the MRe indetermination produces very high indeterminations in the ttr and thus in the resulting post-AGB populations; and (3) the synthetic models give a test check for the ratio of He- to H-burning PNNs. In this paper, disk post-AGB populations are considered. Future applications will include Magellanic Cloud PNs and populations of bulges and elliptical galaxies.

Abstract Copyright: ∼

Journal keyword(s): Galaxy: Stellar Content - Stars: AGB and Post-AGB - Stars: Evolution - Stars: Luminosity Function, Mass Function

Simbad objects: 4

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Number of rows : 4
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
2 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
3 NGC 2516 OpC 07 58 00.5 -60 46 36           ~ 793 0
4 NGC 3451 H2G 10 54 20.859 +27 14 22.76   13.5       ~ 132 0

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