for complete references)
and a new grid of stellar models for very low metallicity (Z=1/50
Z_ Z
(see the original papers for a full
description).
| Grid | database | mass range | paper |
description | ||||
| # | ID | |||||||
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) |
| Basic grids: | ||||||||
| 1 | e | 0.0004 | 0.7584 | 0.2412 | 2 |
0.8 - 150 M_ M |
this paper | basic grid |
| 2 | c | 0.001 | 0.756 | 0.243 | standard | 0.8 - 120 M_ M |
I | basic grid |
| 3 | c | 0.004 | 0.744 | 0.252 | standard | 0.8 - 120 M_ M |
III | basic grid |
| 4 | c | 0.008 | 0.728 | 0.264 | standard | 0.8 - 120 M_ M |
II | basic grid |
| 5 | c | 0.020 | 0.680 | 0.300 | standard | 0.8 - 120 M_ M |
I | basic grid |
| 6 | c | 0.040 | 0.620 | 0.340 | standard | 0.8 - 120 M_ M |
IV | basic grid |
| 7 | c | 0.100 | 0.420 | 0.480 | standard | 0.8 - 60 M_ M |
VII | basic grid |
| Extended grids: | ||||||||
| 8 | e | 0.001 | 0.756 | 0.243 | 2 |
0.8 - 120 M_ M |
V, I | high mass loss for massive stars |
| 9 | e | 0.004 | 0.744 | 0.252 | 2 |
0.8 - 120 M_ M |
V, III | high mass loss for massive stars |
| 10 | e | 0.008 | 0.728 | 0.264 | 2 |
0.8 - 120 M_ M |
V, II | high mass loss for massive stars |
| 11 | e | 0.020 | 0.680 | 0.300 | 2 |
0.8 - 120 M_ M |
V, I | high mass loss for massive stars |
| 12 | e | 0.040 | 0.620 | 0.340 | 2 |
0.8 - 120 M_ M |
V, IV | high mass loss for massive stars |
| 13 | p | 0.001 | 0.756 | 0.243 | standard | 0.8 - 1.7 M_ M |
VI | including HB and EAGB |
| 14 | p | 0.020 | 0.680 | 0.300 | standard | 0.8 - 1.7 M_ M |
VI | including HB and EAGB |
| 15 | m | 0.001 | 0.756 | 0.243 | standard | 0.4 - 1.0 M_ M |
VIII | MHD equation of state |
| 16 | m | 0.020 | 0.700 | 0.280 | standard | 0.4 - 1.0 M_ M |
VIII | MHD equation of state |
| 17 | 0.020 | 0.680 | 0.300 | standard | 0.4 - 1.0 M_ M |
VIII | MHD equation of state | |
| Alternate and combined model sets: | ||||||||
| o | 0.0004 | 0.7584 | 0.2412 | 2 |
0.8 - 2.5 M_ M |
this paper | no overshooting: 1.25 M_ M |
|
| o | 0.001 | 0.756 | 0.243 | standard | 0.8 - 2.5 M_ M |
I | no overshooting: 1.25 M_ M |
|
| o | 0.004 | 0.744 | 0.252 | standard | 0.8 - 2.5 M_ M |
III | no overshooting: 1.25 M_ M |
|
| o | 0.008 | 0.728 | 0.264 | standard | 0.8 - 2.5 M_ M |
II | no overshooting: 1.25 M_ M |
|
| o | 0.020 | 0.680 | 0.300 | standard | 0.8 - 2.5 M_ M |
I | no overshooting: 1.25 M_ M |
|
| o | 0.040 | 0.620 | 0.340 | standard | 0.8 - 2.5 M_ M |
IV | no overshooting: 1.25 M_ M |
|
| l | 0.001 | 0.756 | 0.243 | standard | 0.4 - 2.5 M_ M |
combination: grids 15, 13, 2 | ||
| l | 0.020 | 0.680 | 0.300 | standard | 0.4 - 2.5 M_ M |
combination: grids 17, 14, 5 | ||
I : Schaller et al. (1992) V : Meynet et al. (1994)
II : Schaerer et al. (1993) VI : Charbonnel et al. (1996)
III : Charbonnel et al. (1993) VII : Mowlavi et al. (1998a)
IV : Schaerer et al. (1993) VIII : Charbonnel et al. (1999)
| Database | age range () | description | ||||
| ID | from | to | ||||
| (1) | (2) | (3) | (4) | (5) | ||
| Basic grids: | ||||||
| e | 0.0004 | 3.00 | 10.20 | basic grid | ||
| c | 0.001 | 3.00 | 10.20 | basic grid | ||
| c | 0.004 | 3.00 | 10.20 | basic grid | ||
| c | 0.008 | 3.00 | 10.20 | basic grid | ||
| c | 0.020 | 3.00 | 10.20 | basic grid | ||
| c | 0.040 | 3.00 | 10.20 | basic grid | ||
| c | 0.100 | 3.00 | 10.20 | basic grid | ||
| Extended grids: | ||||||
| e | 0.001 | 3.00 | 7.50 | high mass loss for massive stars | ||
| e | 0.004 | 3.00 | 7.50 | high mass loss for massive stars | ||
| e | 0.008 | 3.00 | 7.50 | high mass loss for massive stars | ||
| e | 0.020 | 3.00 | 7.50 | high mass loss for massive stars | ||
| e | 0.040 | 3.00 | 7.50 | high mass loss for massive stars | ||
| p | 0.001 | 9.00 | 10.20 | including HB and EAGB phases for low mass stars | ||
| p | 0.020 | 9.00 | 10.20 | including HB and EAGB phases for low mass stars | ||
| m | 0.001 | 9.00 | 10.30 | MHD equation of state for low mass stars | ||
| m | 0.020 | 9.00 | 10.30 | MHD equation of state for low mass stars | ||
| Alternate and combined model sets: | ||||||
| o | 0.0004 | 9.00 | 10.20 | no overshooting: 1.25 M_ M |
||
| o | 0.001 | 9.00 | 10.20 | no overshooting: 1.25 M_ M |
||
| o | 0.004 | 9.00 | 10.20 | no overshooting: 1.25 M_ M |
||
| o | 0.008 | 9.00 | 10.20 | no overshooting: 1.25 M_ M |
||
| o | 0.020 | 9.00 | 10.20 | no overshooting: 1.25 M_ M |
||
| o | 0.040 | 9.00 | 10.20 | no overshooting: 1.25 M_ M |
||
| l | 0.001 | 9.00 | 10.30 | combination ``best'' low mass star models | ||
| l | 0.020 | 9.00 | 10.30 | combination ``best'' low mass star models | ||
| File extension | description | |
| dat | Complete set of predicted surface stellar properties | |
| UBVRIJHKLM | Main stellar properties and photometric data for (UBV) |
|
| WFPC2 | Main stellar properties and photometric data for WFPC2 system | |
| geneva | Main stellar properties and photometric data for Geneva system | |
The physical ingredients have been discussed in papers I-VIII. For
completeness sake a brief summary of the basic assumptions common to
most model sets is presented here. Variations are discussed below.
1) OPAL and low temperature opacities of Kurucz (1991) or
Alexander & Ferguson (1994) are used.
2) The initial composition is derived from a linear
chemical enrichment law
with , and
3. for 0.02
and
2.5 for respectively.
3) Mass loss rates are taken from de Jager et al. (1998)
throughout the HR-diagram except on the red giant branch (RGB) and
early asymptotic giant branch (EAGB) for initial masses
_,
where the following expression is used (cf. Reimers 1975):
in units of M_ M
yr,
with at solar metallicity (see Maeder & Meynet 1989).
Mass loss is scaled with metallicity by
_,
except for Wolf-Rayet (WR) stars.
In the WR phases the relation of Langer (1989) for WNE and WC stars,
and
M_ M
yr for WNL stars is used.
4) Moderate core overshooting of
is
included for stars
_. For stars at
_ with
a small or absent convective core tracks with and without overshooting
are provided.
5)
In addition to the effects treated by Maeder & Meynet (1989), partial
ionisation of heavy elements is included in the equation of state.
6) Optically thick envelopes of WR stars are treated in the
framework of the modified Castor, Abbott & Klein (CAK, 1975) theory.
The above ingredients are used in grids 2-7 which cover the
metallicity range from to 0.100 (1/20 - 5 Z_ Z
). Grids 1
and 8-12 were calculated with mass loss rates enhanced by a factor of
2 during the MS, the pre-WR, and WNL phases for massive stars (range
indicated in col. 6); for lower masses the models are complemented
with the tracks from grids 2-6 or represent new calculations (grid 1;
see Appendix).
In grids 1-12, depending on the stellar mass range, the evolution is
in general followed up to the following phases: to the end of
C-burning for massive stars (
_), to the end of the early
asymptotic giant branch (EAGB) for intermediate mass stars (
_), and up to before the helium flash
for low mass stars (
_). Grids 13 and 14
(paper VI) present new calculations for the latter mass range at
metallicities and 0.001 including post-helium flash models,
i.e. covering the horizontal branch (HB) and EAGB phases. The
post-helium flash tracks do not include overshooting and
semi-convection.
The MHD (Mihalas, Hummer & Däppen, 1988) equation of state was used
for the low mass models of paper VIII (grids 15, 16, 17). The
calculations in grids 15-17 are followed up to before the helium flash
or ages larger than the Hubble time ( 20 Gyr). Note that the
solar metallicity grid 16 uses a different composition than the
remaining grids.
The present compilation includes stellar models covering a very large parameter space in terms of mass, metallicity, and evolutionary phases. However, we wish to stress again that e.g. the following evolutionary phases are not covered: 1) pre-main sequence tracks (for Geneva models see Bernasconi 1996 and paper VIII), 2) thermally pulsing AGB stars, and 3) post-AGB stars and white dwarfs. Other phases (e.g. horizontal branch) are given only for a subset of metallicities. These limitations should be recognized by the user of the database. Calculations from other groups partly including such phases are mentioned in Section 4.