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Several
model predictions for studying old and intermediate-aged stellar populations
are provided here. The models
are described in these papers:
|
Reference |
Main model predictions |
|
Vazdekis
et al. 1996 (ApJS,107,306) |
Broadband
colours, mass-to-light ratios and absorption line-strengths at low spectral
resolution for single burst (SSPs) stellar
populations and full chemo-evolutionary models |
|
Vazdekis
1999 (ApJ,513,224) |
SSPs spectral energy
distributions (SEDs) at moderately high resolution
(FWHM=1.8Å) in the optical range |
|
Blakeslee, Vazdekis & Ajhar 2001(MNRAS,320,193) |
Broadband
and WFPC2 HST filter system colours and surface brightness fluctuations |
|
Vazdekis
et al. 2003 (MNRAS,
340,1317) |
Near-IR
SEDs around the CaII
triplet region at resolution 1.5Å (FWHM) and Ca II triplet and Paschen line-strengths |
| Vazdekis et al. 2009 (in preparation) | SSPs spectral energy distributions at resolution (FWHM=2.3Å) in the optical range based on MILES stellar library |
The
main model ingredients are:
·
Initial Mass Function. We adopt the IMF shapes described in Vazdekis et al. 1996 (i.e unimodal and bimodal) and the two IMFs
of Kroupa 2001 (MNRAS,322,231):
o
Unimodal: a power-law function characterized by its slope as a free parameter. The
standard Salpeter (1955) IMF is obtained when the
slope value is 1.3.
o
Bimodal:
similar to the unimodal IMF for stars with masses
above 0.6 Mo, but decreasing the number of the stars with lower masses by means of a transition to a shallower slope. Its
slope is the only free parameter (as in the unimodal
case).
o
Kroupa (2001) universal: a multi-part power-law IMF, which is similar
to the Salpeter (1955) IMF for stars of masses above
0.5 Mo, but with a decreasing contribution of lower masses by means
of two flatter segments.
o
Kroupa (2001) revised: a multi-part power-law IMF, in which the
systematic effects due to unresolved binaries on the single-star IMF have been
taken into account.
·
Theoretical isochrones. We use the homogeneous set of scaled-solar isochrones of Girardi et al. (A&AS,141,371),
whereas in Vazdekis et al. 1996 and Vazdekis 1999 we used the Bertelli
et al. 1994 (A&AS,106,275) and the stellar tracks of Pols
et al. 1995 (MNRAS,274,964) for the very low-mass stars. The Girardi et al. isochrones cover a wide range of ages and metallicities and include the latest stages of the stellar
evolution through the thermally pulsing AGB regime to the point of complete
envelope ejection (employing a synthetic prescription). It is worth to note
that the largest metallicity covered is Z=0.03
(instead of Z=0.05, as in Bertelli et al set). Solar metallicity value is Z=0.019. The input physics of the
isochrones have been updated with an improved version of the equation of state,
the opacities of Alexander & Ferguson 1994 (ApJ,437,879)
and a milder convective overshoot scheme with respect to the Bertelli et al. set.
·
Stellar photometric libraries are used to transform the theoretical
parameters of the isochrones to magnitudes and colours. We use extensive
empirical (not theoretical) stellar libraries to obtain each colour as a function
of temperature, metallicity and gravity. We use the metallicity-dependent relations of Alonso, Arribas & Martinez-Roger (1996,1999)
(A&A,117,227; A&AS,140,261) for dwarfs and giants respectively. This
treatment for the giants is the most important difference with respect to the
models of Vazdekis et al (1996), where we used the calibrations of
Ridgway et al. 1980 (ApJ,235,126) and Johnson 1966 (ARA&A,4,193). The
empirical (not the theoretical) compilation of Lejeune,
Cuisinier & Buser
(1997, 1998) (A&AS,125,229; A&AS,130,65) are used for the coolest and
hottest dwarfs (Teff<4000K) and giants (Teff<3500K), respectively, for solar metallicity;
a semi-empirical approach was applied to other metallicities
on the basis of these relations and the model atmospheres of Bessell et al. (1989,1991) (A&AS,77,1; A&AS,89,335)
and the library of Fluks et al. 1994
(A&AS,105,311). We use the metal-dependent bolometric corrections given by
Alonso, Arribas & Martinez-Roger (1995,1999) (A&A,297,197; A&AS,140,261) for dwarfs and
giants, respectively. For the Sun we adopt the bolometric correction -0.12,
with a bolometric magnitude of 4.70.
· Stellar spectral libraries. Extensive empirical stellar libraries are used to predict the spectral properties of the stellar populations. Two set of predictions are computed:
o
A
number of absorption line-strengths computed on the basis of the, so-called,
empirical fitting functions. These functions describe the strengths of,
previously defined, spectral features in terms of the main atmospheric
parameters. 25 absorption features at resolution (FWHM~9Å) are calculated on
the instrumental dependent LICK/IDS SYSTEM using the fitting functions of Worthey et al. 1994 (ApJS,94,687) and Worthey
& Ottaviani 1997 (ApJS,111,377). The break at
4000A is calculated using the fitting functions of Gorgas et al. 1999 (A&AS,139,29). Using the fitting functions of Cenarro et al. 2002 we compute the CaII
triplet feature around ~8600A at resolution 1.5Å (FWHM) and flux-calibration
response curve.
o
Spectral
energy distributions (with flux-calibrated response curve) at moderately
high resolution are computed for the optical range at FWHM=1.8Å on the basis of
the stellar spectral library of Jones 1999 (PhD thesis, Univ. North Carolina at
Chapel Hill) and MILES (Sánchez-Blázquez et al. 2006) at
FWHM=2.3Å, and for the near-IR around the CaII
triplet feature at resolution 1.5Å (FWHM) using the stellar library of Cenarro et al. (2001).
The
models provide predictions for:
·
SINGLE AGE SINGLE METALLICITY,
STELLAR POPULATIONS, SSPs, i.e. Simple Stellar Populations or
instantaneous bursts.
·
FULL CHEMO-EVOLUTIONARY POPULATION
SYNTHESIS,
following the evolution of a galaxy from an initial gas cloud to the present
time. For the latter, no initial metallicity is
assumed, since it is derived from the IMF, the Star Formation Rate and the Age.
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