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M. Limongi

Publications and source records attributed to M. Limongi.

42 records · Page 3Linked to original sources

The Implications of the New Z=0 Stellar Models and Yields on the Early Metal Pollution of the Intergalactic Medium

Motivated by the recent detection of metals in different components of the high redshift universe and by the abundance ratios measured in the extremely metal-poor stars of our Galaxy, we study the nucleosynthesis constraints that this imposes on an early generation of stars (Population III). To do so we take into account the chemical yields obtained from homogeneous evolutionary calculations of zero metal stars in the mass range $3\la m/M_\odot\la 40$ (Limongi et al. 2000, Chieffi et al. 2001). We also consider the role played by metal-free very massive objects (m$>100$ M$_\odot$). Using both analytical and numerical chemical evolution models, we confront model predictions from the different choices of the mass function proposed for Population III with the observational constraints. We show that low values of star formation efficiency ($<1%$) are required so as not to exceed the minimum metallicity ([C/H]$\approx -2.4$) measured in the high redshift systems for any of the IMFs proposed. We also show that the observational constraints require $Ω_{sr}< 3\times 10^{-3}Ω_b$, confirming previous claims that the possible contribution of the stellar remnants from Population III to the baryonic dark matter is insignificant. At present, however, the scarcity of abundance measurements for high redshift systems does not permit us to put severe limitations on the nature of the initial mass function for Population III. In fact, overabundances of alpha-elements with respect to iron of the order of those measured in damped Lyman-$α$ systems are obtained for any of the IMFs tested. Nevertheless, to account for the very large [C,N/Fe] ratios found in a considerable number of extremely metal-poor stars of our Galaxy, an IMF peaking at the intermediate stellar mass range (4-8 M$_\odot$) is needed.

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Extreme Type IIp Supernovae as Yardsticks for Cosmology

Evolutionary effects with redshift of core collapse supernovae and their application to cosmology have been studied based on an extensive grid of stellar models between 13 and 25 Mo, and their light curves after the explosion. With decreasing metallicity Z and increasing mass, progenitors tend to explode as compact Blue Supergiants (BSG) and produce subluminous supernovae which are about 1.5 mag. dimmer compared to 'normal' SNeII with Red Supergiant (RSG) progenitors. Progenitors with small masses tend to explode as RSGs even with low Z. The consequences are obvious for probing the chemical evolution. We identify 'extreme SNe IIp' supernovae as a rather homogeneous class which may allow their use as standard candles for distance determination accurate within 30 %. Due to their unique light curves, no spectra need to be taken for their identification, and follow-up observations can be limited to a very small dynamical range in brightness. This means that distance determination by 'extreme SNe IIp" are possible up to redshifts of about 3 using 8-meter class telescopes. SIRTIF may push the limit by another magnitude.

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Massive Stars in the Range $\rm 13-25 M_\odot$: Evolution and Nucleosynthesis. II. the Solar Metallicity Models

We present the evolutionary properties of a set of massive stellar models (namely 13, 15, 20 and 25 $\rm M_\odot$) from the main sequence phase up to the onset of the iron core collapse. All these models have initial solar chemical composition, i.e. Y=0.285 and Z=0.02. A 179 isotope network, extending from neutron up to $\rm ^{68}Zn$ and fully coupled to the evolutionary code has been adopted from the Carbon burning onward. Our results are compared, whenever possible, to similar computations available in literature.

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Do zero metal intermediate mass stars experience thermal pulses?

We have studied the evolution of intermediate mass (M.ge.5Mo) zero metal (Z=0) stars with particular attention to the AGB phase. At variance with previous claims we find that these stars experience thermal instability (the so called thermal pulses). The critical quantity which controls the onset of a thermally pulsing phase is the amount of CNO in the envelope during the AGB. For these stars the central He burning starts in the blue side of the HR diagram and the 1^{st} dredge up does not take place. Then the envelope maintains its initial composition up to the beginning of the AGB phase. However, during the early AGB the 2^{nd} dredge-up occurs and fresh He and CNO elements are engulfed in the convective envelope. We find that in stars with M.ge.6Mo the resulting amount of ^{12}C is large enough to sustain a normal CNO burning within the H shell and consequently the star enters the usual thermal pulse phase. In the 5Mo model, owing to the lower ^{12}C enhancement in the envelope after the 2^{nd} dredge-up, the He burning shell suffers weak thermal instabilities. 9 of these thermal oscillation are needed before the He burning luminosity reaches 3x10^5 Lo and a first convective shell develops in between the two burning shells. Later on a second convective shell forms at the base of the H rich envelope. This convective zone cross the H/He discontinuity and partially overlaps the previous one, dredging up fresh ^{12}C. After a huge H flash, a quiescent CNO burning settle on. From this moment a thermal pulse phase starts, which is very similar to the one experienced by the more massive models.

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The giant, horizontal and asymptotic branches of galactic globular clusters. I. The catalog, photometric observables and features

A catalog including a set of the most recent Color Magnitude Diagrams (CMDs) is presented for a sample of 61 Galactic Globular Clusters (GGCs). We used this data-base to perform an homogeneous systematic analysis of the evolved sequences (namely, Red Giant Branch (RGB), Horizontal Branch (HB) and Asymptotic Giant Branch (AGB)). Based on this analysis, we present: (1) a new procedure to measure the level of the ZAHB (V_ZAHB) and an homogeneous set of distance moduli obtained adopting the HB as standard candle; (2) an independent estimate for RGB metallicity indicators and new calibrations of these parameters in terms of both spectroscopic ([Fe/H]_CG97) and global metallicity ([M/H], including also the alpha-elements enhancement). The set of equations presented can be used to simultaneously derive a photometric estimate of the metal abundance and the reddening from the morphology and the location of the RGB in the (V,B-V)-CMD. (3) the location of the RGB-Bump (in 47 GGCs) and the AGB-Bump (in 9 GGCs). The dependence of these features on the metallicity is discussed. We find that by using the latest theoretical models and the new metallicity scales the earlier discrepancy between theory and observations (~0.4 mag) completely disappears.

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