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A large sample of carbon enhanced metal-poor stars enriched in s-process elements (CEMP-s) have been observed in the Galactic halo. These stars of low mass (M ~ 0.9 Msun) are located on the main-sequence or the red giant phase, and do not…

Solar and Stellar Astrophysics · Physics 2015-05-18 S. Bisterzo , R. Gallino , O. Straniero , S. Cristallo , F. Kaeppeler

About a quarter of all post-asymptotic giant branch (AGB) stars are hydrogen-deficient. Stellar evolutionary models explain the carbon-dominated H-deficient stars by a (very) late thermal pulse scenario where the hydrogen-rich envelope is…

Solar and Stellar Astrophysics · Physics 2014-07-02 N. Reindl , T. Rauch , K. Werner , J. W. Kruk , H. Todt

By considering the various CEMP subclasses separately, we try to derive, from the specific signatures imprinted on the abundances, parameters (such as metallicity, mass, temperature, and neutron source) characterizing AGB nucleosynthesis…

Solar and Stellar Astrophysics · Physics 2015-05-13 T. Masseron , J. A. Johnson , B. Plez , S. Van Eck , F. Primas , S. Goriely , A. Jorissen

Stars with initial masses 7 Msun . MZAMS . 9 Msun reach temperatures high enough to ignite C under degenerate conditions after the end of He-core burning (Garcia-Berro & Iben 1994). These isolated stars are expected to evolve into the…

Solar and Stellar Astrophysics · Physics 2023-04-20 F. C. De Gerónimo , M. M. Miller Bertolami , M. Catelan , T. Battich

We have computed detailed evolution and nucleosynthesis models for super and massive AGB stars over the mass range 6.5-9.0 Msun in divisions of 0.5 Msun with metallicities Z=0.02, 0.008 and 0.004. These calculations, in which we find third…

Solar and Stellar Astrophysics · Physics 2015-06-17 Carolyn L. Doherty , Pilar Gil-Pons , Herbert H. B Lau , John C. Lattanzio , Lionel Siess

We briefly review the main problems related to the computation of the evolution of intermediate-mass stars: the treatment of turbulent convection and the occurrence of blue loops during the core He-burning phase. It is shown that, in order…

Astrophysics · Physics 2007-05-23 S. Cassisi

We discuss the synthesis of some short-lived isotopes and of 23Na in thermally pulsing AGB stars with initial mass of 2 Msun and two different metallicities (Z=1.5e-2, corresponding to the metal amount in the Sun, and Z=1e-4),…

Astrophysics · Physics 2007-05-23 S. Cristallo , R. Gallino , O. Straniero , L. Piersanti , I. Dominguez

In our current galaxy formation paradigm, high-redshift galaxies are predominantly fuelled by accretion of cool, metal-poor gas from the intergalactic medium. Hydrodynamical simulations predict that this material should be observable in…

Cosmology and Nongalactic Astrophysics · Physics 2015-06-16 Neil H. M. Crighton , Joseph F. Hennawi , J. Xavier Prochaska

Context: Miras are long-period variables thought to be in the asymptotic giant branch (AGB) phase of evolution. In about one percent of known Miras, the pulsation period is changing. It has been speculated that this changing period is the…

Very-low-mass stars can develop secularly unstable hydrogen-burning shells late in their life. Since the thermal pulses that go along are driven at the bottoms of very shallow envelopes, the stars' luminosities and effective temperatures…

Solar and Stellar Astrophysics · Physics 2013-03-28 Alfred Gautschy

We investigate the physical and chemical evolution of population II stars with initial masses in the range 6.5-8 Msun, which undergo an off centre carbon ignition under partially degenerate conditions, followed by a series of thermal…

Solar and Stellar Astrophysics · Physics 2010-09-24 Paolo Ventura , Francesca D'Antona

Intermediate mass stellar evolution tracks from the main sequence to the tip of the AGB for five initial masses (2 to 6Msun) and metallicity Z=0.0001 have been computed. The detailed 1D structure and evolution models include exponential…

Astrophysics · Physics 2016-08-30 Falk Herwig

The influence of extended convective mixing (overshoot) on asymptotic giant branch stellar evolution is investigated in detail. The extended mixing is treated time-dependently, and the efficiency declines exponentially with the geometric…

Astrophysics · Physics 2007-05-23 Falk Herwig

We present a review of the main phases of stellar evolution with particular emphasis on the nucleosynthesis and mixing mechanisms in low- and intermediate-mass stars. In addition to explicit studies of the effects of the first, second and…

Astrophysics · Physics 2009-10-30 John C. Lattanzio , Arnold I. Boothroyd

Thermal pulses are fundamental to the chemical evolution of AGB stars and their circumstellar envelopes. A further consequence of thermal pulses is the formation of detached shells of gas and dust around the star. We aim to determine the…

Solar and Stellar Astrophysics · Physics 2016-01-20 M. Maercker , W. H. T. Vlemmings , M. Brunner , E. De Beck , E. M. Humphreys , F. Kerschbaum , M. Lindqvist , H. Olofsson , S. Ramstedt

We study the asymptotic giant branch (AGB) evolution of stars with masses between $1~M_{\odot} - 8.5~M_{\odot}$. We focus on stars with a solar chemical composition, which allows us to interpret evolved stars in the Galaxy. We present a…

Solar and Stellar Astrophysics · Physics 2018-02-14 P. Ventura , A. Karakas , F. Dell'Agli , D. A. García-Hernández , L. Guzman-Ramirez

The studies focused on the Thermally-Pulsing Asymptotic Giant Branch phase experienced by low- and intermediate-mass stars are extremely important in many astrophysical contexts. In particular, a detailed computation of their chemical…

Solar and Stellar Astrophysics · Physics 2015-05-13 Paolo Ventura , Paola Marigo

A linear nonadiabatic analysis of the vibrational stability of population III main-sequence stars was carried out. It was demonstrated that, in the case of massive stars with $M \gtrsim 5\Mo$, helium burning (triple alpha reaction) starts…

Solar and Stellar Astrophysics · Physics 2015-06-04 Takafumi Sonoi , Hiromoto Shibahashi

Much of the interstellar medium in disk galaxies is in the form of neutral atomic hydrogen, H I. This gas can be in thermal equilibrium at relatively low temperatures, T < 300 K (the cold neutral medium, or CNM) or at temperatures somewhat…

Astrophysics · Physics 2009-11-07 M. G. Wolfire , C. F. McKee , D. Hollenbach , A. G. G. M. Tielens

The now extinct 205Pb is a pure s-process radionuclide (t_{1/2} = 1.5x10^7 y) of possible substantial cosmochemical interest. As a necessary complement to the detailed theoretical study of the nuclear physics and astrophysics aspects of the…

Astrophysics · Physics 2007-05-23 Nami Mowlavi , Stephane Goriely , Marcel Arnould
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