Grids of stellar models with rotation - III. Models from 0.8 to 120 Msun at a metallicity Z = 0.002

• Published in: arXiv.org 2013-08
• Main Authors: Georgy, Cyril, Ekström, Sylvia, Eggenberger, Patrick, Meynet, Georges, Haemmerlé, Lionnel, Maeder, André, Granada, Anahí, Groh, José H, Hirschi, Raphael, Mowlavi, Nami, Yusof, Norhasliza, Charbonnel, Corinne, Decressin, Thibaut, Barblan, Fabio
• Format: Article
• Language: English
• Subjects: Astronomical models; B stars; Diffusion coefficient; Enrichment; Hertzsprung-Russell diagram; Luminosity; Magellanic clouds; Metallicity; Red giant stars; Stellar evolution; Stellar models; Stellar rotation; Supergiant stars
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.1308.2914

(shortened) We provide a grid of single star models covering a mass range from 0.8 to 120 Msun with an initial metallicity Z = 0.002 with and without rotation. We discuss the impact of a change in the metallicity by comparing the current tracks with models computed with exactly the same physical ingredients but with a metallicity Z = 0.014 (solar). We show that the width of the main-sequence (MS) band in the upper part of the Hertzsprung-Russell diagram (HRD), for luminosity above log(L/Lsun) > 5.5, is very sensitive to rotational mixing. Strong mixing significantly reduces the MS width. We confirm, but here for the first time on the whole mass range, that surface enrichments are stronger at low metallicity provided that comparisons are made for equivalent initial mass, rotation and evolutionary stage. We show that the enhancement factor due to a lowering of the metallicity (all other factors kept constant) increases when the initial mass decreases. Present models predict an upper luminosity for the red supergiants (RSG) of log (L/Lsun) around 5.5 at Z = 0.002 in agreement with the observed upper limit of RSG in the Small Magellanic Cloud. We show that models using shear diffusion coefficient calibrated to reproduce the surface enrichments observed for MS B-type stars at Z = 0.014 can also reproduce the stronger enrichments observed at low metallicity. In the framework of the present models, we discuss the factors governing the timescale of the first crossing of the Hertzsprung gap after the MS phase. We show that any process favouring a deep localisation of the H-burning shell (steep gradient at the border of the H-burning convective core, low CNO content) and/or the low opacity of the H-rich envelope favour a blue position in the HRD for the whole or at least a significant fraction of the core He-burning phase.