Grids of stellar models with rotation VII: models from 0.8 to 300 M⊙ at supersolar metallicity (Z = 0.020)

Author:

Yusof Norhasliza1ORCID,Hirschi Raphael23,Eggenberger Patrick4,Ekström Sylvia4ORCID,Georgy Cyril4,Sibony Yves4ORCID,Crowther Paul A5,Meynet Georges4,Kassim Hasan Abu1,Harun Wan Aishah Wan1,Maeder André4,Groh Jose H6,Farrell Eoin6ORCID,Murphy Laura6

Affiliation:

1. Department of Physics, Faculty of Science, University of Malaya , 50603 Kuala Lumpur, Malaysia

2. Astrophysics Group, Keele University , Keele, Staffordshire ST5 5BG, UK

3. Institute for Physics and Mathematics of the Universe (WPI), University of Tokyo , 5-1-5 Kashiwanoha, Kashiwa 277-8583, Japan

4. Department of Astronomy, University of Geneva , Chemin Pegasi 51, CH-1290 Versoix, Switzerland

5. Department of Physics & Astronomy, University of Sheffield , Hounsfield Road, Sheffield S3 7RH, UK

6. School of Physics, Trinity College Dublin, The University of Dublin , College Green, Dublin 2, Ireland

Abstract

ABSTRACT We present a grid of stellar models at supersolar metallicity (Z = 0.020) extending the previous grids of Geneva models at solar and sub-solar metallicities. A metallicity of Z = 0.020 was chosen to match that of the inner Galactic disc. A modest increase of 43 per cent (= 0.02/0.014) in metallicity compared to solar models means that the models evolve similarly to solar models but with slightly larger mass-loss. Mass-loss limits the final total masses of the supersolar models to 35 M⊙ even for stars with initial masses much larger than 100 M⊙. Mass-loss is strong enough in stars above 20 M⊙ for rotating stars (25 M⊙ for non-rotating stars) to remove the entire hydrogen-rich envelope. Our models thus predict SNII below 20 M⊙ for rotating stars (25 M⊙ for non-rotating stars) and SNIb (possibly SNIc) above that. We computed both isochrones and synthetic clusters to compare our supersolar models to the Westerlund 1 (Wd1) massive young cluster. A synthetic cluster combining rotating and non-rotating models with an age spread between log10(age/yr) = 6.7 and 7.0 is able to reproduce qualitatively the observed populations of WR, RSG, and YSG stars in Wd1, in particular their simultaneous presence at $\log _{10}(L/\mathit {\mathrm{ L}}_{\odot })$ = 5–5.5. The quantitative agreement is imperfect and we discuss the likely causes: synthetic cluster parameters, binary interactions, mass-loss and their related uncertainties. In particular, mass-loss in the cool part of the HRD plays a key role.

Funder

Ministry of Higher Education, Malaysia

Keele University

MEXT

STFC

European Union

Horizon 2020

National Science Foundation

European Cooperation in Science and Technology

European Research Council

Irish Research Council

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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