Evolution of rotating massive stars adopting a newer, self-consistent wind prescription at Small Magellanic Cloud metallicity

被引:5
作者
Gormaz-Matamala, A. C. [1 ,2 ,3 ]
Cuadra, J. [2 ]
Ekstrom, S. [4 ]
Meynet, G. [4 ]
Cure, M. [5 ]
Belczynski, K. [1 ]
机构
[1] Polish Acad Sci, Nicolaus Copernicus Astron Ctr, Bartycka 18, PL-00716 Warsaw, Poland
[2] Univ Adolfo Ibanez, Fac Artes Liberales, Dept Ciencias, Ave Padre Hurtado 750, Vina Del Mar, Chile
[3] Pontificia Univ Catolica Chile, Fac Fis, Inst Astrofis, Santiago 7820436, Chile
[4] Univ Geneva, Geneva Observ, Maillettes 51, CH-1290 Sauverny, Switzerland
[5] Univ Valparaiso, Inst Fis & Astron, Ave Gran Bretana 1111,Casilla 5030, Valparaiso, Chile
基金
瑞士国家科学基金会; 欧洲研究理事会;
关键词
stars: evolution; stars: massive; stars: mass-loss; stars: rotation; stars: winds; outflows; Magellanic Clouds; RADIATION-DRIVEN WINDS; WOLF-RAYET STARS; O-TYPE STARS; STELLAR EVOLUTION; LOSS RATES; CLUMPING PREDICTIONS; CHEMICAL-COMPOSITION; COOL SUPERGIANTS; MODELS; HOT;
D O I
10.1051/0004-6361/202449782
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Aims. We aim to measure the impact of our mass-loss recipe in the evolution of massive stars at the metallicity of the Small Magellanic Cloud (SMC). Methods. We used the Geneva-evolution code (GENEC) to run evolutionary tracks for stellar masses ranging from 20 to 85 M-circle dot at SMC metallicity (Z(SMC) = 0.002). We upgraded the recipe for stellar winds by replacing Vink's formula with our self-consistent m-CAK prescription, which reduces the value of the mass-loss rate, (M) over dot, by a factor of between two and six depending on the mass range. Results. The impact of our new [weaker] winds is wide, and it can be divided between direct and indirect impact. For the most massive models (60 and 85 M-circle dot) with (M) over dot greater than or similar to 2 x 10(-7) M-circle dot yr(-1), the impact is direct because lower mass loss make stars remove less envelope, and therefore they remain more massive and less chemically enriched at their surface at the end of their main sequence (MS) phase. For the less massive models (20 and 25 M-circle dot) with (M) over dot less than or similar to 2 x 10(-8) M-circle dot yr(-1), the impact is indirect because lower mass loss means the stars keep high rotational velocities for a longer period of time, thus extending the H-core burning lifetime and subsequently reaching the end of the MS with higher surface enrichment. In either case, given that the conditions at the end of the H-core burning change, the stars will lose more mass during their He-core burning stages anyway. For the case of M-zams = 20-40 M-circle dot, our models predict stars will evolve through the Hertzsprung gap, from O-type supergiants to blue supergiants (BSGs), and finally red supergiants (RSGs), with larger mass fractions of helium compared to old evolution models. New models also sets the minimal initial mass required for a single star to become a Wolf-Rayet (WR) at metallicity Z = 0.002 at M-zams = 85 M-circle dot. Conclusions. These results reinforce the importance of upgrading mass-loss prescriptions in evolution models, in particular for the earlier stages of stellar lifetime, even for Z << Z(circle dot). New values for (M) over dot need to be complemented with upgrades in additional features such as convective-core overshooting and distribution of rotational velocities, besides more detailed spectroscopical observations from projects such as XShootU, in order to provide a robust framework for the study of massive stars at low-metallicity environments.
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页数:11
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