Journal
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 433, Issue 2, Pages 1114-1132Publisher
OXFORD UNIV PRESS
DOI: 10.1093/mnras/stt794
Keywords
stars: evolution; stars: massive; stars: mass-loss
Categories
Funding
- Ministry of Higher Education
- University of Malaya
- Commonwealth Scholarship Commission at Keele University
- World Premier International Research Center Initiative (WPI Initiative), MEXT, Japan
- Eurogenesis EUROCORE programme
- European Research Council under the European Union [306901]
- Ministry of Higher Education of Malaysia [FRGS/FP009-2012A]
- Science and Technology Facilities Council [PP/D000955/1, ST/J000035/1, ST/J001589/1, PP/F000057/1, ST/G002355/1, ST/J001384/1] Funding Source: researchfish
- STFC [ST/J000035/1, PP/F000057/1, ST/J001384/1, ST/J001589/1, ST/G002355/1, PP/D000955/1] Funding Source: UKRI
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There is observational evidence that supports the existence of very massive stars (VMS) in the local universe. First, VMS (M-ini less than or similar to 320 M-circle dot) have been observed in the Large Magellanic Clouds (LMC). Secondly, there are observed supernovae (SNe) that bear the characteristics of pair creation supernovae (PCSNe, also referred to as pair instability SN) which have VMS as progenitors. The most promising candidate to date is SN 2007bi. In order to investigate the evolution and fate of nearby VMS, we calculated a new grid of models for such objects, for solar, LMC and Small Magellanic Clouds (SMC) metallicities, which covers the initial mass range from 120 to 500 M-circle dot. Both rotating and non-rotating models were calculated using the geneva stellar evolution code and evolved until at least the end of helium burning and for most models until oxygen burning. Since VMS have very large convective cores during the main-sequence phase, their evolution is not so much affected by rotational mixing, but more by mass loss through stellar winds. Their evolution is never far from a homogeneous evolution even without rotational mixing. All the VMS, at all the metallicities studied here, end their life as WC(WO)-type Wolf-Rayet stars. Because of very important mass losses through stellar winds, these stars may have luminosities during the advanced phases of their evolution similar to stars with initial masses between 60 and 120 M-circle dot. A distinctive feature which may be used to disentangle Wolf-Rayet stars originating from VMS from those originating from lower initial masses would be the enhanced abundances of Ne and Mg at the surface of WC stars. This feature is however not always apparent depending on the history of mass loss. At solar metallicity, none of our models is expected to explode as a PCSN. At the metallicity of the LMC, only stars more massive than 300 M-circle dot are expected to explode as PCSNe. At the SMC metallicity, the mass range for the PCSN progenitors is much larger and comprises stars with initial masses between about 100 and 290 M-circle dot. All VMS in the metallicity range studied here produce either a Type Ib SN or a Type Ic SN but not a Type II SN. We estimate that the progenitor of SN 2007bi, assuming a SMC metallicity, had an initial mass between 160 and 175 M-circle dot. None of models presented in this grid produces gamma-ray bursts or magnetars. They lose too much angular momentum by mass loss or avoid the formation of a black hole by producing a completely disruptive PCSN.
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