4.7 Article

Partial stellar explosions - ejected mass and minimal energy

Journal

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY
Volume 501, Issue 3, Pages 4266-4275

Publisher

OXFORD UNIV PRESS
DOI: 10.1093/mnras/staa3969

Keywords

hydrodynamics; shock waves; stars: mass-loss

Funding

  1. Adams Fellowship
  2. ISF
  3. Rose Hills Foundation
  4. Sloan Foundation [FG-2018-10515]

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The study reveals enhanced mass-loss in late stages of evolution for massive stars, and analyzes the impact of explosion energy on ejecta mass. A minimum ejecta mass corresponding to a minimum energy is found across different progenitors. The results show that the minimum ejecta mass varies considerably among different progenitors, but is almost independent of stellar radius.
Many massive stars appear to undergo enhanced mass-loss during late stages of their evolution. In some cases, the ejected mass likely originates from non-terminal explosive outbursts, rather than continuous winds. Here we study the dependence of the ejecta mass, mej, on the energy budget E of an explosion deep within the star, using both analytical arguments and numerical hydrodynamics simulations. Focusing on polytropic stellar models, we find that for explosion energies smaller than the stellar binding energy, the ejected mass scales as m(ej) proportional to E-epsilon m, where epsilon(m) = 2.4-3.0 depending on the polytropic index. The loss of energy due to shock breakout emission near the stellar edge leads to the existence of a minimal mass-shedding explosion energy, corresponding to a minimal ejecta mass. For a wide range of progenitors, from Wolf-Rayet stars to red supergiants (RSGs), we find a similar limiting energy of E-min similar to 10(46)-10(47) erg, almost independent of the stellar radius. The corresponding minimal ejecta mass varies considerably across different progenitors, ranging from similar to 10(-8)M(circle dot) in compact stars, up to similar to 10(-2)M(circle dot) in RSGs. We discuss implications of our results for pre-supernova outbursts driven by wave heating, and complications caused by the non-constant opacity and adiabatic index of realistic stars.

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