4.7 Article

A Diversity of Wave-driven Presupernova Outbursts

Journal

ASTROPHYSICAL JOURNAL
Volume 906, Issue 1, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.3847/1538-4357/abc87c

Keywords

Circumstellar matter; Massive stars; Stellar mass loss; Stellar oscillations; Supernovae

Funding

  1. NASA [HST-AR-15021.001-A, 80NSSC18K1017]
  2. Rose Hills Foundation
  3. Sloan Foundation [FG-2018-10515]

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The passage discusses the process of wave energy transport in core-collapse supernova progenitors, finding that waves excited during oxygen/neon burning stages can transmit substantial energy before core collapse. Different mass progenitors exhibit variations in wave energy transmission, with low-mass and high-mass progenitors showing distinct characteristics in transmitting wave energy.
Many core-collapse supernova (SN) progenitors show indications of enhanced pre-SN mass loss and outbursts, some of which could be powered by wave energy transport within the progenitor star. Depending on the star's structure, convectively excited waves driven by late-stage nuclear burning can carry substantial energy from the core to the envelope, where the wave energy is dissipated as heat. We examine the process of wave energy transport in single-star SNe progenitors with masses between 11 and 50 M. Using MESA stellar evolution simulations, we evolve stars until core collapse and calculate the wave power produced and transmitted to the stars' envelopes. These models improve upon prior efforts by incorporating a more realistic wave spectrum and nonlinear damping effects, reducing our wave-heating estimates by similar to 1 order of magnitude compared to prior work. We find that waves excited during oxygen/neon burning typically transmit similar to 10(46)-10(47) erg of energy at 0.1-10 yr before core collapse in typical (M M) SN progenitors. High-mass progenitors can often transmit similar to 10(47)-10(48) erg of energy during oxygen/neon burning, but this tends to occur later, at about 0.01-0.1 yr before core collapse. Pre-SN outbursts may be most pronounced in low-mass SN progenitors (M less than or similar to 12 M) undergoing semidegenerate neon ignition and in high-mass progenitors (M greater than or similar to 30 M) exhibiting convective shell mergers.

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