Two-dimensional simulations of pulsational pair-instability supernovae

Massive stars that end their lives with helium cores in the range of 35-65 M ☉ are known to produce repeated thermonuclear outbursts due to a recurring pair-instability. In some of these events, solar masses of material are ejected in repeated outbursts of several × 1050 erg each. Collisions between...

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Bibliographic Details
Main Authors: Chen, Ke-Jung (Author) , Woosley, Stan (Author) , Heger, Alexander (Author) , Almgren, Ann (Author) , Whalen, Daniel J. (Author)
Format: Article (Journal)
Language:English
Published: [2014 September 1]
In: The astrophysical journal
Year: 2014, Volume: 792, Issue: 1
ISSN:1538-4357
DOI:10.1088/0004-637X/792/1/28
Online Access:Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1088/0004-637X/792/1/28
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Author Notes:Ke-Jung Chen, Stan Woosley, Alexander Heger, Ann Almgren, and Daniel J. Whalen
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Summary:Massive stars that end their lives with helium cores in the range of 35-65 M ☉ are known to produce repeated thermonuclear outbursts due to a recurring pair-instability. In some of these events, solar masses of material are ejected in repeated outbursts of several × 1050 erg each. Collisions between these shells can sometimes produce very luminous transients that are visible from the edge of the observable universe. Previous one-dimensional (1D) studies of these events produce thin, high-density shells as one ejection plows into another. Here, in the first multi-dimensional simulations of these collisions, we show that the development of a Rayleigh-Taylor instability truncates the growth of the high-density spike and drives mixing between the shells. The progenitor is a 110 M ☉ solar-metallicity star that was shown in earlier work to produce a superluminous supernova. The light curve of this more realistic model has a peak luminosity and duration that are similar to those of 1D models but a structure that is smoother.
Item Description:Gesehen am 16.09.2020
Physical Description:Online Resource
ISSN:1538-4357
DOI:10.1088/0004-637X/792/1/28