Hydrodynamic simulations of electron-capture supernovae: progenitor and dimension dependence

Author:

Zha Shuai1ORCID,O’Connor Evan P2ORCID,Couch Sean M345ORCID,Leung Shing-Chi6ORCID,Nomoto Ken’ichi7ORCID

Affiliation:

1. Tsung-Dao Lee Institute, Shanghai Jiao Tong University , Shanghai 200240, People’s Republic of China

2. The Oskar Klein Centre, Department of Astronomy, Stockholm University , AlbaNova, SE-106 91 Stockholm, Sweden

3. Department of Physics and Astronomy, Michigan State University , East Lansing, MI 48824, USA

4. Department of Computational Mathematics, Science, and Engineering, Michigan State University , East Lansing, MI 48824, USA

5. Facility for Rare Isotope Beams, Michigan State University , East Lansing, MI 48824, USA

6. TAPIR, Mailcode 350-17, California Institute of Technology , Pasadena, CA 91125, USA

7. Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo , Kashiwa, Chiba 277-8583, Japan

Abstract

ABSTRACT We present neutrino-transport hydrodynamic simulations of electron-capture supernovae (ECSNe) in flash with new two-dimensional (2D) collapsing progenitor models. These progenitor models feature the 2D modelling of oxygen-flame propagation until the onset of core collapse. We perform axisymmetric simulations with six progenitor models that, at the time of collapse, span a range of propagating flame front radii. For comparison, we also perform a simulation with the same set-up using the canonical, spherically symmetrical progenitor model n8.8. We found that the variations in the progenitor models inherited from simulations of stellar evolution and flame propagation do not significantly alter the global properties of the neutrino-driven ECSN explosion, such as the explosion energy (∼1.36–1.48 × 1050 erg) and the mass (∼0.017–0.018 M⊙) and composition of the ejecta. Due to aspherical perturbations induced by the 2D flame, the ejecta contains a small amount (≲1.8 × 10−3 M⊙) of low-Ye (0.35 < Ye < 0.4) component. The baryonic mass of the protoneutron star is ∼1.34 M⊙ (∼1.357 M⊙) with the new (n8.8) progenitor models when simulations end at ∼400 ms and the discrepancy is due to updated weak-interaction rates in the progenitor evolutionary simulations. Our results reflect the nature of ECSN progenitors containing a strongly degenerate oxygen–neon–magnesium (ONeMg) core and suggest a standardized ECSN explosion initialized by ONeMg core collapse. Moreover, we carry out a rudimentary three-dimensional simulation and find that the explosion properties are fairly compatible with the 2D counterpart. Our paper facilitates a more thorough understanding of ECSN explosions following the ONeMg core collapse, though more three-dimensional simulations are still needed.

Funder

Swedish Research Council

NASA

MEXT

Japan Society for the Promotion of Science

U.S. Department of Energy

Office of Science

National Nuclear Security Administration

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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