TY - JOUR
T1 - The evolution toward electron capture supernovae
T2 - The flame propagation and the pre-bounce electron-neutrino radiation
AU - Takahashi, Koh
AU - Sumiyoshi, Kohsuke
AU - Yamada, Shoichi
AU - Umeda, Hideyuki
AU - Yoshida, Takashi
N1 - Funding Information:
We acknowledge invaluable comments from the anonymous referee that help to improve the manuscript. Authors appreciate Ken’ichi Nomoto for providing us with the progenitor model N8.8. We thank Andrius Juodagalvis and Shun Furusawa for providing electron capture rates for NSE compositions. We also thank Chinami Kato for fruitful discussions about neutrino reactions and Jonathan Mackey for careful reading of the draft. K.T. was supported by the Japan Society for the Promotion of Science (JSPS) Overseas Research Fellowships. This work was supported by Grant-in-Aid for Scientific Research (26104006, 15K05093, 17H01130, 17K05380) and Grant-in-Aid for Scientific Research on Innovative areas “Gravitational wave physics and astronomy:Genesis” (17H06357, 17H06365) from the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan. For providing high-performance computing resources, the Computing Research Center, KEK, JLDG on SINET4 of NII, Research Center for Nuclear Physics, Osaka University, Yukawa Institute of Theoretical Physics, Kyoto University, and Information Technology Center, University of Tokyo are acknowledged. This work was partly supported by research programs at K-computer of the RIKEN AICS, HPCI Strategic Program of Japanese MEXT, Priority Issue on Post-K computer (Elucidation of the Fundamental Laws and Evolution of the Universe), and Joint Institute for Computational Fundamental Sciences (JICFus).
Publisher Copyright:
© 2019 The American Astronomical Society. All rights reserved.
PY - 2019/2/1
Y1 - 2019/2/1
N2 - A critical-mass ONe core with a high ignition density is considered to end in gravitational collapse leading to neutron star formation. Being distinct from an Fe core collapse, the final evolution involves combustion flame propagation, in which complex phase transition from ONe elements into the nuclear statistical equilibrium (NSE) state takes place. We simulate the core evolution from the O+Ne ignition until the bounce shock penetrates the whole core, using a state-of-the-art 1D Lagrangian neutrino radiation hydrodynamic code, in which important nuclear burning, electron capture, and neutrino reactions are taken into account. Special care is also taken in making a stable initial condition by importing the stellar equation of state, which is used for the progenitor evolution calculation, and by improving the remapping process. We find that the central ignition leads to intense ν e radiation with L νe ≳ 10 51 erg s -1 powered by fast electron captures onto NSE isotopes. This pre-bounce ν e radiation heats the surroundings by the neutrino-electron scattering, which acts as a new driving mechanism of the flame propagation together with the adiabatic contraction. The resulting flame velocity of ∼10 8 cm s -1 will be more than one order of magnitude faster than that of a laminar flame driven by heat conduction. We also find that the duration of the pre-bounce ν e radiation phase depends on the degree of the core hydrostatic/dynamical stability. Therefore, the future detection of the pre-bounce neutrino is important not only to discriminate the ONe core collapse from the Fe core collapse but also to constrain the progenitor hydrodynamical stability.
AB - A critical-mass ONe core with a high ignition density is considered to end in gravitational collapse leading to neutron star formation. Being distinct from an Fe core collapse, the final evolution involves combustion flame propagation, in which complex phase transition from ONe elements into the nuclear statistical equilibrium (NSE) state takes place. We simulate the core evolution from the O+Ne ignition until the bounce shock penetrates the whole core, using a state-of-the-art 1D Lagrangian neutrino radiation hydrodynamic code, in which important nuclear burning, electron capture, and neutrino reactions are taken into account. Special care is also taken in making a stable initial condition by importing the stellar equation of state, which is used for the progenitor evolution calculation, and by improving the remapping process. We find that the central ignition leads to intense ν e radiation with L νe ≳ 10 51 erg s -1 powered by fast electron captures onto NSE isotopes. This pre-bounce ν e radiation heats the surroundings by the neutrino-electron scattering, which acts as a new driving mechanism of the flame propagation together with the adiabatic contraction. The resulting flame velocity of ∼10 8 cm s -1 will be more than one order of magnitude faster than that of a laminar flame driven by heat conduction. We also find that the duration of the pre-bounce ν e radiation phase depends on the degree of the core hydrostatic/dynamical stability. Therefore, the future detection of the pre-bounce neutrino is important not only to discriminate the ONe core collapse from the Fe core collapse but also to constrain the progenitor hydrodynamical stability.
KW - abundances-stars: Evolution-supernovae: General
KW - neutrinos-nuclear reactions
KW - nucleosynthesis
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U2 - 10.3847/1538-4357/aaf8a8
DO - 10.3847/1538-4357/aaf8a8
M3 - Article
AN - SCOPUS:85062046660
SN - 0004-637X
VL - 871
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 2
M1 - 153
ER -