The Progenitor Dependence of Core-collapse Supernovae from Three-dimensional Simulations with Progenitor Models of 12-40 M⊙

被引:108
作者
Ott, Christian D. [1 ,2 ]
Roberts, Luke F. [3 ,4 ]
Schneider, Andre da Silva [2 ]
Fedrow, Joseph M. [1 ]
Haas, Roland [5 ]
Schnetter, Erik [6 ,7 ,8 ]
机构
[1] Kyoto Univ, Yukawa Inst Theoret Phys, Kyoto, Japan
[2] CALTECH, TAPIR, Mailcode 350-17, Pasadena, CA 91125 USA
[3] Michigan State Univ, Natl Superconducting Cyclotron Lab, E Lansing, MI 48824 USA
[4] Michigan State Univ, Dept Phys & Astron, E Lansing, MI 48824 USA
[5] Univ Illinois, Natl Ctr Supercomp Applicat, Urbana, IL 61801 USA
[6] Perimeter Inst Theoret Phys, Waterloo, ON, Canada
[7] Univ Guelph, Dept Phys, Guelph, ON, Canada
[8] Louisiana State Univ, Ctr Computat & Technol, Baton Rouge, LA 70803 USA
基金
美国国家科学基金会;
关键词
neutrinos; stars: black holes; stars: neutron; supernovae: general; MASSIVE STARS; CONVECTION; EXPLOSION; SHOCK; EVOLUTION; REVIVAL;
D O I
10.3847/2041-8213/aaa967
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We present a first study of the progenitor star dependence of the three-dimensional (3D) neutrino mechanism of core-collapse supernovae. We employ full 3D general-relativistic multi-group neutrino radiation-hydrodynamics and simulate the postbounce evolutions of progenitors with zero-age main sequence masses of 12, 15, 20, 27, and 40 M-circle dot. All progenitors, with the exception of the 12 M-circle dot star, experience shock runaway by the end of their simulations. In most cases, a strongly asymmetric explosion will result. We find three qualitatively distinct evolutions that suggest a complex dependence of explosion dynamics on progenitor density structure, neutrino heating, and 3D flow. (1) Progenitors with massive cores, shallow density profiles, and high post-core-bounce accretion rates experience very strong neutrino heating and neutrino-driven turbulent convection, leading to early shock runaway. Accretion continues at a high rate, likely leading to black hole formation. (2) Intermediate progenitors experience neutrino-driven, turbulence-aided explosions triggered by the arrival of density discontinuities at the shock. These occur typically at the silicon/silicon-oxygen shell boundary. (3) Progenitors with small cores and density profiles without strong discontinuities experience shock recession and develop the 3D standing-accretion shock instability (SASI). Shock runaway ensues late, once declining accretion rate, SASI, and neutrino-driven convection create favorable conditions. These differences in explosion times and dynamics result in a non-monotonic relationship between progenitor and compact remnant mass.
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页数:8
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