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AXISYMMETRIC AB INITIO CORE-COLLAPSE SUPERNOVA SIMULATIONS OF 12-25 M⊙ STARS
被引:151
作者:
Bruenn, Stephen W.
[1
]
Mezzacappa, Anthony
[2
,3
,4
]
Hix, W. Raphael
[2
,3
]
Lentz, Eric J.
[2
,3
,5
]
Messer, O. E. Bronson
[3
,4
,6
]
Lingerfelt, Eric J.
[2
,4
]
Blondin, John M.
[7
]
Endeve, Eirik
[4
]
Marronetti, Pedro
[1
,8
]
Yakunin, Konstantin N.
[1
]
机构:
[1] Florida Atlantic Univ, Dept Phys, Boca Raton, FL 33431 USA
[2] Oak Ridge Natl Lab, Div Phys, Oak Ridge, TN 37831 USA
[3] Univ Tennessee, Dept Phys & Astron, Knoxville, TN 37996 USA
[4] Oak Ridge Natl Lab, Comp Sci & Math Div, Oak Ridge, TN 37831 USA
[5] Oak Ridge Natl Lab, Joint Inst Heavy Ion Res, Oak Ridge, TN 37831 USA
[6] Oak Ridge Natl Lab, Natl Ctr Computat Sci, Oak Ridge, TN 37831 USA
[7] N Carolina State Univ, Dept Phys, Raleigh, NC 27695 USA
[8] Natl Sci Fdn, Div Phys, Arlington, VA 22207 USA
基金:
美国国家科学基金会;
关键词:
neutrinos;
radiative transfer;
supernovae: general;
BOLTZMANN NEUTRINO TRANSPORT;
ACCRETION-SHOCK INSTABILITY;
POSTBOUNCE EVOLUTION;
HYDRODYNAMICS CODE;
GRAVITATIONAL-WAVE;
DRIVEN CONVECTION;
EXPLOSION MODELS;
MECHANISM;
STATE;
EQUATION;
D O I:
10.1088/2041-8205/767/1/L6
中图分类号:
P1 [天文学];
学科分类号:
0704 ;
摘要:
We present an overview of four ab initio axisymmetric core-collapse supernova simulations employing detailed spectral neutrino transport computed with our Chimera code and initiated from Woosley & Heger progenitors of mass 12, 15, 20, and 25 M-circle dot. All four models exhibit shock revival over similar to 200 ms (leading to the possibility of explosion), driven by neutrino energy deposition. Hydrodynamic instabilities that impart substantial asymmetries to the shock aid these revivals, with convection appearing first in the 12 M-circle dot model and the standing accretion shock instability appearing first in the 25 M-circle dot model. Three of the models have developed pronounced prolate morphologies (the 20 M-circle dot model has remained approximately spherical). By 500 ms after bounce the mean shock radii in all four models exceed 3000 km and the diagnostic explosion energies are 0.33, 0.66, 0.65, and 0.70 Bethe (B = 10(51) erg) for the 12, 15, 20, and 25 M-circle dot models, respectively, and are increasing. The three least massive of our models are already sufficiently energetic to completely unbind the envelopes of their progenitors (i.e., to explode), as evidenced by our best estimate of their explosion energies, which first become positive at 320, 380, and 440 ms after bounce. By 850 ms the 12 M-circle dot diagnostic explosion energy has saturated at 0.38 B, and our estimate for the final kinetic energy of the ejecta is similar to 0.3 B, which is comparable to observations for lower mass progenitors.
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