Comparison of the Core-collapse Evolution of Two Nearly Equal-mass Progenitors

被引:6
|
作者
Bruenn, Stephen W. [1 ]
Sieverding, Andre [2 ]
Lentz, Eric J. [2 ,3 ]
Sukhbold, Tuguldur [4 ]
Hix, W. Raphael [2 ,3 ]
Huk, Leah N. [5 ]
Harris, J. Austin [5 ]
Messer, O. E. Bronson [2 ,3 ,5 ]
Mezzacappa, Anthony [3 ]
机构
[1] Florida Atlantic Univ, Dept Phys, 777 Glades Rd, Boca Raton, FL 33431 USA
[2] Oak Ridge Natl Lab, Phys Div, POB 2008, Oak Ridge, TN 37831 USA
[3] Univ Tennessee, Dept Phys & Astron, Knoxville, TN 37996 USA
[4] Ohio State Univ, Ctr Cosmol & Astro Particle Phys, Dept Astron, Columbus, OH 43210 USA
[5] Oak Ridge Natl Lab, Natl Ctr Computat Sci, POB 2008, Oak Ridge, TN 37831 USA
来源
ASTROPHYSICAL JOURNAL | 2023年 / 947卷 / 01期
基金
美国国家科学基金会;
关键词
NEUTRINO-DRIVEN SUPERNOVA; HYDRODYNAMICS CODE; SELF-CONSISTENT; ACCRETION SHOCK; BIRTH MASSES; EXPLOSION; SIMULATIONS; MODELS; NUCLEOSYNTHESIS; CONVECTION;
D O I
10.3847/1538-4357/acbb65
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We compare the core-collapse evolution of a pair of 15.8 M-? stars with significantly different internal structures, a consequence of the bimodal variability exhibited by massive stars during their late evolutionary stages. The 15.78 and 15.79 M-? progenitors have core masses (masses interior to an entropy of 4 k (B) baryon(-1)) of 1.47 and 1.78 M-? and compactness parameters ?(1.75) of 0.302 and 0.604, respectively. The core-collapse simulations are carried out in 2D to nearly 3 s postbounce and show substantial differences in the times of shock revival and explosion energies. The 15.78 M-? model begins exploding promptly at 120 ms postbounce when a strong density decrement at the Si-Si/O shell interface, not present in the 15.79 M-? progenitor, encounters the stalled shock. The 15.79 M-? model takes 100 ms longer to explode but ultimately produces a more powerful explosion. Both the larger mass accretion rate and the more massive core of the 15.79 M-? model during the first 0.8 s postbounce time result in larger ?(e )/? over bar e M (?) model resulted in the ejection of twice as much Ni-56. Most of the ejecta in both models are moderately proton rich, though counterintuitively the highest electron fraction (Y-e = 0.61) ejecta in either model are in the less-energetic 15.78 M-? model, while the lowest electron fraction (Y-e = 0.45) ejecta in either model are in the 15.79 M-? model.
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页数:21
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