4.6 Article

AXISYMMETRIC AB INITIO CORE-COLLAPSE SUPERNOVA SIMULATIONS OF 12-25 M⊙ STARS

期刊

ASTROPHYSICAL JOURNAL LETTERS
卷 767, 期 1, 页码 -

出版社

IOP PUBLISHING LTD
DOI: 10.1088/2041-8205/767/1/L6

关键词

neutrinos; radiative transfer; supernovae: general

资金

  1. U.S. Department of Energy Offices of Nuclear Physics and Advanced Scientific Computing Research
  2. NASA Astrophysics Theory and Fundamental Physics Program [NNH08AH71I, NNH11AQ72I]
  3. National Science Foundation PetaApps Program [OCI-0749242, OCI-0749204, OCI-0749248]
  4. NSF through TeraGrid [TG-MCA08X010]
  5. US DoE Office of Science [DE-AC02-05CH11231, DE-AC05-00OR22725]

向作者/读者索取更多资源

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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