2018
DOI: 10.1051/0004-6361/201833705
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Core-collapse supernovae in the hall of mirrors

Abstract: Context. Modeling core-collapse supernovae (SNe) with neutrino transport in three dimensions (3D) requires tremendous computing resources and some level of approximation. We present a first comparison study of core-collapse SNe in 3D with different physics approximations and hydrodynamics codes. Aims. The objective of this work is to assess the impact of the hydrodynamics code, approximations for the neutrino, gravity treatments, and rotation on the simulation of core-collapse SNe in 3D. Methods. We use four d… Show more

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Cited by 49 publications
(33 citation statements)
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References 118 publications
(183 reference statements)
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“…In the determination of the electron fraction, there are two critical quantities: the energy difference be- tween antineutrinos and neutrinos (∆ ν = νe − νe ) and the ratio of neutrino number luminosities (RL n = L n,νe /L n,νe ). Following previous studies based on simulations with accurate neutrino transport (see e.g., Liebendörfer et al 2005;Bruenn et al 2016;Takiwaki et al 2016;Kotake et al 2018;Cabezón et al 2018;Just et al 2018;O'Connor & Couch 2018;Summa et al 2018;Vartanyan et al 2018Vartanyan et al , 2019aMüller 2019;Pan et al 2019;Powell & Müller 2020;Kuroda et al 2020), one can find typical energy differences of ∆ ν = νe − νe ≈ 2 − 2.5 MeV. In our models we have on average ∆ ν = (2.3 ± 0.6) MeV after the explosion time.…”
Section: Evolution In the Long-time Phase And The Neutrino-driven Windsupporting
confidence: 54%
“…In the determination of the electron fraction, there are two critical quantities: the energy difference be- tween antineutrinos and neutrinos (∆ ν = νe − νe ) and the ratio of neutrino number luminosities (RL n = L n,νe /L n,νe ). Following previous studies based on simulations with accurate neutrino transport (see e.g., Liebendörfer et al 2005;Bruenn et al 2016;Takiwaki et al 2016;Kotake et al 2018;Cabezón et al 2018;Just et al 2018;O'Connor & Couch 2018;Summa et al 2018;Vartanyan et al 2018Vartanyan et al , 2019aMüller 2019;Pan et al 2019;Powell & Müller 2020;Kuroda et al 2020), one can find typical energy differences of ∆ ν = νe − νe ≈ 2 − 2.5 MeV. In our models we have on average ∆ ν = (2.3 ± 0.6) MeV after the explosion time.…”
Section: Evolution In the Long-time Phase And The Neutrino-driven Windsupporting
confidence: 54%
“…These represent the minimal set of the most relevant weak processes during the collapse and in the early post-bounce phase. The emission of µ and τ (anti)neutrinos in the post-bounce phase is handled by a gray leakage scheme (Cabezón et al 2018). This scheme has been gauged on detailed Boltzmann transport models, and includes pair annihilation, nucleon-nucleon bremsstrahlung, and scattering off nucleons.…”
Section: Early Evolution Of a Newborn Neutron Starmentioning
confidence: 99%
“…This is a computationally demanding task even for the simplest toy models and perhaps prohibitively difficult for the multidimensional continuous angular distributions found in SN simulations. Second, most of the state-ofthe-art simulations [25][26][27][28][29][30][31][32][33] maintain only the moments of the angular distributions of fluxes and not the full distributions. This lack of information seems to preclude even a linear stability analysis that requires knowing these distributions.…”
Section: Introductionmentioning
confidence: 99%