论文标题

3D非旋转核心折叠超新星模型的中微子驱动爆炸的磁支持

Magnetic support for neutrino-driven explosion of 3D non-rotating core-collapse supernova models

论文作者

Matsumoto, Jin, Asahina, Yuta, Takiwaki, Tomoya, Kotake, Kei, Takahashi, Hiroyuki R.

论文摘要

通过使用光谱中微子转运进行三维磁氢动力学模拟,研究了磁场对非旋转恒星芯后爆炸后超新星动力学的影响。比较了$ 20 $和$ 27 $ $ m _ {\ odot} $ pre-supernova祖细胞的强烈和弱磁化模型的爆炸性。我们发现,尽管中微子加热到湍流能量的转化效率包括增益区域中的磁场并没有显着差异,但由于中微子驱动的大气泡在停滞的冲击后面的大量热气泡上引起的放大磁场引起的放大磁场导致了更快的速度,并且在强磁化强度磁化的模型中会导致更快的爆炸。此外,通过比较强场模型中模拟的2阶空间精度(以$ 27 $ $ $ M _ {\ odot} $祖细胞的差异)之间的差异,我们还发现,太空中的较高订单准确性对爆炸有益,因为它增强了中性驱动对增长区域中中性驱动的对增长区域的增长。基于我们为非旋转模型的核心折叠超新星模拟的结果,提出了Protonutron Star(PNS)磁场起源的新可能性。在PNS表面附近的对流稳定的外壳中,磁场被积累并扩增到磁场水平,即$ \ Mathcal {O}(10^{14})$ G。

The impact of the magnetic field on postbounce supernova dynamics of non-rotating stellar cores is studied by performing three-dimensional magnetohydrodynamics simulations with spectral neutrino transport. The explodability of strongly and weakly magnetized models of $20$ and $27$ $M_{\odot}$ pre-supernova progenitors are compared. We find that although the efficiency for the conversion of the neutrino heating into turbulent energy including magnetic fields in the gain region is not significantly different between the strong and weak field models, the amplified magnetic field due to the neutrino-driven convection on large hot bubbles just behind stalled shock results in a faster and more energetic explosion in the strongly magnetized models. In addition, by comparing the difference between the 2nd- and 5th-order spatial accuracy of the simulation in the strong field model for $27$ $M_{\odot}$ progenitor, we also find that the higher order accuracy in space is beneficial to the explosion because it enhances the growth of neutrino-driven convection in the gain region. Based on our results of core-collapse supernova simulations for the non-rotating model, a new possibility for the origin of the magnetic field of the protoneutron star (PNS) is proposed. The magnetic field is accumulated and amplified to magnetar level, that is, $\mathcal{O}(10^{14})$ G, in the convectively stable shell near the PNS surface.

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