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arXiv 0908.1871astro-ph.HE
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广义相对论中微子辐射流体力学模拟中的质子中子星演化和中微子驱动风

Protoneutron star evolution and the neutrino driven wind in general relativistic neutrino radiation hydrodynamics simulations

T. Fischer, S. C. Whitehouse, A. Mezzacappa, F. -K. Thielemann, M. Liebendörfer

摘要:

大质量恒星在爆炸事件中结束了它们的生命,其动能量级为1贝特。爆炸发生后,在喷出物后面立即形成一个低密度和高熵的区域,该区域持续受到中微子加热。中微子从中心的残余物--质子中子星(PNS)中发射出来,加热PNS表面以上的物质。这些热量部分转化为动能,物质加速流出,这就是中微子驱动风。我们第一次模拟了超过20秒的坍缩、反弹、爆炸和中微子驱动的风相。我们的数值模型是基于球对称的广义相对论辐射流体动力学的光谱三味玻尔兹曼中微子输运。在模拟中,没有爆炸是自然获得的,我们模型中微子驱动的爆炸低和中等质量的铁核祖星通过提高带电电流反应速率。在一个特殊的祖星,O-Ne-Mg-核心的情况下,在球对称的爆炸没有增强的不透明度。爆炸后的演变是在定性协议与静态稳态和参数化的中微子驱动风的动力学模型。另一方面,我们发现一般较小的中微子光度和平均中微子能量以及不同的演化行为的中微子光度和平均中微子能量。中微子驱动风富含质子超过10秒,PNS的收缩与以前中微子驱动风研究中对内边界条件的假设不同。尽管每个重子的熵大约为100,并且膨胀时间尺度很快,但我们模型中发现的条件不太可能有利于......

英文摘要:

Massive stars end their life in an explosion event with kinetic energies of the order 1 Bethe. Immediately after the explosion has been launched, a region of low density and high entropy forms behind the ejecta which is continuously subject to neutrino heating. The neutrinos emitted from the remnant at the center, the protoneutron star (PNS), heat the material above the PNS surface. This heat is partly converted into kinetic energy and the material accelerates to an outflow that is known as the neutrino driven wind. For the first time, we simulate the collapse, bounce, explosion and the neutrino driven wind phases consistently over more than 20 seconds. Our numerical model is based on spherically symmetric general relativistic radiation hydrodynamics using spectral three flavor Boltzmann neutrino transport. In simulations where no explosions are obtained naturally, we model neutrino driven explosions for low and intermediate mass Fe-core progenitor stars by enhancing the charged current reaction rates. In the case of a special progenitor star, the O-Ne-Mg-core, the explosion in spherical symmetry was obtained without enhanced opacities. The post explosion evolution is in qualitative agreement with static steady-state and parametrized dynamic models of the neutrino driven wind. On the other hand, we find generally smaller neutrino luminosities and mean neutrino energies as well as a different evolutionary behavior of the neutrino luminosities and mean neutrino energies. The neutrino driven wind is proton-rich for more than 10 seconds and the contraction of the PNS differs from the assumptions made for the conditions at the inner boundary in previous neutrino driven wind studies. Despite the moderately large entropies per baryon of about 100 and the fast expansion timescale, the conditions found in our model are unlikely to favor...

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