论文标题
3D辐射转移KILONOVA建模用于二进制中子星级合并模拟
3D radiative transfer kilonova modelling for binary neutron star merger simulations
论文作者
论文摘要
GW170817和随附的电磁对应物AT2017GFO的检测为中子星星合并的理论模型,核合成和辐射转移提供了一组重要的观察性约束。我们应用3D蒙特卡洛辐射传递代码工匠,从中子星合并中产生动力弹射的合成光曲线,该弹性合并已通过3D平滑粒子流体动力学(SPH)进行建模,并包括中微子相互作用。核合成计算提供了从R-Process核的放射性衰减中释放出的能量,并使用作为电子级分的功能给出的灰色不透光率进行辐射传输。我们提出了依赖性的侧侧光度光曲线,并发现沿着极地视线的发射比沿赤道的视线高约2倍。我们的降压光曲线不是独特的发射峰,而是单调的下降,其特征是在散装喷射时肩部变细时的肩膀。我们根据辐射温度显示近似带光曲线,并将其与AT2017GFO的观察结果进行比较。我们发现,迅速下降的温度导致蓝色至红色的演变,类似于AT2017GFO所示。我们还研究了一个额外的球形世俗射出成分的影响,我们发现早期的光曲线几乎不受影响,而大约1天后,发射被世俗的喷射强烈增强和支配,导致肩膀从1-2天转移到6-10天。
The detection of GW170817 and the accompanying electromagnetic counterpart, AT2017gfo, have provided an important set of observational constraints for theoretical models of neutron star mergers, nucleosynthesis, and radiative transfer for kilonovae. We apply the 3D Monte Carlo radiative transfer code ARTIS to produce synthetic light curves of the dynamical ejecta from a neutron star merger, which has been modelled with 3D smooth-particle hydrodynamics (SPH) and included neutrino interactions. Nucleosynthesis calculations provide the energy released from radioactive decays of r-process nuclei, and radiation transport is performed using grey opacities given as functions of the electron fraction. We present line-of-sight dependent bolometric light curves, and find the emission along polar lines of sight to be up to a factor of ~2 brighter than along equatorial lines of sight. Instead of a distinct emission peak, our bolometric light curve exhibits a monotonic decline, characterised by a shoulder at the time when the bulk ejecta becomes optically thin. We show approximate band light curves based on radiation temperatures and compare these to the observations of AT2017gfo. We find that the rapidly declining temperatures lead to a blue to red colour evolution similar to that shown by AT2017gfo. We also investigate the impact of an additional, spherically symmetric secular ejecta component, and we find that the early light curve remains nearly unaffected, while after about 1 day the emission is strongly enhanced and dominated by the secular ejecta, leading to the shift of the shoulder from 1-2 to 6-10 days.