论文标题

黑洞中的星星合并事件候选人S190814BV对弹射质量的限制

Constraint on the ejecta mass for a black hole-neutron star merger event candidate S190814bv

论文作者

Kawaguchi, Kyohei, Shibata, Masaru, Tanaka, Masaomi

论文摘要

我们通过具有逼真的弹出密度曲线以及详细的不透明度和加热速度模型的辐射传递模拟S190814BV(黑洞中的星星合并候选者)S190814BV的上限。喷射质量的极限在很大程度上取决于视角。对于面对面的观察($ \ le45^\ circ $),对于S190814BV的平均距离($ d = 267 $ mpc)的总弹出质量应小于$ 0.1 \,m_ \ odot $,而较大的质量可以进行边缘观测值。我们还将动态弹出质量的保守上限推导出$ 0.02 \,m_ \ odot $,$ 0.03 \,m_ \ odot $,$ 0.05 \,m_ \ odot $ for Viewing Angle Angle $ \ le 20^\ le 20^\ circ $,$ \ circ $,$ \ le 50^\ circ $ for $ $ $ $ $ $ $ $ $ 90^\ $ 90^\ cock for $ 90^\ cock for 90^\ coix for 90^\ crock for 90^c。我们表明,在GW触发器之后2 d内,{\ it Iz} -band观察值在$ 0.06 \,m_ \ odot $ $ d = 300 $ mpc的距离之后,比$ 22 $ 22 $ mag更深。我们还表明,如果未来的观察结果将$ 0.03 \,m_ \ odot $的上限放到了BH-NS质量上的BH-NS质量上的$ 0.03 \,m_ \ odot $的上限,则可以获得对NS Mass-Radius关系的强烈限制。

We derive the upper limit to the ejecta mass of S190814bv, a black hole-neutron star merger candidate, through the radiative transfer simulations for kilonovae with the realistic ejecta density profile as well as the detailed opacity and heating rate models. The limits to the ejecta mass strongly depend on the viewing angle. For the face-on observations ($\le45^\circ$), the total ejecta mass should be smaller than $0.1\,M_\odot$ for the average distance of S190814bv ($D=267$ Mpc), while larger mass is allowed for the edge-on observations. We also derive the conservative upper limits of the dynamical ejecta mass to be $0.02\,M_\odot$, $0.03\,M_\odot$, and $0.05\,M_\odot$ for the viewing angle $\le 20^\circ$, $\le 50^\circ$, and for $\le 90^\circ$, respectively. We show that the {\it iz}-band observation deeper than $22$ mag within 2 d after the GW trigger is crucial to detect the kilonova with the total ejecta mass of $0.06\,M_\odot$ at the distance of $D=300$ Mpc. We also show that a strong constraint on the NS mass-radius relation can be obtained if the future observations put the upper limit of $0.03\,M_\odot$ to the dynamical ejecta mass for a BH-NS event with the chirp mass smaller than $\lesssim 3\,M_\odot$ and effective spin larger than $\gtrsim 0.5$.

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