论文标题

从二进制中子恒星合并发射的喷气机:结合中微子的运输和磁场

Jet Launching from Binary Neutron Star Mergers: Incorporating Neutrino Transport and Magnetic Fields

论文作者

Sun, Lunan, Ruiz, Milton, Shapiro, Stuart L., Tsokaros, Antonios

论文摘要

我们对合并二元中微子转运和磁场的二进制中子星进行了一般相对论的磁流失动力学(GRMHD)模拟。我们用于中微子的新的辐射运输模块采用了一种一般的相对论,截短的时刻(M1)形式主义。二进制文件由两个由状态的狡猾核方程(EOS)建模的两个相同的无旋明星。它们最初位于半圆形轨道上,并用一个螺状磁场螺纹,该磁场从恒星内部延伸到外部,如典型的脉冲星。合并后不久,我们插入中微子过程,并关注中微子在高质量中子星(HMN)残留物倒塌后发射射流中的作用。我们处理两个微物理版本:一个(一个“热身”)进化出一种中微子物种,仅考虑带电的流动过程,而另一个进化了三个物种$(ν_e,\barν_e,v _ {\ rm x})$和相关过程。我们追踪演变,直到系统在BH形成后达到准核状态为止。我们发现BH +磁盘残留物最终发射了一架初期喷气机。电磁poynting光度为$ \ sim 10^{53} \ rm \,erg \,s^{ - 1} $,与典型的短伽马射线爆发(sgrbs)一致。中微子冷却的作用缩短了HMN的寿命,并降低了重力波(GW)功率谱的主要峰值的幅度。 BH形成后,中微子有助于清除BH杆附近的物质,从​​而导致较低的BARYON负载周围的碎屑。中微子的光度属于$ \ sim 10^{52-53} \ rm \,Erg \,s^{ - 1} $一旦获得quasiequilibrium。与无中微子模型相比,我们观察到中微子的包含产生相似的射出质量,并且效率低下,从而降低了其他角动量。

We perform general relativistic, magnetohydrodynamic (GRMHD) simulations of merging binary neutron stars incorporating neutrino transport and magnetic fields. Our new radiative transport module for neutrinos adopts a general relativistic, truncated-moment (M1) formalism. The binaries consist of two identical, irrotational stars modeled by the SLy nuclear equation of state (EOS). They are initially in quasicircular orbit and threaded with a poloidal magnetic field that extends from the stellar interior into the exterior, as in typical pulsars. We insert neutrino processes shortly after the merger and focus on the role of neutrinos in launching a jet following the collapse of the hypermassive neutron star (HMNS) remnant to a spinning black hole (BH). We treat two microphysical versions: one (a "warm-up") evolving a single neutrino species and considering only charged-current processes, and the other evolving three species $(ν_e, \barν_e, ν_{\rm x})$ and related processes. We trace the evolution until the system reaches a quasiequilibrium state after BH formation. We find that the BH + disk remnant eventually launches an incipient jet. The electromagnetic Poynting luminosity is $\sim 10^{53} \rm \, erg\, s^{-1}$, consistent with that of typical short gamma-ray bursts (sGRBs). The effect of neutrino cooling shortens the lifetime of the HMNS, and lowers the amplitude of the major peak of the gravitational wave (GW) power spectrum somewhat. After BH formation, neutrinos help clear out the matter near the BH poles, resulting in lower baryon-loaded surrounding debris. The neutrino luminosity resides in the range $\sim 10^{52-53} \rm \,erg\,s^{-1}$ once quasiequilibrium is achieved. Comparing with the neutrino-free models, we observe that the inclusion of neutrinos yields similar ejecta masses and is inefficient in carrying off additional angular momentum.

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