论文标题

解决黑洞质谱的峰值

Resolving The Peak Of The Black Hole Mass Spectrum

论文作者

Farag, Ebraheem, Renzo, Mathieu, Farmer, Robert, Chidester, Morgan T., Timmes, F. X.

论文摘要

二元黑洞(BH)合并的重力波(GW)检测已开始采样宇宙BH质量分布。单个恒星核的演变预测,由于配对超新星(PISN),BH质量分布的差距存在差距。确定BH质量间隙的上和下边缘可用于解释合并BHS的GW检测。我们使用\ mesa \来进化单个,非旋转的,巨大的氦气芯,金属度为$ z = 10^{ - 5} $,直到它们倒塌以形成BH或作为PISN爆炸而不留下紧凑的残留物为PISN。我们计算s(300 keV)=(77,203)kev b的s因子的下BH质量差距的边界,对应于我们的高分辨率表中的$ \ pm3σ$不确定性。我们广泛测试了时间和质量分辨率,以解决BH质谱跨BH质量间隙的理论峰。我们探讨了相对于对流混合和核燃烧的收敛性,发现需要大量的时间分辨率以实现收敛。我们还测试采用最小扩散系数,以帮助较低的分辨率模型达到收敛。我们建立了上层质量间隙的新下边缘,为m \ textsubscript {lower} $ \ simeq $ \,60 $^{+32} _ { - 14} $ \,\ msun \,从$^{12} \ text c} c}(c} $ text {c}(c} $ nary)中的$ \ pm3σ$不确定。我们探讨了较大的3- $α$速率在上部质量间隙的下边缘的效果,找到m \ textSubscript {lower} $ \ simeq $ \,69 $^{+34} _ { - 18} $ \,\ msun。我们将结果与重力波瞬态目录中报道的BHS进行比较。

Gravitational wave (GW) detections of binary black hole (BH) mergers have begun to sample the cosmic BH mass distribution. The evolution of single stellar cores predicts a gap in the BH mass distribution due to pair-instability supernova (PISN). Determining the upper and lower edges of the BH mass gap can be useful for interpreting GW detections from merging BHs. We use \MESA\ to evolve single, non-rotating, massive helium cores with a metallicity of $Z = 10^{-5}$ until they either collapse to form a BH or explode as a PISN without leaving a compact remnant. We calculate the boundaries of the lower BH mass gap for S-factors in the range S(300 keV) = (77,203) keV b, corresponding to the $\pm 3σ$ uncertainty in our high resolution tabulated $^{12}$C($α$,$γ$)$^{16}$O reaction rate probability distribution function. We extensively test the temporal and mass resolution to resolve the theoretical peak of the BH mass spectrum across the BH mass gap. We explore the convergence with respect to convective mixing and nuclear burning, finding that significant time resolution is needed to achieve convergence. We also test adopting a minimum diffusion coefficient to help lower resolution models reach convergence. We establish a new lower edge of the upper mass gap as M\textsubscript{lower} $\simeq$\,60$^{+32}_{-14}$\,\Msun\ from the $\pm 3σ$ uncertainty in the $^{12}\text{C}(α, γ) ^{16}\text{O}$ rate. We explore the effect of a larger 3-$α$ rate on the lower edge of the upper mass gap, finding M\textsubscript{lower} $\simeq$\,69$^{+34}_{-18}$\,\Msun. We compare our results with BHs reported in the Gravitational-Wave Transient Catalog.

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