数着看不见的。2。邻近星系的潮汐破坏事件率与REPTiDE

Christian H. Hannah, Nicholas C. Stone, Anil C. Seth and Sjoert van Velzen
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引用次数: 0

摘要

潮汐破坏事件(TDEs)是一类恒星被大质量黑洞(MBH)的潮汐摧毁时发生的瞬态事件。他们的比率编码了有价值的MBH人口统计信息,但只有在准确的TDE比率预测可以与观察到的比率进行比较的情况下,才能提取这些信息。在这项工作中,我们提出了一个新的,观察者友好的Python包REPTiDE,它实现了一个标准的损失锥模型,用于计算给定恒星密度分布和MBH质量的TDE率。我们将该软件应用于91个附近星系的代表性样本,这些样本的恒星质量范围很广,并采用了C. H. Hannah等人的高分辨率核密度测量。我们测量了每个星系的TDE速率,范围在10 - 7.7和10 - 2.9年- 1之间,发现样本平均速率与观测结果吻合得很好。我们发现TDE率的变化是星系恒星质量和黑洞质量的函数,在星系质量为109.5M⊙和黑洞质量为106.5M⊙的星系中观测到的峰值速率。尽管推断中等质量黑洞的TDE率较低,但我们发现,与高质量黑洞相比,它们通过TDE获得的质量比例更高。低质量黑洞通过tde的增长可以让我们对它们的自旋施加有趣的限制;我们发现质量低于~ 105.5M⊙的黑洞的最大自旋为a•≈0.9。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Counting the Unseen. II. Tidal Disruption Event Rates in Nearby Galaxies with REPTiDE
Tidal disruption events (TDEs) are a class of transients that occur when a star is destroyed by the tides of a massive black hole (MBH). Their rates encode valuable MBH demographic information, but this can only be extracted if accurate TDE rate predictions are available for comparisons with observed rates. In this work, we present a new, observer-friendly Python package called REPTiDE, which implements a standard loss-cone model for computing TDE rates given a stellar density distribution and an MBH mass. We apply this software to a representative sample of 91 nearby galaxies over a wide range of stellar masses with high-resolution nuclear density measurements from C. H. Hannah et al. We measure per-galaxy TDE rates ranging between 10−7.7 and 10−2.9 yr–1 and find that the sample-averaged rates agree well with observations. We find a turnover in the TDE rate as a function of both galaxy stellar mass and black hole mass, with the peak rates being observed in galaxies at a galaxy mass of 109.5M⊙ and a black hole mass of 106.5M⊙. Despite the lower TDE rates inferred for intermediate-mass black holes, we find that they have gained a higher fraction of their mass through TDEs when compared to higher-mass black holes. This growth of lower-mass black holes through TDEs can enable us to place interesting constraints on their spins; we find maximum spins of a• ≈ 0.9 for black holes with masses below ∼105.5M⊙.
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