论文标题

在2+2个四倍系统的低质量和高质量间隙中合并黑洞

Merging Black Holes in the Low-mass and High-mass Gaps from 2+2 Quadruple Systems

论文作者

Fragione, Giacomo, Loeb, Abraham, Rasio, Frederic A.

论文摘要

Ligo-Virgo观察到的黑洞(BH)二进制合并的起源仍然不确定,恒星BH质量功能的边界也是不确定的。恒星进化模型预测,在Masses $ \ gtrsim 50 $ m $ _ \ odot $和$ \ lissim 5 $ m $ _ \ odot $中,BHS的缺乏,因此在BH质量函数中留下了低和高质量的差距。形成这些质量BHS的自然方法是通过中子星(NSS;对于低质量间隙)或低质量BHS(对于高质量间隙)的合并;如果Ligo-Virgo再次与新伴侣合并,则可以检测到作为合并产品产生的低质量BH或高质量BH。我们表明,2+2四个系统的演变自然会导致在低或高质量间隙中具有组分质量的BH合并。在我们的情况下,质量间隙中的BH源自两个NS或两个BHS的合并,在两个二进制文件之一中,并合并产品被赋予后坐力(来自各向异性引力波排放),从而触发了它与Quadruple系统的其他二元组成部分的相互作用。这种三体相互作用的结果通常是一种新的偏心紧凑型二元二进制,其中包含质量间隙中的BH,然后可以再次合并。合并费用为$ \ sim 10^{ - 7} -10^{ - 2} $ gpc $^{ - 3} $ yr $^{ - 1} $和$ \ sim 10^{ - 3} - 3} - 10^{ - 2} $ gpc $ gpc $ gpc $^{ - 3} $ yr $^$ yr $^{ - yr $^{ - 1}随着重力波检测器的灵敏度的提高,很快将对恒星BH质量函数放置更严格的约束。

The origin of the black hole (BH) binary mergers observed by LIGO-Virgo is still uncertain, as are the boundaries of the stellar BH mass function. Stellar evolution models predict a dearth of BHs both at masses $\gtrsim 50$ M$_\odot$ and $\lesssim 5$ M$_\odot$, thus leaving low- and high-mass gaps in the BH mass function. A natural way to form BHs of these masses is through mergers of neutron stars (NSs; for the low-mass gap) or lower-mass BHs (for the high-mass gap); the low- or high-mass-gap BH produced as a merger product can then be detected by LIGO-Virgo if it merges again with a new companion. We show that the evolution of a 2+2 quadruple system can naturally lead to BH mergers with component masses in the low- or high-mass gaps. In our scenario, the BH in the mass gap originates from the merger of two NSs, or two BHs, in one of the two binaries and the merger product is imparted a recoil kick (from anisotropic gravitational wave emission), which triggers its interaction with the other binary component of the quadruple system. The outcome of this three-body interaction is usually a new eccentric compact binary containing the BH in the mass gap, which can then merge again. The merger rate is $\sim 10^{-7} - 10^{-2}$ Gpc$^{-3}$ yr$^{-1}$ and $\sim 10^{-3} - 10^{-2}$ Gpc$^{-3}$ yr$^{-1}$ for BHs in the low-mass and high-mass gap, respectively. As the sensitivity of gravitational wave detectors improves, tighter constraints will soon be placed on the stellar BH mass function.

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