论文标题
用重力波检测器观察中子星塌陷
Towards observing the neutron star collapse with gravitational wave detectors
论文作者
论文摘要
从GW170817中的合并后,已检测到来自二进制中子星灵的引力波以及电磁瞬变。但是,关于连接这两组可观察到的合并后动力学,仍然未知。这包括何时以及何时何时将合并后的恒星崩溃到黑洞,以及为短伽马射线爆发供电的必要条件以及其他观察到的电磁对应物。观察到后中子后星的崩溃会引起这些问题的束缚,限制了短伽马射线爆发发动机的模型和状态的热中子恒星方程。在这项工作中,我们探讨了使用引力波检测器通过建立合并后重力发射的关闭或---更具挑战性的直接检测倒塌信号来间接测量崩溃的时间的范围。对于间接方法,我们考虑使用以前研究的耦合臂腔和信号回收腔共鸣的千霍兹高频检测器设计。该设计将给出0.5 \, - \,8.6(取决于波形参数的变化)的信号 - 噪声比,用于折叠引力波信号,在10 \时出现在10 \,MS二进制后MS 50 \ mpc,MPC和总质量为2.7 m_ \ odot $。对于直接方法,我们提出了狭窄的探测器设计,利用围绕臂空腔频谱范围频率的灵敏度。所提出的检测器的信噪比为0.3 \, - \,1.9,独立于塌陷时间。该探测器受到基本经典和量子噪声的限制,其臂腔功率被选为10 \,MW。
Gravitational waves from binary neutron star inspirals have been detected along with the electromagnetic transients coming from the aftermath of the merger in GW170817. However, much is still unknown about the post-merger dynamics that connects these two sets of observables. This includes if, and when, the post-merger remnant star collapses to a black hole, and what are the necessary conditions to power a short gamma-ray burst, and other observed electromagnetic counterparts. Observing the collapse of the post-merger neutron star would shed led on these questions, constraining models for the short gamma-ray burst engine and the hot neutron star equation of state. In this work, we explore the scope of using gravitational wave detectors to measure the timing of the collapse either indirectly, by establishing the shut-off of the post-merger gravitational emission, or---more challengingly---directly, by detecting the collapse signal. For the indirect approach, we consider a kilohertz high-frequency detector design that utilises a previously studied coupled arm cavity and signal recycling cavity resonance. This design would give a signal-to-noise ratio of 0.5\,-\,8.6 (depending on the variation of waveform parameters) for a collapse gravitational wave signal occurring at 10\,ms post-merger of a binary at 50\,Mpc and with total mass $2.7 M_\odot$. For the direct approach, we propose a narrow-band detector design, utilising the sensitivity around the frequency of the arm cavity free spectral range. The proposed detector achieves a signal-to-noise ratio of 0.3\,-\,1.9, independent of the collapse time. This detector is limited by both the fundamental classical and quantum noise with the arm cavity power chosen as 10\,MW.