论文标题
简单的分析公式,将紧凑物体的质量和旋转与它们的快速X射线变异性有关
Simple analytic formula relating the mass and spin of accreting compact objects to their rapid X-ray variability
论文作者
论文摘要
遵循先前关于黑洞(BHS)和中子星(NSS)的增值盘的振荡的研究,已经提出了一种新的高频准周期振荡(QPOS)的新模型(CPOS)(CT)模型(CT模型),该模型涉及质量流动的tori(i.ee.ee.ee.ee.ee.ee.ee.ee.ee.ee,tori)的振荡。根据初步研究,与相对论进动(RP)模型相比,该模型提供了更好的NS QPO数据。这也意味着银河微验BH旋转的上限显着更高。已经注意到了一个简短的分析公式,可以很好地重现该模型对Schwarzschild SpaceTimes中QPO频率的预测。在这里,我们得出了适用于旋转紧凑对象的该公式的扩展版本。我们从考虑到Kerr的空间开始,并得出一个不限于内部积聚流的特定角度动量分布(例如Keplerian或常数)的公式。最后,我们考虑了hartle-thorne的空间,并包括NS填充性暗示的校正。对于单个参数的特定选择,我们的关系提供了CT模型预测的频率。对于另一个值,它提供了RP模型预测的频率。我们得出的结论是,该公式非常适用于旋转填充性NS和两个模型。我们简要说明了我们的简单公式在几个NS源上的应用,并确认CT模型与NS质量的现实值兼容的期望,并提供了比RP模型更好的数据拟合。
Following the previous research on epicyclic oscillations of accretion disks around black holes (BHs) and neutron stars (NSs), a new model of high-frequency quasi-periodic oscillations (QPOs) has been proposed (CT model), which deals with oscillations of fluid in marginally overflowing accretion tori (i.e., tori terminated by cusps). According to preliminary investigations, the model provides better fits of the NS QPO data compared to the relativistic precession (RP) model. It also implies a significantly higher upper limit on the Galactic microquasars BH spin. A short analytic formula has been noticed to well reproduce the model's predictions on the QPO frequencies in Schwarzschild spacetimes. Here we derive an extended version of this formula that applies to rotating compact objects. We start with the consideration of Kerr spacetimes and derive a formula that is not restricted to a particular specific angular momentum distribution of the inner accretion flow, such as Keplerian or constant. Finally, we consider Hartle-Thorne spacetimes and include corrections implied by the NS oblateness. For a particular choice of a single parameter, our relation provides frequencies predicted by the CT model. For another value, it provides frequencies predicted by the RP model. We conclude that the formula is well applicable for rotating oblateness NSs and both models. We briefly illustrate application of our simple formula on several NS sources and confirm the expectation that the CT model is compatible with realistic values of the NS mass and provides better fits of data than the RP model.