论文标题
使用内部冲击模型测试中子星LMXB 4U 0614+091中的喷气几何形状和磁盘耦合
Testing jet geometries and disk-jet coupling in the neutron star LMXB 4U 0614+091 with the internal shocks model
论文作者
论文摘要
在硬状态下低质量X射线二进制的多波长光谱能量分布取决于射流的发射,对于中央边缘的频率,以及光学上的积聚流的发射到X射线范围。在过去的几年中,使用内部冲击模型描述了黑洞(BH)X射线二进制文件的平坦无线电 - IR光谱,该模型假设弹射速度沿喷气的速度的波动是由X射线功率密度光谱(PDS)描述的振动流动驱动的。在这项工作中,我们试图首次将此模型应用于中子星(NS)LMXB,即4U 0614+091。我们使用了2006年获得的多波长数据集,包括从无线电到X射线的数据,并应用了一个模型,该模型包括用于吸积流的辐照光盘模型,以及用于弹射的内部冲击代码的更新版本。该代码的新版本允许为非核喷气机的情况更改喷气机的几何形状。只有两个替代方案提供了对数据的令人满意的描述:使用X射线PDS,但在非旋转几何形状中,或者使用锥形几何形状,但使用“闪烁噪声” PDS。这两种情况都意味着与BH X射线二进制文件中相似模型获得的结果有所不同,从而阐明了NS和BH二进制文件中的射流可能以某种方式具有不同的几何形状或与增生流的不同耦合的可能性。
Multi-wavelength spectral energy distributions of Low Mass X-ray Binaries in the hard state are determined by the emission from a jet, for frequencies up to mid-infrared, and emission from the accretion flow in the optical to X-ray range. In the last years, the flat radio-to-mid-IR spectra of Black Hole (BH) X-ray binaries was described using the internal shocks model, which assumes that the fluctuations in the velocity of the ejecta along the jet are driven by the fluctuations in the accretion flow, described by the X-ray Power Density Spectrum (PDS). In this work we attempt to apply this model for the first time to a Neutron Star (NS) LMXB, i.e. 4U 0614+091. We used the multi-wavelength data set obtained in 2006, comprising data from radio to X-ray, and applied a model which includes an irradiated disc model for the accretion flow and an updated version of the internal shocks code for the ejection. The new version of the code allows to change the geometry of the jet for the case of non-conical jets. Only two alternative scenarios provide a satisfactory description of the data: using the X-ray PDS but in a non-conical geometry for the jet, or either using a conical geometry but with a "flicker-noise" PDS. Both scenarios would imply some differences with the results obtained with similar models on BH X-ray binaries, shedding light on the possibility that jets in NS and BH binaries might somehow have a different geometry or a different coupling with the accretion flow.