论文标题

黑洞X射线二进制文件的统一积聚量范式。 V.低频准周期振荡

A unified accretion-ejection paradigm for black hole X-ray binaries. V. Low-frequency quasi-periodic oscillations

论文作者

Marcel, G., Cangemi, F., Rodriguez, J., Neilsen, J., Ferreira, J., Petrucci, P. -O., Malzac, J., Barnier, S., Clavel, M.

论文摘要

我们提出,瞬态X射线二进制文件(XRB)的光谱演化是由于两个流之间的相互作用:外部部分中的标准积聚磁盘(SAD)和内部部分中的喷气发射磁盘(JED)。我们在以前的论文中表明,在2010-2011爆发期间,X射线和无线电的光谱演变可以恢复。现在,我们研究了X射线爆发过程中低频准周期振荡(LFQPO)的存在,并解决了这些LFQPOS的频率与两个流量之间的过渡半径之间的可能相关性。我们选择X射线和无线电数据形式的GX339-4爆发。我们使用论文IV中详细介绍的方法来获得$ r_j(t)$和$ \ dot {m} _ {in}(t)$,以重现GX339-4的3个不同活动周期的X射线光谱的相关演变和无线电发射。除文献外,我们还独立搜索并报告了对7个新LFQPO的检测。我们表明,C型QPO型的频率可以链接到动态的JED-SAD过渡半径RJ,而不是光学薄厚的过渡的半径。缩放因子q使得$ν_{qpo} \simeqν_k(r_j) / q $是$ q \ simeq 70-140 $,在4个周期中一致,类似于以前的研究。 JED-SAD混合磁盘配置不仅提供了成功的范式,使我们能够描述XRB周期,而且还与QPO频率的演变相匹配。 QPO提供了一种间接的探测JED-SAD过渡半径的方式,其中未定的过程会产生世俗的变异性。过渡半径之间的相关关系CPOS类型cpos与两个流之间的过渡,将其与喷气机的内部磁化结构绑在一起。喷气机结构与负责C型QPO的过程之间的这种直接连接可以自然解释其令人困惑的多波长行为。

We proposed that the spectral evolution of transient X-ray binaries (XrB) is due to an interplay between two flows: a standard accretion disk (SAD) in the outer parts and a jet-emitting disk (JED) in the inner parts. We showed in previous papers that the spectral evolution in X-ray and radio during the 2010-2011 outburst of GX339-4 can be recovered. We now investigate the presence of low frequency quasi-periodic oscillations (LFQPOs) during an X-ray outburst, and address the possible correlation between the frequencies of these LFQPOs and the transition radius between the two flows, rJ. We select X-ray and radio data form 3 outbursts of GX339-4. We use the method detailed in paper IV to obtain $r_J(t)$ and $\dot{m}_{in}(t)$ for each outburst to reproduce the correlated evolution of the X-ray spectra and the radio emission for 3 different activity cycles of GX339-4. We also independently search and report the detection of 7 new LFQPOs in addition to the literature. We show that the frequency of Type C QPOs can be linked to the dynamical JED-SAD transition radius rJ, rather than the radius of optically thin-thick transition. The scaling factor q such that $ν_{QPO} \simeq ν_K (r_J) / q$ is $q \simeq 70-140$, consistent during the 4 cycles and similar to previous studies. The JED-SAD hybrid disk configuration not only provides a successful paradigm allowing us to describe XrB cycles, but also matches the QPO frequencies evolution. QPOs provide an indirect way to probe the JED-SAD transition radius, where an undetermined process produces secular variability. The demonstrated relation between the transition radius links Type C QPOs to the transition between the two flows, tying it to the inner magnetized structure of the jets. This direct connection between the jets' structure and the process responsible for Type C QPOs could naturally explain their puzzling multi-wavelength behavior.

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