论文标题

相对论AGN喷气机III。双双射电星系中同步加速器发射的合成

Relativistic AGN jets III. Synthesis of synchrotron emission from Double-Double Radio Galaxies

论文作者

Walg, S., Achterberg, A., Markoff, S., Keppens, R., Porth, O.

论文摘要

双双射电星系(DDRG)类别与情节性喷气爆发有关。各种区域和组件如何增加无线电图像中的总强度。在本文中,我们基于特殊的相对论流体动力模拟合成DDRG的同步加速器图像,从而为磁场提供了高级近似值。我们研究:三种不同的径向喷射曲线的同步加速器图像;有序,纠缠或混合磁场;同步加速器冷却的光谱老化;不同喷气组件的贡献;视角和多普勒(DE-)提升; DDRG演变的各个时期。为了将我们的结果与观察数据联系起来,我们将其采用到J1835+6204作为参考来源。在所有情况下,合成的同步加速器图像在内部和外叶中均显示了两个清晰的热点对。对于分段等距喷气机,获得了最佳相似之处,对于$ \ \ vartheta \ sim -71^{\ circ} $的观看角度,即倾向下喷气机的倾向于观察者,并且主要纠结($ \ gtrsim 70 $ 70的磁性压力),而不是有序的领域。当观察频率和截止频率的比率$ν_ {\ rm obs}/ν_ {\ infty,0} \ gtrsim 10^{ - 3} $时,光谱老化的影响变得很重要。为了查看角度$ \ vartheta \ lyssim -30^{\ circ} $,无法再识别DDRG形态。必须在$ \ lyssim内注入第二架喷气机的$ 4%,以示出DDRG结构的第一个喷气机的寿命4%,这与主动银河核反馈约束有关。

The class of Double-Double Radio Galaxies (DDRGs) relates to episodic jet outbursts. How various regions and components add to the total intensity in radio images is less well known. In this paper we synthesize synchrotron images for DDRGs based on special relativistic hydrodynamic simulations, making advanced approximations for the magnetic fields. We study the synchrotron images for: Three different radial jet profiles; Ordered, entangled or mixed magnetic fields; Spectral ageing from synchrotron cooling; The contribution from different jet components; The viewing angle and Doppler (de-)boosting; The various epochs of the evolution of the DDRG. To link our results to observational data, we adopt to J1835+6204 as a reference source. In all cases the synthesized synchrotron images show two clear pairs of hotspots, in the inner and outer lobes. The best resemblance is obtained for the piecewise isochoric jet model, for a viewing angle of approximately $\vartheta \sim -71^{\circ}$, i.e. inclined with the lower jet towards the observer, with predominantly entangled ($\gtrsim 70$ per cent of the magnetic pressure) in turbulent, rather than ordered fields. The effects of spectral ageing become significant when the ratio of observation frequencies and cut-off frequency $ν_{\rm obs}/ν_{\infty,0} \gtrsim 10^{-3}$, corresponding to $\sim 3 \cdot 10^2$ MHz. For viewing angles $\vartheta \lesssim -30^{\circ}$, a DDRG morphology can no longer be recognized. The second jets must be injected within $\lesssim$ 4 per cent of the lifetime of the first jets for a DDRG structure to emerge, which is relevant for Active Galactic Nuclei feedback constraints.

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