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A Chandra Study of the Multicomponent X-Ray Emission from the X-shaped Radio Galaxy 3C 403

机译:X形射电星系3C 403的多分量X射线发射的Chandra研究

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We present results from a 49.4 ks Chandra ACIS-S observation of the nearby (z = 0.059) X-shaped FR type II (FR II) radio galaxy 3C 403. This is the first Chandra observation of an X-shaped radio galaxy, and one of the goals of this pioneering study is to determine the relationship between the X-ray-emitting gas and the X-shaped radio morphology. We find that the X-ray isophotes of the hot gas within ~35 of the central galaxy are highly elliptical (eccentricity ~0.57) and coaligned with the elliptical optical isophotes. This supports the hypothesis that X-shaped radio sources are created by propagation of jets through asymmetric density distributions. Within large uncertainties, there is no evidence that the lobes or wings are overpressurized relative to the interstellar medium (ISM), supporting the scenario in which the wings are the result of strong backflows of material from the jet head and subsequent buoyant evolution. We have detected X-ray emission from several of the radio knots to the east of the active nucleus and diffuse emission from the radio lobe to the west. The X-ray emission from the eastern knots cannot be explained by an inverse Compton model unless they are far from equipartition. Using archival Hubble Space Telescope (HST) data, optical emission is detected from two knots, and the radio/optical/X-ray spectra are well fitted by simple synchrotron models. This is one of the strongest examples to date of X-ray synchrotron emission from multiple knots in the jet of an FR II radio galaxy. X-ray emission is also detected from the radio wings at a flux consistent with inverse Compton scattering of cosmic microwave background (CMB) photons from relativistic electrons if the wings are near equipartition. The nuclear spectrum is well described by a multicomponent model that includes a heavily absorbed power law (NH ~ 4 × 1023 cm-2) and a bright (EW ~ 244 eV), broadened Fe line. A second, less absorbed, power-law component, likely representing unresolved emission from a parsec-scale jet, is also required.
机译:我们提供了来自附近(z = 0.059)X形FR II型(FR II)射电星系3C 403的49.4 ks Chandra ACIS-S观测结果。这是X形射电星系的首次Chandra观测,并且这项开创性研究的目标之一是确定发射X射线的气体与X形射电形态之间的关系。我们发现,在中心星系约35内的热气体的X射线等渗线是高度椭圆形的(偏心率约为0.57),并且与椭圆形光学等距线共线。这支持以下假设:X形无线电源是通过不对称密度分布的射流传播而产生的。在不确定性较大的情况下,没有证据表明叶或机翼相对于星际介质(ISM)压力过高,从而支持机翼是喷头强烈回流物质和随后浮力演化的结果。我们已经检测到活跃核东部的几个无线电波结的X射线发射,以及探测到西部的无线电波瓣的散射发射。除非它们与等分点相距甚远,否则无法用逆康普顿模型解释东部结的X射线发射。使用档案哈勃太空望远镜(HST)数据,可以从两个结中检测出光发射,并且通过简单的同步加速器模型可以很好地拟合无线电/光学/ X射线光谱。这是迄今为止FR II射电星系射流中多个结产生X射线同步加速器的最强例子之一。如果机翼接近等分,还可以从无线电机翼以与来自相对论电子的宇宙微波背景(CMB)光子的康普顿逆康普顿散射一致的通量检测到X射线发射。多组分模型很好地描述了核光谱,该模型包括一个高吸收功率定律(NH〜4×1023 cm-2)和一个明亮的(EW〜244 eV)加宽的Fe线。还需要第二个吸收较少的幂律分量,该分量可能表示来自帕秒级喷射的未解决的发射。

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