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arXiv 1105.2218astro-ph.CO
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Seyfert 1星系XMM-牛顿数据的综合分析方法

A comprehensive approach to analyzing the XMM-Newton data of Seyfert 1 galaxies

Mónica V. Cardaci, María Santos-Lleó, Guillermo F. Hägele, Yair Krongold, Ángeles I. Díaz, Pedro Rodríguez-Pascual

摘要:

目标。我们寻求一个全面的分析所提供的四个塞弗特1星系ESO 359-G19,HE 1143-1810,CTS A08.12和Mrk 110,包括紫外线范围的XMM-牛顿卫星的所有信息,以表征不同的组件,发射和吸收辐射的活动核附近。方法.利用这些相机的光谱范围,通过EPIC光谱研究了连续发射。高分辨率的RGS光谱进行了分析,以表征吸收和发射线的功能,出现在光谱的源。对所有这些数据,加上紫外线信息,进行联合分析,以便对每个物体的观测特征进行一致的定性。结果源的连续发射的特征可以是,对于最弱的物体,由幂律和黑体的组合来表征,或者对于最亮的物体,由两个幂律分量来表征。在任何这些源的视线范围内,连续谱都不会被中性或电离物质吸收。在所有这些,我们已经确定了一个狭窄的Fe-Ka线在6.4 keV。在ESO 559-G19中,我们还发现了约7 keV的FeXXVI线。在软X射线波段,我们在HE 1143-1810和CTS A08.12的光谱中只识别出一条OVII线,在Mrk 110中识别出两条OVII-He α三重态和一条窄的OVIII-Ly α发射线。结论.在低状态物体的视线中没有检测到温暖的材料是由于视线中固有地较弱或不存在吸收,而不是由于数据中的低信噪比。除此之外,没有清晰的发射谱线不能完全归因于强连续谱对这些谱线的稀释。

英文摘要:

Aims. We seek a comprehensive analysis of all the information provided by the XMM-Newton satellite of the four Seyfert 1 galaxies ESO 359-G19, HE 1143-1810, CTS A08.12, and Mrk 110, including the UV range, to characterize the different components that are emitting and absorbing radiation in the vicinity of the active nucleus. Methods. The continuum emission was studied through the EPIC spectra by taking advantage of the spectral range of these cameras. The high-resolution RGS spectra were analyzed to characterize the absorbing and emission line features that arise in the spectra of the sources. All these data, complemented by information in the UV, are analyzed jointly in order to achieve a consistent characterization of the observed features in each object. Results. The continuum emission of the sources can be characterized either by a combination of a power law and a black body for the weakest objects or by two power law components for the brightest ones. The continuum is not absorbed by neutral or ionized material in the line of sight to any of these sources. In all of them we have identified a narrow Fe-Kalpha line at 6.4 keV. In ESO 559-G19 we also find an FeXXVI line at about 7 keV. In the soft X-rays band, we identify only one OVII line in the spectra of HE 1143-1810 and CTS A08.12, and two OVII-He alpha triplets and a narrow OVIII-Ly alpha emission line in Mrk 110. Conclusions. Not detecting warm material in the line of sight to the low state objects is due to intrinsically weaker or absent absorption in the line of sight and not to a low signal-to-noise ratio in the data. Besides this, the absence of clear emission lines cannot be fully attributed to dilution of those lines by a strong continuum.

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