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arXiv 1012.4334astro-ph.CO
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包含扩展射电源的低红移宽线活动星系核的射电性质

Radio Properties of Low Redshift Broad Line Active Galactic Nuclei Including Extended Radio Sources

Stephen E. Rafter, D. Michael Crenshaw, Paul J. Wiita

摘要:

我们对斯隆数字巡天(SDSS)的8434个低红移(z < 0.35)宽线活动星系核(AGN)样本中的扩展射电发射进行了研究。为了计算喷流和叶瓣对总射电光度的贡献,我们已经在我们以前对这个样本的研究中检测到了846个射电核心源,并在20厘米射电天空的微弱图像(FIRST)数据库中进行了系统的搜索,以寻找可能与光学对应物相关的扩展射电发射。我们发现846个射电核心源中有51个具有与活动星系核正相关的扩展辐射(距离光学活动星系核> 4”),另外12个活动星系核具有扩展射电辐射,但没有可探测到的射电核心辐射。在这63个活动星系核中,我们发现了6个巨大的射电星系(GRG),投影发射长度超过750千秒差距,和其他几个活动星系核不寻常的无线电形态也看到在高红移调查。许多扩展源的光谱类似于典型的宽线射电星系光谱,具有宽的H $α$发射线,盒状轮廓和大的M_BH。考虑到扩展发射,我们发现了强有力的证据,在射电响度参数R的双峰分布,其中较低的无线电光度的核心,只有源出现作为一个人口独立于扩展源,在log(R)$\approx 1.75$的分界线。这条分界线确保了这些活动星系核确实是射电最强的活动星系核,与数量更多的射电安静活动星系核相比,它们的中央引擎可能具有不同或极端的物理条件。

英文摘要:

We present a study of the extended radio emission in a sample of 8434 low redshift (z < 0.35) broad line active galactic nuclei (AGN) from the Sloan Digital Sky Survey (SDSS). To calculate the jet and lobe contributions to the total radio luminosity, we have taken the 846 radio core sources detected in our previous study of this sample and performed a systematic search in the Faint Images of the Radio Sky at Twenty-centimeters (FIRST) database for extended radio emission that is likely associated with the optical counterparts. We found 51 out of 846 radio core sources have extended emission (> 4" from the optical AGN) that is positively associated with the AGN, and we have identified an additional 12 AGN with extended radio emission but no detectable radio core emission. Among these 63 AGN, we found 6 giant radio galaxies (GRGs), with projected emission exceeding 750 kpc in length, and several other AGN with unusual radio morphologies also seen in higher redshift surveys. The optical spectra of many of the extended sources are similar to that of typical broad line radio galaxy spectra, having broad H$α$ emission lines with boxy profiles and large M_BH. With extended emission taken into account, we find strong evidence for a bimodal distribution in the radio-loudness parameter R, where the lower radio luminosity core-only sources appear as a population separate from the extended sources, with a dividing line at log(R) $\approx 1.75$. This dividing line ensures that these are indeed the most radio-loud AGN, which may have different or extreme physical conditions in their central engines when compared to the more numerous radio quiet AGN.

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