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Narrow-line region gas kinematics of 24 264 optically selected AGN : the radio connection.

机译:24 264光学选择的AGN的窄线区域气体运动学:无线电连接。

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摘要

Using a sample of 24 264 optically selected active galactic nuclei (AGNs) from the SDSS DR7 data base, we characterize how the profile of the [O III] λ5007 emission line relates to bolometric luminosity (LAGN), Eddington ratio, radio loudness, radio luminosity (L1.4 GHz) and optical class (i.e. broad/narrow-line Seyfert 1, type 2) to determine what drives the kinematics of this kpc-scale line emitting gas. First, we use spectral stacking to characterize how the average [O III] λ5007 profile changes as a function of these five variables. After accounting for the known correlation between LAGN and L1.4 GHz, we report that L1.4 GHz has the strongest influence on the [O III] λ5007 profile, with AGNs of moderate radio luminosity (L1.4 GHz = 1023–1025 W Hz−1) having the broadest [O III] λ5007 profiles. Conversely, we find only a modest change in the [O III] λ5007 profile with increasing radio loudness and find no significant difference between the [O III] λ5007 profiles of broad- and narrow-line Seyfert 1s. When binned according to Eddington ratio, only the AGNs in our highest bin (i.e. >0.3) show any signs of having broadened [O III] λ5007 profiles, although the small numbers of such extreme AGNs in our sample mean we cannot rule out that other processes (e.g. radio jets) are responsible for this broadening. The [O III] λ5007 profiles of type 1 and type 2 AGNs show the same trends in terms of line width, but type 1 AGNs display a much stronger ‘blue wing’, which we interpret as evidence of outflowing ionized gas. We perform multicomponent fitting to the Hβ, [O III] λλ4959, 5007, [N II] λλ6548, 6584 and Hα lines for all the AGNs in our sample to calculate the proportions of AGNs with broad [O III] λ5007 profiles. The individual fits confirm the results from our stacked spectra; AGNs with L1.4 GHz > 1023 W Hz−1 are roughly five times more likely to have extremely broad [O III] λ5007 lines (full width at half-maximum, FWHMAvg > 1000 km s−1) compared to lower L1.4 GHz AGNs, and the width of the [O III] λ5007 line peaks in moderate-radio-luminosity AGNs (L1.4 GHz ∼ 1024 W Hz−1). Our results are consistent with the most disturbed gas kinematics being induced by compact radio cores (rather than powerful radio jets), although broadened [O III] λ5007 lines are also present, but much rarer, in low-L1.4 GHz systems. Our catalogue of multicomponent fits is freely available as an online resource for statistical studies of the kinematics and luminosities of the narrow- and broad-line AGN regions and the identification of potential targets for follow-up observations at http://sites.google.com/site/sdssalpaka.
机译:使用来自SDSS DR7数据库的24 264个光学选择的活动星系核(AGN)样本,我们表征了[O III]λ5007发射谱线与辐射热亮度(LAGN),爱丁顿比,无线电响度,无线电的关系发光度(L1.4 GHz)和光学类别(即,宽/窄线赛弗1号,类型2)来确定是什么因素驱动这种kpc刻度线发射气体的运动学。首先,我们使用光谱叠加来表征平均[O III]λ5007轮廓如何随这五个变量而变化。考虑到LAGN与L1.4 GHz之间的已知相关性后,我们报告L1.4 GHz对[O III]λ5007剖面的影响最大,其AGN具有中等的无线电发光度(L1.4 GHz = 1023–1025 W Hz-1)具有最宽的[O III]λ5007轮廓。相反,我们发现随着无线电响度的增加[O III]λ5007谱线只有适度的变化,而在宽线和窄线塞弗特1s的[O III]λ5007谱线之间没有显着差异。当根据爱丁顿比率进行分类时,只有我们最高分类箱中的AGN(即> 0.3)显示出[O III]λ5007谱变宽的任何迹象,尽管我们样本中的此类极端AGN数量很少,这意味着我们不能排除其他流程(例如射流)是造成这种范围扩大的原因。 1型和2型AGN的[O III]λ5007谱线在线宽方面显示出相同的趋势,但是1型AGN表现出更强的“蓝翼”,我们将其解释为离子化气体流出的证据。我们对样本中所有AGN的Hβ,[O III] λλ4959、5007,[N II] λλ6548、6584和Hα线进行多分量拟合,以计算具有[O III]λ5007轮廓的AGN的比例。个体拟合确定了我们叠加光谱的结果; L1.4 GHz> 1023 W Hz−1的AGN与较低的L1.4相比,具有极宽的[O(III]λ5007线(半高全宽,FWHMAvg> 1000 km roughlys-1)的可能性大约高五倍GHz AGNs,[O III]λ5007线的宽度在中等辐射度的AGNs(L1.4 GHz〜1024 W Hz-1)中达到峰值。我们的结果与紧凑型无线电核心(而不是强大的无线电射流)引起的最扰动的气体运动学是一致的,尽管在低L1.4 GHz系统中也存在加宽的[O III]λ5007谱线,但更为罕见。我们的多分量拟合目录可作为在线资源免费获得,该资源可在http://sites.google上对窄线和宽线AGN地区的运动学和光度进行统计研究,并确定后续观察的潜在目标。 com / site / sdssalpaka。

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