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Defining the intrinsic AGN infrared spectral energy distribution and measuring its contribution to the infrared output of composite galaxies.

机译:定义固有的AGN红外光谱能量分布,并测量其对复合星系红外输出的贡献。

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摘要

We use infrared spectroscopy and photometry to empirically define the intrinsic mid- to far-infrared spectral energy distribution (i.e. 6–100 μm SED) of thermal emission produced by typical (i.e. 2–10 keV luminosity, L2-10 keV∼ 1042–1044 erg s−1) active galactic nuclei (hereafter AGNs). The average infrared SED of typical AGNs is best described as a broken power law at ≲40 μ m that falls steeply at ≳40 μm (i.e. at far-infrared wavelengths). Despite this fall-off at long wavelengths, at least three of the 11 AGNs in our sample have demonstrated SEDs that are AGN dominated even at 60 μ m, demonstrating the importance of accounting for any AGN contribution when calculating galaxy infrared luminosities. We find that the average intrinsic AGN 6–100 μ m SED gets bluer with increasing X-ray luminosity – a trend seen both within our sample and also when we compare it with the intrinsic SEDs of more luminous quasars (i.e. L2-10 keV≳ 1044 erg s−1). The range of intrinsic AGN SEDs is more closely matched by clumpy, rather than continuous, torus models. Using our intrinsic AGN SEDs we define a set of correction factors to convert either monochromatic infrared or X-ray luminosities into total (i.e. 8–1000 μm) AGN infrared luminosities. We outline a procedure that uses our newly defined intrinsic AGN infrared SEDs, in conjunction with a selection of host-galaxy templates, to measure the AGN contribution to the infrared output of composite galaxies from photometry alone. We verify the accuracy of our SED-fitting procedure by comparing our results to two independent measures of AGN contribution: (1) 12-μm luminosities obtained from high spatial resolution observations of nearby galaxies and (2) the equivalent width of the 11.25-μm PAH feature. Our SED-fitting procedure opens up the possibility of measuring the intrinsic AGN luminosities for large numbers of galaxies with well-sampled infrared data (e.g. IRAS, ISO, Spitzer and Herschel).
机译:我们使用红外光谱和光度法以经验方式定义由典型的(例如2–10 keV发光度,L2-10 keV〜1042–1044)产生的热辐射的固有的中红外光谱能量分布(即6–100μmSED) erg s-1)活跃的银河核(以下称为AGNs)。典型的AGN的平均红外SED最好描述为power40μm处的断能定律,它在≳40μm处(即在远红外波长处)急剧下降。尽管在长波长处会出现这种下降,但在我们的样本中的11个AGN中,至少有3个显示出即使在60μm时,SED仍是AGN主导,这证明了在计算星系红外光度时考虑任何AGN贡献的重要性。我们发现,随着X射线光度的增加,平均固有AGN 6–100μm SED会变蓝–在我们的样本中以及将其与更多发光类星体的固有SED(即L2-10 keV compare 1044 erg s-1)。固有的AGN SED的范围与块状而不是连续的圆环模型更紧密地匹配。使用我们的固有AGN SED,我们定义了一组校正因子,可将单色红外或X射线光度转换为总(即8–1000μm)AGN红外光度。我们概述了一个程序,该程序将使用我们新定义的固有AGN红外SED,并结合选定的宿主星系模板,以仅通过光度法测量AGN对复合星系的红外输出的贡献。我们通过将我们的结果与两个独立的AGN贡献量度进行比较来验证SED拟合过程的准确性:(1)从附近星系的高空间分辨率观测获得的12-μm光度,以及(2)11.25-μm的等效宽度PAH功能。我们的SED拟合程序为通过大量采样的红外数据(例如IRAS,ISO,Spitzer和Herschel)测量大量星系的固有AGN发光度提供了可能性。

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