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Mid-infrared luminous quasars in the GOODS–Herschel fields : a large population of heavily obscured, Compton-thick quasars at z ≈ 2.

机译:GOODS–Herschel场中的中红外发光类星体:z≈2时,大量大量被遮盖的康普顿厚类星体。

摘要

We present the infrared (IR) and X-ray properties of a sample of 33 mid-IR luminous quasars (νL6 μm ≥ 6 × 1044 erg s−1) at redshift z ≈ 1–3, identified through detailed spectral energy distribution analyses of distant star-forming galaxies, using the deepest IR data from Spitzer and Herschel in the GOODS–Herschel fields. The aim is to constrain the fraction of obscured, and Compton-thick (CT, NH > 1.5 × 1024 cm−2) quasars at the peak era of nuclear and star formation activities. Despite being very bright in the mid-IR band, ≈30 per cent of these quasars are not detected in the extremely deep 2 and 4 Ms Chandra X-ray data available in these fields. X-ray spectral analysis of the detected sources reveals that the majority (≈67 per cent) are obscured by column densities NH > 1022 cm−2; this fraction reaches ≈80 per cent when including the X-ray-undetected sources (9 out of 33), which are likely to be the most heavily obscured, CT quasars. We constrain the fraction of CT quasars in our sample to be ≈24–48 per cent, and their space density to be Φ = (6.7 ± 2.2) × 10−6 Mpc−3. From the investigation of the quasar host galaxies in terms of star formation rates (SFRs) and morphological distortions, as a sign of galaxy mergers/interactions, we do not find any direct relation between SFRs and quasar luminosity or X-ray obscuration. On the other hand, there is tentative evidence that the most heavily obscured quasars have, on average, more disturbed morphologies than the unobscured/moderately obscured quasar hosts, which preferentially live in undisturbed systems. However, the fraction of quasars with disturbed morphology amongst the whole sample is ≈40 per cent, suggesting that galaxy mergers are not the main fuelling mechanism of quasars at z ≈ 2.
机译:我们介绍了33个中红外发光类星体(νL6μm≥6×1044 erg s-1)在红移z≈1-3时的红外(X)和X射线特性,通过详细的光谱能量分布分析确定利用来自GOODS–Herchel场中Spitzer和Herschel的最深红外数据,形成了遥远的恒星系。目的是在核活动和恒星形成活动的高峰期限制模糊和康普顿厚(CT,NH> 1.5×1024 cm-2)类星体的比例。尽管在中红外波段非常亮,但在这些领域中可用的极深的2和4 Ms Chandra X射线数据中,未检测到这类类星体的≈30%。对检测到的源进行的X射线光谱分析表明,大多数(≈67%)被色谱柱密度NH> 1022 cm-2所掩盖。当包括未检测到X射线的放射源(33个中的9个)时,这一比例达到≈80%,这可能是最模糊的CT类星体。我们将样本中CT类星体的比例限制为≈24–48%,其空间密度为Φ=(6.7±2.2)×10−6 Mpc-3。通过对恒星宿主星系的恒星形成率(SFR)和形态畸变的调查,作为星系合并/相互作用的标志,我们没有发现SFR与类星体的光度或X射线模糊之间有任何直接关系。另一方面,有初步证据表明,与那些优先生活在不受干扰的系统中的,未被遮盖/中度遮盖的类星体相比,被遮盖最严重的类星体平均而言具有更多的干扰形态。但是,在整个样本中,形态受到干扰的类星体的比例约为40%,这表明星系合并不是z≈2时类星体的主要推动力。

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