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A Statistical Study of Rest-Frame Optical Emission Properties in Luminous Quasars at 2.0?z?2.5*

机译:统计量为2.0?z?2.5 *的发光类星体中静止帧光发射特性的统计研究

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We have obtained H-band spectra of 32 luminous quasars at 2.0≤z≤2.5 with the Multiple Mirror Telescope. The sample contains 15 radio-loud quasars (RLQs) and 17 radio-quiet quasars (RQQs). We have measured emission line properties from the rest-frame wavelength range of approximately λλ4500-5500 by fitting the data with composite model spectra. Our analysis includes comparison of RLQs versus RQQs, as well as comparison between the broad-absorption-line quasar (BALQSO) and non-broad-absorption-line quasar (nonBALQSO) subsets of the RQQ sample. In addition, we calculated the complete correlation matrix of the measured properties. We combined our high-redshift sample with the sample of 87 low-redshift quasars from Boroson & Green to determine the luminosity and redshift dependences of the measured emission properties. Our main results are the following: (1) The RLQ sample has significantly (at more than 97.2% confidence) stronger [O III] λ5007 emission than the RQQ sample, which favors scenarios including two populations of quasars that are intrinsically different. We are not aware of a unified model based upon orientation that can explain enhanced [O III] emission with increased radio power. (2) The RLQ sample has significantly narrower (in full width at half-maximum) Hβ broad component line profiles than the RQQ sample. (3) At the sensitivity of our observations, there are no statistically significant (95%) differences between the rest-frame optical emission line properties of the BALQSO and nonBALQSO subsamples. This result is consistent with the view that all RQQs have broad-absorption-line clouds with a small (~10%-20%) covering factor and that differences between the two types are merely a function of viewing angle and covering factor. (4) The significant [O III]-Fe II anticorrelation found in lower redshift quasars holds at this higher redshift range; however, it is the [O III] emission in this relationship that appears to be related to the physical distinction between the RLQ and RQQ classes instead of the Fe II emission that distinguishes at low redshifts and luminosities. We also find significant relationships between (i) the [O III] emission strength and the radio power, the broad-emission-line widths, and the X-ray continuum shape; (ii) positive correlations relating the strength of optical Fe II emission to broad-emission-line widths and the shape of the ionizing continuum; and (iii) similar relations for the strength and width of the Hβ emission. Many of these correlations have been found in lower redshift and luminosity studies. (5) We report a previously unknown luminosity and/or redshift dependence of the narrow-line region velocity width over the range 0z2.5, such that emission line widths increase with increasing luminosity. We confirm a similar dependence for the Hβ broad-line width. These findings may be evidence for a physical connection between the continuum and line-emitting regions at similar energies. Furthermore, we find a "Baldwin Effect" for the [O III] λ5007 line in the RQQ-only sample over this same range in redshifts.
机译:我们使用多镜望远镜获得了在2.0≤z≤2.5时32个发光类星体的H波段光谱。该样本包含15个无线电大类星体(RLQ)和17个无线电大类星体(RQQ)。通过将数据与复合模型光谱拟合,我们已经在大约λλ4500-5500的其余帧波长范围内测量了发射线特性。我们的分析包括RLQ与RQQ的比较,以及RQQ样本的宽吸收线类星体(BALQSO)和非宽吸收线类星体(nonBALQSO)子集之间的比较。此外,我们计算了所测特性的完整相关矩阵。我们将高红移样本与来自Boroson&Green的87个低红移类星体样本进行了组合,以确定测得的发射特性的光度和红移依赖性。我们的主要结果如下:(1)RLQ样本比RQQ样本具有显着(大于97.2%的置信度)更强的[O III]λ5007发射,这有利于包括两个本质不同的类星体的场景。我们尚不清楚基于方向的统一模型,该模型可以解释随着无线电功率的增加而增强的[O III]发射。 (2)与RQQ样本相比,RLQ样本的Hβ宽分量线轮廓明显更窄(在最大宽度处为一半)。 (3)在我们观察的敏感性下,BALQSO和非BALQSO子样本的其余帧光发射谱线特性之间在统计学上没有显着差异(> 95%)。该结果与以下观点一致:所有RQQ都具有宽吸收线云,覆盖率很小(〜10%-20%),并且两种类型之间的差异仅仅是视角和覆盖率的函数。 (4)在较低的红移类星体中发现的显着[O III] -Fe II反相关性在此较高的红移范围内保持;但是,这种关系中的[O III]发射似乎与RLQ和RQQ类之间的物理区别有关,而不是与Fe II发射有关,在低红移和发光度上有所区别。我们还发现(i)[O III]发射强度和无线电功率,宽发射线宽度和X射线连续谱形状之间的重要关系; (ii)光学Fe II发射强度与宽发射线宽度和电离连续体形状之间的正相关关系; (iii)Hβ发射的强度和宽度的相似关系。在较低的红移和亮度研究中已经发现了许多这些相关性。 (5)我们报告了以前未知的亮度和/或窄线区域速度宽度在0

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