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首页> 外文期刊>The Astrophysical journal >REVEALING THE HEAVILY OBSCURED ACTIVE GALACTIC NUCLEUS POPULATION OF HIGH-REDSHIFT 3CRR SOURCES WITH CHANDRA X-RAY OBSERVATIONS
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REVEALING THE HEAVILY OBSCURED ACTIVE GALACTIC NUCLEUS POPULATION OF HIGH-REDSHIFT 3CRR SOURCES WITH CHANDRA X-RAY OBSERVATIONS

机译:利用CHANDRA X射线观测揭示高折光3CRR源的重度活跃主动银河系核种群

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摘要

Chandra observations of a complete, flux-limited sample of 38 high-redshift (1 z 2), low-frequency-selected (and so unbiased in orientation) 3CRR radio sources are reported. The sample includes 21 quasars (=broad-line radio galaxies) and 17 narrow-line radio galaxies (NLRGs) with matched 178?MHz radio luminosity (log L R(5 GHz) ~44-45). The quasars have high radio core fraction, high X-ray luminosities (log L X ~45-46), and soft X-ray hardness ratios (HR ~–0.5) indicating low obscuration. The NLRGs have lower core fraction, lower apparent X-ray luminosities (log L X ~43-45), and mostly hard X-ray hardness ratios (HR 0) indicating obscuration (N H ~1022-1024?cm–2). These properties and the correlation between obscuration and radio core fraction are consistent with orientation-dependent obscuration as in unification models. About half the NLRGs have soft X-ray hardness ratios and/or a high [O III] emission line to X-ray luminosity ratio suggesting obscuration by Compton thick (CT) material so that scattered nuclear or extended X-ray emission dominates (as in NGC?1068). The ratios of unobscured to Compton-thin (1022?cm–2 N H(int) 1.5 × 1024?cm–2) to CT (N H(int) 1.5 × 1024?cm–2) is 2.5:1.4:1 in this high-luminosity, radio-selected sample. The obscured fraction is 0.5, higher than is typically reported for active galactic nuclei at comparable luminosities from multi-wavelength surveys (0.1-0.3). Assuming random nuclear orientation, the unobscured half-opening angle of the disk/wind/torus structure is ~60° and the obscuring material covers 30°, ~12° of which is CT. The multi-wavelength properties reveal that many NLRGs have intrinsic absorption 10-1000 × higher than indicated by their X-ray hardness ratios, and their true L X values are ~10-100× larger than the hardness-ratio absorption corrections would indicate.
机译:Chandra报告了38个高红移(1 0),指示暗度(NH〜1022-1024?cm–2)。这些属性以及模糊和无线电核心分数之间的相关性与统一模型中与方向相关的模糊一致。大约一半的NLRG具有柔和的X射线硬度比和/或较高的[O III]发射线与X射线光度比,表明被康普顿厚(CT)材料遮盖,因此散射核或扩展X射线发射占主导地位(如在NGC?1068中)。康普顿薄(1022?cm–2 1.5×1024?cm–2)的通畅比为2.5:1.4:1在这种高亮度,无线电选择的样本中。遮蔽分数是0.5,比在多波长调查(0.1-0.3)的可比较亮度下通常报告的活跃银河核的分数高。假设核方向随机,则圆盘/风/环的结构的半开角未遮挡为〜60°,遮盖材料的遮盖角为30°,其中CT为〜12°。多波长特性表明,许多NLRG的固有吸收比其X射线硬度比所指示的高10-1000×,并且它们的真实L X值比硬度比吸收校正所指示的要大10-100×。
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