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首页> 外文期刊>The Astrophysical journal >Ionized Absorbers in Active Galactic Nuclei: The Role of Collisional Ionization and Time-evolving Photoionization
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Ionized Absorbers in Active Galactic Nuclei: The Role of Collisional Ionization and Time-evolving Photoionization

机译:活跃银河原子核中的电离吸收剂:碰撞电离和随时间演化的光电离的作用

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In this paper we explore collisional ionization and time-evolving photoionization in the X-ray-discovered, ionized absorbers in Seyfert galaxies. These absorbers show temporal changes inconsistent with simple equilibrium models. We develop a simple code to follow the temporal evolution of nonequilibrium photoionized gas. As a result several effects appear that are easily observable and that, in fact, may explain otherwise paradoxical behavior. Specifically, we find the following: 1. In many important astrophysical conditions (O VII, O VIII dominant and high [1022.5 cm-2] column density) pure collisional and photoionization equilibria can be distinguished with moderate spectral resolution observations, because of a strong absorption structure between 1 and 3 keV. This feature is due mainly to iron L XVII-XIX and neon K IX-X absorption, which is much stronger in collisional models. This absorption structure may be misinterpreted as a flattening of the intrinsic emission spectrum above ~1 keV in low-resolution data. 2. In time-evolving nonequilibrium photoionization models the response of the ionization state of the gas to sudden changes of the ionizing continuum is smoothed and delayed at low gas densities (usually up to 108 cm-3), even when the luminosity increases. The recombination time can be much longer (up to orders of magnitude) than the photoionization timescale. Hence, a photoionized absorber subject to frequent, quick, and consistent changes of ionizing luminosity is likely to be overionized with respect to the equilibrium ionization state. 3. If the changes of the ionizing luminosity are not instantaneous, and the electron density is low enough (the limit depends on the average ionization state of the gas but is usually ~107 to ~108 cm-3), the ionization state of the gas can continue to increase while the source luminosity decreases, so a maximum in the ionization state of a given element may occur during a minimum of the ionizing intensity (the opposite of the prediction of equilibrium models). 4. Different ions of different elements reach their equilibrium configuration on different timescales, so models in which all ions of all elements are in photoionization equilibrium so often fail to describe active galactic nucleus (AGN) spectral evolution. These properties are similar to those seen in several ionized absorbers in AGNs, properties that had hitherto been puzzling. We applied these models to a high signal-to-noise ratio ROSAT PSPC observation of the Seyfert 1 galaxy NGC 4051. The compressed dynamical range of variation of the ionization parameter U and the ionization delays seen in the ROSAT observations of NGC 4051 may be simply explained by a nonequilibrium photoionization model, giving well-constrained parameters: n=(1.0)×108 cm-3 and R=(0.74)×1016 cm (~3 light-days).
机译:在本文中,我们探索了塞弗特星系中X射线发现的电离吸收体中的碰撞电离和随时间演化的电离。这些吸收体显示出与简单平衡模型不一致的时间变化。我们开发了一个简单的代码来跟踪非平衡光电离气体的时间演化。结果,出现了几种效应,这些效应很容易观察到,并且实际上可以解释相反的行为。具体来说,我们发现以下内容:1.在许多重要的天体物理条件(O VII,O VIII占主导地位和高[1022.5 cm-2]列密度)下,纯碰撞碰撞和光电离平衡可通过中等光谱分辨率观察来区分,因为1至3 keV之间的吸收结构。此功能主要是由于铁L XVII-XIX和霓虹灯K IX-X的吸收,这在碰撞模型中要强得多。在低分辨率数据中,此吸收结构可能被误解为高于〜1 keV的本征发射光谱的展平。 2.在随时间演变的非平衡光电离模型中,即使发光度增加,在低气体密度(通常高达108 cm-3)下,气体的电离状态对电离连续谱突然变化的响应也会变得平滑和延迟。重组时间可能比光电离时间尺度长得多(最多几个数量级)。因此,相对于平衡电离状态,经受频繁,快速且一致的电离发光度变化的光离化吸收体可能被过度电离。 3.如果电离光度的变化不是瞬时的,并且电子密度足够低(极限取决于气体的平均电离状态,但通常为〜107至〜108 cm-3),则电离状态气体会继续增加,而光源的发光度会降低,因此给定元素的电离状态可能会在最小电离强度期间发生最大值(与平衡模型的预测相反)。 4.不同元素的不同离子在不同的时间尺度上达到其平衡构型,因此其中所有元素的所有离子均处于光电离平衡的模型常常无法描述活性银河原子核(AGN)光谱演化。这些性质类似于AGN中几种离子吸收剂中所见的性质,这些性质迄今一直令人困惑。我们将这些模型应用于塞弗特1号星系NGC 4051的高信噪比ROSAT PSPC观测。电离参数U的变化动态压缩范围和NGC 4051的ROSAT观测中看到的电离延迟可能很简单用非平衡光电离模型解释,给出了很好约束的参数:n =(1.0)×108 cm-3和R =(0.74)×1016 cm(〜3个光天)。

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