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ASCA Observations of the Absorption Line Features from the Superluminal Jet Source GRS 1915+105

机译:ASCA观测的超光速射流源GRS 1915 + 105的吸收线特征

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We have carried out a precise energy spectral analysis of the superluminal jet source GRS 1915+105 observed with ASCA six times from 1994 to 1999. The source was so bright that most SIS data suffered from event pileup. We have developed a new technique to circumvent the pileup effect, which enabled us to study the spectrum in detail and at high resolution (ΔE/E ≈ 2%). In the energy spectra of 1994 and 1995, resonant absorption lines of Ca XX Kα, Fe XXV Kα, Fe XXVI Kα, as well as blends of the absorption lines of Ni XXVII Kα + Fe XXV Kβ and Ni XXVIII Kα + Fe XXVI Kβ, were observed. Such absorption lines have not been found in other objects, except for iron absorption lines from GRO J1655-40, another superluminal jet source. We carried out a "curve of growth" analysis for the absorption lines and estimated column densities of the absorbing ions. We found that a plasma of moderate temperature (0.1-10 keV) and cosmic abundance cannot account for the observed large equivalent widths. The hydrogen column density of such plasma would be so high that the optical depth of Thomson scattering would be too thick (NH 1024 cm-2). We require either a very high kinetic temperature of the ions (100 keV) or extreme overabundances (100 Z☉). In the former case, the ion column densities have reasonable values of 1017-1018 cm-2. We modeled the absorber as a photoionized disk which envelops the central X-ray source. Using a photoionization calculation code, we constrain physical parameters of the plasma disk, such as the ionization parameter, radius, and density. Estimated parameters were found to be consistent with those of a radiation-driven disk wind. These absorption line features may be peculiar to superluminal jet sources and related to the jet formation mechanism. Alternatively, they may be common characteristics of supercritical edge-on systems.
机译:我们对1994年至1999年用ASCA观测到的六次超光速射流源GRS 1915 + 105进行了精确的能谱分析。该源是如此明亮,以致大多数SIS数据都受到事件堆积的影响。我们已经开发出一种新技术来规避堆积效应,从而使我们能够以高分辨率(ΔE/ E≈2%)详细研究光谱。在1994和1995年的能谱中,Ca XXKα,Fe XXVKα,Fe XXVIKα的共振吸收线,以及Ni XXVIIKα+ Fe XXVKβ和Ni XXVIIIKα+ Fe XXVIKβ的吸收线的共混物,被观察。除其他超光源射流源GRO J1655-40的铁吸收线外,在其他物体中也未发现这种吸收线。我们对吸收线和吸收离子的估计柱密度进行了“增长曲线”分析。我们发现中等温度(0.1-10 keV)和宇宙丰度的等离子体不能解释观察到的较大等效宽度。这种等离子体的氢柱密度会很高,以至于汤姆森散射的光学深度会太厚(NH 1024 cm-2)。我们需要非常高的离子动力学温度(100 keV)或极端过量的离子(100Z☉)。在前一种情况下,离子柱密度的合理值为1017-1018 cm-2。我们将吸收器建模为包围中心X射线源的光电离盘。使用光电离计算代码,我们限制了等离子体盘的物理参数,例如电离参数,半径和密度。发现估计的参数与辐射驱动的盘绕的参数一致。这些吸收线特征可能是超腔射流源所特有的,并且与射流形成机制有关。或者,它们可能是超临界边沿式系统的共同特征。

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