论文标题
XMM-NEWTON狭窄线Seyfert 1 Galaxy IRAS 13224 $ - $ 3809:X射线光谱分析II II
XMM-Newton Observations of the Narrow-Line Seyfert 1 Galaxy IRAS 13224$-$3809 : X-ray Spectral Analysis II
论文作者
论文摘要
以前,我们使用固定电子密度为$ 10^{15} $ cm $^{ - 3} $的光盘反射模型对窄线Seyfert 1 Galaxy Iras 13224 $ -3809进行了建模。需要一个额外的黑体组件以适合2 keV以下的软X射线。在这项工作中,我们同时分析了该来源的五个磁通分辨的XMM-Newton光谱,其中包含在2 M女士的数据中收集的数据,其电子密度为$ n _ {\ rm e} \ rm e} \ lm e} \ loct of10^{20} $ cm $ $ $ $ $^{ - 3} $^{ - 3} $和$ z _ _ _ { fe} = 3.2 \ pm0.5z _ {\ odot} $用于适合此源的宽带光谱。不需要额外的组件才能适应软过量。与假定低圆盘密度的先前模型一样,我们的最佳拟合模型可提供对黑洞自旋和圆盘倾斜角的一致测量。最后,我们根据最佳拟合密度和电离参数计算IRAS 13224 $ - $ 3809中的电晕与反射区域之间的平均照明距离,该参数从0.43 $ \ sqrt {f _ {\ rm ad}/f _ {\ rm ad}/f _ {通量状态至1.71 $ \ sqrt {f _ {\ rm ad}/f _ {\ rm inf}} $ $ r _ {\ rm g} $在最高通量状态下,假设黑洞质量为$ 2 \ times10^{6} m _ {6} m _ {\ odot} $。 $ f _ {\ rm ad}/f _ {\ rm inf} $是到达积聚盘和无穷大的冠状发射的通量之间的比率。该比率取决于IRAS 13224 $ -3809的冠状区域的几何形状。因此,我们仅根据简单的“ Lamp-Post”模型讨论其价值,尽管以后需要对IRAS 13224 $ - $ 3809的光盘发射率概况的详细建模来揭示Corona的确切几何形状。
Previously, we modelled the X-ray spectra of the narrow-line Seyfert 1 galaxy IRAS 13224$-$3809 using a disc reflection model with a fixed electron density of $10^{15}$ cm$^{-3}$. An additional blackbody component was required to fit the soft X-ray excess below 2 keV. In this work, we analyse simultaneously five flux-resolved XMM-Newton spectra of this source comprising data collected over 2 Ms. A disc reflection model with an electron density of $n_{\rm e}\approx10^{20}$ cm$^{-3}$ and an iron abundance of $Z_{\rm Fe}=3.2\pm0.5Z_{\odot}$ is used to fit the broad-band spectra of this source. No additional component is required to fit the soft excess. Our best-fit model provides consistent measurements of black hole spin and disc inclination angle as in previous models where a low disc density was assumed. In the end, we calculate the average illumination distance between the corona and the reflection region in the disc of IRAS 13224$-$3809 based on best-fit density and ionisation parameters, which changes from 0.43$\sqrt{f_{\rm AD}/f_{\rm INF}}$ $r_{\rm g}$ in the lowest flux state to 1.71$\sqrt{f_{\rm AD}/f_{\rm INF}}$ $r_{\rm g}$ in the highest flux state assuming a black hole mass of $2\times10^{6}M_{\odot}$. $f_{\rm AD}/f_{\rm INF}$ is the ratio between the flux of the coronal emission that reaches the accretion disc and infinity. This ratio depends on the geometry of the coronal region in IRAS 13224$-$3809. So we only discuss its value based on the simple `lamp-post' model, although detailed modelling of the disc emissivity profile of IRAS 13224$-$3809 is required in future to reveal the exact geometry of the corona.