论文标题
紧凑的对象日食期间HMXB XTE J1855-026的第一个X射线频谱
The first X-ray spectrum of the HMXB XTE J1855-026 during the compact object eclipse
论文作者
论文摘要
我们介绍了第一个{\ it xmm-newton}对经典超级巨大X射线X射线二进制XTE J1855 $ - $ 026的观察,完全涵盖了中子星(NS),涵盖轨道阶段$ ϕ = 0.00-0.11 $。数据的分析使我们能够a)与现有的日食观察期间获得的参数进行比较,b)探索B0I型供体的背部照明恒星风。在日食期间未观察到用于描述预蚀过程中柔软过量的黑体组件。然后必须在NS附近或供体NS线附近生产它。 Eclipse期间的$ 0.3-10 $ KEV光度($ \ sim 10^{34} $ erg s $^{ - 1} $)比pre Eclipse低70倍。在平均日食频谱中,Fe K $α$线的强度为$ \ sim 7.4 $ 7.4 $ $倍,比在日食期间测得的强度低。由于K $α$光子无法在风中散布,因此绝大多数Fe K $α$排放必须来自NS $ 1R _ {*} $的距离。 Eclipse频谱通过添加了两个光电离等离子体成功建模($ \logξ_ {\ rm 2,热} = 3.7 $)和低排放度量($ em _ {\ rm hot} \大约2 \ times 10^{56} $ cm $^{ - 3} $)。假设寒冷和热气相是恒星风的团块和次数,以及$ \ $ \的团块填充因子约为[0.04-0.05] $,典型的大型恒星,巨大的恒星的密度对比,团块与$ n _ _ {\ rm c}/n n _ n _ _ _ i的clumpump介质与$ n _ {理论上的期望和巨大恒星风的光学观察。
We present the first {\it XMM-Newton} observation of the classical supergiant high-mass X-ray binary XTE J1855$-$026 taken entirely during the eclipse of the neutron star (NS), covering the orbital phases $ϕ= 0.00-0.11$. The analysis of the data allows us to a) compare with the parameters obtained during the existing pre eclipse observation and b) explore the back illuminated stellar wind of the B0I type donor. The black body component, used to describe the soft excess during pre eclipse, is not observed during eclipse. It must be then produced near the NS or along the donor-NS line. The $0.3-10$ keV luminosity during eclipse ($\sim 10^{34}$ erg s$^{-1}$) is 70 times lower than pre eclipse. The intensity of the Fe K$α$ line, in the average eclipse spectrum, is $\sim 7.4$ times lower than the one measured during pre eclipse. Since K$α$ photons can not be resonantly scattered in the wind, the vast majority of Fe K$α$ emission must come from distances within $1R_{*}$ from the NS. The eclipse spectrum is successfully modelled through the addition of two photoionized plasmas, one with low ionization ($\logξ_{\rm 1,cold}=0.36$) and high emission measure ($EM_{\rm 1,cold}\approx 3\times 10^{59}$ cm$^{-3}$) and another with high ionization ($\logξ_{\rm 2,hot}=3.7$) and low emission measure ($EM_{\rm hot}\approx 2\times 10^{56}$ cm$^{-3}$). Assuming that the cold and hot gas phases are the clumps and the interclump medium of the stellar wind, respectively, and a clump volume filling factor of $\approx [0.04-0.05]$, typical for massive stars, a density contrast between clumps and the interclump medium of $n_{\rm c}/n_{\rm i}\approx 180$ is deduced, in agreement with theoretical expectations and optical-UV observations of massive star winds.