论文标题

明亮环礁源GX 9+9中的反射组件

Reflection component in the Bright Atoll Source GX 9+9

论文作者

Iaria, R., Mazzola, S. M., Di Salvo, T., Marino, A., Gambino, A. F., Sanna, A., Riggio, A., Burderi, L.

论文摘要

GX 9+9(4U 1728-16)是具有中子星的低质量X射线二进制(LMXB)。尽管它属于明亮的环礁源的子类,以及GX 9+1,GX 3+1和GX 13+1,但其宽带光谱的研究很差,并且显然没有在光谱中显示出反射特征。 为了很好地限制连续体并验证是否存在相对论涂片的反射组件,我们使用{\ it beppoSax}和\ textit {xmm-newton}光谱分析了GX 9+9的宽带光谱,覆盖了0.3-40 kev Energy。 我们符合采用磁盘黑体和成分组件的模型的频谱,其种子光子具有黑体光谱(东部模型)。统计上等效的模型由一个组成的组件组成,其种子光子具有磁盘黑体分布以及模仿可能与边界层(西部模型)相关的饱和组合的黑体。其他试验并没有恢复健康。 在柔软的状态下观察到GX 9+9的光谱,其发光度为$ 2.3 \ times 10^{37} $ erg s $^{ - 1} $,假设与5 kpc的来源距离。在东部型号的情况下,我们发现,成分组件的种子 - 光子温度和电子温度为$ 1.14^{+0.10} _ { - 0.07} $ kev和$ 2.80^{+0.09} _ { - 0.09} _ { - 0.04} $ kev,分别分别是$ kev的$ 0.99 $8.999999999。内部积聚盘的色温为$ 0.86^{+0.08} _ { - 0.02} $ keV和$ 0.82 \ pm 0.02 $ kev,分别为{\ it beppoSax}和\ textit {xmm-newton} spect。相反,在西方模型方案中,我们发现种子 - 光子温度为$ 0.87 \ pm 0.07 $ keV和$ 1.01 \ pm 0.08 $ kev,分别为{\ it beppoSax}和\ textit {xmm-newton} spectrum。 (删节摘要)

GX 9+9 (4U 1728-16) is a low mass X-ray binary (LMXB) source harboring a neutron star. Although it belongs to the subclass of the bright Atoll sources together with GX 9+1, GX 3+1, and GX 13+1, its broadband spectrum is poorly studied and apparently does not show reflection features in the spectrum. To constrain the continuum well and verify whether a relativistic smeared reflection component is present, we analyze the broadband spectrum of GX 9+9 using {\it BeppoSAX} and \textit{XMM-Newton} spectra covering the 0.3-40 keV energy band. We fit the spectrum adopting a model composed of a disk-blackbody plus a Comptonized component whose seed photons have a blackbody spectrum (Eastern Model). A statistically equivalent model is composed of a Comptonized component whose seed photons have a disk-blackbody distribution plus a blackbody that mimics a saturated Comptonization likely associated with a boundary layer (Western model). Other trials did not return a good fit. The spectrum of GX 9+9 was observed in a soft state and its luminosity is $2.3 \times 10^{37}$ erg s$^{-1}$ assuming a distance to the source of 5 kpc. In the Eastern Model scenario, we find the seed-photon temperature and electron temperature of the Comptonized component to be $1.14^{+0.10}_{-0.07}$ keV and $2.80^{+0.09}_{-0.04}$ keV, respectively, while the optical depth of the Comptonizing corona is $8.9\pm0.4$. The color temperature of the inner accretion disk is $0.86^{+0.08}_{-0.02}$ keV and $0.82 \pm 0.02$ keV for the {\it BeppoSAX} and \textit{XMM-Newton} spectrum, respectively. In the Western Model scenario, instead, we find that the seed-photon temperature is $0.87 \pm 0.07$ keV and $1.01 \pm 0.08$ keV for the {\it BeppoSAX} and \textit{XMM-Newton} spectrum, respectively. (Abridged abstract)

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