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arXiv 2111.12976astro-ph.IMastro-ph.HE
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Einstein探测器上theFollow-up X射线望远镜的本底和灵敏度估算

Estimate of the Background and Sensitivity of theFollow-up X-ray Telescope onboard Einstein Probe

Juan Zhang, Liqiang Qi, Yanji Yang, Juan Wang, Yuan Liu, Weiwei Cui, Donghua Zhao, Shumie Jia, Tianming Li, Tianxiang Chen, Gang Li, Xiaofan Zhao, Yong Chen, Hu… 展开作者

Juan Zhang, Liqiang Qi, Yanji Yang, Juan Wang, Yuan Liu, Weiwei Cui, Donghua Zhao, Shumie Jia, Tianming Li, Tianxiang Chen, Gang Li, Xiaofan Zhao, Yong Chen, Huaqiu Liu, Congying Bao, Ju Guan, Liming Song, Weimin Yuan

摘要:

作为一项致力于时域天体物理研究的空间X射线成像任务,“爱因斯坦探测器”(EP)携带两种科学有效载荷,即宽视场X射线望远镜(WXT)和后续X射线望远镜(FXT)。FXT采用Wolter-I型反射镜和pn-CCD探测器。在这项工作中,我们调查的FXT的在轨背景的基础上Geant 4模拟。考虑了EP轨道环境中存在的各种空间成分的影响,例如宇宙光子背景、宇宙射线初级和次级粒子(例如质子、电子和正电子)、γ射线和地磁赤道附近的低能质子。所获得的主要由宇宙射线质子和宇宙光子背景诱导的0.5-10 keV的仪器背景对应于焦平面探测器(FPD)的成像区域中的$\sim$ 3.1 $\times$ 10 $^{-2}$计数s $^{-1}$ keV $^{-1}$的水平,即归一化后的3.7 $\times$ 10 $^{-3}$计数s $^{-1}$ keV $^{-1}$ cm $^{-2}$。与仪器背景相比,视场(FOV)背景,这是由宇宙光子反射的光学镜,占主导地位低于2 keV。基于焦点内的模拟背景水平(30 $^{\prime\prime}$半径的圆),计算FXT的灵敏度,理论上可以实现几个$μ$螃蟹(数量级为10 $^{-14}$ erg cm $^{-2}$ s $^{-1}$)(大约10 $^{-13}$ erg cm $^{-2}$ s $^{-1}$),用于25分钟曝光的定点观察。如果包括背景扣除的额外10%系统不确定性,则该灵敏度将变差$\sim2$。

英文摘要:

As a space X-ray imaging mission dedicated to time-domain astrophysics, the Einstein Probe (EP) carries two kinds of scientific payloads, the wide-field X-ray telescope (WXT) and the follow-up X-ray telescope (FXT). FXT utilizes Wolter-I type mirrors and the pn-CCD detectors. In this work, we investigate the in-orbit background of FXT based on Geant4 simulation. The impact of various space components present in the EP orbital environment are considered, such as the cosmic photon background, cosmic ray primary and secondary particles (e.g. protons, electrons and positrons), albedo gamma rays, and the low-energy protons near the geomagnetic equator. The obtained instrumental background at 0.5-10 keV, which is mainly induced by cosmic ray protons and cosmic photon background, corresponds to a level of $\sim$3.1$\times$10$^{-2}$ counts s$^{-1}$ keV$^{-1}$ in the imaging area of the focal plane detector (FPD), i.e. 3.7$\times$10$^{-3}$ counts s$^{-1}$ keV$^{-1}$ cm$^{-2}$ after normalization. Compared with the instrumental background, the field of view (FOV) background, which is induced by cosmic photons reflected by the optical mirror, dominates below 2 keV. Based on the simulated background level within the focal spot (a 30$^{\prime\prime}$-radius circle), the sensitivity of FXT is calculated, which could theoretically achieve several $μ$crab (in the order of 10$^{-14}$ erg cm$^{-2}$ s$^{-1}$) in 0.5-2 keV and several tens of $μ$crab (in the order of 10$^{-13}$ erg cm$^{-2}$ s$^{-1}$) in 2-10 keV for a pointed observation with an exposure of 25 minutes. This sensitivity becomes worse by a factor of $\sim2$ if additional 10% systematic uncertainty of the background subtraction is included.

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