Estimate of the background and sensitivity of the follow-up X-ray telescope onboard Einstein Probe

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 invest...

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Published inAstroparticle physics Vol. 137; p. 102668
Main Authors Zhang, Juan, Qi, Liqiang, Yang, Yanji, Wang, Juan, Liu, Yuan, Cui, Weiwei, Zhao, Donghua, Jia, Shumei, Li, Tianming, Chen, Tianxiang, Li, Gang, Zhao, Xiaofan, Chen, Yong, Liu, Huaqiu, Bao, Congying, Guan, Ju, Song, Liming, Yuan, Weimin
Format Journal Article
LanguageEnglish
Published Elsevier B.V 01.04.2022
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Summary: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 0.5–10keV, which is mainly induced by cosmic ray protons and cosmic photon background, corresponds to a level of ∼3.1×10−2 countss−1keV−1 in the imaging area of the focal plane detector (FPD), i.e. 3.7 × 10−3 countss−1keV−1cm−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 2keV. Based on the simulated background level within the focal spot (a 30′′-radius circle), the sensitivity of FXT is calculated, which could theoretically achieve several μcrab (in the order of 10−14ergcm−2s−1) in 0.5–2keV and several tens of μcrab (in the order of 10−13ergcm−2s−1) in 2–10keV for a pointed observation with an exposure of 25 min. This sensitivity becomes worse by a factor of ∼2 if additional 10% systematic uncertainty of the background subtraction is included.
ISSN:0927-6505
1873-2852
DOI:10.1016/j.astropartphys.2021.102668