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arXiv 1702.01660astro-ph.HEastro-ph.GA
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钱德拉COSMOS遗产巡天:宇宙X射线背景的能谱和对未探测粒子群的限制

The Chandra COSMOS legacy survey: Energy Spectrum of the Cosmic X-ray Background and constraints on undetected populations

Nico Cappelluti, Yanxia Li, Angelo Ricarte, Bhaskar Agarwal, Viola Allevato, Tonima Tasnim Ananna, Marco Ajello, Francesca Civano, Andrea Comastri, Martin Elvis… 展开作者

Nico Cappelluti, Yanxia Li, Angelo Ricarte, Bhaskar Agarwal, Viola Allevato, Tonima Tasnim Ananna, Marco Ajello, Francesca Civano, Andrea Comastri, Martin Elvis, Alexis Finoguenov, Roberto Gilli, Guenther Hasinger, Stefano Marchesi, Priyamvada Natarajan, Fabio Pacucci, E. Treister, C. Megan Urry

摘要:

使用{ \em钱德拉}观测在2.15度$^{2}$ COSMOS遗产领域,我们提出了一个最准确的测量宇宙X射线背景(CXB)光谱的日期在[0.3-7] keV的能量带。CXB有三个不同的组成部分:来自两个银河系碰撞热等离子体在kT $\sim$ 0.27和0.07千电子伏和河外幂律与光子光谱指数$Γ$ =1.45 $\pm{0.02}$的贡献。河外分量的1 keV标准化为10.91 $\pm{0.16}$ keV cm $^{-2}$ s $^{-1}$ sr $^{-1}$ keV $^{-1}$。去除所有X射线探测源,剩余的未分辨CXB通过幂律最佳拟合,归一化为4.18 $\pm{0.26}$ keV cm $^{-2}$ s $^{-1}$ sr $^{-1}$ keV $^{-1}$,光子谱指数$Γ$ =1.57 $\pm{0.10}$。去除暗星系到i $_{AB}\sim$ 27-28留下了硬光谱,$Γ\sim$为1.25,$\sim$为1.37 keV cm $^{-2}$ s $^{-1}$ sr $^{-1}$ keV $^{-1}$。这意味着观测到的CXB的$\sim$ 91%被分解为探测到的X射线源和未探测到的星系。贡献总CXB的$\sim 8-9\%$的未解析来源显示出比解析来源更难且可能更模糊的边缘证据。CXB的另一个$\sim$ 1可以归因于尚未被发现的恒星形成星系和被吸收的活动星系核。根据这些限制,我们研究了一种情况下,早期黑洞完全占非源CXB分数和限制他们的一些性质。为了不超过剩余的CXB和$z\sim$ 6的吸积质量密度,这样的黑洞群必须在康普顿厚度的包络中生长,N $_{H}>$ 1.6 $\times$ 10 $^{25}$ cm $^{-2}$,并在极低金属丰度的环境$(Z_\odot)\sim10^{-3}$中形成。

英文摘要:

Using {\em Chandra} observations in the 2.15 deg$^{2}$ COSMOS legacy field, we present one of the most accurate measurements of the Cosmic X-ray Background (CXB) spectrum to date in the [0.3-7] keV energy band. The CXB has three distinct components: contributions from two Galactic collisional thermal plasmas at kT$\sim$0.27 and 0.07 keV and an extragalactic power-law with photon spectral index $Γ$=1.45$\pm{0.02}$. The 1 keV normalization of the extragalactic component is 10.91$\pm{0.16}$ keV cm$^{-2}$ s$^{-1}$ sr$^{-1}$ keV$^{-1}$. Removing all X-ray detected sources, the remaining unresolved CXB is best-fit by a power-law with normalization 4.18$\pm{0.26}$ keV cm$^{-2}$ s$^{-1}$ sr$^{-1}$ keV$^{-1}$ and photon spectral index $Γ$=1.57$\pm{0.10}$. Removing faint galaxies down to i$_{AB}\sim$27-28 leaves a hard spectrum with $Γ\sim$1.25 and a 1 keV normalization of $\sim$1.37 keV cm$^{-2}$ s$^{-1}$ sr$^{-1}$ keV$^{-1}$. This means that $\sim$91\% of the observed CXB is resolved into detected X-ray sources and undetected galaxies. Unresolved sources that contribute $\sim 8-9\%$ of the total CXB show a marginal evidence of being harder and possibly more obscured than resolved sources. Another $\sim$1\% of the CXB can be attributed to still undetected star forming galaxies and absorbed AGN. According to these limits, we investigate a scenario where early black holes totally account for non source CXB fraction and constrain some of their properties. In order to not exceed the remaining CXB and the $z\sim$6 accreted mass density, such a population of black holes must grow in Compton-thick envelopes with N$_{H}>$1.6$\times$10$^{25}$ cm$^{-2}$ and form in extremely low metallicity environments $(Z_\odot)\sim10^{-3}$.

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