The Chandra COSMOS Legacy Survey: Energy Spectrum of the Cosmic X-Ray Background and Constraints on Undetected Populations
Journal Article
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· Astrophysical Journal
- Yale Center for Astronomy and Astrophysics, P.O. Box 208121, New Haven, CT 06520 (United States)
- Department of Astronomy, Yale University, P.O. Box 208101, New Haven, CT 06520 (United States)
- Department of Physics, University of Helsinki, Gustaf Hällströmin katu 2a, FI-00014 Helsinki (Finland)
- Department of Physics and Astronomy, Clemson University, Kinard Lab of Physics, Clemson, SC 29634-0978 (United States)
- Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138 (United States)
- INAF-Osservatorio Astronomico di Bologna, via Ranzani 1, I-40127 Bologna (Italy)
- Institute for Astronomy, 2680 Woodlawn Drive, University of Hawaii, Honolulu, HI 96822 (United States)
- Department of Physics, Yale University, P.O. Box 208121, New Haven, CT 06520 (United States)
- Instituto de Astrofisica, Facultad de Fisica, Pontificia Universidad Catolica de Chile, Casilla 306, Santiago 22 (Chile)
Using Chandra observations in the 2.15 deg{sup 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 ∼ 0.27 and 0.07 keV and an extragalactic power law with a photon spectral index Γ = 1.45 ± 0.02. The 1 keV normalization of the extragalactic component is 10.91 ± 0.16 keV cm{sup −2} s{sup −1} sr{sup −1} keV{sup −1}. Removing all X-ray-detected sources, the remaining unresolved CXB is best fit by a power law with normalization 4.18 ± 0.26 keV cm{sup −2} s{sup −1} sr{sup −1} keV{sup −1} and photon spectral index Γ = 1.57 ± 0.10. Removing faint galaxies down to i{sub AB}∼27--28 leaves a hard spectrum with Γ∼1.25 and a 1 keV normalization of ∼1.37 keV cm{sup −2} s{sup −1} sr{sup −1} keV{sup −1}. This means that ∼91% of the observed CXB is resolved into detected X-ray sources and undetected galaxies. Unresolved sources that contribute ∼8%–9% of the total CXB show marginal evidence of being harder and possibly more obscured than resolved sources. Another ∼1% of the CXB can be attributed to still undetected star-forming galaxies and absorbed active galactic nuclei. 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∼6 accreted mass density, such a population of black holes must grow in Compton-thick envelopes with N{sub H} > 1.6 × 10{sup 25} cm{sup −2} and form in extremely low-metallicity environments (Z{sub ⊙})∼10{sup −3}.
- OSTI ID:
- 22869290
- Journal Information:
- Astrophysical Journal, Journal Name: Astrophysical Journal Journal Issue: 1 Vol. 837; ISSN ASJOAB; ISSN 0004-637X
- Country of Publication:
- United States
- Language:
- English
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