posted on 2018-08-16, 08:28authored byA. Del Moro, D. M. Alexander, J. A. Aird, F. E. Bauer, F. Civano, J. R. Mullaney, D. R. Ballantyne, W. N. Brandt, A. Comastri, P. Gandhi, F. A. Harrison, G. B. Lansbury, L. Lanz, B. Luo, S. Marchesi, S. Puccetti, C. Ricci, C. Saez, D. Stern, E. Treister, L. Zappacosta
We present a study of the average X-ray spectral properties of the sources detected by the NuSTAR extragalactic
survey, comprising observations of the Extended Chandra Deep Field South (E-CDFS), Extended Groth Strip
(EGS), and the Cosmic Evolution Survey (COSMOS). The sample includes 182 NuSTAR sources (64 detected at
8–24 keV), with 3–24 keV fluxes ranging between f(3-24 keV) ≈ 10^-14 – and 6 × 10^−13 erg cm^−2 s^−1
(f(8–24 keV) ≈ 3 x 10^-14 - 3 x 10^-13 erg cm^−2 s^−1) and redshifts in the range of z = 0.04 - 3.21. We produce
composite spectra from the Chandra + NuSTAR data (E ≈ 2- 40 keV, rest frame) for all the sources with redshift
identifications (95%) and investigate the intrinsic, average spectra of the sources, divided into broad-line (BL) and
narrow-line (NL) active galactic nuclei (AGNs), and also in different bins of X-ray column density and luminosity.
The average power-law photon index for the whole sample is Γ = 1.65^+0.03,-3.21 flatter than the Γ ≈ 1.8 typically
found for AGNs. While the spectral slope of BL and X-ray unabsorbed AGNs is consistent with the typical values
(Γ = 1.79^+0.01,-0.01) a significant flattening is seen in NL AGNs and heavily absorbed sources (Γ = 1.60^+0.08,-0.05 and 1.38^+0.12,-0.12, respectively), likely due to the effect of absorption and to the contribution from the Compton
reflection component to the high-energy flux (E > 10 keV). We find that the typical reflection fraction in our
spectra is R ≈ 0.5 (for Γ = 1.8), with a tentative indication of an increase of the reflection strength with X-ray
column density. While there is no significant evidence for a dependence of the photon index on X-ray luminosity in
our sample, we find that R decreases with luminosity, with relatively high levels of reflection (R ≈ 1.2) for
L(10-40 keV) < 10^44 erg s^−1 and R ≈ 0.3 for L(10-40 keV) > 10^44 erg s^−1 AGNs, assuming a fixed spectral slope
of Γ = 1.8.
Funding
A.D.M. thanks the
financial support from the Max Plank Society and the UK
Science and Technology Facilities Council (STFC, ST/
L00075X/1, A.D.M. and D.M.A.; ST/K501979/1, G.B.L.).
F.E.B. and E.T. acknowledge support from CONICYT-Chile
(Basal-CATA PFB-06/2007, “EMBIGGEN” Anillo
ACT1101, FONDECYT Regular 1141218 [F.E.B.] and
1160999 [E.T.]); F.E.B. also thanks the Ministry of Economy,
Development, and Tourism’s Millennium Science Initiative
through grant IC120009, awarded to the Millennium Institute
of Astrophysics (MAS). P.G. thanks the STFC for support
(ST/J003697/2). W.N.B. acknowledges support from the
Caltech NuSTAR subcontract 44A-1092750 and NASA ADP
grant NNX10AC99G. A.C. and L.Z. acknowledge support
from the ASI/INAF grant I/037/12/0 011/13.
This work was supported under NASA contract no.
NNG08FD60C and made use of data from the NuSTAR
mission, a project led by the California Institute of Technology,
managed by the Jet Propulsion Laboratory, and funded by the
National Aeronautics and Space Administration. We thank the
NuSTAR Operations, Software, and Calibration teams for
support with the execution and analysis of these observations.
This research has made use of the NuSTAR Data Analysis
Software (NuSTARDAS) jointly developed by the ASI Science
Data Center (ASDC, Italy) and the California Institute of
Technology (USA).
History
Citation
Astrophysical Journal, 2017, 849, pp. 57-57
Author affiliation
/Organisation/COLLEGE OF SCIENCE AND ENGINEERING/Department of Physics and Astronomy