posted on 2018-08-10, 11:43authored byL. Zappacosta, A. Comastri, F. Civano, S. Puccetti, F. Fiore, J. Aird, A. Del Moro, G. B. Lansbury, G. Lanzuisi, A. Goulding, J. R. Mullaney, D. Stern, M. Ajello, D. M. Alexander, D. R. Ballantyne, F. E. Bauer, W. N. Brandt, C-T. J. Chen, D. Farrah, F. A. Harrison, P. Gandhi, L. Lanz, A. Masini, S. Marchesi, C. Ricci, E. Treister
We discuss the spectral analysis of a sample of 63 active galactic nuclei (AGN) detected above a limiting flux
of S(8-24 keV) = 7 x 10^-14 erg s^-1 cm^-2 in the multi-tiered NuSTAR extragalactic survey program. The sources
span a redshift range z = 0 - 2.1 (median = 0.58). The spectral analysis is performed over the broad 0.5–24 keV
energy range, combining NuSTAR with Chandra and/or XMM-Newton data and employing empirical and
physically motivated models. This constitutes the largest sample of AGN selected at >10 keV to be
homogeneously spectrally analyzed at these flux levels. We study the distribution of spectral parameters such
as photon index, column density (NH), reflection parameter (R), and 10–40 keV luminosity (LX). Heavily obscured
(log[NH/cm^-2] >= 23) and Compton-thick (CT; log[NH/cm^-2] >= 24 ) AGN constitute ∼25% (15–17 sources) and
∼2–3% (1–2 sources) of the sample, respectively. The observed NH distribution agrees fairly well with predictions
of cosmic X-ray background population-synthesis models (CXBPSM). We estimate the intrinsic fraction of AGN
as a function of NH, accounting for the bias against obscured AGN in a flux-selected sample. The fraction of CT
AGN relative to log[NH/cm^-2] = 20-24 AGN is poorly constrained, formally in the range 2–56% (90% upper
limit of 66%). We derived a fraction ( fabs) of obscured AGN (log[NH/cm^-2] = 20-24 ) as a function of LX in
agreement with CXBPSM and previous z < 1 X-ray determinations. Furthermore, fabs at z = 0.1-0.5 and
log(LX/erg s ^-1) ~~ 43.6-44.3 agrees with observational measurements/trends obtained over larger redshift
intervals. We report a significant anti-correlation of R with LX (confirmed by our companion paper on stacked
spectra) with considerable scatter around the median R values.
Funding
We thank Johannes Buchner and Yoshihiro Ueda for providing machine-readable results on the absorbed fractions. L.Z. thanks R. Gilli, F. Nicastro, E. Piconcelli, R. Valiante, F. Vito, and D. Burlon for useful discussions. L.Z., A.C., F.F., G.L., and A.M. acknowledge financial support under ASI/INAF contract I/037/12/0. A.C. acknowledges the Caltech Kingsley fellowship program. G.L. acknowledges financial support from the CIG grant eEASY No. 321913. F.E.B. acknowledges support from CONICYT-Chile (Basal-CATA PFB-06/2007, FONDECYT Regular 1141218), the Ministry of Economy, Development, and Tourism's Millennium Science Initiative through grant IC120009, awarded to The Millennium Institute of Astrophysics, MAS. This work was supported under NASA Contract 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 NASA. 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, 2018, 854, pp. 33-33
Author affiliation
/Organisation/COLLEGE OF SCIENCE AND ENGINEERING/Department of Physics and Astronomy