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<i>NuSTAR</i>AND MULTIFREQUENCY STUDY OF THE TWO HIGH-REDSHIFT BLAZARS S5 0836+710 AND PKS 2149–306

G. TagliaferriINAF—Osservatorio Astronomico di Brera, via E. Bianchi 46, I-23807 Merate, Italy; [email protected]G. GhiselliniINAF—Osservatorio Astronomico di Brera, via E. Bianchi 46, I-23807 Merate, Italy; [email protected]M. PerriASI—Science Data Center, via del Politecnico, I-00133 Rome, ItalyM. HayashidaInstitute for Cosmic Ray Research, University of Tokyo, 5-1-5 Kashiwanoha, Kashiwa, Chiba, 277-8582, JapanMislav BalokovićCahill Center for Astrophysics, California Institute of Technology, 1200 East California Boulevard, Pasadena, CA 91125, USAS. CovinoINAF—Osservatorio Astronomico di Brera, via E. Bianchi 46, I-23807 Merate, Italy; [email protected]P. GiommiASI—Science Data Center, via del Politecnico, I-00133 Rome, ItalyG. M. MadejskiKavli Institute for Particle Astrophysics and Cosmology, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USASimonetta PuccettiASI—Science Data Center, via del Politecnico, I-00133 Rome, ItalyT. SbarratoDipartimento di Fisica G. Occhialini, Università di Milano Bicocca, Piazza della Scienza 3, I-20126 Milano, ItalySteven E. BoggsSpace Sciences Laboratory, University of California, Berkeley, CA 94720, USAJ. ChiangKavli Institute for Particle Astrophysics and Cosmology, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USAFinn E. ChristensenDTU Space—National Space Institute, Technical University of Denmark, Elektrovej 327, DK-2800 Lyngby, DenmarkWilliam W. CraigDTU Space—National Space Institute, Technical University of Denmark, Elektrovej 327, DK-2800 Lyngby, DenmarkCharles J. HaileyColumbia Astrophysics Laboratory, Columbia University, New York, NY 10027, USAFiona A. HarrisonCahill Center for Astrophysics, California Institute of Technology, 1200 East California Boulevard, Pasadena, CA 91125, USADaniel SternJet Propulsion Laboratory, California Institute of Technology, Pasadena, CA 91109, USAW. W. ZhangNASA Goddard Space Flight Center, Greenbelt, MD 20771, USA
2015en
ABI

Abstract

Powerful blazars are flat-spectrum radio quasars whose emission is dominated by a Compton component peaking between a few hundred keV and a few hundred MeV. We observed two bright blazars, PKS 2149–306 at redshift z = 2.345 and S5 0836+710 at z = 2.172, in the hard X-ray band with the Nuclear Spectroscopic Telescope Array satellite. Simultaneous soft-X-rays and UV–optical observations were performed with the Swift satellite, while near-infrared (near-IR) data were obtained with the Rapid Eye Mount telescope. To study their variability, we repeated these observations for both sources on a timescale of a few months. While no fast variability was detected during a single observation, both sources were variable in the X-ray band, up to 50%, between the two observations, with larger variability at higher energies. No variability was detected in the optical/NIR band. These data, together with Fermi-Large Area Telescope, Wide-field Infrared Survey Explorer, and other literature data, are then used to study the overall spectral energy distributions (SEDs) of these blazars. Although the jet nonthermal emission dominates the SED, it leaves the UV band unhidden, allowing us to detect the thermal emission of the disk and to estimate the black hole mass. The nonthermal emission is well reproduced by a one-zone leptonic model by the synchrotron, self-Compton, and external Compton processes. Our data are better reproduced if we assume that the location of the dissipation region of the jet, R_(diss), is in between the torus and the broad-line region. The observed variability is explained by changing a minimum number of model parameters by a very small amount.

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