Evidence for Shocks as the Origin of Gamma-Ray Flares in Blazars

We present centimeter-band total flux density and linear polarization light curves illustrating the signature of shocks during radio band outbursts associated in time with -ray flares detected by the Fermi LAT. The general characteristics of the spectral evolution during these events is well-explained by new radiative transfer simulations incorporating propagating oblique shocks and assuming an initially turbulent magnetic field. This finding supports the idea that oblique shocks in the jet are a viable explanation for activity from the radio to the -ray band in at least some -ray flares. 1. Overview Since the mid-1980s, the leading paradigm for the production of flares in AGN in the radio-to-optical bands has been shocks which propagate down the relativistic jets of these sources [1, 2]; hydrodynamical simulations have demonstrated that these structures develop naturally within the jets [3], making this scenario a plausible explanation. In contrast, the location and nature of the emission site giving rise to the GeV -ray flares, detected first by EGRET and now by the Fermi LAT, have remained contentious issues. While both a site near to the central engine and a location in the parsec scale jet have been discussed in the literature, mounting evidence based on correlated broadband activity (including high resolution VLBA imaging of the inner jet) supports a location within the jet at a site near to the millimeter-band radio core (e.g. [4] and references therein). This result supports a direct relation between the flaring in the radio and in the -ray spectral bands and the production of the flaring by the same disturbance. The emitting region itself could take the form of a shock (standing or propagating) or a ‘blob’ with a chaotic magnetic field where turbulence accelerates the high energy electrons. The propagating shock scenario, used successfully for the radio band data has now been proposed as a possible explanation for the -ray flares in some recent studies, e.g. [5]. However, this hypothesis has not been rigorously tested. Radiative transfer modeling carried out in the mid-to-late 1980s and early 1990s incorporating transverse shocks successfully reproduced the spectral evolution of the total flux density and linear polarization in centimeter-band monitoring data during a few carefully selected radio band events. However, the transverse shock models failed to match the variability in later events in the same sources; there the swings in electric vector position

[1]  Paul S. Smith,et al.  ON THE LOCATION OF THE γ-RAY OUTBURST EMISSION IN THE BL LACERTAE OBJECT AO 0235+164 THROUGH OBSERVATIONS ACROSS THE ELECTROMAGNETIC SPECTRUM , 2011, 1105.0549.

[2]  M. Aller,et al.  OBLIQUE SHOCKS AS THE ORIGIN OF RADIO TO GAMMA-RAY VARIABILITY IN ACTIVE GALACTIC NUCLEI , 2011, 1104.4256.

[3]  Paul S. Smith,et al.  LOCATION OF γ-RAY FLARE EMISSION IN THE JET OF THE BL LACERTAE OBJECT OJ287 MORE THAN 14 pc FROM THE CENTRAL ENGINE , 2010, 1011.6454.

[4]  J. Chiang,et al.  GAMMA-RAY LIGHT CURVES AND VARIABILITY OF BRIGHT FERMI-DETECTED BLAZARS , 2010, 1004.0348.

[5]  Paul S. Smith,et al.  PROBING THE INNER JET OF THE QUASAR PKS 1510−089 WITH MULTI-WAVEBAND MONITORING DURING STRONG GAMMA-RAY ACTIVITY , 2010, 1001.2574.

[6]  M. Cohen,et al.  MOJAVE: MONITORING OF JETS IN ACTIVE GALACTIC NUCLEI WITH VLBA EXPERIMENTS. XI. SPECTRAL DISTRIBUTIONS , 2014, 1404.0014.

[7]  P. Hughes The Origin of Complex Behavior of Linearly Polarized Components in Parsec-Scale Jets , 2004, astro-ph/0411725.

[8]  M. Aller,et al.  Synchrotron emission from shocked relativistic jets. III. Models for the centimeter wave band quiescent and burst emission from 3C 279 and OT 081 , 1991 .

[9]  Walter Kieran Gear,et al.  Models for high-frequency radio outbursts in extragalactic sources, with application to the early 1983 millimeter-to-infrared flare of 3C 273. , 1985 .

[10]  M. Aller,et al.  Polarized Radio Outbursts in Bl-Lacertae - Part Two - the Flux and Polarization of a Piston-Driven Shock , 1985 .