Modelling blazar flaring using a time-dependent fluid jet emission model - an explanation for orphan flares and radio lags

TL;DR

This paper introduces a time-dependent fluid jet emission model for blazars that explains multiwavelength flares, radio lags, and orphan flares, successfully fitting observed spectra and lightcurves.

Contribution

It is the first to model optically thick radio flares in blazars and explains their delayed response and various flare types with a comprehensive inhomogeneous jet approach.

Findings

Radio flares lag behind optical emissions by months to decades.

The model predicts symmetric and extended flares based on flare duration.

Successfully fits multiwavelength spectra and lightcurves of PKS1502+106.

Abstract

Blazar jets are renowned for their rapid violent variability and multiwavelength flares, however, the physical processes responsible for these flares are not well understood. In this paper we develop a time-dependent inhomogeneous fluid jet emission model for blazars. We model optically thick radio flares for the first time and show that they are delayed with respect to the prompt optically thin emission by ~ months to decades, with a lag that increases with the jet power and observed wavelength. This lag is caused by a combination of the travel time of the flaring plasma to the optically thin radio emitting sections of the jet and the slow rise time of the radio flare. We predict two types of flares: symmetric flares - with the same rise and decay time, which occur for flares whose duration is shorter than both the radiative lifetime and the geometric path-length delay timescale; extended flares - whose luminosity tracks the power of particle acceleration in the flare, which occur for flares with a duration longer than both the radiative lifetime and geometric delay. Our model naturally produces orphan X-ray and $\gamma$-ray flares. These are caused by flares which are only observable above the quiescent jet emission in a narrow band of frequencies. Our model is able to successfully fit to the observed multiwavelength flaring spectra and lightcurves of PKS1502+106 across all wavelengths, using a transient flaring front located within the broad-line region.