Origin of the broadband emission from the transition blazar B2 1308+326

TL;DR

This study investigates the multi-wavelength emission and variability of the transition blazar B2 1308+326 over 14 years, revealing a flare, spectral changes, and a possible transition from LSP to ISP driven by Doppler factor variations.

Contribution

It provides the first detailed analysis of the broadband SEDs during different flux states of B2 1308+326, linking spectral changes to jet dynamics and blazar subclass transition.

Findings

Detected a major flare in 2022 with highest gamma-ray flux.

Observed a shift in synchrotron peak frequency from LSP to ISP.

Modelled SEDs with consistent parameters except for Doppler factor.

Abstract

Transition blazars exhibit a shift from one subclass to the next during different flux states. It is therefore crucial to study them to understand the underlying physics of blazars. We probe the origin of the multi-wavelength emission from the transition blazar B2 1308+326 using 14-year-long gamma-ray light curve from Fermi and the quasi-simultaneous data from Swift. We used the Bayesian block algorithm to identify epochs of flaring and quiescent flux states and modelled the broadband SEDs for these epochs. We employed the one-zone leptonic model in which the synchrotron emission causes the low-energy part of the SED and the high-energy part is produced by the IC emission of external seed photons. We also investigated its multi-band variability properties and gamma-ray flux distribution, and the correlation between optical and gamma-ray emissions. We observed a historically bright flare from B2 1308+326 across the optical to gamma-ray bands in June and July 2022. The highest daily averaged gamma-ray flux was (14.24$\pm$2.36) $\times$ 10$^{-7}$ ph cm$^{-2}$ s$^{-1}$ and was detected on 1 July 2022. The gamma-ray flux distribution was found to be log-normal. The optical and gamma-ray emissions are well correlated with zero time lag. The synchrotron peak frequency changes from $\sim 8 \times$ 10$^{12}$ Hz (in the quiescent state) to $\sim 6 \times$ 10$^{14}$ Hz (in the flaring state), together with a decrease in the Compton dominance providing a hint that the source transitions from a LSP to an ISP. The SEDs for these two states are well-fitted by one-zone leptonic models. The parameters in the model fits are essentially consistent between both SEDs, except for the Doppler-beaming factor, which changes from $\sim$15.6 to $\sim$27 during the transition. An increase in the Doppler factor might cause both the flare and the transition of B2 1308+326 from an LSP to an ISP blazar.