# Revealing the Nature and Location of High Energy Emission in the Candidate Binary SMBH System OJ 287

## TL;DR

This study investigates the multi-wavelength variability and high-energy emission mechanisms in the binary SMBH candidate OJ 287, revealing new features and the origin of gamma-ray emissions during different activity phases.

## Contribution

It provides the first detailed analysis of OJ 287's broadband spectral energy distributions during recent flares, identifying emission regions and mechanisms, including a two-zone model for VHE gamma-ray production.

## Key findings

- Detection of VHE gamma-ray emission during the 2016-2017 phase.
- Identification of a thermal accretion disk component in the SED.
- Evidence for a two-zone emission model at different scales.

## Abstract

The latest flare of the regular $\sim$ 12 years quasi-periodic optical outbursts in the binary SMBH candidate system OJ 287 occurred in December 2015. Following this, the source has exhibited enhanced multi-wavelength (MW) variability in spectral, temporal and polarization domains with new features never seen before. Our MW investigation show that the overall MW variability can be divided into two-phase, (i) November 2015 -- May 2016 with variability from near-infrared (NIR) to Fermi-LAT $\rm \gamma$-ray energies (0.1 -- 300 GeV), and (ii) September 2016 -- July 2017 with intense NIR to X-ray variability but without any activity in the Fermi-LAT band, and the very first detection at very high energies (VHEs, E $>$ 100 GeV) by VERITAS. The broadband SEDs during the first phase show a thermal bump in the NIR-optical region and a hardening in the $\rm \gamma$-ray spectra with a shift in its peak. The thermal bump like feature is consistent with the description of the standard accretion-disk associated with the primary SMBH of mass $\sim 1.8\times10^{10} M_\odot$ while the $\rm \gamma$-ray emission can be naturally reproduced by inverse Compton scattering of photons from the broad line region which has been seen during the close encounter duration of the binary SMBHs, thereby suggesting a sub-parsec scale origin. The SEDs during the second phase (VHE detection) is a mixture of typical OJ 287 SED with hardened $\rm \gamma$-ray spectra and an HBL SED and can be explained in a two-zone model, one located at sub-parsec scales and other at parsec scales. During both the phases, the MW variability is simultaneous and almost always accompanied by changes in the polarization properties, exhibiting random and systematic variations, suggesting a strong role of magnetic field and turbulence.