A4 Refereed article in a conference publication

Multiwavelength observations in 2019-2020 of a new very-high-energy γ-ray emitter: the flat spectrum radio quasar QSO B1420+326




AuthorsD'Ammando F., Angioni R., Orienti M., Sitarek J., Nozaki S., Lindfors E., Bonnoli G., Ramazani V.F.

EditorsN/A

Conference nameInternational Cosmic Ray Conference

PublisherSissa Medialab Srl

Publication year2022

JournalPOS Proceedings of Science

Book title 37th International Cosmic Ray Conference (ICRC2021)

Journal name in sourceProceedings of Science

Series titlePOS Proceedings of Science

Volume395

First page 775

ISSN1824-8039

DOIhttps://doi.org/10.22323/1.395.0775

Web address https://pos.sissa.it/395/775

Self-archived copy’s web addresshttps://research.utu.fi/converis/portal/detail/Publication/178548576


Abstract

The flat-spectrum radio quasar QSO B1420+326 underwent an enhanced γ
-ray flux state seen by Fermi-LAT at the turn of 2019/2020. Compared to the low state both the position and luminosity of the two spectral energy distribution peaks changed by at least two orders of magnitude. The high state resulted in the discovery of the very-high-energy (>100 GeV) γ-ray emission from the source by the MAGIC telescopes. The organized multiwavelength campaign allow us to trace the broadband emission of the source through different phases of the flaring activity. The source was observed by 20 instruments in radio, near-infrared, optical, ultra-violet, X-ray and γ-ray bands. We use dedicated optical spectroscopy results to estimate the accretion disc and the dust torus luminosity. The optical spectroscopy shows a prominent FeII bump with flux evolving together with the continuum emission and a MgII line with varying equivalent width. The γ-ray flare was accompanied by a rotation of the optical polarization vector and emission of a new superluminal radio knot. We model spectral energy distributions in different flare phases in the framework of combined synchrotron-self-Compton and external Compton scenario in which the shape of the electron energy distribution is determined from cooling processes.


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