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




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

ToimittajaN/A

Konferenssin vakiintunut nimiInternational Cosmic Ray Conference

KustantajaSissa Medialab Srl

Julkaisuvuosi2022

JournalPOS Proceedings of Science

Kokoomateoksen nimi37th International Cosmic Ray Conference (ICRC2021)

Tietokannassa oleva lehden nimiProceedings of Science

Sarjan nimiPOS Proceedings of Science

Vuosikerta395

Aloitussivu775

ISSN1824-8039

DOIhttps://doi.org/10.22323/1.395.0775

Verkko-osoitehttps://pos.sissa.it/395/775

Rinnakkaistallenteen osoitehttps://research.utu.fi/converis/portal/detail/Publication/178548576


Tiivistelmä

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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Last updated on 2025-27-03 at 21:57