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25 April 2024
 
  » arxiv » 1107.2926

 Article overview



Identification of gamma-ray emission from 3C345 and NRAO512
F.K. Schinzel ; K.V. Sokolovsky ; F. D'Ammando ; T.H. Burnett ; W. Max-Moerbeck ; C.C. Cheung ; S.J. Fegan ; J.M. Casandjian ; L.C. Reyes ; M. Villata ; C.M. Raiteri ; I. Agudo ; O.J.A. Bravo Calle ; D. Carosati ; R. Casas ; J.L. Gomez ; M.A. Gurwell ; H.Y. Hsiao ; S.G. Jorstad ; G. Kimeridze ; T.S. Konstantinova ; E.N. Kopatskaya ; E. Koptelova ; O.M. Kurtanidze ; S.O. Kurtanidze ; V.M. Larionov ; E.G. Larionova ; L.V. Larionova ; A.P. Marscher ; D.A. Morozova ; M.G. Nikolashvili ; M. Roca-Sogorb ; J.A. Ros ; L.A. Sigua ; O. Spiridonova ; I.S. Troitsky ; V.V. Vlasyuk ; A.P. Lobanov ; J.A. Zensus ;
Date 14 Jul 2011
AbstractFor more than 15 years, since the days of the Energetic Gamma-Ray Experiment Telescope (EGRET) on board the Compton Gamma-Ray Observatory (CGRO; 1991-2000), it has remained an open question why the prominent blazar 3C 345 was not reliably detected at gamma-ray energies <=20 MeV. Recently a bright gamma-ray source (0FGL J1641.4+3939/1FGL J1642.5+3947), potentially associated with 3C 345, was detected by the Large Area Telescope (LAT) on Fermi. Multiwavelength observations from radio bands to X-rays (mainly GASP-WEBT and Swift) of possible counterparts (3C 345, NRAO 512, B3 1640+396) were combined with 20 months of Fermi-LAT monitoring data (August 2008 - April 2010) to associate and identify the dominating gamma-ray emitting counterpart of 1FGL J1642.5+3947. The source 3C 345 is identified as the main contributor for this gamma-ray emitting region. However, after November 2009 (15 months), a significant excess of photons from the nearby quasar NRAO 512 started to contribute and thereafter was detected with increasing gamma-ray activity, possibly adding flux to 1FGL J1642.5+3947. For the same time period and during the summer of 2010, an increase of radio, optical and X-ray activity of NRAO 512 was observed. No gamma-ray emission from B3 1640+396 was detected.
Source arXiv, 1107.2926
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