Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/7141
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dc.contributor.authorPaliya, Vaidehi S-
dc.contributor.authorDiltz, Chris-
dc.contributor.authorBottcher, Markus-
dc.contributor.authorStalin, C. S-
dc.contributor.authorBuckley, David-
dc.date.accessioned2020-11-17T14:19:55Z-
dc.date.available2020-11-17T14:19:55Z-
dc.date.issued2016-01-
dc.identifier.citationThe Astrophysical Journal, Vol. 817, No. 1, 61en_US
dc.identifier.issn0004-637X-
dc.identifier.urihttp://prints.iiap.res.in/handle/2248/7141-
dc.descriptionRestricted Access © The American Astronomical Society http://dx.doi.org/10.3847/0004-637X/817/1/61en_US
dc.description.abstractThe blazar 3C 279 exhibited twin γ -ray fl ares of similar intensity in 2013 December and 2014 April. In this work, we present a detailed multi-wavelength analysis of the 2013 December fl aring event. Multi-frequency observations reveal the uncorrelated variability patterns with X-ray and optical – UV fl uxes peaking after the γ -ray maximum. The broadband spectral energy distribution ( SED ) at the peak of the γ -ray activity shows a rising γ -ray spectrum but a declining optical – UV fl ux. This observation along with the detection of uncorrelated variability behavior rules out the one-zone leptonic emission scenario. We, therefore, adopt two independent methodologies to explain the SED: a time-dependent lepto-hadronic modeling and a two-zone leptonic radiative modeling approach. In the lepto-hadronic modeling, a distribution of electrons and protons subjected to a randomly orientated magnetic fi eld produces synchrotron radiation. Electron synchrotron is used to explain the IR to UV emission while proton synchrotron emission is used to explain the high-energy γ -ray emission. A combination of both electron synchrotron self-Compton emission and proton synchrotron emission is used to explain the X-ray spectral break seen during the later stage of the fl are. In the two-zone modeling, we assume a large emission region emitting primarily in IR to X-rays and γ -rays to come primarily from a fast-moving compact emission region. We conclude by noting that within a span of four months, 3C 279 has shown the dominance of a variety of radiative processes over each other and this re fl ects the complexity involved in understanding the physical properties of blazar jets in general.en_US
dc.language.isoenen_US
dc.publisherIOP Publishingen_US
dc.subjectGalaxies: activeen_US
dc.subjectGalaxies: jetsen_US
dc.subjectGamma rays: galaxiesen_US
dc.subjectQuasars: individual (3C 279)en_US
dc.titleA Hard gamma-ray flare from 3C 279 in 2013 Decemberen_US
dc.typeArticleen_US
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