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http://hdl.handle.net/2248/7141
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DC Field | Value | Language |
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dc.contributor.author | Paliya, Vaidehi S | - |
dc.contributor.author | Diltz, Chris | - |
dc.contributor.author | Bottcher, Markus | - |
dc.contributor.author | Stalin, C. S | - |
dc.contributor.author | Buckley, David | - |
dc.date.accessioned | 2020-11-17T14:19:55Z | - |
dc.date.available | 2020-11-17T14:19:55Z | - |
dc.date.issued | 2016-01 | - |
dc.identifier.citation | The Astrophysical Journal, Vol. 817, No. 1, 61 | en_US |
dc.identifier.issn | 0004-637X | - |
dc.identifier.uri | http://prints.iiap.res.in/handle/2248/7141 | - |
dc.description | Restricted Access © The American Astronomical Society http://dx.doi.org/10.3847/0004-637X/817/1/61 | en_US |
dc.description.abstract | The 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.iso | en | en_US |
dc.publisher | IOP Publishing | en_US |
dc.subject | Galaxies: active | en_US |
dc.subject | Galaxies: jets | en_US |
dc.subject | Gamma rays: galaxies | en_US |
dc.subject | Quasars: individual (3C 279) | en_US |
dc.title | A Hard gamma-ray flare from 3C 279 in 2013 December | en_US |
dc.type | Article | en_US |
Appears in Collections: | IIAP Publications |
Files in This Item:
File | Description | Size | Format | |
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A Hard gamma-ray flare from 3C 279 in 2013 December.pdf | Restricted Access | 1.14 MB | Adobe PDF | View/Open |
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