Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/8367
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dc.contributor.authorRajput, Bhoomika-
dc.contributor.authorMandal, Amit Kumar-
dc.contributor.authorPandey, Ashwani-
dc.contributor.authorStalin, C. S-
dc.contributor.authorMax-Moerbeck, Walter-
dc.contributor.authorMathew, Blesson-
dc.date.accessioned2024-03-04T09:48:06Z-
dc.date.available2024-03-04T09:48:06Z-
dc.date.issued2024-02-
dc.identifier.citationMonthly Notices of the Royal Astronomical Society, Vol. 527, No. 4, pp.11900-11914en_US
dc.identifier.issn1365-2966-
dc.identifier.urihttp://hdl.handle.net/2248/8367-
dc.descriptionOpen Accessen_US
dc.descriptionThis is an Open Access article distributed under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted reuse, distribution, and reproduction in any medium, provided the original work is properly cited.-
dc.description.abstractThe correlation between optical and γ-ray flux variations in blazars reveals a complex behaviour. In this study, we present our analysis of the connection between changes in optical and γ-ray emissions in the blazar Ton 599 over a span of approximately 15 years, from August 2008 to March 2023. Ton 599 reached its highest flux state across the entire electromagnetic spectrum during the second week of January 2023. To investigate the connection between changes in optical and γ-ray flux, we have designated five specific time periods, labeled as epochs A, B, C, D, and E. During periods B, C, D, and E, the source exhibited optical flares, while it was in its quiescent state during period A. The γ-ray counterparts to these optical flares are present during periods B, C, and E, however during period D, the γ-ray counterpart is either weak or absent. We conducted a broadband spectral energy distribution (SED) fitting by employing a one-zone leptonic emission model for these epochs. The SED analysis unveiled that the optical-UV emission primarily emanated from the accretion disk in quiescent period A, whereas synchrotron radiation from the jet dominated during periods B, C, D, and E. Diverse correlated patterns in the variations of optical and γ-ray emissions, like correlated optical and γ-ray flares, could be accounted for by changes in factors such as the magnetic field, bulk Lorentz factor, and electron density. On the other hand, an orphan optical flare could result from increased magnetic field and bulk Lorentz factor.en_US
dc.language.isoenen_US
dc.publisherPublished by Oxford University Press on behalf of Royal Astronomical Societyen_US
dc.relation.urihttps://doi.org/10.1093/mnras/stad4003-
dc.rights© 2023 The Author(s)-
dc.subjectGalaxies: activeen_US
dc.subjectGalaxies: jetsen_US
dc.subjectGalaxies: nucleien_US
dc.subjectGamma-rays: galaxiesen_US
dc.titleInvestigation of the correlation between optical and γ-ray flux variation in the blazar Ton 599en_US
dc.typeArticleen_US
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