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The nature of the late achromatic bump in GRB 120326A
The long \({\it Swift}\) gamma-ray burst GRB 120326A at redshift \(z=1.798\) exhibited a multi-band light curve with a striking feature: a late-time, long-lasting achromatic rebrightening, rarely seen in such events. Peaking in optical and X-ray bands \(\sim 35\) ks (\(\sim 12.5\) ks in the GRB rest...
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Published in: | arXiv.org 2014-09 |
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | The long \({\it Swift}\) gamma-ray burst GRB 120326A at redshift \(z=1.798\) exhibited a multi-band light curve with a striking feature: a late-time, long-lasting achromatic rebrightening, rarely seen in such events. Peaking in optical and X-ray bands \(\sim 35\) ks (\(\sim 12.5\) ks in the GRB rest frame) after the 70-s GRB prompt burst, the feature brightens nearly two orders of magnitude above the underlying optical power-law decay. Modelling the multiwavelength light curves, we investigate possible causes of the rebrightening in the context of the standard fireball model. We exclude a range of scenarios for the origin of this feature: reverse-shock flash, late-time forward shock peak due to the passage of the maximal synchrotron frequency through the optical band, late central engine optical/X-ray flares, interaction between the expanding blast wave and a density enhancement in the circumburst medium and gravitational microlensing. Instead we conclude that the achromatic rebrightening may be caused by a refreshed forward shock or a geometrical effect. In addition, we identify an additional component after the end of the prompt emission, that shapes the observed X-ray and optical light curves differently, ruling out a single overall emission component to explain the observed early time emission. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.1409.6467 |